An electrochemical biosensor based on DNA tetrahedron nanoprobe for sensitive and selective detection of doxorubicin

Doxorubicin (DOX) is a clinical chemotherapeutic drug and patients usually suffer from dose-dependent cytotoxic and side effects during chemotherapy process with DOX. Therefore, developing a reliable strategy for DOX analysis in biological samples for dosage guidance during chemotherapy process is of great significance. Herein, a sensitive and selective electrochemical biosensor for DOX detection was designed based on gold nanoparticles (AuNPs) and DNA tetrahedron (TDN) nanoprobe bifunctional glassy carbon electrode that could detect DOX in human serum and cell lysate samples. AuNPs not only could enhance electron transfer efficiency and detection sensitivity, but also could improve the biocompatibility of electrode. TDN nanoprobes were employed as specific DOX bind sites that could bind abundant DOX through intercalative characteristics to contribute to sensitive and selective detection. Under the optimal conditions, the proposed TDN nanoprobes-based DOX biosensor exhibited a wide linear range that ranged from 1.0 nM to 50 μM and a low detection limit that was 0.3 nM. Moreover, the proposed DOX biosensor displayed nice selectivity, reproducibility and stability, and was successfully applied for DOX detection in human serum and cell lysate samples. These promising results maybe pave a way for DOX dosage guidance and therapeutic efficacy optimization in clinic.

The FAK/occludin/ZO-1 complex is critical for cadmium-induced testicular damage by disruption of the integrity of the blood-testis barrier in chickens

Cadmium (Cd) is a well-known testis toxicant. The blood-testis barrier (BTB) is a crucial component of the testis. Cd can disrupt the integrity of the BTB and reproductive function. However, the mechanism of Cd-induced disruption of BTB and testicular damage has not been fully elucidated. Here, our study investigates the effects of Cd on BTB integrity and testicular dysfunction. 80 (aged 1 day) Hy-Line white variety chickens were randomly designed into 4 groups and treated for 90 days, as follows: control group (essential diet), 35 Cd, 70 Cd and 140 Cd groups (35, 70 and 140 mg/kg Cd). The results found that Cd exposure diminished volume of the testes and induced histopathological lesions in the testes. Exposure to Cd induced an inflammatory response, disrupted the structure and function of the FAK/occludin/ZO-1 protein complex and disrupted the tight junction and adherens junction in the BTB. In addition, Cd exposure reduced the expression of steroid-related proteins and inhibited testosterone synthesis. Taken together, these data elucidate that Cd disrupts the integrity of the BTB and further inhibits spermatogenesis by dissociating the FAK/occludin/ZO-1 complex, which provides a basis for further investigation into the mechanisms of Cd-induced impairment of male reproductive function and pharmacological protection.

Large-scale array for radio astronomy on the farside (LARAF)

At the Royal Society meeting in 2023, we have mainly presented our lunar orbit array concept called DSL, and also briefly introduced a concept of a lunar surface array, LARAF. As the DSL concept had been presented before, in this article, we introduce the LARAF. We propose to build an array in the far side of the Moon, with a master station which handles the data collection and processing, and 20 stations with maximum baseline of 10 km. Each station consists of 12 membrane antenna units, and the stations are connected to the master station by power line and optical fibre. The array will make interferometric observation in the 0.1-50 MHz band during the lunar night, powered by regenerated fuel cells. The whole array can be carried to the lunar surface with a heavy rocket mission, and deployed with a rover in eight months. Such an array would be an important step in the long-term development of lunar-based ultralong wavelength radio astronomy. It has a sufficiently high sensitivity to observe many radio sources in the sky, though still short of the dark age fluctuations. We discuss the possible options in the power supply, data communication, deployment etc. This article is part of a discussion meeting issue 'Astronomy from the Moon: the next decades (part 2)'.

Research on aquatic microcosm: Bibliometric analysis, toxicity comparison and model prediction

Recently, aquatic microcosms have attracted considerable attention because they can be used to simulate natural aquatic ecosystems. First, to evaluate the development of trends, hotspots, and national cooperation networks in the field, bibliometric analysis was performed based on 1841 articles on aquatic microcosm (1962-2022). The results of the bibliometric analysis can be categorized as follows: (1) Aquatic microcosm research can be summarized in two sections, with the first part focusing on the ecological processes and services of aquatic ecosystems, and the second focusing on the toxicity and degradation of pollutants. (2) The United States (number of publications: 541, proportion: 29.5%) and China (248, 13.5%) are the two most active countries. Second, to determine whether there is a difference between single-species and microcosm tests, that is, to perform different-tier assessments, the recommended aquatic safety thresholds in risk assessment [i.e., the community-level no effect concentration (NOECcommunity), hazardous concentrations for 5% of species (HC5) and predicted no effect concentration (PNEC)] were compared based on these tests. There was a significant difference between the NOECcommunity and HC5 (P < 0.05). Moreover, regression models predicting microcosm toxicity values were constructed to provide a reference for ecological systemic risk assessments based on aquatic microcosms.

CT venography combined with ultrasound-guided minimally invasive treatment for recurrent varicose veins: a pilot paired-design clinical trial

AIM

To compare 1-year outcomes of computed tomography venography (CTV) combined with ultrasound-guided minimally invasive treatment with ascending phlebography and ultrasound-guided treatment for recurrent varicose veins.

MATERIALS AND METHODS

Consecutive patients with unilateral recurrent varicose veins were matched by gender, age, C classification, and degree of obesity, and randomised in a 1:1 ratio to receive either CTV (CTV group) or ascending phlebography (control group) combined with ultrasound-guided minimally invasive treatment. Patients were followed up by clinical and ultrasound examination. Follow-up was scheduled at 1 week, and 3, 6, and 12 months. The primary outcome measure was the Venous Clinical Severity Score (VCSS) at 12 months. Measures of secondary outcome included Chronic Insufficiency Venous International Questionnaire-20 (CIVIQ-20) score, recurrence of varicose vein or ulcer during 12 months, ulcer healing time, detection and location of treated veins.

RESULTS

Eighty patients were enrolled. Median VCSS in the CTV group was lower than it in the control group (p=0.04) and the CIVIQ-20 score was higher than the control group (p=0.02). By 12 months, no symptomatically recurrent varicose veins or ulcers had occurred. The ulcer healing time in CTV group was shorter (p<0.01). A greater number of patients had treated veins detected using CTV than by ascending venography (p=0.01), especially among patients with recurrence reflux veins in the groin, perineum, and vulva (p<0.01).

CONCLUSION

CTV combined with ultrasound may be more helpful than ascending phlebography combined with ultrasound to improve treatment efficacy for recurrent varices. These results should be verified by an future study with more patients and long-term follow-up.

Low-intensity transcranial ultrasound stimulation improves memory in vascular dementia by enhancing neuronal activity and promoting spine formation

Memory is closely associated with neuronal activity and dendritic spine formation. Low-intensity transcranial ultrasound stimulation (TUS) improves the memory of individuals with vascular dementia (VD). However, it is unclear whether neuronal activity and dendritic spine formation under ultrasound stimulation are involved in memory improvement in VD. In this study, we found that seven days of TUS improved memory in VD model while simultaneously increasing pyramidal neuron activity, promoting dendritic spine formation, and reducing dendritic spine elimination. These effects lasted for 7 days but disappeared on 14 d after TUS. Neuronal activity and dendritic spine formation strongly corresponded to improvements in memory behavior over time. In addition, we also found that the memory, neuronal activity and dendritic spine of VD mice cannot be restored again by TUS of 7 days after 28 d. Collectively, these findings suggest that TUS increases neuronal activity and promotes dendritic spine formation and is thus important for improving memory in patients with VD.

Covalent organic frameworks-derived carbon nanospheres based nanoplatform for tumor specific synergistic therapy via oxidative stress amplification and calcium overload

Combinational therapy in cancer treatment that integrates the merits of different therapies is an effective approach to improve therapeutic outcomes. Herein, a simple nanoplatform (N-CNS-CaO2-HA/Ce6 NCs) that synergized chemodynamic therapy (CDT), photodynamic therapy (PDT), photothermal therapy (PTT), and Ca2+ interference therapy (CIT) has been developed to combat hypoxic tumors. With high photothermal effect, excellent peroxidase-like activity, and inherent mesoporous structure, N-doped carbon nanospheres (N-CNSs) were prepared via in situ pyrolysis of an established nanoscale covalent organic frameworks (COFs) precursor. These N-CNSs acted as PTT/CDT agents and carriers for the photosensitizer chlorin e6 (Ce6), thereby yielding a minimally invasive PDT/PTT/CDT synergistic therapy. Hyaluronic acid (HA)-modified CaO2 nanoparticles (CaO2-HA NPs) coated on the surface of the nanoplatform endowed the nanoplatform with O2/H2O2 self-supply capability to respond to and modulate the tumor microenvironment (TME), which greatly facilitated the tumor-specific performance of CDT and PDT. Moreover, the reactive oxygen species (ROS) produced during PDT and CDT enhanced the Ca2+ overloading due to CaO2 decomposition, amplifying the intracellular oxidative stress and leading to mitochondrial dysfunction. Notably, the HA molecules not only increased the cancer-targeting efficiency but also prevented CaO2 degradation during blood circulation, providing double insurance of tumor-selective CIT. Such a nanotherapeutic system possessed boosted antitumor efficacy with minimized systemic toxicity and showed great potential for treating hypoxic tumors.

CircUBE3A(2,3,4,5) promotes adenylate-uridylate-rich binding factor 1 nuclear translocation to suppress prostate cancer metastasis

Metastatic progression is the primary cause of mortality in prostate cancer (PCa) patients. Although circular RNAs (circRNAs) have been implicated in cancer progression and metastasis, our current understanding of their role in PCa metastasis remains limited. In this study, we identified that circUBE3A(2,3,4,5), which originated from exons 2, 3, 4 and 5 of the human ubiquitin-protein ligase E3A (UBE3A) gene, was specifically downregulated in PCa tissues and correlated with the Gleason score, bone metastasis, and D'Amico risk classification. Through the in vitro and in vivo experiments, we demonstrated that overexpression of circUBE3A(2,3,4,5) inhibited PCa cell migration, invasion, metastasis, and proliferation. Mechanistically, circUBE3A(2,3,4,5) was found to bind to adenylate-uridylate-rich binding factor 1 (AUF1), promoting the translocation of AUF1 into the nucleus. This led to decreased AUF1 in the cytoplasm, resulting in methylenetetrahydrofolate dehydrogenase 2 (MTHFD2) mRNA instability and a subsequent reduction at the protein level. The downregulation of MTHFD2 further inhibited vimentin expression, thereby suppressing PCa cell epithelial-mesenchymal transition. Additionally, two pairs of the short-inverted repeats (TSIRs) in flanking introns were identified to synergistically facilitate the generation of circUBE3A(2,3,4,5) and other circRNAs. In summary, TSIRs-induced circUBE3A(2,3,4,5) acts as a suppressor of PCa metastasis by enhancing AUF1 nuclear translocation, reducing MTHFD2, and subsequently inhibiting vimentin expression. This study characterizes circUBE3A(2,3,4,5) as a functional circRNA and proposes it as a highly promising target for preventing PCa metastasis.

Neutrophil depletion attenuates antibody-mediated rejection in a renal transplantation mouse model

Antibody-mediated rejection (AMR) can cause graft failure following renal transplantation. Neutrophils play a key role in AMR progression, but the exact mechanism remains unclear. We investigated the effect of neutrophils on AMR in a mouse kidney transplantation model. The mice were divided into five groups: syngeneic transplantation (Syn), allograft transplantation (Allo), and three differently treated AMR groups. The AMR mouse model was established using skin grafts to pre-sensitize recipient mice. Based on the AMR model, Ly6G-specific monoclonal antibodies were administered to deplete neutrophils (NEUT-/- + AMR) and TACI-Fc was used to block B-cell-activating factor (BAFF)/a proliferation-inducing ligand (APRIL) signaling (TACI-Fc + AMR). Pathological changes were assessed using hematoxylin-eosin and immunohistochemical staining. Banff values were evaluated using the Banff 2015 criteria. Donor-specific antibody (DSA) levels were assessed using flow cytometry, and BAFF and APRIL concentrations were measured using ELISA. Compared to the Syn and Allo groups, a significantly increased number of neutrophils and increased C4d and IgG deposition were observed in AMR mice, accompanied by elevated DSA levels. Neutrophil depletion inhibited inflammatory cell infiltration and reduced C4d and IgG deposition. Neutrophil depletion significantly decreased DSA levels after transplantation and suppressed BAFF and APRIL concentrations, suggesting a mechanism for attenuating AMR-induced graft damage. Similar results were obtained after blockading BAFF/APRIL using a TACI-Fc fusion protein. In summary, neutrophil infiltration increased in the AMR mouse renal transplantation model. Neutrophil depletion or blockading the BAFF/APRIL signaling pathway significantly alleviated AMR and may provide better options for the clinical treatment of AMR.

A framework for longitudinal latent factor modelling of treatment response in clinical trials with applications to Psoriatic Arthritis and Rheumatoid Arthritis

OBJECTIVE

Clinical trials involve the collection of a wealth of data, comprising multiple diverse measurements performed at baseline and follow-up visits over the course of a trial. The most common primary analysis is restricted to a single, potentially composite endpoint at one time point. While such an analytical focus promotes simple and replicable conclusions, it does not necessarily fully capture the multi-faceted effects of a drug in a complex disease setting. Therefore, to complement existing approaches, we set out here to design a longitudinal multivariate analytical framework that accepts as input an entire clinical trial database, comprising all measurements, patients, and time points across multiple trials.

METHODS

Our framework composes probabilistic principal component analysis with a longitudinal linear mixed effects model, thereby enabling clinical interpretation of multivariate results, while handling data missing at random, and incorporating covariates and covariance structure in a computationally efficient and principled way.

RESULTS

We illustrate our approach by applying it to four phase III clinical trials of secukinumab in Psoriatic Arthritis (PsA) and Rheumatoid Arthritis (RA). We identify three clinically plausible latent factors that collectively explain 74.5% of empirical variation in the longitudinal patient database. We estimate longitudinal trajectories of these factors, thereby enabling joint characterisation of disease progression and drug effect. We perform benchmarking experiments demonstrating our method's competitive performance at estimating average treatment effects compared to existing statistical and machine learning methods, and showing that our modular approach leads to relatively computationally efficient model fitting.

CONCLUSION

Our multivariate longitudinal framework has the potential to illuminate the properties of existing composite endpoint methods, and to enable the development of novel clinical endpoints that provide enhanced and complementary perspectives on treatment response.

Improvement of diabetes-induced spinal cord axon injury with taurine via nerve growth factor-dependent Akt/mTOR pathway

Diabetic neuropathy (DN) is a common neurological complication caused by diabetes mellitus (DM). Axonal degeneration is generally accepted to be the major pathological change in peripheral DN. Taurine has been evidenced to be neuroprotective in various aspects, but its effect on spinal cord axon injury (SCAI) in DN remains barely reported. This study showed that taurine significantly ameliorated axonal damage of spinal cord (SC), based on morphological and functional analyses, in a rat model of DN induced by streptozotocin (STZ). Taurine was also found to induce neurite outgrowth in cultured cerebral cortex neurons with high glucose exposure. Moreover, taurine up-regulated the expression of nerve growth factor (NGF) and neurite outgrowth relative protein GAP-43 in rat DN model and cultured cortical neurons/VSC4.1 cells. Besides, taurine increased the activating phosphorylation signals of TrkA, Akt, and mTOR. Mechanistically, the neuroprotection by taurine was related to the NGF-pAKT-mTOR axis, because either NGF-neutralizing antibody or Akt or mTOR inhibitors was found to attenuate its beneficial effects. Together, our results demonstrated that taurine promotes spinal cord axon repair in a model of SCAI in STZ-induced diabetic rats, mechanistically associating with the NGF-dependent activation of Akt/mTOR pathway.

Engineering Streptomyces sp. CPCC 204095 for the targeted high-level production of isatropolone A by elucidating its pathway-specific regulatory mechanism

BACKGROUND

Isatropolone A and C, produced by Streptomyces sp. CPCC 204095, belong to an unusual class of non-benzenoid aromatic compounds and contain a rare seven-membered ring structure. Isatropolone A exhibits potent activity against Leishmania donovani, comparable to the only oral drug miltefosine. However, its variably low productivity represents a limitation for this lead compound in the future development of new anti-leishmaniasis drugs to meet unmet clinical needs.

RESULTS

Here we first elucidated the regulatory cascade of biosynthesis of isatropolones, which consists of two SARP family regulators, IsaF and IsaJ. Through a series of in vivo and in vitro experiments, IsaF was identified as a pathway-specific activator that orchestrates the transcription of the gene cluster essential for isatropolone biosynthesis. Interestingly, IsaJ was found to only upregulate the expression of the cytochrome P450 monooxygenase IsaS, which is crucial for the yield and proportion of isatropolone A and C. Through targeted gene deletions of isaJ or isaS, we effectively impeded the conversion of isatropolone A to C. Concurrently, the facilitation of isaF overexpression governed by selected promoters, prompted the comprehensive activation of the production of isatropolone A. Furthermore, meticulous optimization of the fermentation parameters was conducted. These strategies culminated in the attainment of an unprecedented maximum yield-980.8 mg/L of isatropolone A-achieved in small-scale solid-state fermentation utilizing the genetically modified strains, thereby establishing the highest reported titer to date.

CONCLUSION

In Streptomyces sp. CPCC 204095, the production of isatropolone A and C is modulated by the SARP regulators IsaF and IsaJ. IsaF serves as a master pathway-specific regulator for the production of isatropolones. IsaJ, on the other hand, only dictates the transcription of IsaS, the enzyme responsible for the conversion of isatropolone A and C. By engineering the expression of these pivotal genes, we have devised a strategy for genetic modification aimed at the selective and high-yield biosynthesis of isatropolone A. This study not only unveils the unique regulatory mechanisms governing isatropolone biosynthesis for the first time, but also establishes an essential engineering framework for the targeted high-level production of isatropolone A.

Comparison of different sewage sludge pretreatment technologies for improving sludge solubilization and anaerobic digestion efficiency: A comprehensive review

Anaerobic digestion (AD) of sewage sludge reduces organic solids and produces methane, but the complex nature of sludge, especially the difficulty in solubilization, limits AD efficiency. Pretreatments, by destroying sludge structure and promoting disintegration and hydrolysis, are valuable strategies to enhance AD performance. There is a plethora of reviews on sludge pretreatments, however, quantitative comparisons from multiple perspectives across different pretreatments remain scarce. This review categorized various pretreatments into three groups: Physical (ultrasonic, microwave, thermal hydrolysis, electric decomposition, and high pressure homogenization), chemical (acid, alkali, Fenton, calcium peroxide, and ozone), and biological (microaeration, exogenous bacteria, and exogenous hydrolase) pretreatments. The optimal conditions of various pretreatments and their impacts on enhancing AD efficiency were summarized; the effects of different pretreatments on microbial community in the AD system were comprehensively compared. The quantitative comparison based on dissolution degree of COD (DDCOD) indicted that the sludge solubilization performance is in the order of physical, chemical, and biological pretreatments, although with each below 40 % DDCOD. Biological pretreatment, particularly microaeration and exogenous bacteria, excel in AD enhancement. Pretreatments alter microbial ecology, favoring Firmicutes and Methanosaeta (acetotrophic methanogens) over Proteobacteria and Methanobacterium (hydrogenotrophic methanogens). Most pretreatments have unfavorable energy and economic outcomes, with electric decomposition and microaeration being exceptions. On the basis of the overview of the above pretreatments, a full energy and economy assessment for sewage sludge treatment was suggested. Finally, challenges associated with sludge pretreatments and AD were analyzed, and future research directions were proposed. This review may broaden comprehension of sludge pretreatments and AD, and provide an objective basis for the selection of sludge pretreatment technologies.

Ultrafine Co-MoC particles in porous carbon derived from polyoxometalate-based metal organic framework for efficient hydrogen evolution reaction

Accurately regulating ultrafine molybdenum carbide (MoC)-based catalysts is a significant challenge in the rational design of hydrogen evolution reaction (HER) electrocatalysts. Herein, under the guidance of the first principle calculations, we proposed an in-situ polyoxometalate-confined strategy for creating uniformly distributed ultrafine Co-MoC bimetallic nanoparticles in porous carbon nanostars, with the assistance of precisely designed metal-organic framework (MOF). The Co-MoC@C electrocatalyst has a high specific surface area of 969 m2·g-1 because of the conductive carbon substrate with abundant mesopores, which makes for exposing more active sites of Co-MoC nanocrystals (∼1.5 nm) and facilitating electron/ion transport. Thus, Co-MoC@C electrocatalyst shows the excellent electrochemical activity with overpotentials of 88.4 mV and 66.6 mV at a current density of 10 mA·cm-2 under acidic and alkaline conditions, respectively. The in-situ polyoxometalate-confined strategy will provide a new guideline for the design and preparation of efficient HER electrocatalysts.

Fine mapping and analysis of a candidate gene controlling Phytophthora blight resistance in cucumber

Cucumber blight is a destructive disease. The best way to control this disease is resistance breeding. This study focuses on disease resistance gene mapping and molecular marker development. We used the resistant cucumber, JSH, and susceptible cucumber, B80, as parents to construct F2 populations. Bulked segregant analysis (BSA) combined with specific length amplified fragment sequencing (SLAF-seq) were used, from which we developed cleaved amplified polymorphic sequence (CAPs) markers to map the resistance gene. Resistance in F2 individuals showed a segregation ratio of resistance:susceptibility close to 3:1. The gene in JSH resistant cucumber was mapped to an interval of 9.25 kb, and sequencing results for the three genes in the mapped region revealed three mutations at base sites 225, 302, and 591 in the coding region of Csa5G139130 between JSH and B80, but no mutations in coding regions of Csa5G139140 and Csa5G139150. The mutations caused changes in amino acids 75 and 101 of the protein encoded by Csa5G139130, suggesting that Csa5G139130 is the most likely resistance candidate gene. We developed a molecular marker, CAPs-4, as a closely linked marker for the cucumber blight resistance gene. This is the first report on mapping of a cucumber blight resistance gene and will provideg a useful marker for molecular breeding of cucumber resistance to Phytophthora blight.

Study of association between corneal shape parameters and axial length elongation during orthokeratology using image-pro plus software

BACKGROUND

The aim was to validate the correlation between corneal shape parameters and axial length growth (ALG) during orthokeratology using Image-Pro Plus (IPP) 6.0 software.

METHODS

This retrospective study used medical records of myopic children aged 8-13 years (n = 104) undergoing orthokeratology. Their corneal topography and axial length were measured at baseline and subsequent follow-ups after lens wear. Corneal shape parameters, including the treatment zone (TZ) area, TZ diameter, TZ fractal dimension, TZ radius ratio, eccentric distance, pupil area, and pupillary peripheral steepened zone(PSZ) area, were measured using IPP software. The impact of corneal shape parameters at 3 months post-orthokeratology visit on 1.5-year ALG was evaluated using multivariate linear regression analysis.

RESULTS

ALG exhibited significant associations with age, TZ area, TZ diameter, TZ fractal dimension, and eccentric distance on univariate linear regression analysis. Multivariate regression analysis identified age, TZ area, and eccentric distance as significantly correlated with ALG (all P < 0.01), with eccentric distance showing the strongest correlation (β = -0.370). The regressive equation was y = 1.870 - 0.235a + 0.276b - 0.370c, where y represents ALG, a represents age, b represents TZ area, and c represents eccentric distance; R2 = 0.27). No significant relationships were observed between the TZ radius ratio, pupillary PSZ area, and ALG.

CONCLUSIONS

IPP software proves effective in capturing precise corneal shape parameters after orthokeratology. Eccentric distance, rather than age or the TZ area, significantly influences ALG retardation.

Exploring the body surface temperature of the lumbosacral region and relevant back-shu points in patients with lumbar disc herniation induced low back pain based on infrared thermography

OBJECTIVES

To observe the body surface temperature of the lumbosacral region and relevant back-shu points in patients with lumbar disc herniation (LDH) induced low back pain utilizing infrared thermography, and to explore the functional attribute changes of acupoints under pathological conditions.

METHODS

A total of 50 patients with LDH induced low back pain were included as the observation group, and 45 healthy subjects were included as the control group. Using infrared thermography, the body surface temperature of the lumbosacral region and bilateral Sanjiaoshu (BL 22), Shenshu (BL 23), Qihaishu (BL 24), Dachangshu (BL 25), Guanyuanshu (BL 26), Xiaochangshu (BL 27), and Pangguangshu (BL 28) was measured in both groups. The temperature difference values between the bilateral lumbosacral regions and back-shu points of the two groups were calculated. Additionally, the body surface temperature of the affected and healthy sides of the lumbosacral region and relevant back-shu points was compared in the observation group.

RESULTS

Compared with the control group, the body surface temperature of the lumbosacral region and the bilateral temperature difference values of the lumbosacral regions were increased in the observation group (P<0.001). The body surface temperature difference values of bilateral Shenshu (BL 23), Qihaishu (BL 24), Dachangshu (BL 25), Guanyuanshu (BL 26) and Xiaochangshu (BL 27) in the observation group were higher than those in the control group (P<0.05, P<0.01, P<0.001). In the observation group, the body surface temperature of the affected side of the lumbosacral region as well as Shenshu (BL 23) and Dachangshu (BL 25) was elevated compared with that of healthy side (P<0.001).

CONCLUSIONS

The patients with LDH induced low back pain have imbalanced and asymmetrical distribution of body surface temperature in the lumbosacral region and related back-shu points, Shenshu (BL 23) and Dachangshu (BL 25) have the relative specificity.

Decision-Making With Speculative Opponent Models

Opponent modeling has proven effective in enhancing the decision-making of the controlled agent by constructing models of opponent agents. However, existing methods often rely on access to the observations and actions of opponents, a requirement that is infeasible when such information is either unobservable or challenging to obtain. To address this issue, we introduce distributional opponent-aided multiagent actor-critic (DOMAC), the first speculative opponent modeling algorithm that relies solely on local information (i.e., the controlled agent's observations, actions, and rewards). Specifically, the actor maintains a speculated belief about the opponents using the tailored speculative opponent models that predict the opponents' actions using only local information. Moreover, DOMAC features distributional critic models that estimate the return distribution of the actor's policy, yielding a more fine-grained assessment of the actor's quality. This thus more effectively guides the training of the speculative opponent models that the actor depends upon. Furthermore, we formally derive a policy gradient theorem with the proposed opponent models. Extensive experiments under eight different challenging multiagent benchmark tasks within the MPE, Pommerman, and starcraft multiagent challenge (SMAC) demonstrate that our DOMAC successfully models opponents' behaviors and delivers superior performance against state-of-the-art (SOTA) methods with a faster convergence speed.

In-field and non-destructive determination of comprehensive maturity index and maturity stages of Camellia oleifera fruits using a portable hyperspectral imager

To efficiently detect the maturity stages of Camellia oleifera fruits, this study proposed a non-invasive method based on hyperspectral imaging technology. First, a portable hyperspectral imager was used for the in-field image acquisition of Camellia oleifera fruits at three maturity stages, and ten quality indexes were measured as reference standards. Then, factor analysis was performed to obtain the comprehensive maturity index (CMI) by analyzing the change trends and correlations of different indexes. To reduce the high dimensionality of spectral data, the successive projection algorithm (SPA) was employed to select effective feature wavelengths. The prediction models for CMI, including partial least squares regression (PLSR), support vector regression (SVR), extreme learning machine (ELM), and convolutional neural network regression (CNNR), were constructed based on full spectra and feature wavelengths; for CNNR, only the raw spectra were used as input. The SPA-CNNR model exhibited more promising performance (RP = 0.839, RMSEP = 0.261, and RPD = 1.849). Furthermore, PLS-DA models for maturity discrimination of Camellia oleifera fruits were developed using full wavelength, characteristic wavelengths and their fusion CMI, respectively. The PLS-DA model using the fused dataset achieved the highest maturity classification accuracy, with the best simplified model achieving 88.6 % accuracy in prediction set. This study indicated that a portable hyperspectral imager can be used for in-field determination of the internal quality and maturity stages of Camellia oleifera fruits. It provides strong support for non-destructive quality inspection and timely harvesting of Camellia oleifera fruits in the field.

[Effect of LAG3 deficiency on natural killer cell function and hepatic fibrosis in mice infected with Echinococcus multilocularis]

OBJECTIVE

To investigate the effect of LAG-3 deficiency (LAG3-/-) on natural killer (NK) cell function and hepatic fibrosis in mice infected with Echinococcus multilocularis.

METHODS

C57BL/6 mice, each weighing (20 ± 2) g, were divided into the LAG3-/- and wild type (WT) groups, and each mouse in both groups was inoculated with 3 000 E. multilocularis protoscoleces via the hepatic portal vein. Mouse liver and spleen specimens were collected 12 weeks post-infection, sectioned and stained with sirius red, and the hepatic lesions and fibrosis were observed. Mouse hepatic and splenic lymphocytes were isolated, and flow cytometry was performed to detect the proportions of hepatic and splenic NK cells, the expression of CD44, CD25 and CD69 molecules on NK cell surface, and the secretion of interferon γ (IFN-γ), tumor necrosis factor α (TNF-α), interleukin (IL)-4, IL-10 and IL-17A.

RESULTS

Sirius red staining showed widening of inflammatory cell bands and hyperplasia of fibrotic connective tissues around mouse hepatic lesions, as well as increased deposition of collagen fibers in the LAG3-/-group relative to the WT group. Flow cytometry revealed lower proportions of mouse hepatic (6.29% ± 1.06% vs. 11.91% ± 1.85%, P < 0.000 1) and splenic NK cells (4.44% ± 1.22% vs. 5.85% ± 1.10%, P > 0.05) in the LAG3-/- group than in the WT group, and the mean fluorescence intensity of CD44 was higher on the surface of mouse hepatic NK cells in the LAG3-/- group than in the WT group (t = -3.234, P < 0.01), while no significant differences were found in the mean fluorescence intensity of CD25 or CD69 on the surface of mouse hepaticNK cells between the LAG3-/- and WT groups (both P values > 0.05). There were significant differences between the LAG3-/- and WT groups in terms of the percentages of IFN-γ (t = -0.723, P > 0.05), TNF-α (t = -0.659, P > 0.05), IL-4 (t = -0.263, P > 0.05), IL-10 (t = -0.455, P > 0.05) or IL-17A secreted by mouse hepatic NK cells (t = 0.091, P > 0.05), and the percentage of IFN-γ secreted by mouse splenic NK cells was higher in the LAG3-/- group than in the WT group (58.40% ± 1.64% vs. 50.40% ± 4.13%; t = -4.042, P < 0.01); however, there were no significant differences between the two groups in terms of the proportions of TNF-α (t = -1.902, P > 0.05), IL-4 (t = -1.333, P > 0.05), IL-10 (t = -1.356, P > 0.05) or IL-17A secreted by mouse splenic NK cells (t = 0.529, P > 0.05).

CONCLUSIONS

During the course of E. multilocularis infections, LAG3-/- promotes high-level secretion of IFN-γ by splenic NK cells, which may participate in the reversal the immune function of NK cells, resulting in aggravation of hepatic fibrosis.

Causal association of monocytes with chronic kidney disease and the mediation role of frailty: A study integrating large-scale two-sample Mendelian randomization and single-cell analysis

BACKGROUND

Recent research reported that frailty was prevalent among adults with chronic kidney disease (CKD) in clinical trials, and monocytes illustrated a similar difference in these two diseases compared to the normal. However, the scientific evidence for a causal relationship between these two diseases was lacking, with further exploration into whether monocytes co-regulate them.

METHODS

We aimed to integrate large-scale Mendelian randomization (MR) and single-cell transcriptome analysis to determine whether there was a causal relationship between frailty and CKD (Bidirectional two-sample Mendelian determined the causal direction), whether monocytes impacted them, and whether the two diseases shared genetic variation sites. Based on 441 Genome-wide association study datasets, this study utilized five MR methods, multiple sensitivity analysis, and corresponding single-cell transcriptome datasets as proof.

RESULTS

The association between frailty and CKD was significantly causal, and frailty increased the risk of CKD in patients (OR (95 %CI): 3.5597 (1.8369-6.8982), p = 0.000168909). The exposure monocyte can increase the risk of frailty and CKD in patients, especially with high expression of HLA genes in these cells. The existing two-sample MR results cannot reject the hypothesis that monocytes increase the risk of CKD by inducing frailty. rs9275271' 1mb genetic location above and below had been proven to be an effective genetic space for both frailty and CKD.

CONCLUSION

We conducted the largest MR to date on frailty, monocyte, and CKD, and found a significant causal association between frailty and CKD, with the single-cell analysis confirmed. The exposure monocytes increased the risk of frailty and CKD, particularly with high expression of HLA genes in these cells. We identified a potential common genetic variant space, rs9275271, associated with frailty and CKD, providing insights into the genetic basis of these conditions.

Construction of a prognostic model with CAFs for predicting the prognosis and immunotherapeutic response of lung squamous cell carcinoma

Lung squamous cell carcinoma (LUSC) is one of the subtypes of lung cancer (LC) that contributes to approximately 25%-30% of its prevalence. Cancer-associated fibroblasts (CAFs) are key cellular components of the TME, and the large number of CAFs in tumour tissues creates a favourable environment for tumour development. However, the function of CAFs in the LUSC is complex and uncertain. First, we processed the scRNA-seq data and classified distinct types of CAFs. We also identified prognostic CAFRGs using univariate Cox analysis and conducted survival analysis. Additionally, we assessed immune cell infiltration in CAF clusters using ssGSEA. We developed a model with a significant prognostic correlation and verified the prognostic model. Furthermore, we explored the immune landscape of LUSC and further investigated the correlation between malignant features and LUSC. We identified CAFs and classified them into three categories: iCAFs, mCAFs and apCAFs. The survival analysis showed a significant correlation between apCAFs and iCAFs and LUSC patient prognosis. Kaplan-Meier analysis showed that patients in CAF cluster C showed a better survival probability compared to clusters A and B. In addition, we identified nine significant prognostic CAFRGs (CLDN1, TMX4, ALPL, PTX3, BHLHE40, TNFRSF12A, VKORC1, CST3 and ADD3) and subsequently employed multivariate Cox analysis to develop a signature and validate the model. Lastly, the correlation between CAFRG and malignant features indicates the potential role of CAFRG in promoting tumour angiogenesis, EMT and cell cycle alterations. We constructed a CAF prognostic signature for identifying potential prognostic CAFRGs and predicting the prognosis and immunotherapeutic response for LUSC. Our study may provide a more accurate prognostic assessment and immunotherapy targeting strategies for LUSC.

Decolorization, spectral broadening, and luminescence enhancement in Tb:Y2O3 transparent ceramics through vacuum thermal reduction

Tb3+ is extensively employed in magneto-optical devices and luminescent materials owing to its distinctive physical properties. However, under certain conditions, trivalent Tb3+ readily undergoes oxidation to tetravalent Tb4+, significantly reducing the performance of devices containing Tb3+. In this Letter, we report a technique called dual-annealing (DA) post-treatment, which effectively solves Tb oxidation issues by utilizing the reducibility of the vacuum environment. High-quality Tb:Y2O3 transparent ceramics were prepared with in-line transmittance of ∼80% at 800 nm. Subsequently, the prepared ceramics were subjected to DA treatment. The optical, photoluminescence, radioluminescence, and x-ray imaging properties of DA samples were comprehensively compared with those of conventionally single-annealed (SA) samples. The coloration of Tb:Y2O3 transparent ceramics due to Tb4+ absorption was eliminated by DA. Notably, the DA sample showed a 3.28-fold increase in photoluminescence intensity and a 2.73-fold increase in radioluminescence intensity compared with the traditional SA sample. DA post-treatment enables Tb: Y2O3 transparent ceramics to achieve x-ray imaging capabilities. This Letter presents a simple, efficient, and universally applicable post-treatment technique expected to replace conventional hydrogen annealing in numerous scenarios.

Oxyberberine sensitizes liver cancer cells to sorafenib via inhibiting NOTCH1-USP7-c-Myc pathway

BACKGROUND

Sorafenib is the first-line therapy for patients with advanced-stage HCC, but its clinical cure rate is unsatisfactory due to adverse reactions and drug resistance. Novel alternative strategies to overcome sorafenib resistance are urgently needed. Oxyberberine (OBB), a major metabolite of berberine in vivo, exhibits potential antitumor potency in various human malignancies, including liver cancer. However, it remains unknown whether and how OBB sensitizes liver cancer cells to sorafenib.

METHODS

Cell viability, trypan blue staining and flow cytometry assays were employed to determine the synergistic effect of OBB and sorafenib on killing HCC cells. PCR, western blot, co-immunoprecipitation and RNA interference assays were used to decipher the mechanism by which OBB sensitizes sorafenib. HCC xenograft models and clinical HCC samples were utilized to consolidate our findings.

RESULTS

We found for the first time that OBB sensitized liver cancer cells to sorafenib, enhancing its inhibitory effect on cell growth and induction of apoptosis in vitro. Interestingly, we observed that OBB enhanced the sensitivity of HCC cells to sorafenib by reducing ubiquitin-specific peptidase 7 (USP7) expression, a well-known tumor-promoting gene. Mechanistically, OBB inhibited notch homolog 1-mediated USP7 transcription, leading to the downregulation of V-Myc avian myelocytomatosis viral oncogene homolog (c-Myc), which synergized with sorafenib to suppress liver cancer. Furthermore, animal results showed that cotreatment with OBB and sorafenib significantly inhibited the tumor growth of liver cancer xenografts in mice.

CONCLUSIONS

These results indicate that OBB enhances the sensitivity of liver cancer cells to sorafenib through inhibiting notch homolog 1-USP7-c-Myc signaling pathway, which potentially provides a novel therapeutic strategy for liver cancer to improve the effectiveness of sorafenib.

Clinical outcomes of SMILE and WFG-LASIK used to treat myopia and astigmatism: A systematic review and meta-analysis

PURPOSE

To evaluate the safety, efficacy and postoperative visual quality of small incision lenticule extraction (SMILE) and Wavefront-Guided Laser in situ keratomileusis (WFG-LASIK) and to analyze their efficacy in correcting astigmatism.

METHODS

A systematic literature search was performed using Cochrane Collaboration methodology. Databases searched included PubMed, Embase, the Cochrane Library and Web of Science. RevMan software version 5.3.0 was used for meta-analysis.

RESULTS

A total of 976 eyes were included in 8 studies, of which 539 eyes underwent SMILE and 437 eyes underwent WFG-LASIK. There were no statistically significant differences in the proportion of eyes achieving uncorrected distance visual acuity of 20/20 or better (P=0.18), the proportion of eyes within±0.50 diopter of target refraction postoperatively (P=0.10), or the postoperative magnitude of cylinder (P=0.10). Regarding the Alpins vector analysis of astigmatism, there was no statistically significant difference in the surgical magnitude of error (P=0.09) between the two groups. WFG-LASIK has a lower surgical angle of error (P= 0.002) and higher surgical correction index of cylinder (P=0.03) than SMILE. In terms of aberrations, higher order aberrations (P=0.46), spherical aberrations (P=0.22) and trefoil (P=0.56) were not statistically different, while WFG-LASIK induced less coma than SMILE surgery (P=0.02).

CONCLUSION

Both SMILE and WFG-LASIK are safe and effective ways to correct myopia and astigmatism. Compared with SMILE, WFG-LASIK has a lower surgical angle of error, higher surgical correction index of cylinder and induces less coma.

Impact of stalling events on microcirculatory hemodynamics in the aged brain

OBJECTIVE

The role of cerebral microvasculature in cognitive dysfunction can be investigated by identifying the impact of blood flow on cortical tissue oxygenation. In this paper, the impact of capillary stalls on microcirculatory characteristics such as flow and hematocrit (Ht) in the cortical angioarchitecture is studied.

METHODS

Using a deterministic mathematical model to simulate blood flow in a realistic mouse cortex, hemodynamics parameters, including pressure, flow, vessel diameter-adjustable hematocrit, and transit time are calculated as a function of stalling events.

RESULTS

Using a non-linear plasma skimming model, it is observed that Ht increases in the penetrating arteries from the pial vessels as a function of cortical depth. The incidence of stalling on Ht distribution along the blood network vessels shows reduction of RBCs around the tissue near occlusion sites and decreased Ht concentration downstream from the blockage points. Moreover, upstream of the occlusion, there is a noticeable increase of the Ht, leading to larger flow resistance due to higher blood viscosity. We predicted marked changes in transit time behavior due to stalls which match trends observed in mice in vivo.

CONCLUSIONS

These changes to blood cell quantity and quality may be implicated in the development of Alzheimer's disease and contribute to the course of the illness.

Amplitude Analysis of the B^{0}→K^{*0}μ^{+}μ^{-} Decay

An amplitude analysis of the B^{0}→K^{*0}μ^{+}μ^{-} decay is presented using a dataset corresponding to an integrated luminosity of 4.7  fb^{-1} of pp collision data collected with the LHCb experiment. For the first time, the coefficients associated to short-distance physics effects, sensitive to processes beyond the standard model, are extracted directly from the data through a q^{2}-unbinned amplitude analysis, where q^{2} is the μ^{+}μ^{-} invariant mass squared. Long-distance contributions, which originate from nonfactorizable QCD processes, are systematically investigated, and the most accurate assessment to date of their impact on the physical observables is obtained. The pattern of measured corrections to the short-distance couplings is found to be consistent with previous analyses of b- to s-quark transitions, with the largest discrepancy from the standard model predictions found to be at the level of 1.8 standard deviations. The global significance of the observed differences in the decay is 1.4 standard deviations.

Drug resistance in ovarian cancer: from mechanism to clinical trial

Ovarian cancer is the leading cause of gynecological cancer-related death. Drug resistance is the bottleneck in ovarian cancer treatment. The increasing use of novel drugs in clinical practice poses challenges for the treatment of drug-resistant ovarian cancer. Continuing to classify drug resistance according to drug type without understanding the underlying mechanisms is unsuitable for current clinical practice. We reviewed the literature regarding various drug resistance mechanisms in ovarian cancer and found that the main resistance mechanisms are as follows: abnormalities in transmembrane transport, alterations in DNA damage repair, dysregulation of cancer-associated signaling pathways, and epigenetic modifications. DNA methylation, histone modifications and noncoding RNA activity, three key classes of epigenetic modifications, constitute pivotal mechanisms of drug resistance. One drug can have multiple resistance mechanisms. Moreover, common chemotherapies and targeted drugs may have cross (overlapping) resistance mechanisms. MicroRNAs (miRNAs) can interfere with and thus regulate the abovementioned pathways. A subclass of miRNAs, "epi-miRNAs", can modulate epigenetic regulators to impact therapeutic responses. Thus, we also reviewed the regulatory influence of miRNAs on resistance mechanisms. Moreover, we summarized recent phase I/II clinical trials of novel drugs for ovarian cancer based on the abovementioned resistance mechanisms. A multitude of new therapies are under evaluation, and the preliminary results are encouraging. This review provides new insight into the classification of drug resistance mechanisms in ovarian cancer and may facilitate in the successful treatment of resistant ovarian cancer.

Perisaccadic and attentional remapping of receptive fields in lateral intraparietal area and frontal eye fields

The nature and function of perisaccadic receptive field (RF) remapping have been controversial. We use a delayed saccade task to reduce previous confounds and examine the remapping time course in the lateral intraparietal area and frontal eye fields. In the delay period, the RF shift direction turns from the initial fixation to the saccade target. In the perisaccadic period, RFs first shift toward the target (convergent remapping), but around the time of saccade onset/offset, the shifts become predominantly toward the post-saccadic RF locations (forward remapping). Thus, unlike forward remapping that depends on the corollary discharge (CD) of the saccade command, convergent remapping appears to follow attention from the initial fixation to the target. We model the data with attention-modulated and CD-gated connections and show that both sets of connections emerge automatically in neural networks trained to update stimulus retinal locations across saccades. Our work thus unifies previous findings into a mechanism for transsaccadic visual stability.

[Application value of laparoscopic double stapler firings and double stapling technique combined with rectal eversion and total extra-abdominal resection in the sphincter-preserving resection of low rectal cancer]

Objectives: To investigate the application value of laparoscopic double stapler firings and double stapling technique combined with rectal eversion and total extra-abdominal resection (LDER) in the anal preservation treatment of low rectal cancer. Methods: Inclusion criteria: (1) age was 18-70; (2) the distance of the lower tumor edge from the anal verge was 4-5 cm; (3) primary tumor with a diameter ≤3 cm; (4) preoperative staging of T1~2N1~2M0; (5) "difficult pelvis", defined as ischial tuberosity diameter<10 cm or body mass index>25 kg/m2; (6) patients with strong intention for sphincter preservation; (7) no preoperative treatment (e.g., chemotherapy, radiotherapy, molecular targeted therapy, or immunotherapy); (8) no lateral lymph node enlargement; (9) no previous anorectal surgery; (10) patients with good basic condition who could tolerate surgery. Exclusion criteria: (1) previously suffered from malignant tumors of the digestive tract or currently suffering from malignant tumors out of the digestive tract; (2) patients with preoperative anal dysfunction (Wexner score ≥ 10), or fecal incontinence. The specific surgical steps are as follows: the distal end of the rectum was dissected to the level of the interspace between internal and external sphincters of anal canal. Five centimeters proximal to the tumor, the mesorectum was ligated, and a liner stapler was used to transect the rectum. The distal rectum with the tumor were then everted and extracted through the anus. The rectum was transected 0.5-1.0 cm distal to the tumor with a linear stapler. Full thickness suture was used to reinforce the stump of the rectum, which was then brought back into the pelvic cavity. Finally, an end-to-end anastomosis between the colon and the rectum was performed. A retrospective descriptive study was performed of the clinical and pathological data of 12 patients with T1-T2 stage low rectal cancer treated with LDER at Henan Provincial People's Hospital from January 2020 to December 2022. Results: All 12 patients successfully completed LDER with sphincter preservation, without conversion to open surgery or changes in surgical approach. The median surgical time was 272 (155-320) minutes, with a median bleeding volume of 100 (50-200) mL. No protective stoma was performed, and all patients received R0 resection. The average hospital stay was 9 (7-15) days. There were no postoperative anastomotic leakage or perioperative deaths. All 12 patients received postoperative follow-up, with a median follow-up of 12 months (6-36 months) and a Wexner score of 8 (5-14) at 6 months postoperatively. There was no tumor recurrence or metastasis during the follow-up period. Conclusions: LDER is safe and effective for the treatment of low rectal cancer.

Ammonia distribution and ecological risk assessment in nine fresh lakes in China

With the development of industry and economy, ammonia nitrogen pollutions in surface water are of great concern worldwide. This study investigated the historical contents of total ammonia nitrogen (TAN) and unionized ammonia molecules (NH3) in nine fresh lakes in China during 2014-2022. Three different classification methods (flood season, season, and geographical distribution) were used to analyze the concentration variation of TAN and NH3. The concentration of TAN first decreased and then increased in the flood season, showing a lower concentration in summer and a higher concentration in winter. The variation trend of NH3 was in an opposite way with TAN. Correlation analysis between ammonia and 10 water quality parameters and 4 pollution emission and treatment parameters showed that the correlation coefficient between TAN and total phosphorus (total nitrogen) was 0.44 (0.43), respectively. The correlation coefficients between average annual TAN concentration and total emissions (waste water treatment input) were 0.35 (0.53), respectively. Combined with ecotoxicity data from a series of aquatic species, the ecological risks of TAN and NH3 in lakes were evaluated using hazard quotient and joint probability curve methods. From 2014 to 2022, the probability of 5% species affected in the acute ecological risk of TAN and NH3 is lower than 0.01, but for the chronic ecological risk of TAN and NH3, the probabilities of 5% species affected are 0.003-0.030 and 0.04-0.14, respectively. The chronic ecological risks were higher than the acute ecological risks, and high risks in plateau lakes like Dianchi Lake should be paid more attention to.

[Research progress in the regulation of pathogenesis and the transformation of chronic liver disease by short-chain fatty acids]

Short-chain fatty acids are metabolites of the intestinal flora and serve as the main energy source for intestinal epithelial cells. At the same time, as important signaling molecules, it regulate a variety of cellular inflammatory responses and homeostatic proliferation through receptor-dependent and independent pathways. Short-chain fatty acids regulate the gut-liver axis and thereby directly act on the liver, participating in the pathogenesis and transformation of various liver diseases, including alcoholic liver disease, metabolic dysfunction-related liver disease, autoimmune liver disease, liver fibrosis, and hepatocellular carcinoma. In addition, short-chain fatty acids can inhibit HBV DNA replication. This article reviews the research progress on the role of short-chain fatty acids in aspects of the pathogenesis and transformation of chronic liver diseases.

Dissecting the chiral recognition of TLR4/MD2 with Neoseptin-3 enantiomers by molecular dynamics simulations

Toll-like receptor 4 (TLR4) is a pivotal innate immune recognition receptor that regulates intricate signaling pathways within the immune system. Neoseptin-3 (Neo-3), a recently identified small-molecule agonist for mouse TLR4/MD2, exhibits chiral recognition properties. Specifically, the L-enantiomer of Neo-3 (L-Neo-3) effectively activates the TLR4 signaling pathway, while D-Neo-3 fails to induce TLR4 activation. However, the underlying mechanism by which TLR4 enantioselectively recognizes Neo-3 enantiomers remains poorly understood. In this study, in silico simulations were performed to investigate the mechanism of chiral recognition of Neo-3 enantiomers by TLR4/MD2. Two L-Neo-3 molecules stably resided within the cavity of MD2 as a dimer, and the L-Neo-3 binding stabilized the (TLR4/MD2)2 dimerization state. However, the strong electrostatic repulsion between the hydrogen atoms on the chiral carbon of D-Neo-3 molecules caused the relative positions of two D-Neo-3 molecules to continuously shift during the simulation process, thus preventing the formation of D-Neo-3 dimer as well as their stable interactions with the surrounding residues in (TLR4/MD2)2. Considering that L-Neo-3 could not sustain a stable dimeric state in the bulk aqueous environment, it is unlikely that L-Neo-3 entered the cavity of MD2 as a dimeric unit. Umbrella sampling simulations revealed that the second L-Neo-3 molecule entering the cavity of MD2 exhibited a lower binding energy (-25.75 kcal mol-1) than that of the first L-Neo-3 molecule (-14.31 kcal mol-1). These results imply that two L-Neo-3 molecules enter the cavity of MD2 sequentially, with the binding of the first L-Neo-3 molecule facilitating the entry of the second one. This study dissects the binding process of Neo-3 enantiomers, offering a comprehensive understanding of the atomic-level mechanism underlying TLR4's chiral recognition of Neo-3 molecules.

Periplcymarin targets glycolysis and mitochondrial oxidative phosphorylation of esophageal squamous cell carcinoma: Implication in anti-cancer therapy

BACKGROUND

Esophageal squamous cell carcinoma (ESCC) is the predominant histological subtype of esophageal cancer (EC) in China, and demonstrates varying levels of resistance to multiple chemotherapeutic agents. Our previous studies have proved that periplocin (CPP), derived from the extract of cortex periplocae, exhibiting the capacity to hinder proliferation and induce apoptosis in ESCC cells. Several studies have identified additional anti-cancer constituents in the extract of cortex periplocae, named periplcymarin (PPM), sharing similar compound structure with CPP. Nevertheless, the inhibitory effects of PPM on ESCC and their underlying mechanisms remain to be further elucidated.

PURPOSE

The aim of this study was to investigate function of PPM inhibiting the growth of ESCC in vivo and in vitro and to explore its underlying mechanism, providing the potential anti-tumor drug for ESCC.

METHODS

Initially, a comparative analysis was conducted on the inhibitory activity of three naturally compounds obtained from the extract of cortex periplocae on ESCC cells. Among these compounds, PPM was chosen for subsequent investigation owing to its comparatively structure and anti-tumor activity simultaneously. Subsequently, a series of biological functional experiments were carried out to assess the impact of PPM on the proliferation, apoptosis and cell cycle arrest of ESCC cells in vitro. In order to elucidate the molecular mechanism of PPM, various methodologies were employed, including bioinformatics analyses and mechanistic experiments such as high-performance liquid chromatography combined with mass spectrometry (HPLC-MS), cell glycolysis pressure and mitochondrial pressure test. Additionally, the anti-tumor effects of PPM on ESCC cells and potential toxic side effects were evaluated in vivo using the nude mice xenograft assay.

RESULTS

Our study revealed that PPM possesses the ability to impede the proliferation of ESCC cells, induce apoptosis, and arrest the cell cycle of ESCC cells in the G2/M phase in vitro. Mechanistically, PPM exerted its effects by modulating glycolysis and mitochondrial oxidative phosphorylation (OXPHOS), as confirmed by glycolysis pressure and mitochondrial pressure tests. Moreover, rescue assays demonstrated that PPM inhibits glycolysis and OXPHOS in ESCC cells through the PI3K/AKT and MAPK/ERK signaling pathways. Additionally, we substantiated that PPM effectively suppresses the growth of ESCC cells in vivo, with only modest potential toxic side effects.

CONCLUSION

Our study provides novel evidence that PPM has the potential to simultaneously target glycolysis and mitochondrial OXPHOS in ESCC cells. This finding highlights the need for further investigation into PPM as a promising therapeutic agent that targets the tumor glucose metabolism pathway in ESCC.

Exploring relevant factors of cognitive impairment in the elderly Chinese population using Lasso regression and Bayesian networks

Older adults are highly susceptible to developing cognitive impairment(CI). Various factors contribute to the prevalence of CI, but the potential relationships among these factors remain unclear. This study aims to explore the relevant factors associated with CI in Chinese older adults and analyze the potential relationships between CI and these factors.We analyzed the data on 6886 older adults aged≥60 from the China Health and Retirement Longitudinal Study (CHARLS) 2018. Lasso regression was initially used to screening variables. Bayesian Networks(BNs) were used to identify the correlates of CI and potential associations between factors. After screening with Lasso regression, 11 variables were finally included in the BNs. The BNs, by establishing a complex network relationship, revealed that age, education, and indoor air pollution were the direct correlates affecting the occurrence of CI in older adults. It also indicated that marital status indirectly influenced CI through age, and residence indirectly linked to CI through two pathways: indoor air pollution and education.Our findings underscore the effectiveness of BNs in unveiling the intricate network linkages among CI and its associated factors, holding promising applications. It can serve as a reference for public health departments to address the prevention of CI in the elderly.

Tannic acid and zinc ion coordination of nanase for the treatment of inflammatory bowel disease by promoting mucosal repair and removing reactive oxygen and nitrogen species

Colon mucosal overexpression of reactive oxygen and nitrogen species (RONS) accelerates the development of inflammatory bowel disease (IBD) and destroys the mucosa and its barrier. IBD can be alleviated by removing RONS from the inflamed colon. The preparation of strong and efficient nanoantioxidants remains a challenge despite the development of numerous nanoantioxidants. In this paper, Zn-TA nanoparticles with fine hollow microstructure (HZn-TA) were successfully prepared and could be effectively used to treat IBD. In the first step, ZIF-8 nanoparticles were synthesized by a one-pot method. On this basis, HZn-TA nanoparticles were etched by TA, and a multifunctional nanase was developed for the treatment of IBD. RONS, including reactive oxygen species (ROS) and nitric oxide (NO), can be eliminated to increase cell survival following Hydrogen peroxide (H2O2) stimulation, including reactive oxygen species (ROS) and nitric oxide (NO with hydrogen peroxide (H2O2). In a model for preventing and delaying acute colitis, clearance of RONS has been shown to reduce intestinal inflammation in mice by reducing colon damage, proinflammatory cytokine levels, the spleen index, and body weight. Intestinal mucosal healing can be promoted by HZn-TA nanoparticles, which can upregulate zonula occludens protein 1 (ZO-1) and claudin-1 expression. Based on the results of this study, HZn-TA nanoparticles were able to effectively treat IBD with minimal adverse effects by being biocompatible, multienzyme active, and capable of scavenging RONS. Therefore, we pioneered the application of HZn-TA nanoparticles for the treatment of IBD, which are capable of clearing RONS without significant adverse effects. STATEMENT OF SIGNIFICANCE: ➢ HZn-TA nanoparticles were successfully prepared and could be effectively used to treat IBD. ➢ Intestinal mucosal healing can be promoted by HZn-TA nanoparticles, which can upregulate ZO-1 and claudin-1 expression. ➢ HZn-TA nanoparticles were able to effectively treat IBD with minimal adverse effects by being biocompatible, multienzyme active, and capable of scavenging RONS.

Surfactant-like Additives Assisted the Lateral Growth of Pentacene Films

Lateral growth of thin films is crucial for organic electronic devices, such as field-effect transistors. Here, we report a strategy to improve the lateral growth of pentacene films using rubrene as a surfactant-like additive. Atomic force microscopy (AFM) images confirm the enhanced lateral growth with the presence of rubrene, resulting in smooth and enlarged molecule domains in the films in comparison to those without rubrene. Molecular dynamics simulations are conducted to explore the interlayer diffusion of pentacene molecules during the growth. With the rubrene molecules as surfactant-like additives, mean square displacement (MSD) analysis shows that the pentacene molecules have a descending diffusion coefficient of 2.0 × 10-5 cm2 s-1, which is greater than the ascending diffusion coefficient of 1.6 × 10-5 cm2 s-1. The more descending molecules lead to an enhanced lateral growth of pentacene films, which is in good agreement with the experiments. As a result, the pentacene films grown with rubrene exhibit a rapid increase in carrier mobility over thickness due to the well-connected domains resulting from enhanced lateral growth. This finding will provide a new strategy to modulate the morphology of organic films for high-performance devices.

Biallelic EPCAM deletions induce tissue-specific DNA repair deficiency and cancer predisposition

We report a case of Mismatch Repair Deficiency (MMRD) caused by germline homozygous EPCAM deletion leading to tissue-specific loss of MSH2. Through the use of patient-derived cells and organoid technologies, we performed stepwise in vitro differentiation of colonic and brain organoids from reprogrammed EPCAMdel iPSC derived from patient fibroblasts. Differentiation of iPSC to epithelial-colonic organoids exhibited continuous increased EPCAM expression and hypermethylation of the MSH2 promoter. This was associated with loss of MSH2 expression, increased mutational burden, MMRD signatures and MS-indel accumulation, the hallmarks of MMRD. In contrast, maturation into brain organoids and examination of blood and fibroblasts failed to show similar processes, preserving MMR proficiency. The combined use of iPSC, organoid technologies and functional genomics analyses highlights the potential of cutting-edge cellular and molecular analysis techniques to define processes controlling tumorigenesis and uncovers a new paradigm of tissue-specific MMRD, which affects the clinical management of these patients.

Simultaneous realization of high gain and low DMG of four-mode EDFA under bidirectional hybrid-mode pump

We theoretically and experimentally verify that, the bidirectional hybrid-mode pumping scheme can address the optimization problem of trade-off between high gain and low differential modal gain (DMG) of four-mode erbium-doped fiber amplifier (4M-EDFA), in comparison with traditional both forward and backward hybrid-mode pumping scheme. It is noticed that, when the total pump power is fixed, the bidirectional hybrid-mode pumping scheme can not only achieve higher gain, but also suppress DMG due to different overlap integrals for the forward and backward pumping schemes. The bidirectional hybrid-mode pumped 4M-EDFA is developed with the forward pumping at LP02 mode and the backward pumping at LP21 mode, under a pump power ratio of 30%:70%. Thus, we can achieve an average gain of up to 21.16 dB and a low DMG of 0.43 dB at 1550 nm, and an average gain of up to 20.64 dB with a DMG of less than 1.6 dB over the C-band. In particular, the bidirectional hybrid-mode pumping scheme allows us to tailor the gain characteristics of the few-mode erbium-doped fiber amplifiers (FM-EDFAs), by adjusting the power ratio between forward and backward pumps.

Pairwise Tomlinson-Harashima precoding for multiple-lane IM-DD transmissions

As for the photonic interconnection based on the multiple-lane intensity modulation direct detection (IM-DD) transmission, both intra-channel inter-symbol-interference (ISI) originating from bandwidth constraint, and inter-channel performance discrepancy emerging from inter-channel component differences are the major bottleneck for the throughput enhancement. Here, we propose a pairwise Tomlinson-Harshima precoding (P-THP) scheme, in order to simultaneously deal with both intra-channel ISI and inter-channel performance discrepancy. The effective function of the proposed P-THP scheme is experimentally evaluated by transmitting 4-channel 81-GBaud PAM4 signals over 2 km standard single-mode fiber (SSMF). Compared with the conventional scheme with only applying THP on individual wavelength channel, the required optical received power (ROP) under the back-to-back (B2B) transmission can be reduced by 0.75∼1 dB with the help of proposed P-THP in different experimental component configurations, at the 7% hard decision forward error correction (HD-FEC) threshold of BER = 3.8 × 10-3. After the 2 km SSMF transmission, only the use of proposed P-THP can guarantee to reach the designated HD-FEC threshold, leading to a net rate of >600 Gbit/s.

Fraction of χ_{c} Decays in Prompt J/ψ Production Measured in pPb Collisions at sqrt[s_{NN}]=8.16 TeV

The fraction of χ_{c1} and χ_{c2} decays in the prompt J/ψ yield, F_{χ_{c}→J/ψ}=σ_{χ_{c}→J/ψ}/σ_{J/ψ}, is measured by the LHCb detector in pPb collisions at sqrt[s_{NN}]=8.16  TeV. The study covers the forward (1.5 Collapse

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Affiliation(s)

R Aaij Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
A S W Abdelmotteleb Department of Physics, University of Warwick, Coventry, United Kingdom
C Abellan Beteta Physik-Institut, Universität Zürich, Zürich, Switzerland
F Abudinén Department of Physics, University of Warwick, Coventry, United Kingdom
T Ackernley Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
B Adeva Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
M Adinolfi H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
P Adlarson Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
C Agapopoulou European Organization for Nuclear Research (CERN), Geneva, Switzerland
C A Aidala University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
Z Ajaltouni Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S Akar University of Cincinnati, Cincinnati, Ohio, USA
K Akiba Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
P Albicocco INFN Laboratori Nazionali di Frascati, Frascati, Italy
J Albrecht Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Alessio European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Alexander School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Alfonso Albero ICCUB, Universitat de Barcelona, Barcelona, Spain
Z Aliouche Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
P Alvarez Cartelle Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
R Amalric LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
S Amato Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
J L Amey H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
Y Amhis Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France European Organization for Nuclear Research (CERN), Geneva, Switzerland
L An School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
L Anderlini INFN Sezione di Firenze, Firenze, Italy
M Andersson Physik-Institut, Universität Zürich, Zürich, Switzerland
A Andreianov Affiliated with an institute covered by a cooperation agreement with CERN
P Andreola Physik-Institut, Universität Zürich, Zürich, Switzerland
M Andreotti INFN Sezione di Ferrara, Ferrara, Italy
D Andreou Syracuse University, Syracuse, New York, USA
A A Anelli INFN Sezione di Milano-Bicocca, Milano, Italy
D Ao University of Chinese Academy of Sciences, Beijing, China
F Archilli INFN Sezione di Roma Tor Vergata, Roma, Italy
M Argenton INFN Sezione di Ferrara, Ferrara, Italy
S Arguedas Cuendis Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
A Artamonov Affiliated with an institute covered by a cooperation agreement with CERN
M Artuso Syracuse University, Syracuse, New York, USA
E Aslanides Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
M Atzeni Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
B Audurier Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
D Bacher Department of Physics, University of Oxford, Oxford, United Kingdom
I Bachiller Perea Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
S Bachmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Bachmayer Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J J Back Department of Physics, University of Warwick, Coventry, United Kingdom
A Bailly-Reyre LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
P Baladron Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Balagura Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
W Baldini INFN Sezione di Ferrara, Ferrara, Italy
J Baptista de Souza Leite Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
M Barbetti INFN Sezione di Firenze, Firenze, Italy
I R Barbosa Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil)
R J Barlow Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
S Barsuk Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
W Barter School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Bartolini Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
F Baryshnikov Affiliated with an institute covered by a cooperation agreement with CERN
J M Basels I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
G Bassi INFN Sezione di Pisa, Pisa, Italy
B Batsukh Institute Of High Energy Physics (IHEP), Beijing, China
A Battig Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Bay Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
A Beck Department of Physics, University of Warwick, Coventry, United Kingdom
M Becker Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Bedeschi INFN Sezione di Pisa, Pisa, Italy
I B Bediaga Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
A Beiter Syracuse University, Syracuse, New York, USA
S Belin Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Bellee Physik-Institut, Universität Zürich, Zürich, Switzerland
K Belous Affiliated with an institute covered by a cooperation agreement with CERN
I Belov INFN Sezione di Genova, Genova, Italy
I Belyaev Affiliated with an institute covered by a cooperation agreement with CERN
G Benane Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
G Bencivenni INFN Laboratori Nazionali di Frascati, Frascati, Italy
E Ben-Haim LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
A Berezhnoy Affiliated with an institute covered by a cooperation agreement with CERN
R Bernet Physik-Institut, Universität Zürich, Zürich, Switzerland
S Bernet Andres DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
H C Bernstein Syracuse University, Syracuse, New York, USA
C Bertella Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Bertolin Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
C Betancourt Physik-Institut, Universität Zürich, Zürich, Switzerland
F Betti School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J Bex Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
Ia Bezshyiko Physik-Institut, Universität Zürich, Zürich, Switzerland
J Bhom Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M S Bieker Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
N V Biesuz INFN Sezione di Ferrara, Ferrara, Italy
P Billoir LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
A Biolchini Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Birch Imperial College London, London, United Kingdom
F C R Bishop Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
A Bitadze Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Bizzeti School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
M P Blago Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T Blake Department of Physics, University of Warwick, Coventry, United Kingdom
F Blanc Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J E Blank Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Blusk Syracuse University, Syracuse, New York, USA
D Bobulska School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
V Bocharnikov Affiliated with an institute covered by a cooperation agreement with CERN
J A Boelhauve Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
O Boente Garcia Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
T Boettcher University of Cincinnati, Cincinnati, Ohio, USA
A Bohare School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
A Boldyrev Affiliated with an institute covered by a cooperation agreement with CERN
C S Bolognani Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
R Bolzonella INFN Sezione di Ferrara, Ferrara, Italy
N Bondar Affiliated with an institute covered by a cooperation agreement with CERN
F Borgato Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Borghi Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Borsato INFN Sezione di Milano-Bicocca, Milano, Italy
J T Borsuk Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S A Bouchiba Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
T J V Bowcock Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A Boyer European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Bozzi INFN Sezione di Ferrara, Ferrara, Italy
M J Bradley Imperial College London, London, United Kingdom
S Braun University of Maryland, College Park, Maryland, USA
A Brea Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
N Breer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Brodzicka Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Brossa Gonzalo Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J Brown Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
D Brundu INFN Sezione di Cagliari, Monserrato, Italy
A Buonaura Physik-Institut, Universität Zürich, Zürich, Switzerland
L Buonincontri Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
A T Burke Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C Burr European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Bursche Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
A Butkevich Affiliated with an institute covered by a cooperation agreement with CERN
J S Butter Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J Buytaert European Organization for Nuclear Research (CERN), Geneva, Switzerland
W Byczynski European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Cadeddu INFN Sezione di Cagliari, Monserrato, Italy
H Cai School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
R Calabrese INFN Sezione di Ferrara, Ferrara, Italy
L Calefice Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Cali INFN Laboratori Nazionali di Frascati, Frascati, Italy
M Calvi INFN Sezione di Milano-Bicocca, Milano, Italy
M Calvo Gomez DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
J Cambon Bouzas Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
P Campana INFN Laboratori Nazionali di Frascati, Frascati, Italy
D H Campora Perez Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A F Campoverde Quezada University of Chinese Academy of Sciences, Beijing, China
S Capelli INFN Sezione di Milano-Bicocca, Milano, Italy
L Capriotti INFN Sezione di Ferrara, Ferrara, Italy
R Caravaca-Mora Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
A Carbone INFN Sezione di Bologna, Bologna, Italy
L Carcedo Salgado Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Cardinale INFN Sezione di Genova, Genova, Italy
A Cardini INFN Sezione di Cagliari, Monserrato, Italy
P Carniti INFN Sezione di Milano-Bicocca, Milano, Italy
L Carus Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Casais Vidal Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
R Caspary Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G Casse Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
J Castro Godinez Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
M Cattaneo European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Cavallero INFN Sezione di Ferrara, Ferrara, Italy
V Cavallini INFN Sezione di Ferrara, Ferrara, Italy
S Celani Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J Cerasoli Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
D Cervenkov Department of Physics, University of Oxford, Oxford, United Kingdom
S Cesare INFN Sezione di Milano, Milano, Italy
A J Chadwick Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
I Chahrour University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Charles LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
Ph Charpentier European Organization for Nuclear Research (CERN), Geneva, Switzerland
C A Chavez Barajas Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Chefdeville Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
C Chen Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
S Chen Institute Of High Energy Physics (IHEP), Beijing, China
A Chernov Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S Chernyshenko Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
V Chobanova Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Cholak Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Chrzaszcz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Chubykin Affiliated with an institute covered by a cooperation agreement with CERN
V Chulikov Affiliated with an institute covered by a cooperation agreement with CERN
P Ciambrone INFN Laboratori Nazionali di Frascati, Frascati, Italy
M F Cicala Department of Physics, University of Warwick, Coventry, United Kingdom
X Cid Vidal Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Ciezarek European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Cifra European Organization for Nuclear Research (CERN), Geneva, Switzerland
P E L Clarke School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Clemencic European Organization for Nuclear Research (CERN), Geneva, Switzerland
H V Cliff Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J Closier European Organization for Nuclear Research (CERN), Geneva, Switzerland
J L Cobbledick Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C Cocha Toapaxi Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Coco European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Cogan Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
E Cogneras Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L Cojocariu Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
P Collins European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Colombo European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Comerma-Montells ICCUB, Universitat de Barcelona, Barcelona, Spain
L Congedo INFN Sezione di Bari, Bari, Italy
A Contu INFN Sezione di Cagliari, Monserrato, Italy
N Cooke School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
I Corredoira Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Correia LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
G Corti European Organization for Nuclear Research (CERN), Geneva, Switzerland
J J Cottee Meldrum H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
B Couturier European Organization for Nuclear Research (CERN), Geneva, Switzerland
D C Craik Physik-Institut, Universität Zürich, Zürich, Switzerland
M Cruz Torres Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
R Currie School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
C L Da Silva Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
S Dadabaev Affiliated with an institute covered by a cooperation agreement with CERN
L Dai School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
X Dai School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
E Dall'Occo Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Dalseno Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
C D'Ambrosio European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Daniel Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Danilina Affiliated with an institute covered by a cooperation agreement with CERN
P d'Argent INFN Sezione di Bari, Bari, Italy
A Davidson Department of Physics, University of Warwick, Coventry, United Kingdom
J E Davies Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
A Davis Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
O De Aguiar Francisco Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
C De Angelis INFN Sezione di Cagliari, Monserrato, Italy
J de Boer Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
K De Bruyn Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
S De Capua Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M De Cian Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany European Organization for Nuclear Research (CERN), Geneva, Switzerland
U De Freitas Carneiro Da Graca Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
E De Lucia INFN Laboratori Nazionali di Frascati, Frascati, Italy
J M De Miranda Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L De Paula Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
M De Serio INFN Sezione di Bari, Bari, Italy
D De Simone Physik-Institut, Universität Zürich, Zürich, Switzerland
P De Simone INFN Laboratori Nazionali di Frascati, Frascati, Italy
F De Vellis Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J A de Vries Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
F Debernardis INFN Sezione di Bari, Bari, Italy
D Decamp Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
V Dedu Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
L Del Buono LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
B Delaney Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
H-P Dembinski Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Deng Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
V Denysenko Physik-Institut, Universität Zürich, Zürich, Switzerland
O Deschamps Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
F Dettori INFN Sezione di Cagliari, Monserrato, Italy
B Dey Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland)
P Di Nezza INFN Laboratori Nazionali di Frascati, Frascati, Italy
I Diachkov Affiliated with an institute covered by a cooperation agreement with CERN
S Didenko Affiliated with an institute covered by a cooperation agreement with CERN
S Ding Syracuse University, Syracuse, New York, USA
V Dobishuk Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
A D Docheva School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Dolmatov Affiliated with an institute covered by a cooperation agreement with CERN
C Dong Center for High Energy Physics, Tsinghua University, Beijing, China
A M Donohoe School of Physics, University College Dublin, Dublin, Ireland
F Dordei INFN Sezione di Cagliari, Monserrato, Italy
A C Dos Reis Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L Douglas School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A G Downes Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
W Duan Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
P Duda Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
M W Dudek Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
L Dufour European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Duk INFN Sezione di Perugia, Perugia, Italy
P Durante European Organization for Nuclear Research (CERN), Geneva, Switzerland
M M Duras Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
J M Durham Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
A Dziurda Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
A Dzyuba Affiliated with an institute covered by a cooperation agreement with CERN
S Easo European Organization for Nuclear Research (CERN), Geneva, Switzerland STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
E Eckstein Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
U Egede School of Physics and Astronomy, Monash University, Melbourne, Australia
A Egorychev Affiliated with an institute covered by a cooperation agreement with CERN
V Egorychev Affiliated with an institute covered by a cooperation agreement with CERN
C Eirea Orro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Eisenhardt School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
E Ejopu Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
S Ek-In Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
L Eklund Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
M Elashri University of Cincinnati, Cincinnati, Ohio, USA
J Ellbracht Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Ely Imperial College London, London, United Kingdom
A Ene Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
E Epple University of Cincinnati, Cincinnati, Ohio, USA
S Escher I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
J Eschle Physik-Institut, Universität Zürich, Zürich, Switzerland
S Esen Physik-Institut, Universität Zürich, Zürich, Switzerland
T Evans Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
F Fabiano INFN Sezione di Cagliari, Monserrato, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
L N Falcao Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
Y Fan University of Chinese Academy of Sciences, Beijing, China
B Fang Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
L Fantini INFN Sezione di Perugia, Perugia, Italy
M Faria Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
K Farmer School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
D Fazzini INFN Sezione di Milano-Bicocca, Milano, Italy
L Felkowski Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
M Feng Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
M Feo European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Fernandez Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A D Fernez University of Maryland, College Park, Maryland, USA
F Ferrari INFN Sezione di Bologna, Bologna, Italy
F Ferreira Rodrigues Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
S Ferreres Sole Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Ferrillo Physik-Institut, Universität Zürich, Zürich, Switzerland
M Ferro-Luzzi European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Filippov Affiliated with an institute covered by a cooperation agreement with CERN
R A Fini INFN Sezione di Bari, Bari, Italy
M Fiorini INFN Sezione di Ferrara, Ferrara, Italy
M Firlej AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
K M Fischer Department of Physics, University of Oxford, Oxford, United Kingdom
D S Fitzgerald University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
C Fitzpatrick Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
T Fiutowski AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
F Fleuret Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
M Fontana INFN Sezione di Bologna, Bologna, Italy
F Fontanelli INFN Sezione di Genova, Genova, Italy
L F Foreman Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Forty European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Foulds-Holt Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
M Franco Sevilla University of Maryland, College Park, Maryland, USA
M Frank European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Franzoso INFN Sezione di Ferrara, Ferrara, Italy
G Frau Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Frei European Organization for Nuclear Research (CERN), Geneva, Switzerland
D A Friday Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
L Frontini INFN Sezione di Milano, Milano, Italy
J Fu University of Chinese Academy of Sciences, Beijing, China
Q Fuehring Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
Y Fujii School of Physics and Astronomy, Monash University, Melbourne, Australia
T Fulghesu LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
E Gabriel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
G Galati INFN Sezione di Bari, Bari, Italy
M D Galati Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
A Gallas Torreira Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
D Galli INFN Sezione di Bologna, Bologna, Italy
S Gambetta European Organization for Nuclear Research (CERN), Geneva, Switzerland School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Gandelman Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
P Gandini INFN Sezione di Milano, Milano, Italy
H Gao University of Chinese Academy of Sciences, Beijing, China
R Gao Department of Physics, University of Oxford, Oxford, United Kingdom
Y Gao Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Gao School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Gao Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
M Garau INFN Sezione di Cagliari, Monserrato, Italy
L M Garcia Martin Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
P Garcia Moreno ICCUB, Universitat de Barcelona, Barcelona, Spain
J García Pardiñas European Organization for Nuclear Research (CERN), Geneva, Switzerland
B Garcia Plana Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
K G Garg Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
L Garrido ICCUB, Universitat de Barcelona, Barcelona, Spain
C Gaspar European Organization for Nuclear Research (CERN), Geneva, Switzerland
R E Geertsema Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L L Gerken Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Gersabeck Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Gersabeck Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
T Gershon Department of Physics, University of Warwick, Coventry, United Kingdom
Z Ghorbanimoghaddam H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
L Giambastiani Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
F I Giasemis LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
V Gibson Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
H K Giemza National Center for Nuclear Research (NCBJ), Warsaw, Poland
A L Gilman Department of Physics, University of Oxford, Oxford, United Kingdom
M Giovannetti INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Gioventù ICCUB, Universitat de Barcelona, Barcelona, Spain
P Gironella Gironell ICCUB, Universitat de Barcelona, Barcelona, Spain
C Giugliano INFN Sezione di Ferrara, Ferrara, Italy
M A Giza Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
E L Gkougkousis Imperial College London, London, United Kingdom
F C Glaser Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V V Gligorov LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
C Göbel Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil)
E Golobardes DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
D Golubkov Affiliated with an institute covered by a cooperation agreement with CERN
A Golutvin Affiliated with an institute covered by a cooperation agreement with CERN European Organization for Nuclear Research (CERN), Geneva, Switzerland Imperial College London, London, United Kingdom
A Gomes Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
S Gomez Fernandez ICCUB, Universitat de Barcelona, Barcelona, Spain
F Goncalves Abrantes Department of Physics, University of Oxford, Oxford, United Kingdom
M Goncerz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
G Gong Center for High Energy Physics, Tsinghua University, Beijing, China
J A Gooding Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
I V Gorelov Affiliated with an institute covered by a cooperation agreement with CERN
C Gotti INFN Sezione di Milano-Bicocca, Milano, Italy
J P Grabowski Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
L A Granado Cardoso European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Graugés ICCUB, Universitat de Barcelona, Barcelona, Spain
E Graverini Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
L Grazette Department of Physics, University of Warwick, Coventry, United Kingdom
G Graziani School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
A T Grecu Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
L M Greeven Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
N A Grieser University of Cincinnati, Cincinnati, Ohio, USA
L Grillo School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
S Gromov Affiliated with an institute covered by a cooperation agreement with CERN
C Gu Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
M Guarise INFN Sezione di Ferrara, Ferrara, Italy
M Guittiere Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
V Guliaeva Affiliated with an institute covered by a cooperation agreement with CERN
P A Günther Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A-K Guseinov Affiliated with an institute covered by a cooperation agreement with CERN
E Gushchin Affiliated with an institute covered by a cooperation agreement with CERN
Y Guz School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China Affiliated with an institute covered by a cooperation agreement with CERN European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Gys European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Hadavizadeh School of Physics and Astronomy, Monash University, Melbourne, Australia
C Hadjivasiliou University of Maryland, College Park, Maryland, USA
G Haefeli Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
C Haen European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Haimberger European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Hajheidari European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Halewood-Leagas Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M M Halvorsen European Organization for Nuclear Research (CERN), Geneva, Switzerland
P M Hamilton University of Maryland, College Park, Maryland, USA
J Hammerich Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
Q Han Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
X Han Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Hansmann-Menzemer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L Hao University of Chinese Academy of Sciences, Beijing, China
N Harnew Department of Physics, University of Oxford, Oxford, United Kingdom
T Harrison Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Hartmann Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
C Hasse European Organization for Nuclear Research (CERN), Geneva, Switzerland
J He University of Chinese Academy of Sciences, Beijing, China
K Heijhoff Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
F Hemmer European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Henderson University of Cincinnati, Cincinnati, Ohio, USA
R D L Henderson School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
A M Hennequin European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Hennessy Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
L Henry Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J Herd Imperial College London, London, United Kingdom
J Heuel I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
A Hicheur Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
D Hill Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
S E Hollitt Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
J Horswill Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Hou Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Hou Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
N Howarth Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
J Hu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Hu Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
W Hu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
X Hu Center for High Energy Physics, Tsinghua University, Beijing, China
W Huang University of Chinese Academy of Sciences, Beijing, China
W Hulsbergen Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
R J Hunter Department of Physics, University of Warwick, Coventry, United Kingdom
M Hushchyn Affiliated with an institute covered by a cooperation agreement with CERN
D Hutchcroft Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
M Idzik AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
D Ilin Affiliated with an institute covered by a cooperation agreement with CERN
P Ilten University of Cincinnati, Cincinnati, Ohio, USA
A Inglessi Affiliated with an institute covered by a cooperation agreement with CERN
A Iniukhin Affiliated with an institute covered by a cooperation agreement with CERN
A Ishteev Affiliated with an institute covered by a cooperation agreement with CERN
K Ivshin Affiliated with an institute covered by a cooperation agreement with CERN
R Jacobsson European Organization for Nuclear Research (CERN), Geneva, Switzerland
H Jage I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S J Jaimes Elles Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
S Jakobsen European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Jans Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
B K Jashal Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
A Jawahery University of Maryland, College Park, Maryland, USA
V Jevtic Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Jiang University of Maryland, College Park, Maryland, USA
X Jiang Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
Y Jiang University of Chinese Academy of Sciences, Beijing, China
Y J Jiang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
M John Department of Physics, University of Oxford, Oxford, United Kingdom
D Johnson University of Birmingham, Birmingham, United Kingdom
C R Jones Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T P Jones Department of Physics, University of Warwick, Coventry, United Kingdom
S Joshi National Center for Nuclear Research (NCBJ), Warsaw, Poland
B Jost European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Jurik European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Juszczak Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
D Kaminaris Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
S Kandybei NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine
Y Kang Center for High Energy Physics, Tsinghua University, Beijing, China
M Karacson European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Karpenkov Affiliated with an institute covered by a cooperation agreement with CERN
M Karpov Affiliated with an institute covered by a cooperation agreement with CERN
A M Kauniskangas Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
J W Kautz University of Cincinnati, Cincinnati, Ohio, USA
F Keizer European Organization for Nuclear Research (CERN), Geneva, Switzerland
D M Keller Syracuse University, Syracuse, New York, USA
M Kenzie Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
T Ketel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
B Khanji Syracuse University, Syracuse, New York, USA
A Kharisova Affiliated with an institute covered by a cooperation agreement with CERN
S Kholodenko INFN Sezione di Pisa, Pisa, Italy
G Khreich Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
T Kirn I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
V S Kirsebom Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
O Kitouni Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
S Klaver Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
N Kleijne INFN Sezione di Pisa, Pisa, Italy
K Klimaszewski National Center for Nuclear Research (NCBJ), Warsaw, Poland
M R Kmiec National Center for Nuclear Research (NCBJ), Warsaw, Poland
S Koliiev Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
L Kolk Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Konoplyannikov Affiliated with an institute covered by a cooperation agreement with CERN
P Kopciewicz AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Koppenburg Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Korolev Affiliated with an institute covered by a cooperation agreement with CERN
I Kostiuk Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
O Kot Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
S Kotriakhova School of Physics and Astronomy, Monash University, Melbourne, Australia Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil Center for High Energy Physics, Tsinghua University, Beijing, China Institute Of High Energy Physics (IHEP), Beijing, China School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China University of Chinese Academy of Sciences, Beijing, China Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany School of Physics, University College Dublin, Dublin, Ireland INFN Sezione di Bari, Bari, Italy INFN Sezione di Bologna, Bologna, Italy INFN Sezione di Ferrara, Ferrara, Italy INFN Sezione di Firenze, Firenze, Italy INFN Laboratori Nazionali di Frascati, Frascati, Italy INFN Sezione di Genova, Genova, Italy INFN Sezione di Milano, Milano, Italy INFN Sezione di Milano-Bicocca, Milano, Italy INFN Sezione di Cagliari, Monserrato, Italy Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy INFN Sezione di Perugia, Perugia, Italy INFN Sezione di Pisa, Pisa, Italy INFN Sezione di Roma La Sapienza, Roma, Italy INFN Sezione di Roma Tor Vergata, Roma, Italy Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland National Center for Nuclear Research (NCBJ), Warsaw, Poland Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania Affiliated with an institute covered by a cooperation agreement with CERN DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain ICCUB, Universitat de Barcelona, Barcelona, Spain Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine University of Birmingham, Birmingham, United Kingdom H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom Department of Physics, University of Warwick, Coventry, United Kingdom STFC Rutherford Appleton Laboratory, Didcot, United Kingdom School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom Imperial College London, London, United Kingdom Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom Department of Physics, University of Oxford, Oxford, United Kingdom Massachusetts Institute of Technology, Cambridge, Massachusetts, USA University of Cincinnati, Cincinnati, Ohio, USA University of Maryland, College Park, Maryland, USA Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA Syracuse University, Syracuse, New York, USA Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil (associated with Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil) School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China) Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China) School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China) Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France) Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany) Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland) Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland) Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom) University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA) Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
A Kozachuk Affiliated with an institute covered by a cooperation agreement with CERN
P Kravchenko Affiliated with an institute covered by a cooperation agreement with CERN
L Kravchuk Affiliated with an institute covered by a cooperation agreement with CERN
M Kreps Department of Physics, University of Warwick, Coventry, United Kingdom
S Kretzschmar I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
P Krokovny Affiliated with an institute covered by a cooperation agreement with CERN
W Krupa Syracuse University, Syracuse, New York, USA
W Krzemien National Center for Nuclear Research (NCBJ), Warsaw, Poland
J Kubat Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Kubis Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland (associated with Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland)
W Kucewicz Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M Kucharczyk Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
V Kudryavtsev Affiliated with an institute covered by a cooperation agreement with CERN
E Kulikova Affiliated with an institute covered by a cooperation agreement with CERN
A Kupsc Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
B K Kutsenko Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
D Lacarrere European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Lai INFN Sezione di Cagliari, Monserrato, Italy
A Lampis INFN Sezione di Cagliari, Monserrato, Italy
D Lancierini Physik-Institut, Universität Zürich, Zürich, Switzerland
C Landesa Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J J Lane School of Physics and Astronomy, Monash University, Melbourne, Australia
R Lane H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
C Langenbruch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Langer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
O Lantwin Affiliated with an institute covered by a cooperation agreement with CERN
T Latham Department of Physics, University of Warwick, Coventry, United Kingdom
F Lazzari INFN Sezione di Pisa, Pisa, Italy
C Lazzeroni University of Birmingham, Birmingham, United Kingdom
R Le Gac Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
S H Lee University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
R Lefèvre Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Leflat Affiliated with an institute covered by a cooperation agreement with CERN
S Legotin Affiliated with an institute covered by a cooperation agreement with CERN
M Lehuraux Department of Physics, University of Warwick, Coventry, United Kingdom
O Leroy Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
T Lesiak Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
B Leverington Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Li Center for High Energy Physics, Tsinghua University, Beijing, China
H Li Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
K Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
L Li Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
P Li European Organization for Nuclear Research (CERN), Geneva, Switzerland
P-R Li Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
S Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
T Li Institute Of High Energy Physics (IHEP), Beijing, China
T Li Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Y Li Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Li Institute Of High Energy Physics (IHEP), Beijing, China
Z Li Syracuse University, Syracuse, New York, USA
Z Lian Center for High Energy Physics, Tsinghua University, Beijing, China
X Liang Syracuse University, Syracuse, New York, USA
C Lin University of Chinese Academy of Sciences, Beijing, China
T Lin STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
R Lindner European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Lisovskyi Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R Litvinov INFN Sezione di Cagliari, Monserrato, Italy
G Liu Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
H Liu University of Chinese Academy of Sciences, Beijing, China
K Liu Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
Q Liu University of Chinese Academy of Sciences, Beijing, China
S Liu Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
Y Liu School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
Y Liu Lanzhou University, Lanzhou, China (associated with Institute Of High Energy Physics (IHEP), Beijing, China)
Y L Liu Imperial College London, London, United Kingdom
A Lobo Salvia ICCUB, Universitat de Barcelona, Barcelona, Spain
A Loi INFN Sezione di Cagliari, Monserrato, Italy
J Lomba Castro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
T Long Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
J H Lopes Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
A Lopez Huertas ICCUB, Universitat de Barcelona, Barcelona, Spain
S López Soliño Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G H Lovell Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
C Lucarelli INFN Sezione di Firenze, Firenze, Italy
D Lucchesi Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
S Luchuk Affiliated with an institute covered by a cooperation agreement with CERN
M Lucio Martinez Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
V Lukashenko Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
Y Luo Center for High Energy Physics, Tsinghua University, Beijing, China
A Lupato Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
E Luppi INFN Sezione di Ferrara, Ferrara, Italy
K Lynch School of Physics, University College Dublin, Dublin, Ireland
X-R Lyu University of Chinese Academy of Sciences, Beijing, China
G M Ma Center for High Energy Physics, Tsinghua University, Beijing, China
R Ma University of Chinese Academy of Sciences, Beijing, China
S Maccolini Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
F Machefert Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
F Maciuc Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
I Mackay Department of Physics, University of Oxford, Oxford, United Kingdom
L R Madhan Mohan Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
M M Madurai University of Birmingham, Birmingham, United Kingdom
A Maevskiy Affiliated with an institute covered by a cooperation agreement with CERN
D Magdalinski Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
D Maisuzenko Affiliated with an institute covered by a cooperation agreement with CERN
M W Majewski AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J J Malczewski Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
S Malde Department of Physics, University of Oxford, Oxford, United Kingdom
B Malecki Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Malentacca European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Malinin Affiliated with an institute covered by a cooperation agreement with CERN
T Maltsev Affiliated with an institute covered by a cooperation agreement with CERN
G Manca INFN Sezione di Cagliari, Monserrato, Italy
G Mancinelli Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
C Mancuso Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France INFN Sezione di Milano, Milano, Italy
R Manera Escalero ICCUB, Universitat de Barcelona, Barcelona, Spain
D Manuzzi INFN Sezione di Bologna, Bologna, Italy
D Marangotto INFN Sezione di Milano, Milano, Italy
J F Marchand Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
R Marchevski Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
U Marconi INFN Sezione di Bologna, Bologna, Italy
S Mariani European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Marin Benito ICCUB, Universitat de Barcelona, Barcelona, Spain European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Marks Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A M Marshall H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
P J Marshall Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
G Martelli INFN Sezione di Perugia, Perugia, Italy
G Martellotti INFN Sezione di Roma La Sapienza, Roma, Italy
L Martinazzoli European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Martinelli INFN Sezione di Milano-Bicocca, Milano, Italy
D Martinez Santos Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
F Martinez Vidal Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
A Massafferri Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
M Materok I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
R Matev European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Mathad Physik-Institut, Universität Zürich, Zürich, Switzerland
V Matiunin Affiliated with an institute covered by a cooperation agreement with CERN
C Matteuzzi Syracuse University, Syracuse, New York, USA
K R Mattioli Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
A Mauri Imperial College London, London, United Kingdom
E Maurice Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
J Mauricio ICCUB, Universitat de Barcelona, Barcelona, Spain
P Mayencourt Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Mazurek European Organization for Nuclear Research (CERN), Geneva, Switzerland
M McCann Imperial College London, London, United Kingdom
L Mcconnell School of Physics, University College Dublin, Dublin, Ireland
T H McGrath Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
N T McHugh School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A McNab Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R McNulty School of Physics, University College Dublin, Dublin, Ireland
B Meadows University of Cincinnati, Cincinnati, Ohio, USA
G Meier Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Melnychuk National Center for Nuclear Research (NCBJ), Warsaw, Poland
M Merk Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A Merli INFN Sezione di Milano, Milano, Italy
L Meyer Garcia Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
D Miao Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
H Miao University of Chinese Academy of Sciences, Beijing, China
M Mikhasenko Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
D A Milanes Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
A Minotti INFN Sezione di Milano-Bicocca, Milano, Italy
E Minucci Syracuse University, Syracuse, New York, USA
T Miralles Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S E Mitchell School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
B Mitreska Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D S Mitzel Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
A Modak STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
A Mödden Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
R A Mohammed Department of Physics, University of Oxford, Oxford, United Kingdom
R D Moise I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Mokhnenko Affiliated with an institute covered by a cooperation agreement with CERN
T Mombächer European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Monk School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
I A Monroy Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
S Monteil Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Morcillo Gomez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Morello INFN Laboratori Nazionali di Frascati, Frascati, Italy
M J Morello INFN Sezione di Pisa, Pisa, Italy
M P Morgenthaler Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Moron AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
A B Morris European Organization for Nuclear Research (CERN), Geneva, Switzerland
A G Morris Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
R Mountain Syracuse University, Syracuse, New York, USA
H Mu Center for High Energy Physics, Tsinghua University, Beijing, China
Z M Mu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
E Muhammad Department of Physics, University of Warwick, Coventry, United Kingdom
F Muheim School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Mulder Van Swinderen Institute, University of Groningen, Groningen, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
K Müller Physik-Institut, Universität Zürich, Zürich, Switzerland
F Mũnoz-Rojas Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica
R Murta Imperial College London, London, United Kingdom
P Naik Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
T Nakada Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R Nandakumar STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
T Nanut European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Nasteva Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
M Needham School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
N Neri INFN Sezione di Milano, Milano, Italy
S Neubert Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
N Neufeld European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Neustroev Affiliated with an institute covered by a cooperation agreement with CERN
R Newcombe Imperial College London, London, United Kingdom
J Nicolini Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Nicotra Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
E M Niel Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
N Nikitin Affiliated with an institute covered by a cooperation agreement with CERN
P Nogga Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
N S Nolte Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
C Normand Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France INFN Sezione di Cagliari, Monserrato, Italy
J Novoa Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Nowak University of Cincinnati, Cincinnati, Ohio, USA
C Nunez University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
H N Nur School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Oblakowska-Mucha AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
V Obraztsov Affiliated with an institute covered by a cooperation agreement with CERN
T Oeser I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Okamura INFN Sezione di Ferrara, Ferrara, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Oldeman INFN Sezione di Cagliari, Monserrato, Italy
F Oliva School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Olocco Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
C J G Onderwater Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
R H O'Neil School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J M Otalora Goicochea Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
T Ovsiannikova Affiliated with an institute covered by a cooperation agreement with CERN
P Owen Physik-Institut, Universität Zürich, Zürich, Switzerland
A Oyanguren Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
O Ozcelik School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
K O Padeken Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
B Pagare Department of Physics, University of Warwick, Coventry, United Kingdom
P R Pais Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
T Pajero Department of Physics, University of Oxford, Oxford, United Kingdom
A Palano INFN Sezione di Bari, Bari, Italy
M Palutan INFN Laboratori Nazionali di Frascati, Frascati, Italy
G Panshin Affiliated with an institute covered by a cooperation agreement with CERN
L Paolucci Department of Physics, University of Warwick, Coventry, United Kingdom
A Papanestis STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
M Pappagallo INFN Sezione di Bari, Bari, Italy
L L Pappalardo INFN Sezione di Ferrara, Ferrara, Italy
C Pappenheimer University of Cincinnati, Cincinnati, Ohio, USA
C Parkes Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
B Passalacqua INFN Sezione di Ferrara, Ferrara, Italy
G Passaleva INFN Sezione di Firenze, Firenze, Italy
D Passaro INFN Sezione di Pisa, Pisa, Italy
A Pastore INFN Sezione di Bari, Bari, Italy
M Patel Imperial College London, London, United Kingdom
J Patoc Department of Physics, University of Oxford, Oxford, United Kingdom
C Patrignani INFN Sezione di Bologna, Bologna, Italy
C J Pawley Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
A Pellegrino Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
M Pepe Altarelli INFN Laboratori Nazionali di Frascati, Frascati, Italy
S Perazzini INFN Sezione di Bologna, Bologna, Italy
D Pereima Affiliated with an institute covered by a cooperation agreement with CERN
A Pereiro Castro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
P Perret Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
A Perro European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Petridis H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
A Petrolini INFN Sezione di Genova, Genova, Italy
S Petrucci School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
H Pham Syracuse University, Syracuse, New York, USA
L Pica INFN Sezione di Pisa, Pisa, Italy
M Piccini INFN Sezione di Perugia, Perugia, Italy
B Pietrzyk Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
G Pietrzyk Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
D Pinci INFN Sezione di Roma La Sapienza, Roma, Italy
F Pisani European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Pizzichemi INFN Sezione di Milano-Bicocca, Milano, Italy
V Placinta Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania
M Plo Casasus Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
F Polci LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Poli Lener INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Poluektov Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
N Polukhina Affiliated with an institute covered by a cooperation agreement with CERN
I Polyakov European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Polycarpo Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
S Ponce European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Popov University of Chinese Academy of Sciences, Beijing, China
S Poslavskii Affiliated with an institute covered by a cooperation agreement with CERN
K Prasanth Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
C Prouve Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
V Pugatch Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine
V Puill Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
G Punzi INFN Sezione di Pisa, Pisa, Italy
H R Qi Center for High Energy Physics, Tsinghua University, Beijing, China
W Qian University of Chinese Academy of Sciences, Beijing, China
N Qin Center for High Energy Physics, Tsinghua University, Beijing, China
S Qu Center for High Energy Physics, Tsinghua University, Beijing, China
R Quagliani Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
R I Rabadan Trejo Department of Physics, University of Warwick, Coventry, United Kingdom
B Rachwal AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J H Rademacker H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
M Rama INFN Sezione di Pisa, Pisa, Italy
M Ramírez García University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Ramos Pernas Department of Physics, University of Warwick, Coventry, United Kingdom
M S Rangel Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
F Ratnikov Affiliated with an institute covered by a cooperation agreement with CERN
G Raven Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
M Rebollo De Miguel Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
F Redi European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Reich H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
F Reiss Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
Z Ren University of Chinese Academy of Sciences, Beijing, China
P K Resmi Department of Physics, University of Oxford, Oxford, United Kingdom
R Ribatti INFN Sezione di Pisa, Pisa, Italy
G R Ricart Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France Departement de Physique Nucleaire (SPhN), Gif-Sur-Yvette, France
D Riccardi INFN Sezione di Pisa, Pisa, Italy
S Ricciardi STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
K Richardson Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
M Richardson-Slipper School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
K Rinnert Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
P Robbe Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
G Robertson School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
E Rodrigues European Organization for Nuclear Research (CERN), Geneva, Switzerland Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
E Rodriguez Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J A Rodriguez Lopez Departamento de Fisica, Universidad Nacional de Colombia, Bogota, Colombia (associated with LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France)
E Rodriguez Rodriguez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Rogovskiy STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
D L Rolf European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Rollings Department of Physics, University of Oxford, Oxford, United Kingdom
P Roloff European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Romanovskiy Affiliated with an institute covered by a cooperation agreement with CERN
M Romero Lamas Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Romero Vidal Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
G Romolini INFN Sezione di Ferrara, Ferrara, Italy
F Ronchetti Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Rotondo INFN Laboratori Nazionali di Frascati, Frascati, Italy
S R Roy Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M S Rudolph Syracuse University, Syracuse, New York, USA
T Ruf European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Ruiz Diaz Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R A Ruiz Fernandez Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
J Ruiz Vidal Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)
A Ryzhikov Affiliated with an institute covered by a cooperation agreement with CERN
J Ryzka AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
J J Saborido Silva Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Sadek Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France
N Sagidova Affiliated with an institute covered by a cooperation agreement with CERN
N Sahoo University of Birmingham, Birmingham, United Kingdom
B Saitta INFN Sezione di Cagliari, Monserrato, Italy
M Salomoni INFN Sezione di Milano-Bicocca, Milano, Italy
C Sanchez Gras Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
I Sanderswood Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
R Santacesaria INFN Sezione di Roma La Sapienza, Roma, Italy
C Santamarina Rios Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
M Santimaria INFN Laboratori Nazionali di Frascati, Frascati, Italy
L Santoro Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
E Santovetti INFN Sezione di Roma Tor Vergata, Roma, Italy
A Saputi INFN Sezione di Ferrara, Ferrara, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Saranin Affiliated with an institute covered by a cooperation agreement with CERN
G Sarpis School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M Sarpis Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
A Sarti INFN Sezione di Roma La Sapienza, Roma, Italy
C Satriano INFN Sezione di Roma La Sapienza, Roma, Italy
A Satta INFN Sezione di Roma Tor Vergata, Roma, Italy
M Saur School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Savrina Affiliated with an institute covered by a cooperation agreement with CERN
H Sazak Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L G Scantlebury Smead Department of Physics, University of Oxford, Oxford, United Kingdom
A Scarabotto LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
S Schael I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
S Scherl Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A M Schertz Eotvos Lorand University, Budapest, Hungary (associated with European Organization for Nuclear Research (CERN), Geneva, Switzerland)
M Schiller School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
H Schindler European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Schmelling Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
B Schmidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Schmitt I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
H Schmitz Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany (associated with Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany)
O Schneider Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
A Schopper European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Schulte Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
S Schulte Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M H Schune Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
R Schwemmer European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Schwering I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany
B Sciascia INFN Laboratori Nazionali di Frascati, Frascati, Italy
A Sciuccati European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Sellam Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
A Semennikov Affiliated with an institute covered by a cooperation agreement with CERN
M Senghi Soares Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
A Sergi INFN Sezione di Genova, Genova, Italy
N Serra European Organization for Nuclear Research (CERN), Geneva, Switzerland Physik-Institut, Universität Zürich, Zürich, Switzerland
L Sestini Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
A Seuthe Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
Y Shang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D M Shangase University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)
M Shapkin Affiliated with an institute covered by a cooperation agreement with CERN
I Shchemerov Affiliated with an institute covered by a cooperation agreement with CERN
L Shchutska Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
T Shears Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
L Shekhtman Affiliated with an institute covered by a cooperation agreement with CERN
Z Shen School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
S Sheng Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
V Shevchenko Affiliated with an institute covered by a cooperation agreement with CERN
B Shi University of Chinese Academy of Sciences, Beijing, China
E B Shields INFN Sezione di Milano-Bicocca, Milano, Italy
Y Shimizu Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
E Shmanin Affiliated with an institute covered by a cooperation agreement with CERN
R Shorkin Affiliated with an institute covered by a cooperation agreement with CERN
J D Shupperd Syracuse University, Syracuse, New York, USA
R Silva Coutinho Syracuse University, Syracuse, New York, USA
G Simi Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
S Simone INFN Sezione di Bari, Bari, Italy
N Skidmore Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
R Skuza Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
T Skwarnicki Syracuse University, Syracuse, New York, USA
M W Slater University of Birmingham, Birmingham, United Kingdom
J C Smallwood Department of Physics, University of Oxford, Oxford, United Kingdom
E Smith Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
K Smith Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
M Smith Imperial College London, London, United Kingdom
A Snoch Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L Soares Lavra School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
M D Sokoloff University of Cincinnati, Cincinnati, Ohio, USA
F J P Soler School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A Solomin Affiliated with an institute covered by a cooperation agreement with CERN H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
A Solovev Affiliated with an institute covered by a cooperation agreement with CERN
I Solovyev Affiliated with an institute covered by a cooperation agreement with CERN
R Song School of Physics and Astronomy, Monash University, Melbourne, Australia
Y Song Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
Y Song Center for High Energy Physics, Tsinghua University, Beijing, China
Y S Song School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
F L Souza De Almeida Syracuse University, Syracuse, New York, USA
B Souza De Paula Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil
E Spadaro Norella INFN Sezione di Milano, Milano, Italy
E Spedicato INFN Sezione di Bologna, Bologna, Italy
J G Speer Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
E Spiridenkov Affiliated with an institute covered by a cooperation agreement with CERN
P Spradlin School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
V Sriskaran European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Stagni European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Stahl European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Stahl European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Stanislaus Department of Physics, University of Oxford, Oxford, United Kingdom
E N Stein European Organization for Nuclear Research (CERN), Geneva, Switzerland
O Steinkamp Physik-Institut, Universität Zürich, Zürich, Switzerland
O Stenyakin Affiliated with an institute covered by a cooperation agreement with CERN
H Stevens Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Strekalina Affiliated with an institute covered by a cooperation agreement with CERN
Y Su University of Chinese Academy of Sciences, Beijing, China
F Suljik Department of Physics, University of Oxford, Oxford, United Kingdom
J Sun INFN Sezione di Cagliari, Monserrato, Italy
L Sun School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Y Sun University of Maryland, College Park, Maryland, USA
P N Swallow University of Birmingham, Birmingham, United Kingdom
K Swientek AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
F Swystun Department of Physics, University of Warwick, Coventry, United Kingdom
A Szabelski National Center for Nuclear Research (NCBJ), Warsaw, Poland
T Szumlak AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
M Szymanski European Organization for Nuclear Research (CERN), Geneva, Switzerland
Y Tan Center for High Energy Physics, Tsinghua University, Beijing, China
S Taneja Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M D Tat Department of Physics, University of Oxford, Oxford, United Kingdom
A Terentev Physik-Institut, Universität Zürich, Zürich, Switzerland
F Terzuoli INFN Sezione di Pisa, Pisa, Italy
F Teubert European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Thomas European Organization for Nuclear Research (CERN), Geneva, Switzerland
D J D Thompson University of Birmingham, Birmingham, United Kingdom
H Tilquin Imperial College London, London, United Kingdom
V Tisserand Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S T'Jampens Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
M Tobin Institute Of High Energy Physics (IHEP), Beijing, China
L Tomassetti INFN Sezione di Ferrara, Ferrara, Italy
G Tonani INFN Sezione di Milano, Milano, Italy
X Tong School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Torres Machado Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil
L Toscano Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
D Y Tou Center for High Energy Physics, Tsinghua University, Beijing, China
C Trippl DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
G Tuci Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
N Tuning Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
L H Uecker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Ukleja AGH - University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
D J Unverzagt Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
E Ursov Affiliated with an institute covered by a cooperation agreement with CERN
A Usachov Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands
A Ustyuzhanin Affiliated with an institute covered by a cooperation agreement with CERN
U Uwer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Vagnoni INFN Sezione di Bologna, Bologna, Italy
A Valassi European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Valenti INFN Sezione di Bologna, Bologna, Italy
N Valls Canudas DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
H Van Hecke Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
E van Herwijnen Imperial College London, London, United Kingdom
C B Van Hulse Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
R Van Laak Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M van Veghel Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands
R Vazquez Gomez ICCUB, Universitat de Barcelona, Barcelona, Spain
P Vazquez Regueiro Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
C Vázquez Sierra Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain
S Vecchi INFN Sezione di Ferrara, Ferrara, Italy
J J Velthuis H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
M Veltri INFN Sezione di Firenze, Firenze, Italy
A Venkateswaran Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Vesterinen Department of Physics, University of Warwick, Coventry, United Kingdom
D Vieira University of Cincinnati, Cincinnati, Ohio, USA
M Vieites Diaz European Organization for Nuclear Research (CERN), Geneva, Switzerland
X Vilasis-Cardona DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain
E Vilella Figueras Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom
A Villa INFN Sezione di Bologna, Bologna, Italy
P Vincent LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France
F C Volle Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
D Vom Bruch Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France
V Vorobyev Affiliated with an institute covered by a cooperation agreement with CERN
N Voropaev Affiliated with an institute covered by a cooperation agreement with CERN
K Vos Universiteit Maastricht, Maastricht, Netherlands (associated with Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands)
G Vouters Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France
C Vrahas School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
J Walsh INFN Sezione di Pisa, Pisa, Italy
E J Walton School of Physics and Astronomy, Monash University, Melbourne, Australia
G Wan School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
C Wang Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G Wang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
J Wang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
J Wang Institute Of High Energy Physics (IHEP), Beijing, China
J Wang Center for High Energy Physics, Tsinghua University, Beijing, China
J Wang School of Physics and Technology, Wuhan University, Wuhan, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
M Wang INFN Sezione di Milano, Milano, Italy
N W Wang University of Chinese Academy of Sciences, Beijing, China
R Wang H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
X Wang Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
X W Wang Imperial College London, London, United Kingdom
Y Wang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Z Wang Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
Z Wang Center for High Energy Physics, Tsinghua University, Beijing, China
Z Wang University of Chinese Academy of Sciences, Beijing, China
J A Ward School of Physics and Astronomy, Monash University, Melbourne, Australia Department of Physics, University of Warwick, Coventry, United Kingdom
N K Watson University of Birmingham, Birmingham, United Kingdom
D Websdale Imperial College London, London, United Kingdom
Y Wei School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
B D C Westhenry H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom
D J White Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
M Whitehead School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom
A R Wiederhold Department of Physics, University of Warwick, Coventry, United Kingdom
D Wiedner Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
G Wilkinson Department of Physics, University of Oxford, Oxford, United Kingdom
M K Wilkinson University of Cincinnati, Cincinnati, Ohio, USA
M Williams Massachusetts Institute of Technology, Cambridge, Massachusetts, USA
M R J Williams School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom
R Williams Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
F F Wilson STFC Rutherford Appleton Laboratory, Didcot, United Kingdom
W Wislicki National Center for Nuclear Research (NCBJ), Warsaw, Poland
M Witek Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
L Witola Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C P Wong Los Alamos National Laboratory (LANL), Los Alamos, New Mexico, USA
G Wormser Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
S A Wotton Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom
H Wu Syracuse University, Syracuse, New York, USA
J Wu Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Wu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
K Wyllie European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Xian Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China (associated with Center for High Energy Physics, Tsinghua University, Beijing, China)
Z Xiang Institute Of High Energy Physics (IHEP), Beijing, China
Y Xie Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
A Xu INFN Sezione di Pisa, Pisa, Italy
J Xu University of Chinese Academy of Sciences, Beijing, China
L Xu Center for High Energy Physics, Tsinghua University, Beijing, China
L Xu Center for High Energy Physics, Tsinghua University, Beijing, China
M Xu Department of Physics, University of Warwick, Coventry, United Kingdom
Z Xu Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
Z Xu University of Chinese Academy of Sciences, Beijing, China
Z Xu Institute Of High Energy Physics (IHEP), Beijing, China
D Yang Center for High Energy Physics, Tsinghua University, Beijing, China
S Yang University of Chinese Academy of Sciences, Beijing, China
X Yang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Yang INFN Sezione di Genova, Genova, Italy
Z Yang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Z Yang University of Maryland, College Park, Maryland, USA
V Yeroshenko Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France
H Yeung Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom
H Yin Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
C Y Yu School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
J Yu School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
X Yuan Institute Of High Energy Physics (IHEP), Beijing, China
E Zaffaroni Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland
M Zavertyaev Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany
M Zdybal Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
M Zeng Center for High Energy Physics, Tsinghua University, Beijing, China
C Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
D Zhang Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
J Zhang University of Chinese Academy of Sciences, Beijing, China
L Zhang Center for High Energy Physics, Tsinghua University, Beijing, China
S Zhang School of Physics and Electronics, Hunan University, Changsha City, China (associated with Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China)
S Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Zhang School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
Y Zhang Department of Physics, University of Oxford, Oxford, United Kingdom
Y Z Zhang Center for High Energy Physics, Tsinghua University, Beijing, China
Y Zhao Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Zharkova Affiliated with an institute covered by a cooperation agreement with CERN
A Zhelezov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
X Z Zheng Center for High Energy Physics, Tsinghua University, Beijing, China
Y Zheng University of Chinese Academy of Sciences, Beijing, China
T Zhou School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
X Zhou Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Y Zhou University of Chinese Academy of Sciences, Beijing, China
V Zhovkovska Department of Physics, University of Warwick, Coventry, United Kingdom
L Z Zhu University of Chinese Academy of Sciences, Beijing, China
X Zhu Center for High Energy Physics, Tsinghua University, Beijing, China
X Zhu Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China
Z Zhu University of Chinese Academy of Sciences, Beijing, China
V Zhukov I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany Affiliated with an institute covered by a cooperation agreement with CERN
J Zhuo Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain
Q Zou Institute Of High Energy Physics (IHEP), Beijing, China University of Chinese Academy of Sciences, Beijing, China
D Zuliani Università degli Studi di Padova, Università e INFN, Padova, Padova, Italy
G Zunica Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom

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[Predictive value of whole brain perfusion on admission for shunt-dependent hydrocephalus fllowing aneurysmal subarachnoid hemorrhage]

Objective: To explore the value of predicting shunt-dependent hydrocephalus (SDHC) in patients with aneurysmal subarachnoid hemorrhage (aSAH) based on whole brain CT perfusion(CTP) and clinical data within 24 hours at admission. Methods: The clinical and imaging data of aSAH patients who received interventional embolization in our hospital were retrospectively collected from March 2018 to August 2022. All patients underwent one-stop whole brain CT examination within 24 hours after symptom onset, and the qualitative and quantitative CTP parameters were obtained after post-processing. Follow-up was conducted once every 2 months by consulting electronic medical records or by telephone for 6 months. According to whether SDHC occurred or not, the patients were divided into SDHC group and non-SDHC group. The differences between the two groups were compared. Logistic regression model was used to analyze and determine the predictive factors of SDHC, and the SDHC predictive model was established. The effectiveness of the predictive model was evaluated by drawing the receiver operating characteristic (ROC) curve of the subjects. Results: A total of 414 patients were included, including 132 males and 282 females, aged (59±11) years. 17.6%(73/414) patients had SDHC. There were significant differences in the occurrence of acute hydrocephalus, the World Neurosurgical League Scale (WFNS), the Hunt-Hess scale, the modified Fisher score (mFS), and the qualitative and quantitative parameters of CTP between the two groups (both P<0.001). Multivariate logistic regression analysis showed that acute hydrocephalus (OR=8.621, 95%CI: 4.237-17.542),old age (OR=1.107, 95%CI: 1.068-1.148), high mFS and high Hunt-Hess classification (OR=3.740, 95%CI: 1.352-10.342) were the risk factors of SDHC in aSAH patients, and high mean cerebral blood flow (mCBF) (OR=0.931, 95%CI: 0.885-0.980) was a protective factor of SDHC.The area under ROC curve (AUC) of the prediction model constructed by these five variables was 0.923(95%CI: 0.89-0.95), with 84.5% sensitivity and 87.7% specificity. Conclusion: The mCBF and acute hydrocephalus, age, mFS and Hunt-Hess classification within 24 hours at admission can be used to predict SDHC for aSAH patients.

Causal effects of gut microbiome on HIV infection: a two-sample mendelian randomization analysis

BACKGROUND

The causal association between gut microbiome and HIV infection remains to be elucidated. We conducted a two-sample mendelian randomization analysis to estimate the causality between gut microbiome and HIV infection.

METHODS

Publicly released genome-wide association studies summary data were collected to perform the mendelian analysis. The GWAS summary data of gut microbiome was retrieved from the MiBioGen consortium, which contains 18 340 samples from 24 cohorts. GWAS summary data of HIV infection was collected from the R5 release of FinnGen consortium, including 357 HIV infected cases and 218 435 controls. The SNPs were selected as instrumental variables according to our selection rules. And SNPs with a F-statistics less than ten were regarded as weak instrumental variables and excluded. Mendelian randomization analysis was conducted by five methods, including inverse variance weighted (IVW), MR-Egger, weighted median, weighted mode, and simple mode. The Cochran's Q test and MR-Egger intercept test were performed to identify heterogeneity and pleiotropy. Leave-one-out analysis were used to test the sensitivity of the results.

RESULTS

Fifteen gut microbiota taxa showed causal effects on HIV infection according to the MR methods. Four taxa were observed to increase the risk of HIV infection, including Ruminococcaceae (OR: 2.468[1.043, 5.842], P: 0.039), Ruminococcaceae UCG005 (OR: 2.051[1.048, 4.011], P: 0.036), Subdoligranulum (OR: 3.957[1.762, 8.887], P < 0.001) and Victivallis (OR: 1.605[1.012, 2.547], P=0.044). Erysipelotrichaceae was protective factor of HIV infection (OR: 0.278[0.106, 0.731], P < 0.001) and Methanobrevibacter was also found to be associated with reduced risk of HIV infection (OR: 0.509[0.265, 0.980], P=0.043). Horizontal pleiotropy was found for Fusicatenibacter (P<0.05) according to the MR-Egger regression intercept analysis. No heterogeneity was detected.

CONCLUSION

Our results demonstrate significant causal effects of gut microbiome on HIV infection. These findings facilitate future studies to develop better strategies for HIV prophylaxis through gut microbiome regulation. Further explorations are also warranted to dissect the mechanism of how gut microbiome affects HIV susceptibility.

Hypertension associated with niraparib in cancer patients: A pharmacovigilance analysis based on the FAERS database and meta-analysis of randomized controlled trials

BACKGROUND

Niraparib plays a crucial role in the treatment of ovarian cancer. A comprehensive understanding of the incidence and risk of hypertension associated with niraparib would be of vital importance to healthcare practitioners.

METHODS

In this study, an observational, retrospective, pharmacovigilance study was conducted based on the FDA Adverse Event Reporting System (FAERS) database. Cases of hypertension related to niraparib were extracted for disproportionality analysis from the first quarter (Q1) of 2017 to Q1 of 2023. Moreover, a separate meta-analysis was performed using the randomized controlled trials (RCTs) on niraparib for cancer treatment published in PubMed, Embase, and Web of Science from inception to May 31st, 2023. The primary outcomes were the incidence and risk of hypertension associated with niraparib.

RESULTS

In the FAERS, 1196 hypertension cases were found to be related to niraparib treatment. Notably, niraparib exhibited the highest level of disproportionality, as indicated by a reporting odds ratio (ROR) of 2.85 (95% CI, 2.69-3.01), suggesting a greater likelihood of causing hypertension compared to other poly-ADP-ribose polymerase (PARP) inhibitors (P < 0.01). Our safety meta-analysis included five pivotal RCTs of niraparib that reported hypertension. In comparison to placebo treatment, the meta-analysis demonstrated a significant increase in the risk of hypertension with niraparib (OR 2.84 [95% CI, 2.17-3.72], P < 0.01), with no heterogeneity observed among the studies (I2 = 0%, χ2 = 2.02, P = 0.73). The incidence of niraparib-induced hypertension was determined to be 16.9% (95% CI, 14.9-18.9; I2 = 34%).

CONCLUSIONS

These findings suggest that hypertension is a distinctive adverse event associated with niraparib compared to other PARP inhibitors. Niraparib significantly increases the risk of hypertension that needs early recognition and management in clinical medication.

Association between area under the C-peptide curve during an oral glucose tolerance test and diabetic retinopathy in type 2 diabetes patients

AIMS/INTRODUCTION

To evaluate the relative contributions of the area under the C-peptide curve (AUCC ) in diabetic retinopathy (DR) during an oral glucose tolerance test and C-peptide release test in patients with type 2 diabetes.

MATERIALS AND METHODS

We retrospectively analyzed the data of 969 patients. Their general characteristics were retrieved. A series of parameters for assessing pancreatic β-cells function, such as the AUCC for six time periods: 0-60 min (AUCC0-60 ), 0-120 min (AUCC0-120 ), 0-180 min (AUCC0-180 ), 60-120 min (AUCC60-120 ), 60-180 min (AUCC60-180 ) and 120-180 min (AUCC120-180 ); the area under the glucose-time curve for six time periods: 0-60 min (AUCG0-60 ), 0-120 min (AUCG0-120 ), 0-180 min (AUCG0-180 ), 60-120 min (AUCG60-120 ), 60-180 min (AUCG60-180 ) and 120-180 min (AUCG120-180 ) and their related indexes, were calculated through 0-180 min oral glucose tolerance test and C-peptide release test. We used univariate analysis to examine the potential factors affecting DR. Spearman's correlation was used to analyze the correlation between AUCC -related indexes and DR. The logistic regression model was used to investigate AUCC and its related indexes' contribution to incidence DR. A smooth curve fitting model was used to determine the correlation, non-linear relationship, and threshold effect between AUCC and DR.

RESULTS

Of the 969 patients with type 2 diabetes, 469 (48.40%) and 500 (51.60%) were classified as the DR group and non-DR group. Compared with the non-DR group, the DR patients had lower AUCC and AUCC /AUCG . Spearman's correlation analysis showed that AUCC -related indexes were all negatively correlated with DR. The logistic regression analysis determined that there were associations between AUCC and DR in the adjusted models. The odds ratio values of AUCC0-60 , AUCC0-120 , AUCC0-180 , AUCC0-60 /AUCG0-60 , AUCC0-120 /AUCG0-120 , AUCC0-180 /AUCG0-180 , AUCC60-120 , AUCC60-180 , AUCC120-180 , AUCC60-120 /AUCG60-120 , AUCC60-180 /AUCG60-180 and AUCC120-180 /AUCG120-180 were 0.817 (0.750, 0.890), 0.925 (0.895, 0.955), 0.951 (0.932, 0.970), 0.143 (0.060, 0.340), 0.194 (0.093, 0.406), 0.223 (0.116, 0.427), 0.886 (0.842, 0.933), 0.939 (0.915, 0.963), 0.887 (0.846, 0.930), 0.253 (0.133, 0.479), 0.282 (0.160, 0.497) and 0.355 (0.220, 0.573), respectively. AUCC showed a non-linear relationship with DR, with an inflection point. The inflection points of AUCC180 /AUCG180 , AUCC60-120 , AUCC60-180 , AUCC120-180 , AUCC60-120 /AUCG60-120 , AUCC60-180 /AUCG60-180 , AUCC120-180 /AUCG120-180 and DR were 17.51, 0.542, 6.6, 15.7, 8.23, 0.534, 0.593 and 0.808 (P < 0.0001). When the indexes related to the AUCC were less than the inflection point value, they were significantly negatively associated with DR.

CONCLUSIONS

The indexes related to the AUCC for six time periods during an oral glucose tolerance test and C-peptide release test was closely associated with the incidence to DR in patients with type 2 diabetes. AUCC has the added advantage of being a cheap and convenient risk assessment over traditional ophthalmic screening.

[Advances in the technology of surgical treatment for atlantoaxial dislocation]

The etiology and pathological morphology of atlantoaxial dislocation (AAD) are complex. Based on the pathological anatomical characteristics of AAD, combined with clinical techniques, it is essential to formulate reasonable classification criteria and develop corresponding treatment strategies for different types of AAD. The satisfactory outcome of surgical treatment for AAD can only be achieved through the comprehensive application of various atlantoaxial reduction techniques, tension band releasing techniques, internal fixation and fusion techniques. This article discusses the latest advancements in surgical treatment techniques for AAD, thoroughly explores treatment strategies based on different types of AAD, and analyzes the practicality and effectiveness of clinical classification and treatment strategies. The posterior atlantoaxial facet releasing and distraction compression reduction technique may pose challenges to traditional treatment strategies in the future. In the development of surgical treatment techniques for AAD, microspinal surgical techniques may play a significant role in improving surgical methods and enhancing treatment outcomes.

Probiotic-fermented edible herbs as functional foods: A review of current status, challenges, and strategies

Recently, consumers have become increasingly interested in natural, health-promoting, and chronic disease-preventing medicine and food homology (MFH). There has been accumulating evidence that many herbal medicines, including MFH, are biologically active due to their biotransformation through the intestinal microbiota. The emphasis of scientific investigation has moved from the functionally active role of MFH to the more subtle role of biotransformation of the active ingredients in probiotic-fermented MFH and their health benefits. This review provides an overview of the current status of research on probiotic-fermented MFH. Probiotics degrade toxins and anti-nutritional factors in MFH, improve the flavor of MFH, and increase its bioactive components through their transformative effects. Moreover, MFH can provide a material base for the growth of probiotics and promote the production of their metabolites. In addition, the health benefits of probiotic-fermented MFH in recent years, including antimicrobial, antioxidant, anti-inflammatory, anti-neurodegenerative, skin-protective, and gut microbiome-modulating effects, are summarized, and the health risks associated with them are also described. Finally, the future development of probiotic-fermented MFH is prospected in combination with modern development technologies, such as high-throughput screening technology, synthetic biology technology, and database construction technology. Overall, probiotic-fermented MFH has the potential to be used in functional food for preventing and improving people's health. In the future, personalized functional foods can be expected based on synthetic biology technology and a database on the functional role of probiotic-fermented MFH.

Association of Metabolic Syndrome with Macular Thickness and Volume in Older Adults: A Population-Based Optical Coherence Tomography Study

Background: To explore the associations of the metabolic syndrome (MetS) and individual components with macular thickness and volume among rural-dwelling Chinese older adults. Methods: This population-based cross-sectional study included 705 participants (age ≥60 years) derived from the MIND-China study. In 2018-2019, we collected data through face-to-face interview, clinical examination, optical coherence tomography (OCT) examination, and blood test. We measured macular thickness and volume using spectral-domain OCT. MetS was defined following the International Diabetes Federation (IDF) criteria, the IDF/American Heart Association (AHA) criteria, the National Cholesterol Education Program-Adult Treatment Panel III criteria, and the Chinese Diabetes Society (CDS) criteria. Data were analyzed with multivariable general linear models. Results: MetS was significantly associated with thinner macula in central (multivariable-adjusted β = -5.29; 95% confidence interval: -9.31 to -1.26), parafoveal (-2.85; -5.73 to 0.04) and perifoveal regions (-4.37; -6.79 to -1.95) when using the IDF criteria, in the perifoveal regions (-3.82; -6.18 to -1.47) when using the IDF/AHA criteria, and in the central region (-5.63; -10.25 to -1.02) when using the CDS criteria, and with reduced macular volume when using the IDF (-0.16; -0.26 to -0.07) and IDF/AHA (-0.13; -0.22 to -0.04) criteria. In the parafoveal region, the IDF-defined MetS was significantly associated with thinner retina in men (β = -6.25; -10.94 to -1.56) but not in women. Abdominal obesity (-2.83; -5.41 to -0.25) and elevated fasting blood glucose (-2.65; -5.08 to -0.21) were associated with thinner macular thickness in the perifoveal region. Conclusion: MetS is associated with macular thinning and reduced macular volume among rural-dwelling older adults, and the associations vary by the defining criteria of MetS.

Lipocalin 2 (LCN2) confers acquired resistance to almonertinib in NSCLC through LCN2-MMP-9 signaling pathway

Almonertinib, a third-generation epidermal growth factor receptor (EGFR) tyrosine kinase inhibitor, is highly selective for EGFR-activating mutations as well as the EGFR T790M mutation in patients with advanced non-small cell lung cancer (NSCLC). However, the development of resistance inevitably occurs and poses a major obstacle to the clinical efficacy of almonertinib. Therefore, a clear understanding of the mechanism is of great significance to overcome drug resistance to almonertinib in the future. In this study, NCI-H1975 cell lines resistant to almonertinib (NCI-H1975 AR) were developed by concentration-increasing induction and were employed for clarification of underlying mechanisms of acquired resistance. Through RNA-seq analysis, the HIF-1 and TGF-β signaling pathways were significantly enriched by gene set enrichment analysis. Lipocalin-2 (LCN2), as the core node in these two signaling pathways, were found to be positively correlated to almonertinib-resistance in NSCLC cells. The function of LCN2 in the drug resistance of almonertinib was investigated through knockdown and overexpression assays in vitro and in vivo. Moreover, matrix metalloproteinases-9 (MMP-9) was further identified as a critical downstream effector of LCN2 signaling, which is regulated via the LCN2-MMP-9 axis. Pharmacological inhibition of MMP-9 could overcome resistance to almonertinib, as evidenced in both in vitro and in vivo models. Our findings suggest that LCN2 was a crucial regulator for conferring almonertinib-resistance in NSCLC and demonstrate the potential utility of targeting the LCN2-MMP-9 axis for clinical treatment of almonertinib-resistant lung adenocarcinoma.

Nano-selenium alleviates cadmium-induced neurotoxicity in cerebrum via inhibiting gap junction protein connexin 43 phosphorylation

Cadmium (Cd) as a ubiquitous toxic heavy metal is reported to affect the nervous system. Selenium (Se) has been shown to have antagonistic effects against heavy metal toxicity. In addition, it shows potential antioxidant and anti-inflammatory properties. Thus, the purpose of this study was to determine the possible mechanism of brain injury after high Cd exposure and the mitigation of Nano-selenium (Nano-Se) against Cd-induced brain injury. In this study, the Cd-treated group showed a decrease in the number of neurons in brain tissue, swelling of the endoplasmic reticulum and mitochondria, and the formation of autophagosomes. Nano-Se intervention restored Cd-caused alterations in neuronal morphology, endoplasmic reticulum, and mitochondrial structure, thereby reducing neuronal damage. Furthermore, we found that some differentially expressed genes were involved in cell junction and molecular functions. Subsequently, we selected eleven (11) related differentially expressed genes for verification. The qRT-PCR results revealed the same trend of results as determined by RNA-Seq. Our findings also showed that Nano-Se supplementation alleviated Cx43 phosphorylation induced by Cd exposure. Based on immunofluorescence colocalization it was demonstrated that higher expression of GFAP and lower expressions of Cx43 were restored by Nano-Se supplementation. In conclusion, the data presented in this study establish a direct association between the phosphorylation of Cx43 and the occurrence of autophagy and neuroinflammation. However, it is noteworthy that the introduction of Nano-Se supplementation has been observed to mitigate these alterations. These results elucidate the relieving effect of Nano-Se on Cd exposure-induced brain injury.