RNA genome packaging and capsid assembly of bluetongue virus visualized in host cells

Unlike those of double-stranded DNA (dsDNA), single-stranded DNA (ssDNA), and ssRNA viruses, the mechanism of genome packaging of dsRNA viruses is poorly understood. Here, we combined the techniques of high-resolution cryoelectron microscopy (cryo-EM), cellular cryoelectron tomography (cryo-ET), and structure-guided mutagenesis to investigate genome packaging and capsid assembly of bluetongue virus (BTV), a member of the Reoviridae family of dsRNA viruses. A total of eleven assembly states of BTV capsid were captured, with resolutions up to 2.8 Å, with most visualized in the host cytoplasm. ATPase VP6 was found underneath the vertices of capsid shell protein VP3 as an RNA-harboring pentamer, facilitating RNA packaging. RNA packaging expands the VP3 shell, which then engages middle- and outer-layer proteins to generate infectious virions. These revealed "duality" characteristics of the BTV assembly mechanism reconcile previous contradictory co-assembly and core-filling models and provide insights into the mysterious RNA packaging and capsid assembly of Reoviridae members and beyond.

Multi-Gene Recombinant Baculovirus Expression Systems: From Inception to Contemporary Applications

Many protein expression systems are primarily utilised to produce a single, specific recombinant protein. In contrast, most biological processes such as virus assembly rely upon a complex of several interacting proteins rather than the activity of a sole protein. The high complexity of the baculovirus genome, coupled with a multiphase replication cycle incorporating distinct transcriptional steps, made it the ideal system to manipulate for high-level expression of a single, or co-expression of multiple, foreign proteins within a single cell. We have developed and utilised a series of recombinant baculovirus systems to unravel the sequential assembly process of a complex non-enveloped model virus, bluetongue virus (BTV). The high protein yields expressed by the baculovirus system not only facilitated structure-function analysis of each viral protein but were also advantageous to crystallography studies and supported the first atomic-level resolution of a recombinant viral protein, the major BTV capsid protein. Further, the formation of recombinant double-shelled virus-like particles (VLPs) provided insights into the structure-function relationships among the four major structural proteins of the BTV whilst also representing a potential candidate for a viral vaccine. The baculovirus multi-gene expression system facilitated the study of structurally complex viruses (both non-enveloped and enveloped viruses) and heralded a new generation of viral vaccines.

A new instrumentation for simultaneous terahertz and mid-infrared spectroscopy in corrosive gaseous mixtures

The correct interpretation of infrared (IR) observations of planetary atmospheres requires an accurate knowledge of temperature and partial and global pressures. Precise laboratory measurements of absorption intensities and line profiles, in the 200-350 K temperature range, are, therefore, critical. However, for gases only existing in complex chemical equilibria, such as nitrous or hypobromous acids, it is not possible to rely on absolute pressure measurements to measure absolute integrated optical absorption cross sections or IR line intensities. To overcome this difficulty, a novel dual-beam terahertz (THz)/mid-IR experimental setup has been developed, relying on the simultaneous use of two instruments. The setup involves a newly constructed temperature-controlled (200-350 K) cross-shaped absorption cell made of inert materials. The cell is traversed by the mid-IR beam from a high-resolution Fourier transform spectrometer using along a White-cell optical configuration providing absorption path lengths from 2.8 to 42 m and by a THz radiation beam (82.5 GHz to 1.1 THz), probing simultaneously the same gaseous sample. The THz channel records pure rotational lines of molecules for which the dipole moment was previously measured with high precision using Stark spectroscopy. This allows for a determination of the partial pressure in the gaseous mixture and enables absolute line intensities to be retrieved for the mid-IR range. This new instrument opens a new possibility for the retrieval of spectroscopic parameters for unstable molecules of atmospheric interest. The design and performance of the equipment are presented and illustrated by an example of simultaneous THz and mid-IR measurement on nitrous acid (HONO) equilibrium.

Measurements of Groomed-Jet Substructure of Charm Jets Tagged by D^{0} Mesons in Proton-Proton Collisions at sqrt[s]=13 TeV

Understanding the role of parton mass and Casimir color factors in the quantum chromodynamics parton shower represents an important step in characterizing the emission properties of heavy quarks. Recent experimental advances in jet substructure techniques have provided the opportunity to isolate and characterize gluon emissions from heavy quarks. In this Letter, the first direct experimental constraint on the charm-quark splitting function is presented, obtained via the measurement of the groomed shared momentum fraction of the first splitting in charm jets, tagged by a reconstructed D^{0} meson. The measurement is made in proton-proton collisions at sqrt[s]=13  TeV, in the low jet transverse-momentum interval of 15≤p_{T}^{jet ch}<30  GeV/c where the emission properties are sensitive to parton mass effects. In addition, the opening angle of the first perturbative emission of the charm quark, as well as the number of perturbative emissions it undergoes, is reported. Comparisons to measurements of an inclusive-jet sample show a steeper splitting function for charm quarks compared with gluons and light quarks. Charm quarks also undergo fewer perturbative emissions in the parton shower, with a reduced probability of large-angle emissions.

Measurement of the Lifetime and Λ Separation Energy of _{Λ}^{3}H

The most precise measurements to date of the _{Λ}^{3}H lifetime τ and Λ separation energy B_{Λ} are obtained using the data sample of Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV collected by ALICE at the LHC. The _{Λ}^{3}H is reconstructed via its charged two-body mesonic decay channel (_{Λ}^{3}H→^{3}He+π^{-} and the charge-conjugate process). The measured values τ=[253±11(stat)±6(syst)]  ps and B_{Λ}=[102±63(stat)±67(syst)]  keV are compatible with predictions from effective field theories and confirm that the _{Λ}^{3}H structure is consistent with a weakly bound system.

[Predictive factors of spontaneous pregnancies among women with diminished ovarian reserve patients treated with DHEA]

INTRODUCTION

Diminished ovarian reserve remains a challenge in the reproductive medicine field. Treatment options for these patients are limited and there is no consensus to make any recommendations. Regarding adjuvant supplements, DHEA could play a role in follicular recruitment and, therefore, may increase spontaneous pregnancy rate.

MATERIALS AND METHODS

This study was a monocentric historical and observational cohort study carried out in the reproductive medicine department at the University Hospital, Femme-Mère-Enfant in Lyon. All women presenting with a diminished ovarian reserve treated with 75mg/day of DHEA were consecutively included. The main objective was to evaluate the spontaneous pregnancy rate. The secondary objectives were to identify predictive factors for pregnancy and the evaluation of treatment side effects.

RESULTS

Four hundred and thirty-nine women were included. In all, 277 were analyzed, 59 had a spontaneous pregnancy (21.3%). The probability of being pregnant was respectively 13.2% (IC95 9-17.2%), 21.3% (IC95 15.1-27%) and 38.8% (IC95 29.3-48.4%) at 6, 12 and 24 months. Only 20.6% of patients complained of side effects.

CONCLUSION

DHEA may improve spontaneous pregnancies in women with diminished ovarian reserve without any stimulation.

Production and separation of positron emitters for hadron therapy at FRS-Cave M

The FRagment Separator FRS at GSI is a versatile spectrometer and separator for experiments with relativistic in-flight separated short-lived exotic beams. One branch of the FRS is connected to the target hall where the bio-medical cave (Cave M) is located. Recently a joint activity between the experimental groups of the FRS and the biophysics at the GSI and Department of physics at LMU was started to perform biomedical experiments relevant for hadron therapy with positron emitting carbon and oxygen beams. This paper presents the new ion-optical mode and commissioning results of the FRS-Cave M branch where positron emitting ¹⁵O-ions were provided to the medical cave for the first time. An overall conversion efficiency of 2.9±0.2×10^{-4 15}O fragments per primary ¹⁶O ion accelerated in the synchrotron SIS18 was reached.

Measurement of the J/ψ Polarization with Respect to the Event Plane in Pb-Pb Collisions at the LHC

We study the polarization of inclusive J/ψ produced in Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV at the LHC in the dimuon channel, via the measurement of the angular distribution of its decay products. We perform the study in the rapidity region 2.5 Collapse

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Affiliation(s)

S Acharya Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
D Adamová Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
A Adler Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
G Aglieri Rinella European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Agnello Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
N Agrawal INFN, Sezione di Bologna, Bologna, Italy
Z Ahammed Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Ahmad Department of Physics, Aligarh Muslim University, Aligarh, India
S U Ahn Korea Institute of Science and Technology Information, Daejeon, Republic of Korea
I Ahuja Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
A Akindinov Affiliated with an institute covered by a cooperation agreement with CERN
M Al-Turany Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Aleksandrov Affiliated with an institute covered by a cooperation agreement with CERN
B Alessandro INFN, Sezione di Torino, Turin, Italy
H M Alfanda Central China Normal University, Wuhan, China
R Alfaro Molina Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
B Ali Department of Physics, Aligarh Muslim University, Aligarh, India
Y Ali COMSATS University Islamabad, Islamabad, Pakistan
A Alici Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
N Alizadehvandchali University of Houston, Houston, Texas, USA
A Alkin European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Alme Department of Physics and Technology, University of Bergen, Bergen, Norway
G Alocco INFN, Sezione di Cagliari, Cagliari, Italy
T Alt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I Altsybeev Affiliated with an institute covered by a cooperation agreement with CERN
M N Anaam Central China Normal University, Wuhan, China
C Andrei Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
A Andronic Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
V Anguelov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
F Antinori INFN, Sezione di Padova, Padova, Italy
P Antonioli INFN, Sezione di Bologna, Bologna, Italy
C Anuj Department of Physics, Aligarh Muslim University, Aligarh, India
N Apadula Lawrence Berkeley National Laboratory, Berkeley, California, USA
L Aphecetche SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
H Appelshäuser Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S Arcelli Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
R Arnaldi INFN, Sezione di Torino, Turin, Italy
I C Arsene Department of Physics, University of Oslo, Oslo, Norway
M Arslandok Yale University, New Haven, Connecticut, USA
A Augustinus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Averbeck Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
S Aziz Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
M D Azmi Department of Physics, Aligarh Muslim University, Aligarh, India
A Badalà INFN, Sezione di Catania, Catania, Italy
Y W Baek Gangneung-Wonju National University, Gangneung, Republic of Korea
X Bai Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
R Bailhache Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
Y Bailung Indian Institute of Technology Indore, Indore, India
R Bala Physics Department, University of Jammu, Jammu, India
A Balbino Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
A Baldisseri Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
B Balis AGH University of Science and Technology, Cracow, Poland
D Banerjee Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
Z Banoo Physics Department, University of Jammu, Jammu, India
R Barbera Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
L Barioglio Physik Department, Technische Universität München, Munich, Germany
M Barlou Department of Physics, School of Science, National and Kapodistrian University of Athens, Athens, Greece
G G Barnaföldi Wigner Research Centre for Physics, Budapest, Hungary
L S Barnby Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
V Barret Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
L Barreto Universidade de São Paulo (USP), São Paulo, Brazil
C Bartels University of Liverpool, Liverpool, United Kingdom
K Barth European Organization for Nuclear Research (CERN), Geneva, Switzerland
E Bartsch Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
F Baruffaldi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
N Bastid Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
S Basu Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
G Batigne SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
D Battistini Physik Department, Technische Universität München, Munich, Germany
B Batyunya Affiliated with an international laboratory covered by a cooperation agreement with CERN
D Bauri Indian Institute of Technology Bombay (IIT), Mumbai, India
J L Bazo Alba Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
I G Bearden Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C Beattie Yale University, New Haven, Connecticut, USA
P Becht Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Behera Indian Institute of Technology Indore, Indore, India
I Belikov Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
A D C Bell Hechavarria Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
F Bellini Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
R Bellwied University of Houston, Houston, Texas, USA
S Belokurova Affiliated with an institute covered by a cooperation agreement with CERN
V Belyaev Affiliated with an institute covered by a cooperation agreement with CERN
G Bencedi Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico Wigner Research Centre for Physics, Budapest, Hungary
S Beole Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A Bercuci Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
Y Berdnikov Affiliated with an institute covered by a cooperation agreement with CERN
A Berdnikova Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L Bergmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M G Besoiu Institute of Space Science (ISS), Bucharest, Romania
L Betev European Organization for Nuclear Research (CERN), Geneva, Switzerland
P P Bhaduri Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
A Bhasin Physics Department, University of Jammu, Jammu, India
I R Bhat Physics Department, University of Jammu, Jammu, India
M A Bhat Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
B Bhattacharjee Department of Physics, Gauhati University, Guwahati, India
L Bianchi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
N Bianchi INFN, Laboratori Nazionali di Frascati, Frascati, Italy
J Bielčík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
J Bielčíková Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
J Biernat The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
A Bilandzic Physik Department, Technische Universität München, Munich, Germany
G Biro Wigner Research Centre for Physics, Budapest, Hungary
S Biswas Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
J T Blair The University of Texas at Austin, Austin, Texas, USA
D Blau Affiliated with an institute covered by a cooperation agreement with CERN
M B Blidaru Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
N Bluhme Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Blume Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
G Boca Dipartimento di Fisica, Università di Pavia, Pavia, Italy INFN, Sezione di Pavia, Pavia, Italy
F Bock Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
T Bodova Department of Physics and Technology, University of Bergen, Bergen, Norway
A Bogdanov Affiliated with an institute covered by a cooperation agreement with CERN
S Boi Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
J Bok Inha University, Incheon, Republic of Korea
L Boldizsár Wigner Research Centre for Physics, Budapest, Hungary
A Bolozdynya Affiliated with an institute covered by a cooperation agreement with CERN
M Bombara Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
P M Bond European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Bonomi INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
H Borel Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
A Borissov Affiliated with an institute covered by a cooperation agreement with CERN
H Bossi Yale University, New Haven, Connecticut, USA
E Botta Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
L Bratrud Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P Braun-Munzinger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Bregant Universidade de São Paulo (USP), São Paulo, Brazil
M Broz Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G E Bruno Dipartimento Interateneo di Fisica "M. Merlin" and Sezione INFN, Bari, Italy Politecnico di Bari and Sezione INFN, Bari, Italy
M D Buckland University of Liverpool, Liverpool, United Kingdom
D Budnikov Affiliated with an institute covered by a cooperation agreement with CERN
H Buesching Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S Bufalino Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
O Bugnon SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
P Buhler Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
Z Buthelezi iThemba LABS, National Research Foundation, Somerset West, South Africa University of the Witwatersrand, Johannesburg, South Africa
J B Butt COMSATS University Islamabad, Islamabad, Pakistan
A Bylinkin University of Kansas, Lawrence, Kansas, USA
S A Bysiak The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Cai Central China Normal University, Wuhan, China Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
H Caines Yale University, New Haven, Connecticut, USA
A Caliva Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
E Calvo Villar Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
J M M Camacho Universidad Autónoma de Sinaloa, Culiacán, Mexico
R S Camacho High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
P Camerini Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
F D M Canedo Universidade de São Paulo (USP), São Paulo, Brazil
M Carabas University Politehnica of Bucharest, Bucharest, Romania
F Carnesecchi European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Caron CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
J Castillo Castellanos Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
F Catalano Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
C Ceballos Sanchez Affiliated with an international laboratory covered by a cooperation agreement with CERN
I Chakaberia Lawrence Berkeley National Laboratory, Berkeley, California, USA
P Chakraborty Indian Institute of Technology Bombay (IIT), Mumbai, India
S Chandra Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Chapeland European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Chartier University of Liverpool, Liverpool, United Kingdom
S Chattopadhyay Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Chattopadhyay Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
T G Chavez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
T Cheng Central China Normal University, Wuhan, China
C Cheshkov CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
B Cheynis CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
V Chibante Barroso European Organization for Nuclear Research (CERN), Geneva, Switzerland
D D Chinellato Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
E S Chizzali Physik Department, Technische Universität München, Munich, Germany
J Cho Inha University, Incheon, Republic of Korea
S Cho Inha University, Incheon, Republic of Korea
P Chochula European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Christakoglou Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
C H Christensen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
P Christiansen Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
T Chujo University of Tsukuba, Tsukuba, Japan
M Ciacco Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
C Cicalo INFN, Sezione di Cagliari, Cagliari, Italy
L Cifarelli Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
F Cindolo INFN, Sezione di Bologna, Bologna, Italy
M R Ciupek Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G Clai INFN, Sezione di Bologna, Bologna, Italy
F Colamaria INFN, Sezione di Bari, Bari, Italy
J S Colburn School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
D Colella Dipartimento Interateneo di Fisica "M. Merlin" and Sezione INFN, Bari, Italy Politecnico di Bari and Sezione INFN, Bari, Italy
A Collu Lawrence Berkeley National Laboratory, Berkeley, California, USA
M Colocci European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Concas INFN, Sezione di Torino, Turin, Italy
G Conesa Balbastre Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
Z Conesa Del Valle Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
G Contin Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
J G Contreras Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M L Coquet Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
T M Cormier Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
P Cortese INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
M R Cosentino Universidade Federal do ABC, Santo Andre, Brazil
F Costa European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Costanza Dipartimento di Fisica, Università di Pavia, Pavia, Italy INFN, Sezione di Pavia, Pavia, Italy
P Crochet Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
R Cruz-Torres Lawrence Berkeley National Laboratory, Berkeley, California, USA
E Cuautle Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
P Cui Central China Normal University, Wuhan, China
L Cunqueiro Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
A Dainese INFN, Sezione di Padova, Padova, Italy
M C Danisch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Danu Institute of Space Science (ISS), Bucharest, Romania
P Das National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
P Das Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Das Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Dash Indian Institute of Technology Bombay (IIT), Mumbai, India
A De Caro Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
G de Cataldo INFN, Sezione di Bari, Bari, Italy
L De Cilladi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
J de Cuveland Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A De Falco Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
D De Gruttola Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
N De Marco INFN, Sezione di Torino, Turin, Italy
C De Martin Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
S De Pasquale Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
S Deb Indian Institute of Technology Indore, Indore, India
H F Degenhardt Universidade de São Paulo (USP), São Paulo, Brazil
K R Deja Warsaw University of Technology, Warsaw, Poland
R Del Grande Physik Department, Technische Universität München, Munich, Germany
L Dello Stritto Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
W Deng Central China Normal University, Wuhan, China
P Dhankher Department of Physics, University of California, Berkeley, California, USA
D Di Bari Dipartimento Interateneo di Fisica "M. Merlin" and Sezione INFN, Bari, Italy
A Di Mauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
R A Diaz Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba Affiliated with an international laboratory covered by a cooperation agreement with CERN
T Dietel University of Cape Town, Cape Town, South Africa
Y Ding Central China Normal University, Wuhan, China CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
R Divià European Organization for Nuclear Research (CERN), Geneva, Switzerland
D U Dixit Department of Physics, University of California, Berkeley, California, USA
Ø Djuvsland Department of Physics and Technology, University of Bergen, Bergen, Norway
U Dmitrieva Affiliated with an institute covered by a cooperation agreement with CERN
A Dobrin Institute of Space Science (ISS), Bucharest, Romania
B Dönigus Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A K Dubey Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
J M Dubinski Warsaw University of Technology, Warsaw, Poland
A Dubla Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
S Dudi Physics Department, Panjab University, Chandigarh, India
P Dupieux Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
M Durkac Technical University of Košice, Košice, Slovak Republic
N Dzalaiova Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
T M Eder Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
R J Ehlers Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
V N Eikeland Department of Physics and Technology, University of Bergen, Bergen, Norway
F Eisenhut Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Elia INFN, Sezione di Bari, Bari, Italy
B Erazmus SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
F Ercolessi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
F Erhardt Physics Department, Faculty of Science, University of Zagreb, Zagreb, Croatia
M R Ersdal Department of Physics and Technology, University of Bergen, Bergen, Norway
B Espagnon Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
G Eulisse European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Evans School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S Evdokimov Affiliated with an institute covered by a cooperation agreement with CERN
L Fabbietti Physik Department, Technische Universität München, Munich, Germany
M Faggin Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
J Faivre Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
F Fan Central China Normal University, Wuhan, China
W Fan Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Fantoni INFN, Laboratori Nazionali di Frascati, Frascati, Italy
M Fasel Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
P Fecchio Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
A Feliciello INFN, Sezione di Torino, Turin, Italy
G Feofilov Affiliated with an institute covered by a cooperation agreement with CERN
A Fernández Téllez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
M B Ferrer European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Ferrero Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
A Ferretti Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
V J G Feuillard Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Figiel The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
V Filova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
D Finogeev Affiliated with an institute covered by a cooperation agreement with CERN
F M Fionda INFN, Sezione di Cagliari, Cagliari, Italy
G Fiorenza Politecnico di Bari and Sezione INFN, Bari, Italy
F Flor University of Houston, Houston, Texas, USA
A N Flores The University of Texas at Austin, Austin, Texas, USA
S Foertsch iThemba LABS, National Research Foundation, Somerset West, South Africa
I Fokin Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Fokin Affiliated with an institute covered by a cooperation agreement with CERN
E Fragiacomo INFN, Sezione di Trieste, Trieste, Italy
E Frajna Wigner Research Centre for Physics, Budapest, Hungary
U Fuchs European Organization for Nuclear Research (CERN), Geneva, Switzerland
N Funicello Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
C Furget Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
A Furs Affiliated with an institute covered by a cooperation agreement with CERN
J J Gaardhøje Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M Gagliardi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A M Gago Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
A Gal Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
C D Galvan Universidad Autónoma de Sinaloa, Culiacán, Mexico
P Ganoti Department of Physics, School of Science, National and Kapodistrian University of Athens, Athens, Greece
C Garabatos Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J R A Garcia High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
E Garcia-Solis Chicago State University, Chicago, Illinois, USA
K Garg SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
C Gargiulo European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Garibli National Nuclear Research Center, Baku, Azerbaijan
K Garner Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
E F Gauger The University of Texas at Austin, Austin, Texas, USA
A Gautam University of Kansas, Lawrence, Kansas, USA
M B Gay Ducati Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil
M Germain SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S K Ghosh Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
M Giacalone Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
P Gianotti INFN, Laboratori Nazionali di Frascati, Frascati, Italy
P Giubellino INFN, Sezione di Torino, Turin, Italy Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
P Giubilato Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
A M C Glaenzer Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
P Glässel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
E Glimos University of Tennessee, Knoxville, Tennessee, USA
D J Q Goh Nagasaki Institute of Applied Science, Nagasaki, Japan
V Gonzalez Wayne State University, Detroit, Michigan, USA
L H González-Trueba Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
S Gorbunov Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M Gorgon AGH University of Science and Technology, Cracow, Poland
L Görlich The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
S Gotovac Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
V Grabski Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
L K Graczykowski Warsaw University of Technology, Warsaw, Poland
E Grecka Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
L Greiner Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Grelli Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
C Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Grigoriev Affiliated with an institute covered by a cooperation agreement with CERN
S Grigoryan A.I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia Affiliated with an international laboratory covered by a cooperation agreement with CERN
F Grosa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J F Grosse-Oetringhaus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Grosso Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
D Grund Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G G Guardiano Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
R Guernane Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
M Guilbaud SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
K Gulbrandsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
T Gunji University of Tokyo, Tokyo, Japan
W Guo Central China Normal University, Wuhan, China
A Gupta Physics Department, University of Jammu, Jammu, India
R Gupta Physics Department, University of Jammu, Jammu, India
S P Guzman High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
L Gyulai Wigner Research Centre for Physics, Budapest, Hungary
M K Habib Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
C Hadjidakis Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
H Hamagaki Nagasaki Institute of Applied Science, Nagasaki, Japan
M Hamid Central China Normal University, Wuhan, China
Y Han Yonsei University, Seoul, Republic of Korea
R Hannigan The University of Texas at Austin, Austin, Texas, USA
M R Haque Warsaw University of Technology, Warsaw, Poland
A Harlenderova Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J W Harris Yale University, New Haven, Connecticut, USA
A Harton Chicago State University, Chicago, Illinois, USA
J A Hasenbichler European Organization for Nuclear Research (CERN), Geneva, Switzerland
H Hassan Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
D Hatzifotiadou INFN, Sezione di Bologna, Bologna, Italy
P Hauer Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
L B Havener Yale University, New Haven, Connecticut, USA
S T Heckel Physik Department, Technische Universität München, Munich, Germany
E Hellbär Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
H Helstrup Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
T Herman Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
G Herrera Corral Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
F Herrmann Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
K F Hetland Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
B Heybeck Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H Hillemanns European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Hills University of Liverpool, Liverpool, United Kingdom
B Hippolyte Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
B Hofman Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
B Hohlweger Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
J Honermann Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
G H Hong Yonsei University, Seoul, Republic of Korea
D Horak Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
A Horzyk AGH University of Science and Technology, Cracow, Poland
R Hosokawa Creighton University, Omaha, Nebraska, USA
Y Hou Central China Normal University, Wuhan, China
P Hristov European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Hughes University of Tennessee, Knoxville, Tennessee, USA
P Huhn Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
L M Huhta University of Jyväskylä, Jyväskylä, Finland
C V Hulse Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
T J Humanic Ohio State University, Columbus, Ohio, USA
H Hushnud Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
A Hutson University of Houston, Houston, Texas, USA
D Hutter Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J P Iddon University of Liverpool, Liverpool, United Kingdom
R Ilkaev Affiliated with an institute covered by a cooperation agreement with CERN
H Ilyas COMSATS University Islamabad, Islamabad, Pakistan
M Inaba University of Tsukuba, Tsukuba, Japan
G M Innocenti European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Ippolitov Affiliated with an institute covered by a cooperation agreement with CERN
A Isakov Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
T Isidori University of Kansas, Lawrence, Kansas, USA
M S Islam Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
M Ivanov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
V Ivanov Affiliated with an institute covered by a cooperation agreement with CERN
V Izucheev Affiliated with an institute covered by a cooperation agreement with CERN
M Jablonski AGH University of Science and Technology, Cracow, Poland
B Jacak Lawrence Berkeley National Laboratory, Berkeley, California, USA
N Jacazio European Organization for Nuclear Research (CERN), Geneva, Switzerland
P M Jacobs Lawrence Berkeley National Laboratory, Berkeley, California, USA
S Jadlovska Technical University of Košice, Košice, Slovak Republic
J Jadlovsky Technical University of Košice, Košice, Slovak Republic
L Jaffe Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Jahnke Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
M A Janik Warsaw University of Technology, Warsaw, Poland
T Janson Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
M Jercic Physics Department, Faculty of Science, University of Zagreb, Zagreb, Croatia
O Jevons School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A A P Jimenez Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
F Jonas Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
P G Jones School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
J M Jowett European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
J Jung Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M Jung Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A Junique European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Jusko School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M J Kabus European Organization for Nuclear Research (CERN), Geneva, Switzerland Warsaw University of Technology, Warsaw, Poland
J Kaewjai Suranaree University of Technology, Nakhon Ratchasima, Thailand
P Kalinak Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
A S Kalteyer Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Kalweit European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Kaplin Affiliated with an institute covered by a cooperation agreement with CERN
A Karasu Uysal KTO Karatay University, Konya, Turkey
D Karatovic Physics Department, Faculty of Science, University of Zagreb, Zagreb, Croatia
O Karavichev Affiliated with an institute covered by a cooperation agreement with CERN
T Karavicheva Affiliated with an institute covered by a cooperation agreement with CERN
P Karczmarczyk Warsaw University of Technology, Warsaw, Poland
E Karpechev Affiliated with an institute covered by a cooperation agreement with CERN
V Kashyap National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
A Kazantsev Affiliated with an institute covered by a cooperation agreement with CERN
U Kebschull Johann-Wolfgang-Goethe Universität Frankfurt Institut für Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany
R Keidel Zentrum für Technologie und Transfer (ZTT), Worms, Germany
D L D Keijdener Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
M Keil European Organization for Nuclear Research (CERN), Geneva, Switzerland
B Ketzer Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
A M Khan Central China Normal University, Wuhan, China
S Khan Department of Physics, Aligarh Muslim University, Aligarh, India
A Khanzadeev Affiliated with an institute covered by a cooperation agreement with CERN
Y Kharlov Affiliated with an institute covered by a cooperation agreement with CERN
A Khatun Department of Physics, Aligarh Muslim University, Aligarh, India
A Khuntia The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
B Kileng Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
B Kim Department of Physics, Pusan National University, Pusan, Republic of Korea
C Kim Department of Physics, Pusan National University, Pusan, Republic of Korea
D J Kim University of Jyväskylä, Jyväskylä, Finland
E J Kim Jeonbuk National University, Jeonju, Republic of Korea
J Kim Yonsei University, Seoul, Republic of Korea
J S Kim Gangneung-Wonju National University, Gangneung, Republic of Korea
J Kim Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J Kim Jeonbuk National University, Jeonju, Republic of Korea
M Kim Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Kim Department of Physics, Sejong University, Seoul, Republic of Korea
T Kim Yonsei University, Seoul, Republic of Korea
S Kirsch Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I Kisel Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S Kiselev Affiliated with an institute covered by a cooperation agreement with CERN
A Kisiel Warsaw University of Technology, Warsaw, Poland
J P Kitowski AGH University of Science and Technology, Cracow, Poland
J L Klay California Polytechnic State University, San Luis Obispo, California, USA
J Klein European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Klein Lawrence Berkeley National Laboratory, Berkeley, California, USA
C Klein-Bösing Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M Kleiner Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T Klemenz Physik Department, Technische Universität München, Munich, Germany
A Kluge European Organization for Nuclear Research (CERN), Geneva, Switzerland
A G Knospe University of Houston, Houston, Texas, USA
C Kobdaj Suranaree University of Technology, Nakhon Ratchasima, Thailand
T Kollegger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Kondratyev Affiliated with an international laboratory covered by a cooperation agreement with CERN
N Kondratyeva Affiliated with an institute covered by a cooperation agreement with CERN
E Kondratyuk Affiliated with an institute covered by a cooperation agreement with CERN
J Konig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S A Konigstorfer Physik Department, Technische Universität München, Munich, Germany
P J Konopka European Organization for Nuclear Research (CERN), Geneva, Switzerland
G Kornakov Warsaw University of Technology, Warsaw, Poland
S D Koryciak AGH University of Science and Technology, Cracow, Poland
A Kotliarov Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
O Kovalenko National Centre for Nuclear Research, Warsaw, Poland
V Kovalenko Affiliated with an institute covered by a cooperation agreement with CERN
M Kowalski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
I Králik Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
A Kravčáková Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
L Kreis Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Krivda Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
F Krizek Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
K Krizkova Gajdosova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M Kroesen Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Krüger Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D M Krupova Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
E Kryshen Affiliated with an institute covered by a cooperation agreement with CERN
M Krzewicki Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
V Kučera European Organization for Nuclear Research (CERN), Geneva, Switzerland
C Kuhn Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
P G Kuijer Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
T Kumaoka University of Tsukuba, Tsukuba, Japan
D Kumar Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
L Kumar Physics Department, Panjab University, Chandigarh, India
N Kumar Physics Department, Panjab University, Chandigarh, India
S Kundu European Organization for Nuclear Research (CERN), Geneva, Switzerland
P Kurashvili National Centre for Nuclear Research, Warsaw, Poland
A Kurepin Affiliated with an institute covered by a cooperation agreement with CERN
A B Kurepin Affiliated with an institute covered by a cooperation agreement with CERN
S Kushpil Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic
J Kvapil School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M J Kweon Inha University, Incheon, Republic of Korea
J Y Kwon Inha University, Incheon, Republic of Korea
Y Kwon Yonsei University, Seoul, Republic of Korea
S L La Pointe Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P La Rocca Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
Y S Lai Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Lakrathok Suranaree University of Technology, Nakhon Ratchasima, Thailand
M Lamanna European Organization for Nuclear Research (CERN), Geneva, Switzerland
R Langoy University of South-Eastern Norway, Kongsberg, Norway
P Larionov INFN, Laboratori Nazionali di Frascati, Frascati, Italy
E Laudi European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Lautner European Organization for Nuclear Research (CERN), Geneva, Switzerland Physik Department, Technische Universität München, Munich, Germany
R Lavicka Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
T Lazareva Affiliated with an institute covered by a cooperation agreement with CERN
R Lea INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
J Lehrbach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R C Lemmon Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
I León Monzón Universidad Autónoma de Sinaloa, Culiacán, Mexico
M M Lesch Physik Department, Technische Universität München, Munich, Germany
E D Lesser Department of Physics, University of California, Berkeley, California, USA
M Lettrich Physik Department, Technische Universität München, Munich, Germany
P Lévai Wigner Research Centre for Physics, Budapest, Hungary
X Li China Institute of Atomic Energy, Beijing, China
X L Li Central China Normal University, Wuhan, China
J Lien University of South-Eastern Norway, Kongsberg, Norway
R Lietava School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
B Lim Department of Physics, Pusan National University, Pusan, Republic of Korea
S H Lim Department of Physics, Pusan National University, Pusan, Republic of Korea
V Lindenstruth Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A Lindner Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
C Lippmann Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Liu Department of Physics, University of California, Berkeley, California, USA
D H Liu Central China Normal University, Wuhan, China
J Liu University of Liverpool, Liverpool, United Kingdom
I M Lofnes Department of Physics and Technology, University of Bergen, Bergen, Norway
V Loginov Affiliated with an institute covered by a cooperation agreement with CERN
C Loizides Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
P Loncar Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
J A Lopez Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
X Lopez Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
E López Torres Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
P Lu Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany University of Science and Technology of China, Hefei, China
J R Luhder Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M Lunardon Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
G Luparello INFN, Sezione di Trieste, Trieste, Italy
Y G Ma Fudan University, Shanghai, China
A Maevskaya Affiliated with an institute covered by a cooperation agreement with CERN
M Mager European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Mahmoud Helmholtz-Institut für Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universität Bonn, Bonn, Germany
A Maire Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
M Malaev Affiliated with an institute covered by a cooperation agreement with CERN
N M Malik Physics Department, University of Jammu, Jammu, India
Q W Malik Department of Physics, University of Oslo, Oslo, Norway
S K Malik Physics Department, University of Jammu, Jammu, India
L Malinina Affiliated with an international laboratory covered by a cooperation agreement with CERN
D Mal'Kevich Affiliated with an institute covered by a cooperation agreement with CERN
D Mallick National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
N Mallick Indian Institute of Technology Indore, Indore, India
G Mandaglio Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
V Manko Affiliated with an institute covered by a cooperation agreement with CERN
F Manso Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
V Manzari INFN, Sezione di Bari, Bari, Italy
Y Mao Central China Normal University, Wuhan, China
G V Margagliotti Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
A Margotti INFN, Sezione di Bologna, Bologna, Italy
A Marín Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
C Markert The University of Texas at Austin, Austin, Texas, USA
M Marquard Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N A Martin Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
P Martinengo European Organization for Nuclear Research (CERN), Geneva, Switzerland
J L Martinez University of Houston, Houston, Texas, USA
M I Martínez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
G Martínez García SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Masciocchi Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
M Masera Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
A Masoni INFN, Sezione di Cagliari, Cagliari, Italy
L Massacrier Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
A Mastroserio INFN, Sezione di Bari, Bari, Italy Università degli Studi di Foggia, Foggia, Italy
A M Mathis Physik Department, Technische Universität München, Munich, Germany
O Matonoha Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
P F T Matuoka Universidade de São Paulo (USP), São Paulo, Brazil
A Matyja The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
C Mayer The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
A L Mazuecos European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Mazzaschi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
M Mazzilli European Organization for Nuclear Research (CERN), Geneva, Switzerland
J E Mdhluli University of the Witwatersrand, Johannesburg, South Africa
A F Mechler Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
Y Melikyan Affiliated with an institute covered by a cooperation agreement with CERN
A Menchaca-Rocha Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
E Meninno Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
A S Menon University of Houston, Houston, Texas, USA
M Meres Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
S Mhlanga iThemba LABS, National Research Foundation, Somerset West, South Africa University of Cape Town, Cape Town, South Africa
Y Miake University of Tsukuba, Tsukuba, Japan
L Micheletti INFN, Sezione di Torino, Turin, Italy
L C Migliorin CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
D L Mihaylov Physik Department, Technische Universität München, Munich, Germany
K Mikhaylov Affiliated with an institute covered by a cooperation agreement with CERN Affiliated with an international laboratory covered by a cooperation agreement with CERN
A N Mishra Wigner Research Centre for Physics, Budapest, Hungary
D Miśkowiec Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
A Modak Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
A P Mohanty Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
B Mohanty National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
M Mohisin Khan Department of Physics, Aligarh Muslim University, Aligarh, India
M A Molander Helsinki Institute of Physics (HIP), Helsinki, Finland
Z Moravcova Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C Mordasini Physik Department, Technische Universität München, Munich, Germany
D A Moreira De Godoy Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
I Morozov Affiliated with an institute covered by a cooperation agreement with CERN
A Morsch European Organization for Nuclear Research (CERN), Geneva, Switzerland
T Mrnjavac European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Muccifora INFN, Laboratori Nazionali di Frascati, Frascati, Italy
E Mudnic Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
S Muhuri Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
J D Mulligan Lawrence Berkeley National Laboratory, Berkeley, California, USA
A Mulliri Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
M G Munhoz Universidade de São Paulo (USP), São Paulo, Brazil
R H Munzer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H Murakami University of Tokyo, Tokyo, Japan
S Murray University of Cape Town, Cape Town, South Africa
L Musa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J Musinsky Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovak Republic
J W Myrcha Warsaw University of Technology, Warsaw, Poland
B Naik University of the Witwatersrand, Johannesburg, South Africa
R Nair National Centre for Nuclear Research, Warsaw, Poland
B K Nandi Indian Institute of Technology Bombay (IIT), Mumbai, India
R Nania INFN, Sezione di Bologna, Bologna, Italy
E Nappi INFN, Sezione di Bari, Bari, Italy
A F Nassirpour Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
A Nath Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Nattrass University of Tennessee, Knoxville, Tennessee, USA
A Neagu Department of Physics, University of Oslo, Oslo, Norway
A Negru University Politehnica of Bucharest, Bucharest, Romania
L Nellen Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
S V Nesbo Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
G Neskovic Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Nesterov Affiliated with an institute covered by a cooperation agreement with CERN
B S Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
E G Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S Nikolaev Affiliated with an institute covered by a cooperation agreement with CERN
S Nikulin Affiliated with an institute covered by a cooperation agreement with CERN
V Nikulin Affiliated with an institute covered by a cooperation agreement with CERN
F Noferini INFN, Sezione di Bologna, Bologna, Italy
S Noh Chungbuk National University, Cheongju, Republic of Korea
P Nomokonov Affiliated with an international laboratory covered by a cooperation agreement with CERN
J Norman University of Liverpool, Liverpool, United Kingdom
N Novitzky University of Tsukuba, Tsukuba, Japan
P Nowakowski Warsaw University of Technology, Warsaw, Poland
A Nyanin Affiliated with an institute covered by a cooperation agreement with CERN
J Nystrand Department of Physics and Technology, University of Bergen, Bergen, Norway
M Ogino Nagasaki Institute of Applied Science, Nagasaki, Japan
A Ohlson Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
V A Okorokov Affiliated with an institute covered by a cooperation agreement with CERN
J Oleniacz Warsaw University of Technology, Warsaw, Poland
A C Oliveira Da Silva University of Tennessee, Knoxville, Tennessee, USA
M H Oliver Yale University, New Haven, Connecticut, USA
A Onnerstad University of Jyväskylä, Jyväskylä, Finland
C Oppedisano INFN, Sezione di Torino, Turin, Italy
A Ortiz Velasquez Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A Oskarsson Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
J Otwinowski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Oya Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
K Oyama Nagasaki Institute of Applied Science, Nagasaki, Japan
Y Pachmayer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S Padhan Indian Institute of Technology Bombay (IIT), Mumbai, India
D Pagano INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
G Paić Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A Palasciano INFN, Sezione di Bari, Bari, Italy
S Panebianco Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
J Park Inha University, Incheon, Republic of Korea
J E Parkkila European Organization for Nuclear Research (CERN), Geneva, Switzerland University of Jyväskylä, Jyväskylä, Finland
S P Pathak University of Houston, Houston, Texas, USA
R N Patra Physics Department, University of Jammu, Jammu, India
B Paul Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
H Pei Central China Normal University, Wuhan, China
T Peitzmann Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
X Peng Central China Normal University, Wuhan, China
L G Pereira Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil
H Pereira Da Costa Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
D Peresunko Affiliated with an institute covered by a cooperation agreement with CERN
G M Perez Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
S Perrin Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
Y Pestov Affiliated with an institute covered by a cooperation agreement with CERN
V Petráček Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
V Petrov Affiliated with an institute covered by a cooperation agreement with CERN
M Petrovici Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
R P Pezzi Instituto de Física, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Piano INFN, Sezione di Trieste, Trieste, Italy
M Pikna Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
P Pillot SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
O Pinazza European Organization for Nuclear Research (CERN), Geneva, Switzerland INFN, Sezione di Bologna, Bologna, Italy
L Pinsky University of Houston, Houston, Texas, USA
C Pinto Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy Physik Department, Technische Universität München, Munich, Germany
S Pisano INFN, Laboratori Nazionali di Frascati, Frascati, Italy
M Płoskoń Lawrence Berkeley National Laboratory, Berkeley, California, USA
M Planinic Physics Department, Faculty of Science, University of Zagreb, Zagreb, Croatia
F Pliquett Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M G Poghosyan Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
S Politano Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
N Poljak Physics Department, Faculty of Science, University of Zagreb, Zagreb, Croatia
A Pop Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
S Porteboeuf-Houssais Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
J Porter Lawrence Berkeley National Laboratory, Berkeley, California, USA
V Pozdniakov Affiliated with an international laboratory covered by a cooperation agreement with CERN
S K Prasad Bose Institute, Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
S Prasad Indian Institute of Technology Indore, Indore, India
R Preghenella INFN, Sezione di Bologna, Bologna, Italy
F Prino INFN, Sezione di Torino, Turin, Italy
C A Pruneau Wayne State University, Detroit, Michigan, USA
I Pshenichnov Affiliated with an institute covered by a cooperation agreement with CERN
M Puccio European Organization for Nuclear Research (CERN), Geneva, Switzerland
S Qiu Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
L Quaglia Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
R E Quishpe University of Houston, Houston, Texas, USA
S Ragoni School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A Rakotozafindrabe Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
L Ramello INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
F Rami Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
S A R Ramirez High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
T A Rancien Laboratoire de Physique Subatomique et de Cosmologie, Université Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
R Raniwala Physics Department, University of Rajasthan, Jaipur, India
S Raniwala Physics Department, University of Rajasthan, Jaipur, India
S S Räsänen Helsinki Institute of Physics (HIP), Helsinki, Finland
R Rath Indian Institute of Technology Indore, Indore, India
I Ravasenga Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
K F Read Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA University of Tennessee, Knoxville, Tennessee, USA
A R Redelbach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
K Redlich National Centre for Nuclear Research, Warsaw, Poland
A Rehman Department of Physics and Technology, University of Bergen, Bergen, Norway
P Reichelt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
F Reidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
H A Reme-Ness Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
Z Rescakova Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
K Reygers Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Riabov Affiliated with an institute covered by a cooperation agreement with CERN
V Riabov Affiliated with an institute covered by a cooperation agreement with CERN
R Ricci Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
T Richert Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
M Richter Department of Physics, University of Oslo, Oslo, Norway
W Riegler European Organization for Nuclear Research (CERN), Geneva, Switzerland
F Riggi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Catania, Italy
C Ristea Institute of Space Science (ISS), Bucharest, Romania
M Rodríguez Cahuantzi High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
K Røed Department of Physics, University of Oslo, Oslo, Norway
R Rogalev Affiliated with an institute covered by a cooperation agreement with CERN
E Rogochaya Affiliated with an international laboratory covered by a cooperation agreement with CERN
T S Rogoschinski Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D Rohr European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Röhrich Department of Physics and Technology, University of Bergen, Bergen, Norway
P F Rojas High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
S Rojas Torres Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
P S Rokita Warsaw University of Technology, Warsaw, Poland
F Ronchetti INFN, Laboratori Nazionali di Frascati, Frascati, Italy
A Rosano Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
E D Rosas Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A Rossi INFN, Sezione di Padova, Padova, Italy
A Roy Indian Institute of Technology Indore, Indore, India
P Roy Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
S Roy Indian Institute of Technology Bombay (IIT), Mumbai, India
N Rubini Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
O V Rueda Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
D Ruggiano Warsaw University of Technology, Warsaw, Poland
R Rui Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
B Rumyantsev Affiliated with an international laboratory covered by a cooperation agreement with CERN
P G Russek AGH University of Science and Technology, Cracow, Poland
R Russo Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
A Rustamov National Nuclear Research Center, Baku, Azerbaijan
E Ryabinkin Affiliated with an institute covered by a cooperation agreement with CERN
Y Ryabov Affiliated with an institute covered by a cooperation agreement with CERN
A Rybicki The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
H Rytkonen University of Jyväskylä, Jyväskylä, Finland
W Rzesa Warsaw University of Technology, Warsaw, Poland
O A M Saarimaki Helsinki Institute of Physics (HIP), Helsinki, Finland
R Sadek SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
S Sadovsky Affiliated with an institute covered by a cooperation agreement with CERN
J Saetre Department of Physics and Technology, University of Bergen, Bergen, Norway
K Šafařík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
S K Saha Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Saha National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
B Sahoo Indian Institute of Technology Bombay (IIT), Mumbai, India
P Sahoo Indian Institute of Technology Bombay (IIT), Mumbai, India
R Sahoo Indian Institute of Technology Indore, Indore, India
S Sahoo Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
D Sahu Indian Institute of Technology Indore, Indore, India
P K Sahu Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
J Saini Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
K Sajdakova Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
S Sakai University of Tsukuba, Tsukuba, Japan
M P Salvan Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
S Sambyal Physics Department, University of Jammu, Jammu, India
T B Saramela Universidade de São Paulo (USP), São Paulo, Brazil
D Sarkar Wayne State University, Detroit, Michigan, USA
N Sarkar Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
P Sarma Department of Physics, Gauhati University, Guwahati, India
V Sarritzu Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
V M Sarti Physik Department, Technische Universität München, Munich, Germany
M H P Sas Yale University, New Haven, Connecticut, USA
J Schambach Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
H S Scheid Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C Schiaua Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
R Schicker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A Schmah Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C Schmidt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
H R Schmidt Physikalisches Institut, Eberhard-Karls-Universität Tübingen, Tubingen, Germany
M O Schmidt European Organization for Nuclear Research (CERN), Geneva, Switzerland
M Schmidt Physikalisches Institut, Eberhard-Karls-Universität Tübingen, Tubingen, Germany
N V Schmidt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA
A R Schmier University of Tennessee, Knoxville, Tennessee, USA
R Schotter Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
J Schukraft European Organization for Nuclear Research (CERN), Geneva, Switzerland
K Schwarz Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
K Schweda Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G Scioli Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
E Scomparin INFN, Sezione di Torino, Turin, Italy
J E Seger Creighton University, Omaha, Nebraska, USA
Y Sekiguchi University of Tokyo, Tokyo, Japan
D Sekihata University of Tokyo, Tokyo, Japan
I Selyuzhenkov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany Affiliated with an institute covered by a cooperation agreement with CERN
S Senyukov Université de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France
J J Seo Inha University, Incheon, Republic of Korea
D Serebryakov Affiliated with an institute covered by a cooperation agreement with CERN
L Šerkšnytė Physik Department, Technische Universität München, Munich, Germany
A Sevcenco Institute of Space Science (ISS), Bucharest, Romania
T J Shaba iThemba LABS, National Research Foundation, Somerset West, South Africa
A Shabanov Affiliated with an institute covered by a cooperation agreement with CERN
A Shabetai SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
R Shahoyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
W Shaikh Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
A Shangaraev Affiliated with an institute covered by a cooperation agreement with CERN
A Sharma Physics Department, Panjab University, Chandigarh, India
D Sharma Indian Institute of Technology Bombay (IIT), Mumbai, India
H Sharma The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M Sharma Physics Department, University of Jammu, Jammu, India
N Sharma Physics Department, Panjab University, Chandigarh, India
S Sharma Physics Department, University of Jammu, Jammu, India
U Sharma Physics Department, University of Jammu, Jammu, India
A Shatat Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
O Sheibani University of Houston, Houston, Texas, USA
K Shigaki Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
M Shimomura Nara Women's University (NWU), Nara, Japan
S Shirinkin Affiliated with an institute covered by a cooperation agreement with CERN
Q Shou Fudan University, Shanghai, China
Y Sibiriak Affiliated with an institute covered by a cooperation agreement with CERN
S Siddhanta INFN, Sezione di Cagliari, Cagliari, Italy
T Siemiarczuk National Centre for Nuclear Research, Warsaw, Poland
T F Silva Universidade de São Paulo (USP), São Paulo, Brazil
D Silvermyr Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
T Simantathammakul Suranaree University of Technology, Nakhon Ratchasima, Thailand
R Simeonov Faculty of Physics, Sofia University, Sofia, Bulgaria
G Simonetti European Organization for Nuclear Research (CERN), Geneva, Switzerland
B Singh Physics Department, University of Jammu, Jammu, India
B Singh Physik Department, Technische Universität München, Munich, Germany
R Singh National Institute of Science Education and Research, Homi Bhabha National Institute, Jatni, India
R Singh Physics Department, University of Jammu, Jammu, India
R Singh Indian Institute of Technology Indore, Indore, India
V K Singh Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
V Singhal Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
T Sinha Saha Institute of Nuclear Physics, Homi Bhabha National Institute, Kolkata, India
B Sitar Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
M Sitta INFN, Sezione di Torino, Turin, Italy Università del Piemonte Orientale, Vercelli, Italy
T B Skaali Department of Physics, University of Oslo, Oslo, Norway
G Skorodumovs Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Slupecki Helsinki Institute of Physics (HIP), Helsinki, Finland
N Smirnov Yale University, New Haven, Connecticut, USA
R J M Snellings Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
E H Solheim Department of Physics, University of Oslo, Oslo, Norway
C Soncco Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
J Song University of Houston, Houston, Texas, USA
A Songmoolnak Suranaree University of Technology, Nakhon Ratchasima, Thailand
F Soramel Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Padova, Italy
S Sorensen University of Tennessee, Knoxville, Tennessee, USA
R Spijkers Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
I Sputowska The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
J Staa Lund University Department of Physics, Division of Particle Physics, Lund, Sweden
J Stachel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
I Stan Institute of Space Science (ISS), Bucharest, Romania
P J Steffanic University of Tennessee, Knoxville, Tennessee, USA
S F Stiefelmaier Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D Stocco SUBATECH, IMT Atlantique, Nantes Université, CNRS-IN2P3, Nantes, France
I Storehaug Department of Physics, University of Oslo, Oslo, Norway
M M Storetvedt Faculty of Engineering and Science, Western Norway University of Applied Sciences, Bergen, Norway
P Stratmann Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S Strazzi Dipartimento di Fisica e Astronomia dell'Università and Sezione INFN, Bologna, Italy
C P Stylianidis Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
A A P Suaide Universidade de São Paulo (USP), São Paulo, Brazil
C Suire Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
M Sukhanov Affiliated with an institute covered by a cooperation agreement with CERN
M Suljic European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Sumberia Physics Department, University of Jammu, Jammu, India
S Sumowidagdo National Research and Innovation Agency - BRIN, Jakarta, Indonesia
S Swain Institute of Physics, Homi Bhabha National Institute, Bhubaneswar, India
A Szabo Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
I Szarka Comenius University Bratislava, Faculty of Mathematics, Physics and Informatics, Bratislava, Slovak Republic
U Tabassam COMSATS University Islamabad, Islamabad, Pakistan
S F Taghavi Physik Department, Technische Universität München, Munich, Germany
G Taillepied Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
J Takahashi Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
G J Tambave Department of Physics and Technology, University of Bergen, Bergen, Norway
S Tang Central China Normal University, Wuhan, China Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France
Z Tang University of Science and Technology of China, Hefei, China
J D Tapia Takaki University of Kansas, Lawrence, Kansas, USA
N Tapus University Politehnica of Bucharest, Bucharest, Romania
L A Tarasovicova Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
M G Tarzila Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
A Tauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
A Telesca European Organization for Nuclear Research (CERN), Geneva, Switzerland
L Terlizzi Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
C Terrevoli University of Houston, Houston, Texas, USA
G Tersimonov Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, Kiev, Ukraine
S Thakur Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
D Thomas The University of Texas at Austin, Austin, Texas, USA
R Tieulent CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
A Tikhonov Affiliated with an institute covered by a cooperation agreement with CERN
A R Timmins University of Houston, Houston, Texas, USA
M Tkacik Technical University of Košice, Košice, Slovak Republic
T Tkacik Technical University of Košice, Košice, Slovak Republic
A Toia Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N Topilskaya Affiliated with an institute covered by a cooperation agreement with CERN
M Toppi INFN, Laboratori Nazionali di Frascati, Frascati, Italy
F Torales-Acosta Department of Physics, University of California, Berkeley, California, USA
T Tork Laboratoire de Physique des 2 Infinis, Irène Joliot-Curie, Orsay, France
A G Torres Ramos Dipartimento Interateneo di Fisica "M. Merlin" and Sezione INFN, Bari, Italy
A Trifiró Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
A S Triolo Dipartimento di Scienze MIFT, Università di Messina, Messina, Italy INFN, Sezione di Catania, Catania, Italy
S Tripathy INFN, Sezione di Bologna, Bologna, Italy
T Tripathy Indian Institute of Technology Bombay (IIT), Mumbai, India
S Trogolo European Organization for Nuclear Research (CERN), Geneva, Switzerland
V Trubnikov Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, Kiev, Ukraine
W H Trzaska University of Jyväskylä, Jyväskylä, Finland
T P Trzcinski Warsaw University of Technology, Warsaw, Poland
R Turrisi INFN, Sezione di Padova, Padova, Italy
T S Tveter Department of Physics, University of Oslo, Oslo, Norway
K Ullaland Department of Physics and Technology, University of Bergen, Bergen, Norway
B Ulukutlu Physik Department, Technische Universität München, Munich, Germany
A Uras CNRS/IN2P3, Institut de Physique des 2 Infinis de Lyon, Université de Lyon, Lyon, France
M Urioni INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy
G L Usai Dipartimento di Fisica dell'Università and Sezione INFN, Cagliari, Italy
M Vala Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
N Valle Dipartimento di Fisica, Università di Pavia, Pavia, Italy
S Vallero INFN, Sezione di Torino, Turin, Italy
L V R van Doremalen Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
M van Leeuwen Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
C A van Veen Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R J G van Weelden Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
P Vande Vyvre European Organization for Nuclear Research (CERN), Geneva, Switzerland
D Varga Wigner Research Centre for Physics, Budapest, Hungary
Z Varga Wigner Research Centre for Physics, Budapest, Hungary
M Varga-Kofarago Wigner Research Centre for Physics, Budapest, Hungary
M Vasileiou Department of Physics, School of Science, National and Kapodistrian University of Athens, Athens, Greece
A Vasiliev Affiliated with an institute covered by a cooperation agreement with CERN
O Vázquez Doce Physik Department, Technische Universität München, Munich, Germany
V Vechernin Affiliated with an institute covered by a cooperation agreement with CERN
E Vercellin Dipartimento di Fisica dell'Università and Sezione INFN, Turin, Italy
S Vergara Limón High Energy Physics Group, Universidad Autónoma de Puebla, Puebla, Mexico
L Vermunt Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
R Vértesi Wigner Research Centre for Physics, Budapest, Hungary
M Verweij Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
L Vickovic Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
Z Vilakazi University of the Witwatersrand, Johannesburg, South Africa
O Villalobos Baillie School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
G Vino INFN, Sezione di Bari, Bari, Italy
A Vinogradov Affiliated with an institute covered by a cooperation agreement with CERN
T Virgili Dipartimento di Fisica "E.R. Caianiello" dell'Università and Gruppo Collegato INFN, Salerno, Italy
V Vislavicius Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
A Vodopyanov Affiliated with an international laboratory covered by a cooperation agreement with CERN
B Volkel European Organization for Nuclear Research (CERN), Geneva, Switzerland
M A Völkl Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
K Voloshin Affiliated with an institute covered by a cooperation agreement with CERN
S A Voloshin Wayne State University, Detroit, Michigan, USA
G Volpe Dipartimento Interateneo di Fisica "M. Merlin" and Sezione INFN, Bari, Italy
B von Haller European Organization for Nuclear Research (CERN), Geneva, Switzerland
I Vorobyev Physik Department, Technische Universität München, Munich, Germany
N Vozniuk Affiliated with an institute covered by a cooperation agreement with CERN
J Vrláková Faculty of Science, Pavol Jozef Šafárik University, Košice, Slovak Republic
B Wagner Department of Physics and Technology, University of Bergen, Bergen, Norway
C Wang Fudan University, Shanghai, China
D Wang Fudan University, Shanghai, China
M Weber Stefan Meyer Institut für Subatomare Physik (SMI), Vienna, Austria
A Wegrzynek European Organization for Nuclear Research (CERN), Geneva, Switzerland
F T Weiglhofer Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S C Wenzel European Organization for Nuclear Research (CERN), Geneva, Switzerland
J P Wessels Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
S L Weyhmiller Yale University, New Haven, Connecticut, USA
J Wiechula Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J Wikne Department of Physics, University of Oslo, Oslo, Norway
G Wilk National Centre for Nuclear Research, Warsaw, Poland
J Wilkinson Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
G A Willems Westfälische Wilhelms-Universität Münster, Institut für Kernphysik, Munster, Germany
B Windelband Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M Winn Départment de Physique Nucléaire (DPhN), Université Paris-Saclay Centre d'Etudes de Saclay (CEA), IRFU, Saclay, France
J R Wright The University of Texas at Austin, Austin, Texas, USA
W Wu Fudan University, Shanghai, China
Y Wu University of Science and Technology of China, Hefei, China
R Xu Central China Normal University, Wuhan, China
A K Yadav Variable Energy Cyclotron Centre, Homi Bhabha National Institute, Kolkata, India
S Yalcin KTO Karatay University, Konya, Turkey
Y Yamaguchi Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
K Yamakawa Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
S Yang Department of Physics and Technology, University of Bergen, Bergen, Norway
S Yano Physics Program and International Institute for Sustainability with Knotted Chiral Meta Matter (SKCM2), Hiroshima University, Hiroshima, Japan
Z Yin Central China Normal University, Wuhan, China
I-K Yoo Department of Physics, Pusan National University, Pusan, Republic of Korea
J H Yoon Inha University, Incheon, Republic of Korea
S Yuan Department of Physics and Technology, University of Bergen, Bergen, Norway
A Yuncu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
V Zaccolo Dipartimento di Fisica dell'Università and Sezione INFN, Trieste, Italy
C Zampolli European Organization for Nuclear Research (CERN), Geneva, Switzerland
H J C Zanoli Institute for Gravitational and Subatomic Physics (GRASP), Utrecht University/Nikhef, Utrecht, Netherlands
F Zanone Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
N Zardoshti European Organization for Nuclear Research (CERN), Geneva, Switzerland School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A Zarochentsev Affiliated with an institute covered by a cooperation agreement with CERN
P Závada Institute of Physics of the Czech Academy of Sciences, Prague, Czech Republic
N Zaviyalov Affiliated with an institute covered by a cooperation agreement with CERN
M Zhalov Affiliated with an institute covered by a cooperation agreement with CERN
B Zhang Central China Normal University, Wuhan, China
S Zhang Fudan University, Shanghai, China
X Zhang Central China Normal University, Wuhan, China
Y Zhang University of Science and Technology of China, Hefei, China
M Zhao China Institute of Atomic Energy, Beijing, China
V Zherebchevskii Affiliated with an institute covered by a cooperation agreement with CERN
Y Zhi China Institute of Atomic Energy, Beijing, China
N Zhigareva Affiliated with an institute covered by a cooperation agreement with CERN
D Zhou Central China Normal University, Wuhan, China
Y Zhou Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
J Zhu Central China Normal University, Wuhan, China Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
Y Zhu Central China Normal University, Wuhan, China
G Zinovjev Bogolyubov Institute for Theoretical Physics, National Academy of Sciences of Ukraine, Kiev, Ukraine
N Zurlo INFN, Sezione di Pavia, Pavia, Italy Università di Brescia, Brescia, Italy

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First Measurement of Antideuteron Number Fluctuations at Energies Available at the Large Hadron Collider

The first measurement of event-by-event antideuteron number fluctuations in high energy heavy-ion collisions is presented. The measurements are carried out at midrapidity (|η|<0.8) as a function of collision centrality in Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV using the ALICE detector. A significant negative correlation between the produced antiprotons and antideuterons is observed in all collision centralities. The results are compared with a state-of-the-art coalescence calculation. While it describes the ratio of higher order cumulants of the antideuteron multiplicity distribution, it fails to describe quantitatively the magnitude of the correlation between antiproton and antideuteron production. On the other hand, thermal-statistical model calculations describe all the measured observables within uncertainties only for correlation volumes that are different with respect to those describing proton yields and a similar measurement of net-proton number fluctuations.

A multidisciplinary approach to the identification of the protein-RNA connectome in double-stranded RNA virus capsids

How multi-segmented double-stranded RNA (dsRNA) viruses correctly incorporate their genomes into their capsids remains unclear for many viruses, including Bluetongue virus (BTV), a Reoviridae member, with a genome of 10 segments. To address this, we used an RNA-cross-linking and peptide-fingerprinting assay (RCAP) to identify RNA binding sites of the inner capsid protein VP3, the viral polymerase VP1 and the capping enzyme VP4. Using a combination of mutagenesis, reverse genetics, recombinant proteins and in vitro assembly, we validated the importance of these regions in virus infectivity. Further, to identify which RNA segments and sequences interact with these proteins, we used viral photo-activatable ribonucleoside crosslinking (vPAR-CL) which revealed that the larger RNA segments (S1-S4) and the smallest segment (S10) have more interactions with viral proteins than the other smaller segments. Additionally, using a sequence enrichment analysis we identified an RNA motif of nine bases that is shared by the larger segments. The importance of this motif for virus replication was confirmed by mutagenesis followed by virus recovery. We further demonstrated that these approaches could be applied to a related Reoviridae member, rotavirus (RV), which has human epidemic impact, offering the possibility of novel intervention strategies for a human pathogen.

Comparison of Wet Mount Microscopy and Giemsa Staining to PCR in the Diagnosis of Vaginal Trichomoniasis in a Tertiary Level Hospital of Bangladesh

Trichomonas vaginalis (T vaginalis) is the most prevalent non-viral sexually transmitted infection of the reproductive age group, which may lead to various complications, if left untreated. This study aimed to diagnose Trichomonas vaginalis infection by different diagnostic procedures and to evaluate the efficacy of different diagnostic procedures. This cross-sectional descriptive study was conducted among 102 women with vaginal discharge at the Department of Obstetrics & Gynecology at Mymensingh Medical College Hospital (MMCH) from July 2019 to December 2020. Three ectocervical swabs were collected from each patient. Saline wet mount microscopy, giemsa staining and PCR were performed for each patient. Data were collected using a structured questionnaire and analyzed using Excel 2007, statistical package for social sciences (SPSS) version 26.0. The PCR assay detected Trichomonas vaginalis positivity in 6(5.9%) of 102 patients, followed by Giemsa staining 4.9% and Wet mount examination 2.9%. Wet mount microscopy showed less sensitivity 33.33%, but high specificity 98.95%, 66.67% positive predictive value, 95.96% negative predictive value and accuracy 95.09%. The sensitivity, specificity, PPV, NPV and accuracy of Giemsa staining were 66.67%, 98.96%, 80.0%, 97.94% and 97.06% respectively. Statistical significance was observed when both WMM and Giemsa staining were compared to gold standard test PCR. In resource limited settings, a wet mount is a good option for diagnosis of T vaginalis infection as giemsa staining requires heavy T vaginalis infection to be positive. But wherever facilities are available, PCR should be performed.

Virus structures and molecular biology exchange glances

The definition of structure as the arrangement of and relations between the parts of something complex has always been a challenge in virology. The balance required for a virus to be sufficiently stable to allow transmission yet also be primed for disassembly on contact with a permissive cell is precarious and seemingly difficult to attain. Add to this that virus structural components often have multiple functions such as receptor binding, fusion, and cleavage, and the puzzle deepens. It also has consequences: virus yields may be compromised, vaccine shelf-life may be limited, and the ability to quickly evolve away from an intervention may be underestimated. Progress in understanding virus structure and the ways in which it might be exploited were the subject of the latest International Virus Assembly Symposium. Whole viruses, individual components, and transient intermediates were revealed at sufficiently high resolution to deduce the mechanisms concerned.

Measurement of the ν_{e}-Nucleus Charged-Current Double-Differential Cross Section at ⟨E_{ν}⟩=2.4 GeV Using NOvA

The inclusive electron neutrino charged-current cross section is measured in the NOvA near detector using 8.02×10^{20} protons-on-target in the NuMI beam. The sample of GeV electron neutrino interactions is the largest analyzed to date and is limited by ≃17% systematic rather than the ≃7.4% statistical uncertainties. The double-differential cross section in final-state electron energy and angle is presented for the first time, together with the single-differential dependence on Q^{2} (squared four-momentum transfer) and energy, in the range 1  GeV≤E_{ν}<6  GeV. Detailed comparisons are made to the predictions of the GENIE, GiBUU, NEUT, and NuWro neutrino event generators. The data do not strongly favor a model over the others consistently across all three cross sections measured, though some models have especially good or poor agreement in the single differential cross section vs Q^{2}.

Early Release Science of the exoplanet WASP-39b with JWST NIRSpec PRISM

Transmission spectroscopy1-3 of exoplanets has revealed signatures of water vapour, aerosols and alkali metals in a few dozen exoplanet atmospheres4,5. However, these previous inferences with the Hubble and Spitzer Space Telescopes were hindered by the observations' relatively narrow wavelength range and spectral resolving power, which precluded the unambiguous identification of other chemical species-in particular the primary carbon-bearing molecules6,7. Here we report a broad-wavelength 0.5-5.5 µm atmospheric transmission spectrum of WASP-39b8, a 1,200 K, roughly Saturn-mass, Jupiter-radius exoplanet, measured with the JWST NIRSpec's PRISM mode9 as part of the JWST Transiting Exoplanet Community Early Release Science Team Program10-12. We robustly detect several chemical species at high significance, including Na (19σ), H2O (33σ), CO2 (28σ) and CO (7σ). The non-detection of CH4, combined with a strong CO2 feature, favours atmospheric models with a super-solar atmospheric metallicity. An unanticipated absorption feature at 4 µm is best explained by SO2 (2.7σ), which could be a tracer of atmospheric photochemistry. These observations demonstrate JWST's sensitivity to a rich diversity of exoplanet compositions and chemical processes.

Enhanced Zika virus-like particle development using Baculovirus spp. constructs

Zika virus (ZIKV) is one of several examples of an unprecedented pandemic spread and against which there is currently no suitable vaccine or treatment. Here, we constructed and characterized recombinant baculovirus-derived ZIKV-like particles (Zika VLPs) to study ZIKV-antibody interactions. These VLPs, uniquely consisted of the full-length ZIKV capsid (C), pre-membrane (prM), and envelope (E) proteins with either: a) the viral nonstructural NS2B and NS3 protease unit under one or two different promoters or b) an alternative host-cell furin protease encoding cleavage sequence inserted between the C and prM genes, together with lobster tropomyosin leader and honeybee signal sequences with one promoter for increased extracellular secretion. All these Zika VLPs displayed typical virion morphology in transmission electron microscopic analysis when expressed in both insect (Sf9) and mammalian (HEK293T) cells and no uncleaved prM glycoprotein was detected, as are present on immature virions. The importance of glycosylation of the E glycoprotein was shown by the effects on both polyclonal and monoclonal antibody reactions after these N-linked carbohydrate residues were disrupted by oxidation or enzymatic cleavage. Importantly, the construct which contained the host-cell furin protease cleavage sequence together with a lobster tropomyosin leader and honeybee signal sequences under one promoter produced higher Zika VLP titers and protein concentrations and which can now be tested as a superior construct in multifunctional diagnostic (ELISA and neutralization/antibody-dependent enhancement) assays and immunogenic assessments possibly leading to vaccine trials.

Assessment of post-vaccination immune response to peste des petits ruminants virus in small ruminants in the central and western regions of India

The cross-sectional serosurvey for post-vaccination assessment of peste des petits ruminants (PPR) virus (PPRV) antibodies in sheep and goats was carried out in different states in the central and western regions of India after the implementation of vaccination under the PPR control programme. The serum samples (n = 4687) were collected from sheep (n = 1539) and goats (n = 3148) from August 2017 to March 2018 at various epidemiological units (n = 301) of the studied regions using a stratified random sampling method and PPR competitive ELISA kit was employed to detect PPRV antibodies. The results revealed 34, 21, 52, 74, 68, and 65% of prevalence of PPRV antibodies in small ruminants in Madhya Pradesh, Goa, Chhattisgarh, Maharashtra, Gujarat, and Rajasthan states, respectively, with a difference in seropositivity in sheep and goats across the states in sheep (p < 0.01) and goats (p < 0.01). Further, this serosurvey revealed that 60% of the epi-units (n = 185) had > 50% prevalence of post vaccination PPRV antibodies across states due to variations in vaccination rates and patterns. The vaccination coverage and the reported outbreaks varied between the states in the studied regions. Due to continuous vaccination under the control program, the reported PPR outbreaks have progressively declined in most of the studied states, and the PPR risk areas are confined to a few districts and sporadically, outbreaks are reported indicating the effectiveness of vaccination. These findings provide valuable information on potential PPRV episystems, and will assist with activities regarding intensive surveillance, vaccination, biosecurity, and modification of policy decisions towards designing and implementing control and eradication measures. Further, the present situation necessitates continuous mass vaccination and active surveillance programs to make these regions free from PPR in consonance with the PPR Global Control and Eradication Strategy under the PPR Global Eradication Program.

Supplementary Information

The online version contains supplementary material available at 10.1007/s13337-022-00796-6.

Role of NS2 specific RNA binding and phosphorylation in liquid-liquid phase separation and virus assembly

Liquid-liquid phase separation (LLPS) has assumed a prominent role in biological cell systems, where it underpins the formation of subcellular compartments necessary for cell function. We investigated the underlying mechanism of LLPS in virus infected cells, where virus inclusion bodies are formed by an RNA-binding phosphoprotein (NS2) of Bluetongue virus to serve as sites for subviral particle assembly and virus maturation. We show that NS2 undergoes LLPS that is dependent on protein phosphorylation and RNA-binding and that LLPS occurrence is accompanied by a change in protein secondary structure. Site-directed mutagenesis identified two critical arginine residues in NS2 responsible for specific RNA binding and thus for NS2-RNA complex driven LLPS. Reverse genetics identified the same residues as essential for VIB assembly in infected cells and virus viability. Our findings suggest that a specific arginine-RNA interaction in the context of a phosphorylated state drives LLPS in this, and possibly other, virus infections.

Scintillation light detection in the 6-m drift-length ProtoDUNE Dual Phase liquid argon TPC

DUNE is a dual-site experiment for long-baseline neutrino oscillation studies, neutrino astrophysics and nucleon decay searches. ProtoDUNE Dual Phase (DP) is a 6  ×  6  ×  6 m 3 liquid argon time-projection-chamber (LArTPC) that recorded cosmic-muon data at the CERN Neutrino Platform in 2019-2020 as a prototype of the DUNE Far Detector. Charged particles propagating through the LArTPC produce ionization and scintillation light. The scintillation light signal in these detectors can provide the trigger for non-beam events. In addition, it adds precise timing capabilities and improves the calorimetry measurements. In ProtoDUNE-DP, scintillation and electroluminescence light produced by cosmic muons in the LArTPC is collected by photomultiplier tubes placed up to 7 m away from the ionizing track. In this paper, the ProtoDUNE-DP photon detection system performance is evaluated with a particular focus on the different wavelength shifters, such as PEN and TPB, and the use of Xe-doped LAr, considering its future use in giant LArTPCs. The scintillation light production and propagation processes are analyzed and a comparison of simulation to data is performed, improving understanding of the liquid argon properties.

Hypertriton Production in p-Pb Collisions at sqrt[s_{NN}]=5.02 TeV

The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of _{Λ}^{3}H in p-Pb collisions at sqrt[s_{NN}]=5.02  TeV is presented in this Letter. Its production yield measured in the rapidity interval -1<y<0 for the 40% highest-multiplicity p-Pb collisions is dN/dy=[6.3±1.8(stat)±1.2(syst)]×10^{-7}. The measurement is compared with the expectations of statistical hadronization and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in charged particle multiplicity environments relevant to small collision systems such as p-Pb, and therefore the measurement of dN/dy is crucial to distinguish between them. The precision of this measurement leads to the exclusion with a significance larger than 6.9σ of some configurations of the statistical hadronization model, thus constraining the theory behind the production of loosely bound states at hadron colliders.

Lattice dynamics of BaFe2Se3

This paper presents a study of the lattice dynamics in BaFe₂Se₃. We combined first-principle calculations, infrared measurements and a thorough symmetry analysis. Our study confirms thatPnmacannot be the space group of BaFe₂Se₃, even at room temperature. The phonons assignment requiresPmto be the BaFe₂Se₃space group, not only in the magnetic phase, but also in the paramagnetic phase at room temperature. This is due to a strong coupling between a short-range spin-order along the ladders, and the lattice degrees of freedom associated with the Fe-Fe bond length. This coupling induces a change in the bond-length pattern from an alternated trapezoidal one (as inPnma) to an alternated small/large rectangular one. Out of the two patterns, only the latter is fully compatible with the observed block-type magnetic structure. Finally, we propose a complete symmetry analysis of the BaFe₂Se₃phase diagram in the 0-600 K range.

Polarization of Λ and Λ[over ¯] Hyperons along the Beam Direction in Pb-Pb Collisions at sqrt[s]_{NN}=5.02 TeV

The polarization of the Λ and Λ[over ¯] hyperons along the beam (z) direction, P_{z}, has been measured in Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV recorded with ALICE at the Large Hadron Collider (LHC). The main contribution to P_{z} comes from elliptic flow-induced vorticity and can be characterized by the second Fourier sine coefficient P_{z,s2}=⟨P_{z}sin(2φ-2Ψ_{2})⟩, where φ is the hyperon azimuthal emission angle and Ψ_{2} is the elliptic flow plane angle. We report the measurement of P_{z,s2} for different collision centralities and in the 30%-50% centrality interval as a function of the hyperon transverse momentum and rapidity. The P_{z,s2} is positive similarly as measured by the STAR Collaboration in Au-Au collisions at sqrt[s_{NN}]=200  GeV, with somewhat smaller amplitude in the semicentral collisions. This is the first experimental evidence of a nonzero hyperon P_{z} in Pb-Pb collisions at the LHC. The comparison of the measured P_{z,s2} with the hydrodynamic model calculations shows sensitivity to the competing contributions from thermal and the recently found shear-induced vorticity, as well as to whether the polarization is acquired at the quark-gluon plasma or the hadronic phase.

SARS-CoV-2 Virus-Like Particles Produced by a Single Recombinant Baculovirus Generate Anti-S Antibody and Protect against Variant Challenge

Coronavirus Disease 2019 (COVID-19), caused by infection with Severe Acute Respiratory Syndrome Coronavirus 2 (SARS-CoV-2), has highlighted the need for the rapid generation of efficient vaccines for emerging disease. Virus-like particles, VLPs, are an established vaccine technology that produces virus-like mimics, based on expression of the structural proteins of a target virus. SARS-CoV-2 is a coronavirus where the basis of VLP formation has been shown to be the co-expression of the spike, membrane and envelope structural proteins. Here we describe the generation of SARS-CoV-2 VLPs by the co-expression of the salient structural proteins in insect cells using the established baculovirus expression system. VLPs were heterologous ~100 nm diameter enveloped particles with a distinct fringe that reacted strongly with SARS-CoV-2 convalescent sera. In a Syrian hamster challenge model, non-adjuvanted VLPs induced neutralizing antibodies to the VLP-associated Wuhan S protein and reduced virus shedding and protected against disease associated weight loss following a virulent challenge with SARS-CoV-2 (B.1.1.7 variant). Immunized animals showed reduced lung pathology and lower challenge virus replication than the non-immunized controls. Our data suggest SARS-CoV-2 VLPs offer an efficient vaccine that mitigates against virus load and prevents severe disease.

Psychiatric Morbidity in Irritable Bowel Syndrome

Psychiatric morbidity is frequent among outpatients with Irritable Bowel Syndrome (IBS) attending gastroenterology clinics. The lifetime prevalence of major depressive and anxiety disorders in IBS patients are up to 76% and 54% respectively. The point prevalence of Major depressive disorder and Anxiety disorders in IBS patients are ranged 9.6 to 54% and from 11.1 to 52.4% respectively. IBS is not usually life-threatening but it has a significant impact on quality of life. So, screening for psychiatric disorders in IBS patients attending Gastroenterology clinics is worthwhile. The objective of this study was to evaluate psychiatric morbidity among the patients with IBS. This cross sectional comparative study was conducted in the Department of Psychiatry, Sylhet MAG Osmani Medical College Hospital, Sylhet, Bangladesh during the period from January 2012 to June 2012. Inclusion criteria were patients of irritable bowel syndrome fulfilling the Rome-III criteria, age between 18 to 60 years irrespective of sex. Patients with any red flag sign, serious cognitive impairment such as dementia, schizophrenia, mania, delusional disorder, prior history of abdominal surgery and other chronic diseases were excluded. One hundred and ten patients with IBS were selected according to inclusion and exclusion criteria and categorized as IBS group. Another 110 age and sex matched subjects were selected as control group. The mean±SD age of the patients was 34.3±12.2 years which was almost identical to control group (p=0.820). Most of the patients (66.4%) were below the age of 40 years. There were 64 (58.2%) male and 46 (41.8%) female which was similar to control group (p=0.643). Psychiatric co-morbidity was most frequent in IBS patients (56.4%) as compared to control group (16.4%) p value <0.001. The most common psychiatric disorders were Anxiety disorders (22.7%), followed by major depressive disorder (19.1%) and somatization disorder (14.5%). The results of this study suggest that a significant number of patients with IBS suffer from psychiatric disorders than control, which are similar to the IBS group in age and gender.

Measurement of the Groomed Jet Radius and Momentum Splitting Fraction in pp and Pb-Pb Collisions at sqrt[s_{NN}]=5.02 TeV

This article presents groomed jet substructure measurements in pp and Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV with the ALICE detector. The soft drop grooming algorithm provides access to the hard parton splittings inside a jet by removing soft wide-angle radiation. We report the groomed jet momentum splitting fraction, z_{g}, and the (scaled) groomed jet radius, θ_{g}. Charged-particle jets are reconstructed at midrapidity using the anti-k_{T} algorithm with resolution parameters R=0.2 and R=0.4. In heavy-ion collisions, the large underlying event poses a challenge for the reconstruction of groomed jet observables, since fluctuations in the background can cause groomed parton splittings to be misidentified. By using strong grooming conditions to reduce this background, we report these observables fully corrected for detector effects and background fluctuations for the first time. A narrowing of the θ_{g} distribution in Pb-Pb collisions compared to pp collisions is seen, which provides direct evidence of the modification of the angular structure of jets in the quark-gluon plasma. No significant modification of the z_{g} distribution in Pb-Pb collisions compared to pp collisions is observed. These results are compared with a variety of theoretical models of jet quenching, and provide constraints on jet energy-loss mechanisms and coherence effects in the quark-gluon plasma.

Unlocking synchrotron sources for THz spectroscopy at sub-MHz resolution

Synchrotron radiation (SR) has proven to be an invaluable contributor to the field of molecular spectroscopy, particularly in the terahertz region (1-10 THz) where its bright and broadband properties are currently unmatched by laboratory sources. However, measurements using SR are currently limited to a resolution of around 30 MHz, due to the limits of Fourier-transform infrared spectroscopy. To push the resolution limit further, we have developed a spectrometer based on heterodyne mixing of SR with a newly available THz molecular laser, which can operate at frequencies ranging from 1 to 5.5 THz. This spectrometer can record at a resolution of 80 kHz, with 5 GHz of bandwidth around each molecular laser frequency, making it the first SR-based instrument capable of sub-MHz, Doppler-limited spectroscopy across this wide range. This allows closely spaced spectral features, such as the effects of internal dynamics and fine angular momentum couplings, to be observed. Furthermore, mixing of the molecular laser with a THz comb is demonstrated, which will enable extremely precise determinations of molecular transition frequencies.

What's up with WhatsApp in supplementing surgical education: an objective assessment

INTRODUCTION

This is the first study aimed at objectively quantifying the benefit of virtual education using WhatsApp-based discussion groups.

METHODS

A prospective, non-randomised interventional study was undertaken in the Department of General Surgery, at a tertiary care centre in Kolkata, India, with 200 undergraduate students over a period of 5 days each for 2 weeks, with the first week acting as a control arm. A WhatsApp group was created consisting of 197 eligible undergraduates, faculty members and the authors of this study. Each day, three questions were posted on this group. The second week involved an hour-long WhatsApp-based discussion between the participants and the faculty. Responses were recorded and compared for improvements between the two weeks. Participant feedback was collected and analysed.

RESULTS

Statistically significant improvements were observed in the study group compared with the control group in rates of one in three, two in three and three in three correct responses (p=0.01649, 0.01146 and 0.00946, respectively). A total of 68 (51.92%) feedback respondents were satisfied with the programme. Convenience of use was the principal reason behind satisfaction in 79 respondents (60.31%), whereas 62 participants (47.33%) reported lack of hands-on training as a major drawback.

CONCLUSIONS

WhatsApp was found to be a satisfactory supplement to traditional medical teaching. It can be implemented to fill lapses in medical education, especially in light of the COVID-19 pandemic, which has caused great disruption to traditional teaching methods. Research is needed to assess the feasibility of incorporating it into the curriculum.

Measurement of Prompt D^{0}, Λ_{c}^{+}, and Σ_{c}^{0,++}(2455) Production in Proton-Proton Collisions at sqrt[s]=13 TeV

The p_{T}-differential production cross sections of prompt D^{0}, Λ_{c}^{+}, and Σ_{c}^{0,++}(2455) charmed hadrons are measured at midrapidity (|y|<0.5) in pp collisions at sqrt[s]=13  TeV. This is the first measurement of Σ_{c}^{0,++} production in hadronic collisions. Assuming the same production yield for the three Σ_{c}^{0,+,++} isospin states, the baryon-to-meson cross section ratios Σ_{c}^{0,+,++}/D^{0} and Λ_{c}^{+}/D^{0} are calculated in the transverse momentum (p_{T}) intervals 2<p_{T}<12 and 1<p_{T}<24  GeV/c. Values significantly larger than in e^{+}e^{-} collisions are observed, indicating for the first time that baryon enhancement in hadronic collisions also extends to the Σ_{c}. The feed-down contribution to Λ_{c}^{+} production from Σ_{c}^{0,+,++} is also reported and is found to be larger than in e^{+}e^{-} collisions. The data are compared with predictions from event generators and other phenomenological models, providing a sensitive test of the different charm-hadronization mechanisms implemented in the models.

Measurement of the Cross Sections of Ξ_{c}^{0} and Ξ_{c}^{+} Baryons and of the Branching-Fraction Ratio BR(Ξ_{c}^{0}→Ξ^{-}e^{+}ν_{e})/BR(Ξ_{c}^{0}→Ξ^{-}π^{+}) in pp Collisions at sqrt[s]=13 TeV

The p_{T}-differential cross sections of prompt charm-strange baryons Ξ_{c}^{0} and Ξ_{c}^{+} were measured at midrapidity (|y|<0.5) in proton-proton (pp) collisions at a center-of-mass energy sqrt[s]=13  TeV with the ALICE detector at the LHC. The Ξ_{c}^{0} baryon was reconstructed via both the semileptonic decay (Ξ^{-}e^{+}ν_{e}) and the hadronic decay (Ξ^{-}π^{+}) channels. The Ξ_{c}^{+} baryon was reconstructed via the hadronic decay (Ξ^{-}π^{+}π^{+}) channel. The branching-fraction ratio BR(Ξ_{c}^{0}→Ξ^{-}e^{+}ν_{e})/BR(Ξ_{c}^{0}→Ξ^{-}π^{+})=1.38±0.14(stat)±0.22(syst) was measured with a total uncertainty reduced by a factor of about 3 with respect to the current world average reported by the Particle Data Group. The transverse momentum (p_{T}) dependence of the Ξ_{c}^{0}- and Ξ_{c}^{+}-baryon production relative to the D^{0} meson and to the Σ_{c}^{0,+,++}- and Λ_{c}^{+}-baryon production are reported. The baryon-to-meson ratio increases toward low p_{T} up to a value of approximately 0.3. The measurements are compared with various models that take different hadronization mechanisms into consideration. The results provide stringent constraints to these theoretical calculations and additional evidence that different processes are involved in charm hadronization in electron-positron (e^{+}e^{-}) and hadronic collisions.

What's up with WhatsApp in supplementing surgical education: an objective assessment

INTRODUCTION

This is the first study aimed at objectively quantifying the benefit of virtual education using WhatsApp-based discussion groups.

METHODS

A prospective, non-randomised interventional study was undertaken in the Department of General Surgery, at a tertiary care centre in Kolkata, India, with 200 undergraduate students over a period of 5 days each for 2 weeks, with the first week acting as a control arm. A WhatsApp group was created consisting of 197 eligible undergraduates, faculty members and the authors of this study. Each day, three questions were posted on this group. The second week involved an hour-long WhatsApp-based discussion between the participants and the faculty. Responses were recorded and compared for improvements between the two weeks. Participant feedback was collected and analysed.

RESULTS

Statistically significant improvements were observed in the study group compared with the control group in rates of one in three, two in three and three in three correct responses (p=0.01649, 0.01146 and 0.00946, respectively). A total of 68 (51.92%) feedback respondents were satisfied with the programme. Convenience of use was the principal reason behind satisfaction in 79 respondents (60.31%), whereas 62 participants (47.33%) reported lack of hands-on training as a major drawback.

CONCLUSIONS

WhatsApp was found to be a satisfactory supplement to traditional medical teaching. It can be implemented to fill lapses in medical education, especially in light of the COVID-19 pandemic, which has caused great disruption to traditional teaching methods. Research is needed to assess the feasibility of incorporating it into the curriculum.

Λ_{c}^{+} Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at sqrt[s_{NN}]=5.02 TeV at the LHC

The prompt production of the charm baryon Λ_{c}^{+} and the Λ_{c}^{+}/D^{0} production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sqrt[s_{NN}]=5.02  TeV. These new measurements show a clear decrease of the Λ_{c}^{+}/D^{0} ratio with increasing transverse momentum (p_{T}) in both collision systems in the range 2<p_{T}<12  GeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/π and Λ/K_{S}^{0}. At low p_{T}, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e^{+}e^{-} and e^{-}p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies.

Bluetongue virus capsid protein VP5 perforates membranes at low endosomal pH during viral entry

Bluetongue virus (BTV) is a non-enveloped virus and causes substantial morbidity and mortality in ruminants such as sheep. Fashioning a receptor-binding protein (VP2) and a membrane penetration protein (VP5) on the surface, BTV releases its genome-containing core (VP3 and VP7) into the host cell cytosol after perforation of the endosomal membrane. Unlike enveloped ones, the entry mechanisms of non-enveloped viruses into host cells remain poorly understood. Here we applied single-particle cryo-electron microscopy, cryo-electron tomography and structure-guided functional assays to characterize intermediate states of BTV cell entry in endosomes. Four structures of BTV at the resolution range of 3.4-3.9 Å show the different stages of structural rearrangement of capsid proteins on exposure to low pH, including conformational changes of VP5, stepwise detachment of VP2 and a small shift of VP7. In detail, sensing of the low-pH condition by the VP5 anchor domain triggers three major VP5 actions: projecting the hidden dagger domain, converting a surface loop to a protonated β-hairpin that anchors VP5 to the core and stepwise refolding of the unfurling domains into a six-helix stalk. Cryo-electron tomography structures of BTV interacting with liposomes show a length decrease of the VP5 stalk from 19.5 to 15.5 nm after its insertion into the membrane. Our structures, functional assays and structure-guided mutagenesis experiments combined indicate that this stalk, along with dagger domain and the WHXL motif, creates a single pore through the endosomal membrane that enables the viral core to enter the cytosol. Our study unveils the detailed mechanisms of BTV membrane penetration and showcases general methods to study cell entry of other non-enveloped viruses.

Experimental Evidence for an Attractive p-ϕ Interaction

This Letter presents the first experimental evidence of the attractive strong interaction between a proton and a ϕ meson. The result is obtained from two-particle correlations of combined p-ϕ⊕ p[over ¯]-ϕ pairs measured in high-multiplicity pp collisions at sqrt[s]=13  TeV by the ALICE Collaboration. The spin-averaged scattering length and effective range of the p-ϕ interaction are extracted from the fully corrected correlation function employing the Lednický-Lyuboshits approach. In particular, the imaginary part of the scattering length vanishes within uncertainties, indicating that inelastic processes do not play a prominent role for the p-ϕ interaction. These data demonstrate that the interaction is dominated by elastic p-ϕ scattering. Furthermore, an analysis employing phenomenological Gaussian- and Yukawa-type potentials is conducted. Under the assumption of the latter, the N-ϕ coupling constant is found to be g_{N-ϕ}=0.14±0.03(stat)±0.02(syst). This work provides valuable experimental input to accomplish a self-consistent description of the N-ϕ interaction, which is particularly relevant for the more fundamental studies on partial restoration of chiral symmetry in nuclear medium.

Multiharmonic Correlations of Different Flow Amplitudes in Pb-Pb Collisions at sqrt[s_{NN}]=2.76 TeV

The event-by-event correlations between three flow amplitudes are measured for the first time in Pb-Pb collisions, using higher-order symmetric cumulants. We find that different three-harmonic correlations develop during the collective evolution of the medium when compared to correlations that exist in the initial state. These new results cannot be interpreted in terms of previous lower-order flow measurements since contributions from two-harmonic correlations are explicitly removed in the new observables. A comparison to Monte Carlo simulations provides new and independent constraints for the initial conditions and system properties of nuclear matter created in heavy-ion collisions.

Soft-Dielectron Excess in Proton-Proton Collisions at sqrt[s]=13 TeV

A measurement of dielectron production in proton-proton (pp) collisions at sqrt[s]=13  TeV, recorded with the ALICE detector at the CERN LHC, is presented in this Letter. The data set was recorded with a reduced magnetic solenoid field. This enables the investigation of a kinematic domain at low dielectron (ee) invariant mass m_{ee} and pair transverse momentum p_{T,ee} that was previously inaccessible at the LHC. The cross section for dielectron production is studied as a function of m_{ee}, p_{T,ee}, and event multiplicity dN_{ch}/dη. The expected dielectron rate from hadron decays, called hadronic cocktail, utilizes a parametrization of the measured η/π^{0} ratio in pp and proton-nucleus collisions, assuming that this ratio shows no strong dependence on collision energy at low transverse momentum. Comparison of the measured dielectron yield to the hadronic cocktail at 0.15<m_{ee}<0.6  GeV/c^{2} and for p_{T,ee}<0.4  GeV/c indicates an enhancement of soft dielectrons, reminiscent of the "anomalous" soft-photon and soft-dilepton excess in hadron-hadron collisions reported by several experiments under different experimental conditions. The enhancement factor over the hadronic cocktail amounts to 1.61±0.13(stat)±0.17(syst,data)±0.34(syst,cocktail) in the ALICE acceptance. Acceptance-corrected excess spectra in m_{ee} and p_{T,ee} are extracted and compared with calculations of dielectron production from hadronic bremsstrahlung and thermal radiation within a hadronic many-body approach.

Entry-competent-replication-abortive African horse sickness virus strains elicit robust immunity in ponies against all serotypes

African horse sickness virus (AHSV) is an Orbivirus within the Reoviridae family, spread by Culicoides species of midges, which infects equids with high mortality, particularly in horses and has a considerable impact on the equine industry. In order to control the disease, we previously described Entry Competent Replication Abortive (ECRA) virus strains for each of the nine distinct AHSV serotypes and demonstrated their potential as vaccines, first in type I interferon receptor (IFNAR-/-) knockout mice, and then in ponies. In this report we have investigated whether or not a combination ECRA vaccine comprising nine vaccine strains as two different cocktails is as efficient in ponies and the duration of the immunity triggered by ECRA vaccines. In one study, a group of ponies were vaccinated with a cocktail of 4 vaccine strains, followed by a vaccination of the remaining 5 vaccine strains, mimicking the current live attenuated vaccine regimen. In the second study, ponies were vaccinated with a single ECRA-AHSV strain and monitored for 6 months. The first group of ponies developed neutralising antibody responses against all 9 serotypes, indicating that no cross-serotype interference occurred, while the second group developed robust neutralising antibody responses against the single serotype that were sustained at the same level throughout a 6-month study. The results support our previous data and further validate ECRA vaccines as a safe and efficacious replacement of current live vaccines.

Mining the pervasiveness of surra in different animal species of Northeastern states of India: Assam, Mizoram and Tripura

Trypanosoma evansi is a flagellated, extracellular haemoprotozoan parasite infecting a wide range of mammalian hosts including dromedaries, cattle, equines and dogs cause disease surra. Carrier animals with sub-clinical infection cause significant monetary losses to livestock holders and therefore detection of infection status using molecular diagnostic techniques becomes important in order to control the disease. In the current study cattle, buffalo, goat, pig and dog samples from three northeastern states of India-Assam, Mizoram and Tripura were screened to determine the prevalence of surra. A total of 1702 samples including 795 from Assam, 678 from Mizoram and 229 from Tripura were screened by CATT/T. evansi test out of which 16.8%, 27.1% and 22.3% samples in respective states were found to have antibodies against T. evansi. DNA detection of T. evansi by PCR amplification targeting VSG gene revealed the molecular prevalence of surra in Assam, Mizoram and Tripura as 8.5%, 7.5% and 4.4% respectively. The analysis of amplified partial VSG sequences showed 99% similarity within an animal species whereas 86-94% similarity was observed among different species of animals revealing the homogeneity. The study established the prevalence of surra in different species of animals in the three northeastern states of India-Assam, Mizoram and Tripura and this study is the first report of T. evansi infection in pig and goat from India.

Supplementary Information

The online version contains supplementary material available at 10.1007/s12639-021-01392-z.

Elliptic Flow of Electrons from Beauty-Hadron Decays in Pb-Pb Collisions at sqrt[s_{NN}]=5.02 TeV

The elliptic flow of electrons from beauty hadron decays at midrapidity (|y|<0.8) is measured in Pb-Pb collisions at sqrt[s_{NN}]=5.02  TeV with the ALICE detector at the LHC. The azimuthal distribution of the particles produced in the collisions can be parametrized with a Fourier expansion, in which the second harmonic coefficient represents the elliptic flow, v_{2}. The v_{2} coefficient of electrons from beauty hadron decays is measured for the first time in the transverse momentum (p_{T}) range 1.3-6  GeV/c in the centrality class 30%-50%. The measurement of electrons from beauty-hadron decays exploits their larger mean proper decay length cτ≈500  μm compared to that of charm hadrons and most of the other background sources. The v_{2} of electrons from beauty hadron decays at midrapidity is found to be positive with a significance of 3.75  σ. The results provide insights into the degree of thermalization of beauty quarks in the medium. A model assuming full thermalization of beauty quarks is strongly disfavored by the measurement at high p_{T}, but is in agreement with the results at low p_{T}. Transport models including substantial interactions of beauty quarks with an expanding strongly interacting medium describe the measurement within uncertainties.

Evaluation of the diagnostic potential of recombinant leptospiral OMP A-like protein (Loa22) and transmembrane (OmpL37) protein in latex agglutination test for serodiagnosis of leptospirosis in animals

Leptospirosis is a re-emerging zoonotic disease of animals and humans caused by pathogenic Leptospira, which has major public health concerns. The study is aimed to express the recombinant outer membrane protein (OMP) A-like protein (rLoa22) and transmembrane (rOmpL37) protein of Leptospira interrogans serovar Hardjo in the Escherichia coli and their evaluation as a diagnostic antigen in the latex agglutination test (LAT) to detect anti-leptospiral antibodies in the sera of animals. The Loa22 and OmpL37 genes lacking signal peptide coding sequences were individually amplified (522 and 963 bp), by polymerase chain reaction, and directionally cloned into a pETite N-His Kan vector for expression. The expressed purified proteins were characterized by sodium dodecyl sulphate-polyacrylamide gel electrophoresis and immunoblot, which confirmed leptospiral specific reactive protein with a molecular weight of ~19 and 36 kDa, respectively. The sensitized latex beads coated with these OM proteins separately were evaluated in LAT using cattle sera of microscopic agglutination test (MAT) confirmed positive (n = 53) and negative (n = 52) cases of leptospirosis. The rLoa22 LAT and rOmpL37 LAT revealed the relative diagnostic sensitivity of 94·34 and 96·23%, diagnostic specificity of 92·31 and 96·15% and accuracy of 93·33 and 96·19%, with the excellent agreement of Cohen's kappa value of 0·87 and 0·92, respectively. After extensive evaluation, this rapid recombinant protein-based field diagnostic test can be applied as a screening test for the detection of anti-leptospiral antibodies in the sera of animals in the field conditions.