Elucidation of Palmarumycin Spirobisnaphthalene Biosynthesis Reveals a Set of Previously Unrecognized Oxidases and Reductases

Spirobisnaphthalenes (SBNs) are a class of highly oxygenated, fungal bisnaphthalenes containing a unique spiroketal bridge, that displayed diverse bioactivities. Among the reported SBNs, palmarumycins are the major type, which are precursors for the other type of SBNs structurally. However, the biosynthesis of SBNs is unclear. In this study, we elucidated the biosynthesis of palmarumycins, using gene disruption, heterologous expression, and substrate feeding experiments. The biosynthetic gene cluster for palmarumycins was identified to be distant from the polyketide synthase gene cluster, and included two cytochrome P450s (PalA and PalB), and one short chain dehydrogenase/reductase (PalC) encoding genes as key structural genes. PalA is an unusual, multifunctional P450 that catalyzes the oxidative dimerization of 1,8-dihydroxynaphthalene to generate the spiroketal linkage and 2,3-epoxy group. Chemical synthesis of key intermediate and in vitro biochemical assays proved that the oxidative dimerization proceeded via a binaphthyl ether. PalB installs the C-5 hydroxy group, widely found in SBNs. PalC catalyzes 1-keto reduction, the reverse 1-dehydrogenation, and 2,3-epoxide reduction. Moreover, an FAD-dependent oxidoreductase, encoded by palD, which locates outside the cluster, functions as a 1-dehydrogenase. These results provided the first genetic and biochemical evidence for the biosynthesis of palmarumycin SBNs.

Targeted drug-loaded peptides induce tumor cell apoptosis and immunomodulation to increase antitumor efficacy

Immunotherapy is an emerging approach for the treatment of solid tumors. Although chemotherapy is generally considered immunosuppressive, specific chemotherapeutic agents can induce tumor immunity. In this study, we developed a targeted, acid-sensitive peptide nanoparticle (DT/Pep1) to deliver doxorubicin (DOX) and triptolide (TPL) to breast cancer cells via the enhanced permeability and retention (EPR) effect and the breast cancer-targeting effect of peptide D8. Compared with administration of the free drugs, treatment with the DT/Pep1 system increased the accumulation of DOX and TPL at the tumor site and achieved deeper penetration into the tumor tissue. In an acidic environment, DT/Pep1 transformed from spherical nanoparticles to aggregates with a high aspect ratio, which successfully extended the retention of the drugs in the tumor cells and bolstered the anticancer effect. In both in vivo and in vitro experiments, DT/Pep1 effectively blocked the cell cycle and induced apoptosis. Importantly, the DT/Pep1 system efficiently suppressed tumor development in mice bearing 4T1 tumors while simultaneously promoting immune system activation. Thus, the results of this study provide a system for breast cancer therapy and offer a novel and promising platform for peptide nanocarrier-based drug delivery.

Unraveling the impact of climatic warming and wetting on eukaryotic microbial diversity and assembly mechanisms: A 10-year case study in Lake Bosten, NW China

Over the last six decades, northwest China has undergone a significant climatic shift from "warm-dry" to "warm-wet", profoundly impacting the structures and functions of lake ecosystem across the region. However, the influences of this climatic transition on the diversity patterns, co-occurrence network, and assembly processes of eukaryotic microbial communities in lake ecosystem, along with the underlying mechanisms, remain largely unexplored. To bridge this knowledge gap, our study focused on Lake Bosten, the largest inland freshwater body in China, conducting a comprehensive analysis. Firstly, we examined the dynamics of key water quality parameters in the lake based on long-term monitoring data (1992-2022). Subsequently, we collected 93 water samples spanning two distinctive periods: low water level (WL) and high total dissolved solids (TDS) (PerWLTDS; 2010-2011; attributed to "warm-dry" climate), and high WL and low TDS (PerTDSWL; 2021-2022; associated with "warm-wet" climate). Eukaryotic microorganisms were further investigated using 18S rRNA gene sequencing and various statistical methods. Our findings revealed that climatic warming and wetting significantly increased eukaryotic microbial α-diversity (all Wilcox. test: P<0.05), while simultaneously reducing β-diversity (all Wilcox. test: P<0.001) and network complexity. Through the two sampling periods, assembly mechanisms of eukaryotic microorganisms were predominantly influenced by dispersal limitation (DL) and drift (DR) within stochastic processes, alongside homogeneous selection (HoS) within deterministic processes. WL played a mediating role in eukaryotic microbial DL and HoS processes in the PerTDSWL, whereas water quality and α-diversity influenced the DL process in the PerWLTDS. Collectively, these results underscore the direct and indirect impacts of "warm-wet" conditions on the eukaryotic microorganisms within Lake Bosten. This study provides valuable insights into the evolutionary dynamics of lake ecosystems under such climatic conditions and aids in predicting the ecological ramifications of global climatic changes.

Poly(ethylene oxide)-based composite solid electrolyte for long cycle life solid-state lithium metal batteries: Improvement of interface stability through a dual mechanism

Solid-state lithium metal batteries (SSLMBs) are promising candidates for safe and high-energy-density next-generation applications. However, harmful interfacial decomposition and uneven Li deposition lead to poor ion transport, a short cycle life, and battery failure. Herein, we propose a novel poly(ethylene oxide) (PEO)-based composite solid electrolyte (CSE) containing succinonitrile (SN) and zinc oxide (ZnO) nanoparticles (NPs), which improves interface stability through a dual mechanism. (1) By anchoring bis(trifluoromethanesulfonyl)imide (TFSI) anions to ZnO, a reliable solid electrolyte interface (SEI) later with abundant LiF can be obtained to inhibit interface decomposition. (2) The immobilization of escaping SN molecules in the SEI layer by ZnO NPs promotes the self-polymerization of SN and facilitates charge transfer through the interface. As a result, the ion conductivity of the stainless steel-symmetrical battery reaches 1.1 × 10-4 S cm-1 at room temperature, and a LiFePO4 (LFP) full battery exhibits ultrahigh stability (800 cycles) at 0.5 C. Thus, the present study provides valuable insights for the development of advanced PEO-based SSLMBs.

High-quality genomes of Bombax ceiba and Ceiba pentandra provide insights into the evolution of Malvaceae species and differences in their natural fiber development

Members of the Malvaceae family, including Corchorus spp., Gossypium spp., Bombax spp., and Ceiba spp., are important sources of natural fibers. In the past decade, the genomes of several Malvaceae species have been assembled; however, the evolutionary history of Malvaceae species and the differences in their fiber development remain to be clarified. Here, we report the genome assembly and annotation of two natural fiber plants from the Malvaceae, Bombax ceiba and Ceiba pentandra, whose assembled genome sizes are 783.56 Mb and 1575.47 Mb, respectively. Comparative analysis revealed that whole-genome duplication and Gypsy long terminal repeat retroelements have been the major causes of differences in chromosome number (2n = 14 to 2n = 96) and genome size (234 Mb to 2676 Mb) among Malvaceae species. We also used comparative genomic analyses to reconstruct the ancestral Malvaceae karyotype with 11 proto-chromosomes, providing new insights into the evolutionary trajectories of Malvaceae species. MYB-MIXTA-like 3 is relatively conserved among the Malvaceae and functions in fiber cell-fate determination in the epidermis. It appears to perform this function in any tissue where it is expressed, i.e. in fibers on the endocarp of B. ceiba and in ovule fibers of cotton. We identified a structural variation in a cellulose synthase gene and a higher copy number of cellulose synthase-like genes as possible causes of the finer, less spinnable, weaker fibers of B. ceiba. Our study provides two high-quality genomes of natural fiber plants and offers insights into the evolution of Malvaceae species and differences in their natural fiber formation and development through multi-omics analysis.

Genetic analysis of a Kaijiang duck conservation population through genome-wide scan

1. The Kaijiang duck is a native Chinese breed known for its excellent egg laying performance, killing-out percentage (88.57%), and disease resistance. The assessment of population genetic structure is the basis for understanding the genetics of indigenous breeds and for their protection and management.2. In this study, whole-genome sequencing was performed on 60 Kaijiang ducks to identify genetic variations and investigate the population structure. Homozygosity (ROH) analysis was conducted to assess inbreeding levels in the population.3. The study revealed a moderate level of inbreeding, indicated by an average inbreeding coefficient of 0.1043. This may impact the overall genetic diversity.4. Genomic Regions of Interest identified included 168 genomic regions exhibiting high levels of autozygosity. These regions were associated with processes including muscle growth, pigmentation, neuromodulation, and growth and reproduction.5. The significance of these pathways indicated their potential role in shaping the desirable traits of the Kaijiang duck. These findings provide insights into the genetic basis of the Kaijiang duck's desirable traits and can inform future breeding and conservation efforts.

Identification and characterization of the plasma membrane H+-ATPase genes in Brassica napus and functional analysis of BnHA9 in salt tolerance

As a primary proton pump, plasma membrane (PM) H+-ATPase plays critical roles in regulating plant growth, development, and stress responses. PM H+-ATPases have been well characterized in many plant species. However, no comprehensive study of PM H+-ATPase genes has been performed in Brassica napus (rapeseed). In this study, we identified 32 PM H+-ATPase genes (BnHAs) in the rapeseed genome, and they were distributed on 16 chromosomes. Phylogenetical and gene duplication analyses showed that the BnHA genes were classified into five subfamilies, and the segmental duplication mainly contributed to the expansion of the rapeseed PM H+-ATPase gene family. The conserved domain and subcellular analyses indicated that BnHAs encoded canonical PM H+-ATPase proteins with 14 highly conserved domains and localized on PM. Cis-acting regulatory element and expression pattern analyses indicated that the expression of BnHAs possessed tissue developmental stage specificity. The 25 upstream open reading frames with the canonical initiation codon ATG were predicted in the 5' untranslated regions of 11 BnHA genes and could be used as potential target sites for improving rapeseed traits. Protein interaction analysis showed that BnBRI1.c associated with BnHA2 and BnHA17, indicating that the conserved activity regulation mechanism of BnHAs may be present in rapeseed. BnHA9 overexpression in Arabidopsis enhanced the salt tolerance of the transgenic plants. Thus, our results lay a foundation for further research exploring the biological functions of PM H+-ATPases in rapeseed.

Causal relationship between thyroid dysfunction and gastric cancer: a two-sample Mendelian randomization study

Backgroud

Gastric cancer is one of the most common cancers worldwide, and its development is associated with a variety of factors. Previous observational studies have reported that thyroid dysfunction is associated with the development of gastric cancer. However, the exact relationship between the two is currently unclear. We used a two-sample Mendelian randomization (MR) study to reveal the causal relationship between thyroid dysfunction and gastric cancer for future clinical work.

Materials and methods

This study is based on a two-sample Mendelian randomization design, and all data are from public GWAS databases. We selected hyperthyroidism, hypothyroidism, free thyroxine (FT4), and thyroid-stimulating hormone (TSH) as exposures, with gastric cancer as the outcome. We used three statistical methods, namely Inverse-variance weighted (IVW), MR-Egger, and weighted median, to assess the causal relationship between thyroid dysfunction and gastric cancer. The Cochran's Q test was used to assess the heterogeneity among SNPs in the IVW analysis results, and MR-PRESSO was employed to identify and remove IVs with heterogeneity from the analysis results. MR-Egger is a weighted linear regression model, and the magnitude of its intercept can be used to assess the horizontal pleiotropy among IVs. Finally, the data were visualized through the leave-one-out sensitivity test to evaluate the influence of individual SNPs on the overall causal effect. Funnel plots were used to assess the symmetry of the selected SNPs, forest plots were used to evaluate the confidence and heterogeneity of the incidental estimates, and scatter plots were used to assess the exposure-outcome relationship. All results were expressed as odds ratios (OR) and 95% confidence intervals (95% CI). P<0.05 represents statistical significance.

Results

According to IVW analysis, there was a causal relationship between hypothyroidism and gastric cancer, and hypothyroidism could reduce the risk of gastric cancer (OR=0.936 (95% CI:0.893-0.980), P=0.006).This means that having hypothyroidism is a protective factor against stomach cancer. This finding suggests that hypothyroidism may be associated with a reduced risk of gastric cancer.Meanwhile, there was no causal relationship between hyperthyroidism, FT4, and TSH and gastric cancer.

Conclusions

In this study, we found a causal relationship between hypothyroidism and gastric cancer with the help of a two-sample Mendelian randomisation study, and hypothyroidism may be associated with a reduced risk of gastric cancer, however, the exact mechanism is still unclear. This finding provides a new idea for the study of the etiology and pathogenesis of gastric cancer, and our results need to be further confirmed by more basic experiments in the future.

Efficient gene editing in the slow-growing, non-sporulating, melanized, endophytic fungus Berkleasmium sp. Dzf12 using a CRISPR/Cas9 system

The endophytic fungus Berkleasmium sp. Dzf12 that was isolated from Dioscorea zingiberensis, is a proficient producer of palmarumycins, which are intriguing polyketides of the spirobisnaphthalene class. These compounds displayed a wide range of bioactivities, including antibacterial, antifungal, and cytotoxic activities. However, conventional genetic manipulation of Berkleasmium sp. Dzf12 is difficult and inefficient, partially due to the slow-growing, non-sporulating, and highly pigmented behavior of this fungus. Herein, we developed a CRISPR/Cas9 system suitable for gene editing in Berkleasmium sp. Dzf12. The protoplast preparation was optimized, and the expression of Cas9 in Berkleasmium sp. Dzf12 was validated. To assess the gene disruption efficiency, a putative 1, 3, 6, 8-tetrahydroxynaphthalene synthase encoding gene, bdpks, involved in 1,8-dihydroxynaphthalene (DHN)-melanin biosynthesis, was selected as the target for gene disruption. Various endogenous sgRNA promoters were tested, and different strategies to express sgRNA were compared, resulting in the construction of an optimal system using the U6 snRNA-1 promoter as the sgRNA promoter. Successful disruption of bdpks led to a complete abolishment of the production of spirobisnaphthalenes and melanin. This work establishes a useful gene targeting disruption system for exploration of gene functions in Berkleasmium sp. Dzf12, and also provides an example for developing an efficient CRISPR/Cas9 system to the fungi that are difficult to manipulate using conventional genetic tools.

Optomechanical Frequency Comb Based on Multiple Nonlinear Dynamics

Phonon-based frequency combs that can be generated in the optical and microwave frequency domains have attracted much attention due to the small repetition rates and the simple setup. Here, we experimentally demonstrate a new type of phonon-based frequency comb in a silicon optomechanical crystal cavity including both a breathing mechanical mode (∼GHz) and flexural mechanical modes (tens of MHz). We observe strong mode competition between two approximate flexural mechanical modes, i.e., 77.19 and 90.17 MHz, resulting in only one preponderant lasing, while maintaining the lasing of the breathing mechanical mode. These simultaneous observations of two-mode phonon lasing state and significant mode competition are counterintuitive. We have formulated comprehensive theories to elucidate this phenomenon in response to this intriguing outcome. In particular, the self-pulse induced by the free carrier dispersion and thermo-optic effects interacts with two approximate flexural mechanical modes, resulting in the repetition rate of the comb frequency-locked to exact fractions of one of the flexural mechanical modes and the mode hopping between them. This phonon-based frequency comb has at least 260 comblines and a repetition rate as low as a simple fraction of the flexural mechanical frequency. Our demonstration offers an alternative optomechanical frequency comb for sensing, timing, and metrology applications.

Heterogeneity and interplay: the multifaceted role of cancer-associated fibroblasts in the tumor and therapeutic strategies

The journey of cancer development is a multifaceted and staged process. The array of treatments available for cancer varies significantly, dictated by the disease's type and stage. Cancer-associated fibroblasts (CAFs), prevalent across various cancer types and stages, play a pivotal role in tumor genesis, progression, metastasis, and drug resistance. The strategy of concurrently targeting cancer cells and CAFs holds great promise in cancer therapy. In this review, we focus intently on CAFs, delving into their critical role in cancer's progression. We begin by exploring the origins, classification, and surface markers of CAFs. Following this, we emphasize the key cytokines and signaling pathways involved in the interplay between cancer cells and CAFs and their influence on the tumor immune microenvironment. Additionally, we examine current therapeutic approaches targeting CAFs. This article underscores the multifarious roles of CAFs within the tumor microenvironment and their potential applications in cancer treatment, highlighting their importance as key targets in overcoming drug resistance and enhancing the efficacy of tumor therapies.

Oxygen-Bridged Cu Binuclear Sites for Efficient Electrocatalytic CO2 Reduction to Ethanol at Ultralow Overpotential

Electrocatalytic CO2 reduction (CO2RR) to alcohols offers a promising strategy for converting waste CO2 into valuable fuels/chemicals but usually requires large overpotentials. Herein, we report a catalyst comprising unique oxygen-bridged Cu binuclear sites (CuOCu-N4) with a Cu···Cu distance of 3.0-3.1 Å and concomitant conventional Cu-N4 mononuclear sites on hierarchical nitrogen-doped carbon nanocages (hNCNCs). The catalyst exhibits a state-of-the-art low overpotential of 0.19 V (versus reversible hydrogen electrode) for ethanol and an outstanding ethanol Faradaic efficiency of 56.3% at an ultralow potential of -0.30 V, with high-stable Cu active-site structures during the CO2RR as confirmed by operando X-ray adsorption fine structure characterization. Theoretical simulations reveal that CuOCu-N4 binuclear sites greatly enhance the C-C coupling at low potentials, while Cu-N4 mononuclear sites and the hNCNC support increase the local CO concentration and ethanol production on CuOCu-N4. This study provides a convenient approach to advanced Cu binuclear site catalysts for CO2RR to ethanol with a deep understanding of the mechanism.

Artificial intelligence facial recognition system for diagnosis of endocrine and metabolic syndromes based on a facial image database

AIM

To build a facial image database and to explore the diagnostic efficacy and influencing factors of the artificial intelligence-based facial recognition (AI-FR) system for multiple endocrine and metabolic syndromes.

METHODS

Individuals with multiple endocrine and metabolic syndromes and healthy controls were included from public literature and databases. In this facial image database, facial images and clinical data were collected for each participant and dFRI (disease facial recognition intensity) was calculated to quantify facial complexity of each syndrome. AI-FR diagnosis models were trained for each disease using three algorithms: support vector machine (SVM), principal component analysis k-nearest neighbor (PCA-KNN), and adaptive boosting (AdaBoost). Diagnostic performance was evaluated. Optimal efficacy was achieved as the best index among the three models. Effect factors of AI-FR diagnosis were explored with regression analysis.

RESULTS

462 cases of 10 endocrine and metabolic syndromes and 2310 controls were included into the facial image database. The AI-FR diagnostic models showed diagnostic accuracies of 0.827-0.920 with SVM, 0.766-0.890 with PCA-KNN, and 0.818-0.935 with AdaBoost. Higher dFRI was associated with higher optimal area under the curve (AUC) (P = 0.035). No significant correlation was observed between the sample size of the training set and diagnostic performance.

CONCLUSIONS

A multi-ethnic, multi-regional, and multi-disease facial database for 10 endocrine and metabolic syndromes was built. AI-FR models displayed ideal diagnostic performance. dFRI proved associated with the diagnostic performance, suggesting inherent facial features might contribute to the performance of AI-FR models.

Simulated sunlight/periodate-triggered formation of toxic halogenated bisphenols in highly saline water

Periodate (PI)-based oxidation using the activators, such as metal ions and light irradiation, has emerged as a feasible treatment strategy for the effective remediation of contaminated water and wastewater. Given the pervasive nature of PI residues and solar exposure during application, the role of solar light in remediating the challenging highly saline water matrices needs to be elucidated. In this study, bisphenol A (BPA) was selected as the targeted micropollutant, which can be efficiently eliminated by the simulated sunlight (SSL)/PI system in the presence of high-level Cl- (up to 846.0 mM) at pH 7.0. The presence of different background constituents of water, such as halides, nitrate, and dissolved organic matter, had no effect, or even accelerated BPA abatement. Particularly, the ubiquitous Br- or I- appreciably enhanced the BPA transformation efficiency, which may be ascribed to the generation of high-selective reactive HOBr or HOI. The in silico predictions suggested that the transformation products generated by halide-mediated SSL/PI systems via halogen substitutions showed greater persistence, bioaccumulation, and aquatic toxicity than BPA itself. These findings highlighted a widespread phenomenon during PI-based oxidative treatment of highly saline water, which needs special attention under solar light illumination.

Alleviation of allergic asthma by rosmarinic acid via gut-lung axis

BACKGROUND

Asthma affects 3% of the global population, leading to over 0.25 million deaths. Due to its complexity, asthma is difficult to cure or prevent, and current therapies have limitations. This has led to a growing demand for alternative asthma treatments. We found rosmarinic acid (RosA) as a potential new drug candidate from natural medicine. However, RosA has poor bioavailability and remains mainly in the gastrointestinal tract after oral administration, suggesting the involvement of gut microbiota in its bioactivity.

PURPOSE

To investigate the mechanism of RosA in alleviating allergic asthma by gut-lung axis.

METHODS

We used 16S rRNA gene sequencing and metabolites analysis to investigate RosA's modulation of gut microbiota. Techniques of molecular biology and metabolomics were employed to study the pharmacological mechanism of RosA. Cohousing was used to confirm the involvement of gut microbiota in RosA-induced improvement of allergic asthma.

RESULTS

RosA decreased cholate levels from spore-forming bacteria, leading to reduced 5-hydroxytryptamine (5-HT) synthesis, bronchoconstriction, vasodilation, and inflammatory cell infiltration. It also increased short-chain fatty acids (SCFAs) levels, facilitating the expression of intestinal tight junction proteins to promote intestinal integrity. SCFAs upregulated intestinal monocarboxylate transporters (MCTs), thereby improving their systemic delivery to reduce Th2/ILC2 mediated inflammatory response and suppress eosinophil influx and mucus production in lung. Additionally, RosA inhibited lipopolysaccharide (LPS) production and translocation, leading to reduced TLR4-NFκB mediated pulmonary inflammation and oxidative stress.

CONCLUSIONS

The anti-asthmatic mechanism of oral RosA is primarily driven by modulation of gut microbiota-derived 5-HT, SCFAs, and LPS, achieving a combined synergistic effect. RosA is a safe, effective, and reliable drug candidate that could potentially replace glucocorticoids for asthma treatment.

Achromobacter species (sp.) outbreak caused by hospital equipment containing contaminated water: risk factors for infection

BACKGROUND

Nosocomial outbreaks of urinary tract infections caused by Achromobacter spp. have been rare in recent decades.

AIM

To identify the origin of an Achromobacter sp. outbreak, conduct multi-modal infection control measures, and finally to stop the outbreak. To this end, an epidemiological outbreak investigation and risk factor analysis were performed.

METHODS

Achromobacter sp. was detected in 22 patients in our urology wards and six environmental cultures of specimens obtained from the operating rooms. Strains isolated were submitted for antimicrobial susceptibility testing. An on-site epidemiological investigation, evaluation of patient medical records, and environmental sampling were performed to identify the source of the outbreak, and implementation of infection control intervention. A case-control study was performed to analyse the potential risk factors.

FINDINGS

Environmental sampling showed that the source of the infection for 22 patients was an ISA-IIIA-type medical pressurizer containing contaminated water. A case-control analysis showed that the risk factors for infection were: diagnosis of kidney/ureteral stones, surgery, placement of a double-J stent, and history of hospitalization in the past three months.

CONCLUSION

It was concluded that the outbreak occurred in patients who underwent internal lithotripsy and double-J stent placement, due to contact transmission with the contaminated sensor and connecting tubes of the ISA-IIIA-type medical pressurizer.

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.

An anti-infection and biodegradable TFRD-loaded porous scaffold promotes bone regeneration in segmental bone defects -experimental studies

BACKGROUND

Addressing segmental bone defects remains a complex task in orthopedics, and recent advancements have led to the development of novel drugs to enhance the bone regeneration. However, long-term oral administration can lead to malnutrition and poor patient compliance. Scaffolds loaded with medication are extensively employed to facilitate the restoration of bone defects.

METHODS

Inspired by the local use of total flavonoids of Rhizoma Drynariae (TFRD) in the treatment of fracture, a novel 3D-printed HA/CMCS/PDA/TFRD scaffold with anti-infection, biodegradable and induced angiogenesis was designed, and to explore its preclinical value in segmental bone defect of tibia.

RESULTS

The scaffold exhibited good degradation and drug release performance. In vitro, the scaffold extract promoted osteogenesis by enhancing bone-related gene/protein expression and mineral deposition in BMSCs. It also stimulated endothelial cell migration and promoted angiogenesis through the upregulation of specific genes and proteins associated with cell migration and tube formation. This may be attributed to the activation of the PI3k/AKT/HIF-1α pathway, facilitating the processes of osteogenesis and angiogenesis. Furthermore, the HA/CMCS/PDA/TFRD scaffold was demonstrated to alleviate infection, enhance angiogenesis, promote bone regeneration, and increase the maximum failure force of new formed bone in a rat model of segmental bone defects.

CONCLUSION

Porous scaffolds loaded with TFRD can reduce infection, be biodegradable, and induce angiogenesis, presenting a novel approach for addressing tibial segmental bone defects.

Bilateral Inferior Petrosal Sinus Sampling Without Lateralization Is Less Accurate for the Diagnosis of Cushing Disease

Context

During bilateral inferior petrosal sinus sampling (BIPSS), the side-to-side adrenocorticotropic hormone (ACTH) ratio, referred to as sampling lateralization, was used to predict pituitary adenoma localization.

Objective

To investigate the potential different diagnostic accuracy of BIPSS for differentiating Cushing disease (CD) and ectopic ACTH secretory syndrome (EAS) patients with low lateralization (inferior petrosal sinus [IPS]:IPS ≤ 1.4) and high lateralization (IPS:IPS > 1.4).

Methods

This single-center retrospective study (2011-2021) included (all patients had BIPSS results and confirmed pathologic diagnoses) 220 consecutive CD patients (validation set), 30 EAS patients, and 40 of the CD patients who had digital subtraction angiography (DSA) videos (discovery set).

Results

In the discovery set, the low-lateralization CD group (n = 11) had a higher median plasma ACTH concentration (62.2, IQR 44.7-181.0 ng/L) than the high-lateralization CD group (n = 29) (33.0, IQR 18.5-59.5, P = .013). Lower IPS to peripheral ratios were observed in the low-lateralization group during BIPSS, both before and after stimulation (P = .013 and P = .028). The sensitivity of BIPSS before stimulation in differentiating CD from EAS was lower in the low-lateralization group than the high-lateralization group (54.6% vs 93.1%, P = .003), as validated in the validation set. DSA videos revealed higher vascular area difference visible in the 2 sides of the pituitary in low lateralization (median 1.2 × 105 pixels, IQR 0.5-1.8) than the high-lateralization group (0.4 × 105 pixels, IQR 0.1-0.7, P = .008). The vascular area ratio of the 2 sides was also significantly higher in low (1.55, IQR 1.31-2.20) than high lateralization (1.19, IQR 1.07-1.35, P = .010).

Conclusion

Our study suggested that low lateralization in CD patients may reduce the diagnostic sensitivity of BIPSS, which might be potentially associated with peripituitary vascular anatomy.

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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Transcranial Direct Current Stimulation for Knee Osteoarthritis: A Systematic Review and Meta-Analysis of Randomized Controlled Trials

OBJECTIVE

The effects of transcranial direct current stimulation (tDCS) in the treatment of knee osteoarthritis (KOA) is still unclear. The objective is to evaluate the efficacy and safety of tDCS in improving symptoms in patients with KOA.

METHODS

The following electronic databases were searched for eligible randomized controlled trials (RCTs): PubMed, Embase, Web of Science, and the Cochrane Library. The search was performed from the inception dates to April 30, 2023. Data extraction and quality assessment were performed by two independent reviewers. Standard mean differences (SMDs) with 95% confidence intervals (95% CIs) for pooled data were calculated. A random-effects model was used for the data analyses. The primary outcomes were pain and physical function. Secondary outcomes included stiffness, mobility performance, quality of life, pressure pain tolerance, and plasma levels of brain-derived neurotrophic factor (BDNF).

RESULTS

This meta-analysis included 13 RCTs. tDCS was significantly associated with pain decrease compared with sham tDCS (SMD = -0.62, 95% CI -0.87 to -0.37, P < 0.00001). When comparing tDCS plus other non-tDCS with sham tDCS plus other non-tDCS, there was no longer a significant association with pain decrease (SMD = -0.45, 95% CI -1.08 to 0.17, P = 0.16). The changes in physical function were not significantly different between the tDCS and sham tDCS groups (SMD = -0.09, 95% CI -0.56 to 0.38, P = 0.71). When comparing tDCS plus other non-tDCS with sham tDCS plus other non-tDCS, there was still no significant association with improvement in physical function (SMD = -0.66, 95% CI -1.63 to 0.30, P = 0.18). There was no significant difference with improvement in stiffness (SMD = -0.21, 95% CI -0.77 to 0.34, P = 0.45), mobility performance (SMD = 4.58, 95% CI -9.21 to 18.37, P = 0.51), quality of life (SMD = -7.01, 95% CI -22.61 to 8.59, P = 0.38), and pressure pain tolerance (SMD = 0.30, 95% CI -0.09 to 0.69, P = 0.13). There was a statistically significant reduction in plasma levels of BDNF (SMD = -13.57, 95% CI -24.23 to -2.92, P = 0.01).

CONCLUSION

In conclusion, tDCS could significantly alleviate pain, but it might have no efficacy in physical function, stiffness, mobility performance, quality of life, and pressure pain tolerance among patients with KOA.

Observation of Cabibbo-Suppressed Two-Body Hadronic Decays and Precision Mass Measurement of the Ω_{c}^{0} Baryon

The first observation of the singly Cabibbo-suppressed Ω_{c}^{0}→Ω^{-}K^{+} and Ω_{c}^{0}→Ξ^{-}π^{+} decays is reported, using proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4  fb^{-1}, collected with the LHCb detector between 2016 and 2018. The branching fraction ratios are measured to be B(Ω_{c}^{0}→Ω^{-}K^{+})/B(Ω_{c}^{0}→Ω^{-}π^{+})=[6.08±0.51(stat)±0.40(syst)]%,B(Ω_{c}^{0}→Ξ^{-}π^{+})/B(Ω_{c}^{0}→Ω^{-}π^{+})=[15.81±0.87(stat)±0.44(syst)±0.16(ext)]%. In addition, using the Ω_{c}^{0}→Ω^{-}π^{+} decay channel, the Ω_{c}^{0} baryon mass is measured to be M(Ω_{c}^{0})=2695.28±0.07(stat)±0.27(syst)±0.30(ext)  MeV, improving the precision of the previous world average by a factor of 4.

Enhanced Production of Λ_{b}^{0} Baryons in High-Multiplicity pp Collisions at sqrt[s]=13 TeV

The production rate of Λ_{b}^{0} baryons relative to B^{0} mesons in pp collisions at a center-of-mass energy sqrt[s]=13  TeV is measured by the LHCb experiment. The ratio of Λ_{b}^{0} to B^{0} production cross sections shows a significant dependence on both the transverse momentum and the measured charged-particle multiplicity. At low multiplicity, the ratio measured at LHCb is consistent with the value measured in e^{+}e^{-} collisions, and increases by a factor of ∼2 with increasing multiplicity. At relatively low transverse momentum, the ratio of Λ_{b}^{0} to B^{0} cross sections is higher than what is measured in e^{+}e^{-} collisions, but converges with the e^{+}e^{-} ratio as the momentum increases. These results imply that the evolution of heavy b quarks into final-state hadrons is influenced by the density of the hadronic environment produced in the collision. Comparisons with several models and implications for the mechanisms enforcing quark confinement are discussed.

Eutrophication diminishes bacterioplankton functional dissimilarity and network complexity while enhancing stability: Implications for the management of eutrophic lakes

Eutrophication is a growing environmental concern in lake ecosystems globally, significantly impacting the structures and ecological functions of bacterioplankton communities and posing a substantial threat to the stability of lake ecosystems. However, the patterns of functional dissimilarity, network complexity, and stability within bacterioplankton communities across different trophic states, along with the underlying mechanisms through which eutrophication influences these aspects, are not well-understood. To bridge this knowledge gap, we collected 88 samples from 34 lakes spanning trophic gradients and investigated bacterioplankton communities using network analysis and multiple statistical methods. Our results reveal that eutrophication, progressing from mesotrophic to hyper-eutrophic states, reduces the putative functional dissimilarity of bacterioplankton, particularly affecting the relative proportions of functional groups such as oxygenic photoautotrophy, phototrophy, and photoautotrophy. Network complexity exhibited a unimodal pattern across increasing trophic states, peaking at mesotrophic states and then decreasing towards hyper-eutrophic conditions, while stability exhibited the opposite pattern (U-shaped), indicating a variation in response to trophic state changes. In essence, eutrophication diminishes network complexity but enhances network stability. Collectively, these findings shed light on the ecological impact of eutrophication on bacterioplankton communities and elucidate the potential mechanisms by which eutrophication drives functional dissimilarity, network complexity and stability within bacterioplankton communities. These insights carry significant implications for the ecological management of eutrophic lakes.

Improved Measurement of CP Violation Parameters in B_{s}^{0}→J/ψK^{+}K^{-} Decays in the Vicinity of the ϕ(1020) Resonance

The decay-time-dependent CP asymmetry in B_{s}^{0}→J/ψ(→μ^{+}μ^{-})K^{+}K^{-} decays is measured using proton-proton collision data, corresponding to an integrated luminosity of 6  fb^{-1}, collected with the LHCb detector at a center-of-mass energy of 13 TeV. Using a sample of approximately 349 000 B_{s}^{0} signal decays with an invariant K^{+}K^{-} mass in the vicinity of the ϕ(1020) resonance, the CP-violating phase ϕ_{s} is measured, along with the difference in decay widths of the light and heavy mass eigenstates of the B_{s}^{0}-B[over ¯]_{s}^{0} system, ΔΓ_{s}, and the difference of the average B_{s}^{0} and B^{0} meson decay widths, Γ_{s}-Γ_{d}. The values obtained are ϕ_{s}=-0.039±0.022±0.006  rad, ΔΓ_{s}=0.0845±0.0044±0.0024  ps^{-1}, and Γ_{s}-Γ_{d}=-0.0056_{-0.0015}^{+0.0013}±0.0014  ps^{-1}, where the first uncertainty is statistical and the second systematic. These are the most precise single measurements to date and are consistent with expectations based on the Standard Model and with the previous LHCb analyses of this decay. These results are combined with previous independent LHCb measurements. The phase ϕ_{s} is also measured independently for each polarization state of the K^{+}K^{-} system and shows no evidence for polarization dependence.

Measurement of CP Violation in B^{0}→ψ(→ℓ^{+}ℓ^{-})K_{S}^{0}(→π^{+}π^{-}) Decays

A measurement of time-dependent CP violation in the decays of B^{0} and B[over ¯]^{0} mesons to the final states J/ψ(→μ^{+}μ^{-})K_{S}^{0}, ψ(2S)(→μ^{+}μ^{-})K_{S}^{0} and J/ψ(→e^{+}e^{-})K_{S}^{0} with K_{S}^{0}→π^{+}π^{-} is presented. The data correspond to an integrated luminosity of 6  fb^{-1} collected at a center-of-mass energy of sqrt[s]=13  TeV with the LHCb detector. The CP-violation parameters are measured to be S_{ψK_{S}^{0}}=0.717±0.013(stat)±0.008(syst) and C_{ψK_{S}^{0}}=0.008±0.012(stat)±0.003(syst). This measurement of S_{ψK_{S}^{0}} represents the most precise single measurement of the CKM angle β to date and is more precise than the current world average. In addition, measurements of the CP-violation parameters of the individual channels are reported and a combination with the LHCb Run 1 measurements is performed.

Autonomous ship navigation with an enhanced safety collision avoidance technique

The motion of an autonomous ship is different from that of ground and aerial robots due to its maneuvering and environmental constraints. As a result, many techniques have been introduced for autonomous ship path planning. This paper presents a novel technique for global and local navigation planning of autonomous ships under complex static and dynamic constraints. Our technique, termed safety-enhanced path planning (SPP), has been developed to avoid potential collisions with underwater obstacles near seaside areas. SPP pre-processes the map to preserve the shape of visible obstacles and mark a safety-outline around the shores. Subsequently, an offset safety line (OSL) is drawn about the original shore to protect the ship when passing close to threat-defined offshore areas. The global path is produced with an enhanced A* multi-directional algorithm, considering the kinematic constraint of the ship. To ensure optimal path quality, the global path is further refined with a smoothing filter to improve consistency and smoothness. Additionally, local navigation is introduced to help the autonomous ship avoid collisions with other obstacle ships. Local offset trajectories are produced with 4th and 5th degree polynomials along longitudinal and lateral coordinates in time t. Distance closest point approach (DCPA) is utilized for early obstacle prediction to help the ship maneuver in complex dynamic obstacle avoidance scenarios. The trajectory set is filtered with an efficient cost policy to obtain the best trajectory for dynamic collision avoidance. We conduct simulations in MATLAB and compared with other maritime path planning methods to verify the effectiveness of our approach.

Hollow Spherical Heterostructured FeCo-P Catalysts Derived from MOF-74 for Efficient Overall Water Splitting

The design of catalysts with tunable active sites in heterogeneous interface structures is crucial for addressing challenges in the water-splitting process. Herein, a hollow spherical heterostructure FeCo-P is successfully prepared by hydrothermal and phosphorization methods. This hollow structure, along with the heterogeneous interface between Co2 P and FeP, not only facilitates the exposure of more active sites, but also increases the contact area between the catalyst and the electrolyte, as well as shortens the distance for mass/electron transfer. This enhancement promotes electron transfer to facilitate water decomposition. FeCo-P exhibits excellent hydrogen evolution (HER) and oxygen evolution (OER) performance when reaching @ 10 mA cm-2 in 1 mol L-1  KOH, with overpotentials of 131/240 mV for HER/OER. Furthermore, when FeCo-P is used as both the cathode and anode for overall water splitting (OWS), it only requires low voltages of 1.49, 1.55, and 1.57 V to achieve CDs of 10, 100, and 300 mA cm-2 , respectively. Density functional theory calculations indicate that constructing a Co2 P and FeP heterogeneous interface with good lattice matching can facilitate electron redistribution, thereby enhancing the electrocatalytic performance of OWS. This work opens up new possibilities for the rational design of efficient water electrolysis catalysts derived from MOFs.

The global burden of lymphoma: estimates from the Global Burden of Disease 2019 study

OBJECTIVES

The aim of this study was to describe the global trends in the burden of lymphoma from 1990 to 2019.

STUDY DESIGN

The data used in this study were from the Global Burden of Disease 2019 study.

METHODS

This study described the age-standardised rates of incidence, prevalence, mortality, years of life lost (YLLs), years lived with disability (YLDs), and disability-adjusted life years (DALYs) of lymphoma (non-Hodgkin and Hodgkin's lymphoma, NHL and HL, respectively) annually from 1990 to 2019, stratified by sociodemographic index (SDI) and 21 world regions. The estimated annual percentage changes in these indexes were calculated.

RESULTS

In 2019, the age-standardised rates of HL per 100,000 population were lower than those of NHL in terms of incidence (1.1 vs 6.7 per 100,000 person-years, respectively) and prevalence (0.3 vs 5.7 per 100,000 person-years, respectively) but not mortality (21.6 vs 3.2 per 100,000 person-years, respectively). From 1999 to 2019, the global incidence of HL decreased and the incidence of NHL increased, and the prevalence of both HL and NHL increased, but the mortality rates decreased. When stratified by SDI, the incidence of HL decreased in all but middle-SDI regions, the mortality rate of HL decreased in all regions, and both the incidence and mortality rate of NHL increased in all but high-SDI regions. The prevalence of HL and NHL increased in all SDI regions, especially in middle-SDI regions. YLLs and DALYs of HL in all SDI regions and those of NHL in high-SDI regions decreased. YLDs slightly increased in middle- to high-SDI regions.

CONCLUSIONS

Lymphoma remains a major public health issue, and better prevention, precise identification, and promising treatments are vitally important.

How much organic carbon could the soil store? The carbon sequestration potential of Australian soil

Soil is a huge carbon (C) reservoir, but where and how much extra C can be stored is unknown. Current methods to estimate the maximum amount of mineral-associated organic carbon (MAOC) stabilized in the fine fraction (clay + silt,< 20 μm $$ <20\;\upmu \mathrm{m} $$ ) fit through the MAOC versus clay + silt relationship, not their maxima, making their estimates more uncertain and unreliable. We need a function that 'envelopes' that relationship. Here, using 5089 observations, we estimated that the uppermost 30 cm of Australian soil holds 13 Gt (10-18 Gt) of MAOC. We then fitted frontier lines, by soil type, to the relationship between MAOC and the percentage of clay + silt to estimate the maximum amounts of MAOC that Australian soils could store in their current environments, and calculated the MAOC deficit, or C sequestration potential. We propagated the uncertainties from the frontier line fitting and mapped the estimates of these values over Australia using machine learning and kriging with external drift. The maps show regions where the soil is more in MAOC deficit and has greater sequestration potential. The modelling shows that the variation over the whole continent is determined mainly by climate, linked to vegetation and soil mineralogy. We find that the MAOC deficit in Australian soil is 40 Gt (25-60 Gt). The deficit in the vast rangelands is 20.84 Gt (13.97-29.70 Gt) and the deficit in cropping soil is 1.63 Gt (1.12-2.32 Gt). Management could increase C sequestration in these regions if the climate allowed it. Our findings provide new information on the C sequestration potential of Australian soils and highlight priority regions for soil management. Australia could benefit environmentally, socially and economically by unlocking even a tiny portion of its soil's C sequestration potential.

Proportion of participants with type 2 diabetes achieving a metabolic composite endpoint with once-weekly semaglutide treatment versus comparators: Post hoc pooled analysis from SUSTAIN 1-5, 7-10 and SUSTAIN China

AIM

To compare the proportion of participants with type 2 diabetes (T2D) treated with once-weekly (OW) subcutaneous (SC) semaglutide versus comparators who achieved a composite metabolic endpoint.

MATERIALS AND METHODS

SUSTAIN 1-5, 7-10 and SUSTAIN China trial data were pooled. Participants with T2D (aged ≥18 years) and glycated haemoglobin ≥7.0% (≥53 mmol/mol) who had been randomized to OW SC semaglutide (0.5 or 1.0 mg) or comparator in addition to background medication. Using patient-level data pooled by treatment, proportions of participants achieving the metabolic composite endpoint, defined as glycated haemoglobin <7% (<53 mmol/mol), blood pressure <140/90 mmHg and non-high-density lipoprotein cholesterol <130 mg/dl (<3.37 mmol/L), were evaluated following baseline adjustments. Endpoints were analysed per trial using a binomial logistic regression model with treatment, region/country and stratification factor as fixed effects and baseline value as covariate. Pooled analysis used logistic regression with treatment and trial as fixed effects and baseline value as covariate.

RESULTS

This post hoc analysis included data from 7633 participants across 10 trials. The proportion of participants who achieved the metabolic composite endpoint was significantly higher with OW SC semaglutide 0.5 and 1.0 mg versus comparators (23.7% and 32.0% vs. 11.5%, respectively; p < .0001). Likewise, when the OW SC semaglutide doses were pooled, significantly higher proportions of patients receiving semaglutide achieved the composite metabolic endpoint versus comparators (29.1% vs. 11.4%, respectively; p < .0001).

CONCLUSIONS

Treatment with OW SC semaglutide versus comparators was associated with increased proportions of participants with T2D meeting the composite metabolic endpoint.

Bacterial butyrate mediates the anti-atherosclerotic effect of silybin

Silybin (SIL) is a versatile bioactive compound used for improving liver damage and lipid disorders and is also thought to be beneficial for atherosclerosis (AS). The goal of this study was to investigate the efficacy of SIL in the treatment of AS in ApoE-/-mice fed a high-fat diet and explore the mechanism underlying treatment outcomes. We found that SIL significantly alleviated AS-related parameters, including the extent of aortic plaque formation, hyperlipidemia, and adhesion molecule secretion in the vascular endothelium. 16 S rRNA gene sequencing analysis, together with the application of antibiotics, showed that intestinal butyrate-producing bacteria mediated the ameliorative effect of SIL on AS. Further analysis revealed that SIL facilitated butyrate production by increasing the level of butyryl-CoA: acetate CoA-transferase (BUT). The increased expression of monocarboxylic acid transporter-1 (MCT1) induced by butyrate and MCT4 induced by SIL in the apical and basolateral membranes of colonocytes, respectively, resulted in enhanced absorption of intestinal butyrate into the circulation, leading to the alleviation of arterial endothelium dysfunction. Moreover, the SIL-mediated increase in intestinal butyrate levels restored gut integrity by upregulating the expression of tight junction proteins and promoting gut immunity, thus inhibiting the AS-induced inflammatory response. This is the first study to show that SIL can alleviate AS by modulating the production of bacterial butyrate and its subsequent absorption.

[Relationship between intramuscular fat content in the quadriceps muscle and clinical severity in patients with knee osteoarthritis]

OBJECTIVE

To explore relationship between intramuscular fat content of quadriceps femoris and clinical severity of knee osteoarthritis (KOA).

METHODS

Totally 30 KOA patients were selected from February 2021 to June 2021, including 6 males and 24 females, aged with an average of (64.20±9.19) years old, and body mass index (BMI) was (24.92±3.35) kg·m-2. Patients were divided into relative severe leg (RSL) and relative moderate leg (RML) according to severity of pain on visual analogue scale(VAS). Musculoskeletal ultrasound was used to collect muscle images of quadriceps muscles on both sides of the patient, and Image J was used to analyze echo intensity (EI) of each muscle. Both VAS and Western Ontario and McMaster Universities Osteoarthritis Index (WOMAC) were used to assess pain and function. Quadriceps muscle EI on both sides of patients was compared. Pearson correlation analysis was conducted to analyze correlation between quadriceps muscle EI value between RSL and RML, and linear regression was used to analyze relationship between each muscle EI and VAS and WOMA scores of patients.

RESULTS

The EI of RSL lateral vastus lateralis (VL) was 123.78±36.25 and RSL vastus medialis (VM) was 109.46±30.36 which were significantly higher than those of 108.03±31.34 and 93.32±26.04 of RML (P<0.05), but there was no statistical significance in EI values of rectus femoris (RF) on both sides (P>0.05). EI values of VL and VM on both sides were significantly correlated (P<0.05). There was a significant positive correlation between VM EI value and VAS score in RSL and RML (P<0.05). VM EI values in RSL were positively correlated with total WOMAC (P<0.05), and VM VL EI values in RML were positively correlated with total WOMAC score (P<0.05).

CONCLUSION

Intramuscular fat content of quadriceps is closely related to severity of clinical symptoms in KOA patients, and the most obvious one is VM. Therefore, the intramuscular fat content of quadriceps may be an objective indicator to evaluate severity of KOA patients. At the same time, reducing intramuscular fat content of the quadriceps muscle of KOA patients may be a new direction for the prevention and treatment of KOA.

MYO5A overexpression promotes invasion and correlates with low lymphocyte infiltration in head and neck squamous carcinoma

Head and neck squamous carcinoma (HNSC) poses a significant public health challenge due to its substantial morbidity. Nevertheless, despite advances in current treatments, the prognosis for HNSC remains unsatisfactory. To address this, single-cell RNA sequencing (RNA-seq) and bulk RNA-seq data combined with in vitro studies were conducted to examine the role of MYO5A (Myosin VA) in HNSC. Our investigation revealed an overexpression of MYO5A in HNSC that promotes HNSC migration in vitro. Remarkably, knockdown of MYO5A suppressed vimentin expression. Furthermore, analyzing the TCGA database evidenced that MYO5A is a risk factor for human papillomavirus positive (HPV+) HNSC (HR = 0.81, P < 0.001). In high MYO5A expression HNSC, there was a low count of tumor infiltrating lymphocytes (TIL), including activated CD4+ T cells, CD8+ T cells, and B cells. Of note, CD4+ T cells and B cells were positively associated with improved HPV+ HNSC outcomes. Correlation analysis demonstrated a decreased level of immunostimulators in high MYO5A-expressing HNSC. Collectively, these findings suggest that MYO5A may promote HNSC migration through vimentin and involve itself in the process of immune infiltration in HNSC, advancing the understanding of the mechanisms and treatment of HNSC.

Magnonic Frequency Comb in the Magnomechanical Resonator

An optical frequency comb is a spectrum of optical radiation which consists of evenly spaced and phase-coherent narrow spectral lines and is initially invented in a laser for frequency metrology purposes. A direct analog of frequency combs in the magnonic systems has not been demonstrated to date. In our experiment, we generate a new magnonic frequency comb in the resonator with giant mechanical oscillations through the magnomechanical interaction. We observe the magnonic frequency comb contains up to 20 comb lines, which are separated by the mechanical frequency of 10.08 MHz. The thermal effect based on the strong pump power induces the cyclic oscillation of the magnon frequency shift, which leads to a periodic oscillation of the magnonic frequency comb. Moreover, we demonstrate the stabilization and control of the frequency spacing of the magnonic frequency comb via injection locking. Our Letter lays the groundwork for magnonic frequency combs in the fields of sensing and metrology.

Establishment of Biliary Atresia Prognostic Classification System via Survival-Based Forward Clustering - A New Biliary Atresia Classification

OBJECTIVES

To develop a machine learning algorithm with prognosis data to identify different clinical phenotypes of biliary atresia (BA) and provide instructions for choosing treatment schemes.

METHODS

Six hundred thirty-nine cases of type III BA were retrospectively collected from the Children's Hospital of Fudan University from Jan 1st, 2017 to Dec 1st, 2019 as a training dataset, and a survival-based forward clustering method, which can also be used to predict the subtype of a new patient was developed to identify BA subtypes.

RESULTS

A total of 2 clusters were identified (cluster 1 = 324 and cluster 2 = 315), where cluster 2 had a lower 2 y native liver survival post-Kasai rate. The infant patients in cluster 2 have higher weight, liver, and spleen volume, wider portal vein width, and older operative age; worse coagulation and liver function results; higher grade of liver fibrosis and detection rate of hepatic portal fibrous mass, and higher recent infection detection rate of herpes simplex virus type I. With the proposed prognostic classification system, the authors predicted the subtypes of the 187 cases of type III BA in a testing dataset collected from the whole year of 2020. The p-value computed from the log-rank testing for the Kaplan-Meier survival curves of the predicted two testing groups was 0.0113.

CONCLUSIONS

This classification system would be a convenient tool to choose appropriate treatment and accelerate the choice-making between clinicians and infant patients.

Outer membrane vesicles mediating horizontal transfer of the epidemic blaOXA-232 carbapenemase gene among Enterobacterales

OXA-232 is one of the most common OXA-48-like carbapenemase derivatives and is widely disseminated in nosocomial settings across countries. The blaOXA-232 gene is located on a 6-kb non-conjugative ColKP3-type plasmid, while the dissemination of blaOXA-232 into different Enterobacterales species and the polyclonal dissemination of OXA-232-producing K. pneumoniae revealed the horizontal transfer of blaOXA-232. However, it's still unclear how this non-conjugative ColKP3 plasmid could facilitate the mobilization of blaOXA-232. Here, we observed the in vivo intraspecies transfer of blaOXA-232 during a nosocomial outbreak of OXA-232-producing K. pneumoniae. We demonstrated the presence of ColKP3 OXA-232 plasmid in the outer membrane vesicles (OMVs) derived from clinical isolates, and OMVs could facilitate the horizontal transfer of blaOXA-232 among Enterobacterales. In contrast, for the most prevalent carbapenemase genes, including blaKPC-2 and blaNDM-1, though the presence of carbapenemase genes and plasmid backbones in the vesicular lumen was observed, OMVs couldn't promote effective transformation, probably due to the low copy number of plasmids in clinical isolates and the low number of plasmids loaded into vesicles. Conjugation assay revealed that the epidemic IncX3 NDM-1 and IncFII(pHN7A8)/IncR KPC-2 plasmids were conjugative and could be horizontally transferred via independent conjugation or with the help of a co-existent conjugative plasmid. For the large-size and low-copy number conjugative plasmids carrying carbapenemase genes, OMVs-mediated gene exchange may only serve as an alternative pathway for horizontal transfer. In conclusion, diverse mobilization strategies were employed by plasmids harboring carbapenemase genes, and plasmids display a proper choice of mobility pathway due to their individual properties.

Warming reduces microeukaryotic diversity, network complexity and stability

Unraveling how climate warming affects microorganisms and the underlying mechanisms has been a hot topic in climate change and microbial ecology. To date, many studies have reported microbial responses to climate warming, especially in soil ecosystems, however, knowledge of how warming influences microeukaryotic diversity, network complexity and stability in lake ecosystems, in particular the possible underlying mechanisms, is largely unknown. To address this gap, we conducted 20 mesocosms spanning five temperature scenarios (26 °C, 27.5 °C, 29 °C, 30.5 °C, and 32 °C) in Lake Bosten, a hotspot for studying climate change, and investigated microeukaryotic communities using 18S rRNA gene sequencing. Our results demonstrated that warming, time, and their interactions significantly reduced microeukaryotic α-diversity (two-way ANOVA: P＜0.01). Although warming did not significantly affect microeukaryotic community structure (ANOSIM: P＞0.05), it enhanced species turnover. Microeukaryotic networks exhibited distinct co-occurrence patterns and topological properties across temperature scenarios. Warming reduced network complexity and stability, as well as altered species interactions. Collectively, these findings are likely to have implications for ecological management of lake ecosystems, in particular semi-arid and arid regions, and for predicting ecological consequences of climate change.

Nosocomial dissemination of blaIMP-4 among Klebsiella pneumoniae by horizontal gene transfer and clonal spread: the epidemic IncN plasmids and the emerging high-risk IMP-4-producing ST101 clone

OBJECTIVES

To determine the genomic features of IMP-4-producing Klebsiella pneumoniae isolates recovered from paediatric patients and the transmission dynamics of blaIMP-4.

METHODS

IMP-producing K. pneumoniae isolates were collected from paediatric patients in Shanghai Children's Medical Center from 2013 to 2020. WGS was performed for all isolates, and the complete genomes of three IMP-4-producing isolates were generated. The distribution of blaIMP-4-harbouring plasmids was determined, and a conjugation assay was employed to investigate the horizontal transfer of blaIMP-4-harbouring plasmids.

RESULTS

We collected 21 blaIMP-carrying K. pneumoniae isolates, with IMP-4 (16/21, 76.2%) as the predominant subtype, followed by IMP-8 (n = 3) and IMP-26 (n = 2). IMP-4-producing isolates displayed a diverse population structure and all blaIMP-4 genes were located on plasmids, including IncN (n = 9), IncHI5 (n = 5), IncFII(K) (n = 1) and IncFII(pKP91) (n = 1), although only IncN plasmids were conjugative. Clonal transmission of ST101 strains carrying IncHI5 blaIMP-4-harbouring plasmids was observed, and the acquisition of blaIMP-4 by the international high-risk ST101 clone constituted a novel combination of ST101 clone and carbapenemase genes. Plasmid analysis demonstrated that the conjugal transfer of the IncHI5 blaIMP-4-harbouring plasmid might be blocked by the ST101 bacterial host.

CONCLUSIONS

The horizontal transfer of IncN plasmids and clonal spread of the international high-risk ST101 clone facilitated the nosocomial dissemination of blaIMP-4 among K. pneumoniae. The emerging IMP-4-producing ST101 clone displays diverse combinations of carbapenemase genes, and this clone could be a continually evolving threat and warrants prospective monitoring.

Astragalus membranaceus and Salvia miltiorrhiza ameliorate diabetic kidney disease via the "gut-kidney axis"

BACKGROUND

The combination of Astragalus membranaceus and Salvia miltiorrhiza (AS) is an effective prescription for treating diabetic kidney disease (DKD) in traditional Chinese medicine. Its efficacy in treating DKD has been confirmed, but the potential regulatory mechanism has not yet been fully clarified.

PURPOSE

To explore the mechanism by which AS regulates the "gut-metabolism-transcription" coexpression network under the action of the "gut-kidney axis" to ameliorate DKD.

METHODS

SD rats were used to establish the DKD model by injecting STZ. After AS intervention, the structure and function of the kidney and colon were observed. We sequenced the gut microbiota utilizing 16S rDNA, identified serum differential metabolites using LC‒MS/MS, and observed renal mRNA expression by RNA seq. The "gut-metabolism-transcription" coexpression network was further constructed, and the target bacteria, target metabolites, and target genes of AS were ultimately screened and validated.

RESULTS

AS improved renal pathology and functional damage and increased the abundance of Akkermansia, Akkermansia_muciniphila, Lactobacillus and Lactobacillus_murinus. Fourteen target metabolites of AS were identified, which were mainly concentrated in 19 KEGG pathways, including sphingolipid metabolism and glycerophospholipid metabolism. Sixty-three target mRNAs of AS were identified. The top 20 pathways were closely related to glycolipid metabolism, and 14 differential mRNAs were expressed in these pathways. Correlation analysis showed that Akkermansia, Akkermansia muciniphila, Lactobacillus and Lactobacillus murinus were closely associated with sphingolipid metabolism, glycerophospholipid metabolism, arachidonic acid metabolism, ascorbate and aldarate metabolism and galactose metabolism. Moreover, the target metabolites and target mRNAs of AS were also enriched in five identical pathways of sphingolipid metabolism, glycerophospholipid metabolism, arachidonic acid metabolism, ascorbate and aldarate metabolism and galactose metabolism, including 8 different metabolites, such as sphingosine, and 5 different genes, such as Kng1. The 8 metabolites had high AUC prediction values, and the validation of the 5 genes was consistent with the sequencing results.

CONCLUSION

Our research showed that AS can improve DKD via the "gut-kidney axis". Akkermansia muciniphila and Lactobacillus murinus were the main driving bacteria, and five pathways related to glycolipid metabolism, especially sphingolipid metabolism and glycerophospholipid metabolism, may be important follow-up reactions and regulatory mechanisms.

Loss-free pulverization by confining copper oxide inside hierarchical nitrogen-doped carbon nanocages toward superb potassium-ion batteries

Taking the advantages of hierarchical nitrogen-doped carbon nanocages (hNCNCs) with nanocavities for encapsulation and multiscale micro-meso-macropores/high conductivity for mass/electron synergistic transportation, a conversion-type CuO anode material is confined inside hNCNCs for potassium storage. The so-obtained yolk-shelled CuO@hNCNC hybrids have tunable CuO contents in the range of 11.7-63.7 wt%. The unique architecture leads to the loss-free pulverization of the active components during charge/discharge, which increases the surface-controlled charge storage, shortens the K+ solid diffusion lengths with an enlarged K+ diffusion coefficient, and meanwhile enhances the rate capability and durability. Consequently, the optimized CuO@hNCNC delivers a high specific capacity of 498 mA h g-1 at 0.1 A g-1 and 194 mA h g-1 at 10.0 A g-1 based on the total mass of CuO@hNCNC, and a long-term stability. The capacity based on the CuO active component reaches a record-high 522 mA h g-1 at 1.0 A g-1 after 2000 cycles, which is ca. 2.5 times the state-of-the-art value in the literature. The evolution of the cycling performance with CuO loading is well understood based on the loss-free pulverization. This study demonstrates a new strategy to turn the generally harmful pulverization of active components into a beneficial factor for K+ storage, which paves the way for exploring high-performance anodes for rechargeable batteries.

Improving the therapeutic efficacy of oncolytic viruses for cancer: targeting macrophages

Oncolytic viruses (OVs) for cancer treatment are in a rapid stage of development, and the direct tumor lysis and activation of a comprehensive host immune response are irreplaceable advantages of cancer immunotherapy. However, excessive antiviral immune responses also restrict the spread of OVs in vivo and the infection of tumor cells. Macrophages are functionally diverse innate immune cells that phagocytose tumor cells and present antigens to activate the immune response, while also limiting the delivery of OVs to tumors. Studies have shown that the functional propensity of macrophages between OVs and tumor cells affects the overall therapeutic effect of oncolytic virotherapy. How to effectively avoid the restrictive effect of macrophages on OVs and reshape the function of tumor-associated macrophages in oncolytic virotherapy is an important challenge we are now facing. Here, we review and summarize the complex dual role of macrophages in oncolytic virotherapy, highlighting how the functional characteristics of macrophage plasticity can be utilized to cooperate with OVs to enhance anti-tumor effects, as well as highlighting the importance of designing and optimizing delivery modalities for OVs in the future.

Clinical efficacy in one-year treatment with Artemisia annua-SLIT drops in monosensitized and polysensitized individuals

PURPOSE

Seasonal allergic rhinoconjunctivitis (SARC) caused by Artemisia seriously affects patients' quality of life in northern China. This study aimed to estimate further the efficacy and safety of a one-year course of Artemisia annua-sublingual immunotherapy (SLIT) on SARC patients.

MATERIALS AND METHODS

This was an open-label, randomized, controlled, single-centre study involving 150 SARC patients induced by Artemisia, randomized to SLIT group (n = 75, SLIT along with pharmacotherapy) or control group (n = 75, pharmacotherapy only). According to the skin prick test (SPT) results, the SLIT group was divided into monosensitized and polysensitized groups to analyze the influence of sensitization status on the efficacy of Artemisia annua-SLIT. The clinical indicators of this study were total rhinoconjunctivitis symptom score (TRSS), total medication score (TMS), combined scores of medication and rhinoconjunctivitis symptom (CSMRS), and score of visual analog scale (VAS). Safety was evaluated by the occurrence of adverse events (AEs). Daily administration of the drops was recorded in diaries by the patients.

RESULTS

After nearly one year of treatment and follow-ups, there was a significant decline in TRSS, TMS, CSMRS, and VAS from the baseline scores in the SLIT group (p < 0.001). However, as pollen counts increased in 2022, indicators above in the control group increased significantly during the peak pollen phase (PPP) in 2022 grass pollen season (GPS) compared to the baseline. Meanwhile, we found no significant difference in TRSS, TMS, CSMRS, and VAS between the monosensitized and polysensitized groups (p > 0.05). Moreover, the result indicated that the clinical improvement in TRSS, TMS, CSMRS, and VAS was still observed in polysensitized patients who were allergic to Artemisia pollen and sensitized to house dust mite (HDM) (n = 15) in PPP of 2022, compared to the baseline value (p < 0.001).

CONCLUSION

Artemisia annua-SLIT was proven effective, tolerable and safe in patients with SARC after nearly one year of treatment, whether monosensitization or polysensitization.

Differences in pathogenic community assembly processes and their interactions with bacterial communities in river and lake ecosystems

Pathogenic bacterial infections caused by water quality degradation are one of the most widespread environmental problems. Clarifying the structure of pathogens and their assembly mechanisms in lake ecosystems is vital to prevent the infestation of waterborne pathogens and maintain human health. However, the composition and assembly mechanisms of pathogenic bacterial communities in river and lake ecosystems are still poorly understood. In this study, we collected 17 water and 17 sediment samples from Lake Chaohu and its 11 inflow rivers. Sequencing of 16S rRNA genes was used to study bacterial pathogen communities. The results of the study showed that there was a significant difference (P < 0.05) in the composition of the pathogen community between riverine and lake habitats. Acinetobacter (36.49%) was the dominant bacterium in the river, whereas Flavobacterium (21.6%) was the most abundant bacterium in the lake. Deterministic processes (i.e., environmental filtering and species interaction) drove the assembly of pathogenic bacterial communities in the lake habitat, while stochastic processes shaped river pathogenic bacterial communities. Spearman correlation analysis showed that the α-diversity of bacterial communities was linearly and negatively linked to the relative abundance of pathogens. Having a higher bacterial community diversity had a suppressive effect on pathogen abundance. In addition, co-occurrence network analysis showed that bacterial communities were tightly linked to pathogenic bacteria. Pseudomonas aeruginosa and Salmonella enterica were identified as keystone species in an inflow water sampling network (W_FR), reducing the complexity of the network. These results provide a reference for assessments of water quality safety and pathogenic bacteria posing risks to human health in large freshwater lakes.

Oxidized Low-Density Lipoprotein (Ox-LDL)-Triggered Double-Lock Probe for Spatiotemporal Lipoprotein Oxidation and Atherosclerotic Plaque Imaging

Low-density lipoprotein (LDL), especially oxidative modified LDL (Ox-LDL), is the key risk factor for plaque accumulation and the development of cardiovascular disease. Herein, a highly specific Ox-LDL-triggered fluorogenic-colorimetric probe Pro-P1 is developed for visualizing the oxidation and aggregation progress of lipoproteins and plaque. A series of green fluorescent protein chromophores with modified donor-acceptor structures, containing carbazole as an electron donor and various substituents including pyridine-vinyl (P1), phenol-vinyl (P2), N, N-dimethylaniline-vinyl (P3), and thiophene-vinyl (P4), have been synthesized and evaluated. Emission spectroscopy and theoretical calculations of P1-P4 indicate that P1 shows enhanced green fluorescence (λem = 560 nm) by inhibiting its twisted intramolecular charge transfer in the presence of Ox-LDL. This feature allows the selection of P1 as a sensitive probe to directly visualize ferroptosis and Cu2+ -mediated LDL oxidative aggregation via in situ formation of fluorophore-bound Ox-LDL in living cells. The red-emissive probe Pro-P1 (λem = 660 nm) is prepared via borate protection of P1, which can be cleaved into P1 under high expression of HOCl and Ox-LDL condition at the lesion site, resulting in enhanced green emission. The plaque area and size with clear boundaries can be delineated by colorimetric fluorescence imaging and fluorescence lifetime imaging with precise differentiation.

Ceftazidime/Avibactam Resistance in Carbapenemase-Producing Klebsiella pneumoniae

We identified a novel ceftazidime/avibactam resistance mechanism in sequence type 11 Klebsiella pneumoniae carbapenemase 2-producing K. pneumoniae. Plasmid recombination and chromosomal integration formed a novel virulence plasmid and provided an additional promoter for blaSHV-12, leading to blaSHV-12 overexpression and ceftazidime/avibactam resistance. Genetic rearrangement contributed to convergence of hypervirulence and ceftazidime/avibactam resistance.

Efficacy and safety of Artemisia annua sublingual immunotherapy in patients with seasonal allergic rhinoconjunctivitis over two pollen seasons

OBJECTIVE

This study investigates the efficacy and safety of sublingual immunotherapy (SLIT) with A. annua allergens in patients with seasonal allergic rhinoconjunctivitis over two pollen seasons.

METHODS

Seventy patients with moderate-severe seasonal allergic rhinoconjunctivitis were divided evenly into the SLIT and control groups. The SLIT last from 3 months before the summer-autumn pollen season in 2021 till the end of the summer-autumn pollen season in 2022. The daily individual symptom score, total rhinoconjunctivitis symptom score (dTRSS), total medication score (dTMS), combined score of medication and rhinoconjunctivitis symptom (dCSMRS), visual analog scale (VAS) score, and adverse events (AEs) were evaluated.

RESULTS

The average pollen concentration in 2022 was twice that previous two-year during the pollen season. Fifty-six patients completed treatments (SLIT group: 29, control group: 27). Compared with baseline, the individual symptoms, dTRSS, dTMS, dCSMRS, and VAS scores of SLIT group declined in 2021. After 16 months of SLIT, all efficacy indexes in 2022 were still lower than baseline and equivalent to those in 2021. In control group, the efficacy indexes in 2022 were higher than that in 2020 and 2021. The efficacy indexes of SLIT group were lower than those of control group in 2021 and 2022. SLIT is effective for both mono- and poly-sensitized patients. AEs incidence in SLIT group was 82.7% without severe AEs.

CONCLUSIONS

The A. annua-SLIT can obtain efficacy and safety over two pollen seasons for patients with moderate-severe seasonal allergic rhinoconjunctivitis.

Observation of New Baryons in the Ξ_{b}^{-}π^{+}π^{-} and Ξ_{b}^{0}π^{+}π^{-} Systems

The first observation and study of two new baryonic structures in the final state Ξ_{b}^{0}π^{+}π^{-} and the confirmation of the Ξ_{b}(6100)^{-} state in the Ξ_{b}^{-}π^{+}π^{-} decay mode are reported using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9  fb^{-1}. In addition, the properties of the known Ξ_{b}^{*0}, Ξ_{b}^{'-} and Ξ_{b}^{*-} resonances are measured with improved precision. The new decay mode of the Ξ_{b}^{0} baryon to the Ξ_{c}^{+} π^{-} π^{+} π^{-} final state is observed and exploited for the first time in these measurements.

Precision Measurement of CP Violation in the Penguin-Mediated Decay B_{s}^{0}→ϕϕ

A flavor-tagged time-dependent angular analysis of the decay B_{s}^{0}→ϕϕ is performed using pp collision data collected by the LHCb experiment at the center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 6  fb^{-1}. The CP-violating phase and direct CP-violation parameter are measured to be ϕ_{s}^{ss[over ¯]s}=-0.042±0.075±0.009  rad and |λ|=1.004±0.030±0.009, respectively, assuming the same values for all polarization states of the ϕϕ system. In these results, the first uncertainties are statistical and the second systematic. These parameters are also determined separately for each polarization state, showing no evidence for polarization dependence. The results are combined with previous LHCb measurements using pp collisions at center-of-mass energies of 7 and 8 TeV, yielding ϕ_{s}^{ss[over ¯]s}=-0.074±0.069  rad and |λ|=1.009±0.030. This is the most precise study of time-dependent CP violation in a penguin-dominated B meson decay. The results are consistent with CP symmetry and with the standard model predictions.