Measurement of $\itΛ_\it{b}^0$, $\itΛ_\it{c}^+$ and $\itΛ$ decay parameters using $\itΛ_\it{b}^0 \to \itΛ_\it{c}^+ h^-$ decays
LHCb collaboration R. Aaij A. S. W. Abdelmotteleb C. Abellan Beteta F. Abudinén T. Ackernley A. A. Adefisoye B. Adeva M. Adinolfi P. Adlarson C. Agapopoulou C. A. Aidala Z. Ajaltouni S. Akar K. Akiba P. Albicocco J. Albrecht F. Alessio M. Alexander Z. Aliouche P. Alvarez Cartelle R. Amalric S. Amato J. L. Amey Y. Amhis L. An L. Anderlini M. Andersson A. Andreianov P. Andreola M. Andreotti D. Andreou A. Anelli D. Ao F. Archilli M. Argenton S. Arguedas Cuendis A. Artamonov M. Artuso E. Aslanides R. Ataide Da Silva M. Atzeni B. Audurier D. Bacher I. Bachiller Perea S. Bachmann M. Bachmayer J. J. Back P. Baladron Rodriguez V. Balagura W. Baldini L. Balzani H. Bao J. Baptista de Souza Leite C. Barbero Pretel M. Barbetti I. R. Barbosa R. J. Barlow M. Barnyakov S. Barsuk W. Barter M. Bartolini J. Bartz J. M. Basels S. Bashir G. Bassi B. Batsukh P. B. Battista A. Bay A. Beck M. Becker F. Bedeschi I. B. Bediaga N. B. Behling S. Belin V. Bellee K. Belous I. Belov I. Belyaev G. Benane G. Bencivenni E. Ben-Haim A. Berezhnoy R. Bernet S. Bernet Andres A. Bertolin C. Betancourt F. Betti J. Bex Ia. Bezshyiko J. Bhom M. S. Bieker N. V. Biesuz P. Billoir A. Biolchini M. Birch F. C. R. Bishop A. Bitadze A. Bizzeti T. Blake F. Blanc J. E. Blank S. Blusk V. Bocharnikov J. A. Boelhauve O. Boente Garcia T. Boettcher A. Bohare A. Boldyrev C. S. Bolognani R. Bolzonella N. Bondar A. Bordelius F. Borgato S. Borghi M. Borsato J. T. Borsuk S. A. Bouchiba M. Bovill T. J. V. Bowcock A. Boyer C. Bozzi A. Brea Rodriguez N. Breer J. Brodzicka A. Brossa Gonzalo J. Brown D. Brundu E. Buchanan A. Buonaura L. Buonincontri A. T. Burke C. Burr A. Butkevich J. S. Butter J. Buytaert W. Byczynski S. Cadeddu H. Cai A. C. Caillet R. Calabrese S. Calderon Ramirez L. Calefice S. Cali M. Calvi M. Calvo Gomez P. Camargo Magalhaes J. I. Cambon Bouzas P. Campana D. H. Campora Perez A. F. Campoverde Quezada S. Capelli L. Capriotti R. Caravaca-Mora A. Carbone L. Carcedo Salgado R. Cardinale A. Cardini P. Carniti L. Carus A. Casais Vidal R. Caspary G. Casse J. Castro Godinez M. Cattaneo G. Cavallero V. Cavallini S. Celani D. Cervenkov S. Cesare A. J. Chadwick I. Chahrour M. Charles Ph. Charpentier E. Chatzianagnostou C. A. Chavez Barajas M. Chefdeville C. Chen S. Chen Z. Chen A. Chernov S. Chernyshenko X. Chiotopoulos V. Chobanova S. Cholak M. Chrzaszcz A. Chubykin V. Chulikov P. Ciambrone X. Cid Vidal G. Ciezarek P. Cifra P. E. L. Clarke M. Clemencic H. V. Cliff J. Closier C. Cocha Toapaxi V. Coco J. Cogan E. Cogneras L. Cojocariu P. Collins T. Colombo M. C. Colonna A. Comerma-Montells L. Congedo A. Contu N. Cooke I. Corredoira A. Correia G. Corti J. J. Cottee Meldrum B. Couturier D. C. Craik M. Cruz Torres E. Curras Rivera R. Currie C. L. Da Silva S. Dadabaev L. Dai X. Dai E. Dall'Occo J. Dalseno C. D'Ambrosio J. Daniel A. Danilina P. d'Argent A. Davidson J. E. Davies A. Davis O. De Aguiar Francisco C. De Angelis F. De Benedetti J. de Boer K. De Bruyn S. De Capua M. De Cian U. De Freitas Carneiro Da Graca E. De Lucia J. M. De Miranda L. De Paula M. De Serio P. De Simone F. De Vellis J. A. de Vries F. Debernardis D. Decamp V. Dedu S. Dekkers L. Del Buono B. Delaney H. -P. Dembinski J. Deng V. Denysenko O. Deschamps F. Dettori B. Dey P. Di Nezza I. Diachkov S. Didenko S. Ding L. Dittmann V. Dobishuk A. D. Docheva C. Dong A. M. Donohoe F. Dordei A. C. dos Reis A. D. Dowling W. Duan P. Duda M. W. Dudek L. Dufour V. Duk P. Durante M. M. Duras J. M. Durham O. D. Durmus A. Dziurda A. Dzyuba S. Easo E. Eckstein U. Egede A. Egorychev V. Egorychev S. Eisenhardt E. Ejopu L. Eklund M. Elashri J. Ellbracht S. Ely A. Ene E. Epple J. Eschle S. Esen T. Evans F. Fabiano L. N. Falcao Y. Fan B. Fang L. Fantini M. Faria K. Farmer D. Fazzini L. Felkowski M. Feng M. Feo A. Fernandez Casani M. Fernandez Gomez A. D. Fernez F. Ferrari F. Ferreira Rodrigues M. Ferrillo M. Ferro-Luzzi S. Filippov R. A. Fini M. Fiorini K. M. Fischer D. S. Fitzgerald C. Fitzpatrick F. Fleuret M. Fontana L. F. Foreman R. Forty D. Foulds-Holt M. Franco Sevilla M. Frank E. Franzoso G. Frau C. Frei D. A. Friday J. Fu Q. Fuehring Y. Fujii T. Fulghesu E. Gabriel G. Galati M. D. Galati A. Gallas Torreira D. Galli S. Gambetta M. Gandelman P. Gandini B. Ganie H. Gao R. Gao Y. Gao Y. Gao Y. Gao M. Garau L. M. Garcia Martin P. Garcia Moreno J. García Pardiñas K. G. Garg L. Garrido C. Gaspar R. E. Geertsema L. L. Gerken E. Gersabeck M. Gersabeck T. Gershon S. G. Ghizzo Z. Ghorbanimoghaddam L. Giambastiani F. I. Giasemis V. Gibson H. K. Giemza A. L. Gilman M. Giovannetti A. Gioventù L. Girardey P. Gironella Gironell C. Giugliano M. A. Giza E. L. Gkougkousis F. C. Glaser V. V. Gligorov C. Göbel E. Golobardes D. Golubkov A. Golutvin A. Gomes S. Gomez Fernandez F. Goncalves Abrantes M. Goncerz G. Gong J. A. Gooding I. V. Gorelov C. Gotti J. P. Grabowski L. A. Granado Cardoso E. Graugés E. Graverini L. Grazette G. Graziani A. T. Grecu L. M. Greeven N. A. Grieser L. Grillo S. Gromov C. Gu M. Guarise L. Guerry M. Guittiere V. Guliaeva P. A. Günther A. -K. Guseinov E. Gushchin Y. Guz T. Gys K. Habermann T. Hadavizadeh C. Hadjivasiliou G. Haefeli C. Haen J. Haimberger M. Hajheidari G. H. Hallett M. M. Halvorsen P. M. Hamilton J. Hammerich Q. Han X. Han S. Hansmann-Menzemer L. Hao N. Harnew M. Hartmann S. Hashmi J. He F. Hemmer C. Henderson R. D. L. Henderson A. M. Hennequin K. Hennessy L. Henry J. Herd P. Herrero Gascon J. Heuel A. Hicheur G. Hijano Mendizabal D. Hill S. E. Hollitt J. Horswill R. Hou Y. Hou N. Howarth J. Hu J. Hu W. Hu X. Hu W. Huang W. Hulsbergen R. J. Hunter M. Hushchyn D. Hutchcroft D. Ilin P. Ilten A. Inglessi A. Iniukhin A. Ishteev K. Ivshin R. Jacobsson H. Jage S. J. Jaimes Elles S. Jakobsen E. Jans B. K. Jashal A. Jawahery V. Jevtic E. Jiang X. Jiang Y. Jiang Y. J. Jiang M. John A. John Rubesh Rajan D. Johnson C. R. Jones T. P. Jones S. Joshi B. Jost J. Juan Castella N. Jurik I. Juszczak D. Kaminaris S. Kandybei M. Kane Y. Kang C. Kar M. Karacson D. Karpenkov A. Kauniskangas J. W. Kautz F. Keizer M. Kenzie T. Ketel B. Khanji A. Kharisova S. Kholodenko G. Khreich T. Kirn V. S. Kirsebom O. Kitouni S. Klaver N. Kleijne K. Klimaszewski M. R. Kmiec S. Koliiev L. Kolk A. Konoplyannikov P. Kopciewicz P. Koppenburg M. Korolev I. Kostiuk O. Kot S. Kotriakhova A. Kozachuk P. Kravchenko L. Kravchuk M. Kreps P. Krokovny W. Krupa W. Krzemien O. K. Kshyvanskyi J. Kubat S. Kubis M. Kucharczyk V. Kudryavtsev E. Kulikova A. Kupsc B. K. Kutsenko D. Lacarrere P. Laguarta Gonzalez A. Lai A. Lampis D. Lancierini C. Landesa Gomez J. J. Lane R. Lane G. Lanfranchi C. Langenbruch J. Langer O. Lantwin T. Latham F. Lazzari C. Lazzeroni R. Le Gac H. Lee R. Lefèvre A. Leflat S. Legotin M. Lehuraux E. Lemos Cid O. Leroy T. Lesiak B. Leverington A. Li C. Li H. Li K. Li L. Li P. Li P. -R. Li Q. Li S. Li T. Li T. Li Y. Li Y. Li Z. Lian X. Liang S. Libralon C. Lin T. Lin R. Lindner V. Lisovskyi R. Litvinov F. L. Liu G. Liu K. Liu S. Liu W. Liu Y. Liu Y. Liu Y. L. Liu A. Lobo Salvia A. Loi J. Lomba Castro T. Long J. H. Lopes A. Lopez Huertas S. López Soliño Q. Lu C. Lucarelli D. Lucchesi M. Lucio Martinez V. Lukashenko Y. Luo A. Lupato E. Luppi K. Lynch X. -R. Lyu G. M. Ma R. Ma S. Maccolini F. Machefert F. Maciuc B. Mack I. Mackay L. M. Mackey L. R. Madhan Mohan M. M. Madurai A. Maevskiy D. Magdalinski D. Maisuzenko M. W. Majewski J. J. Malczewski S. Malde L. Malentacca A. Malinin T. Maltsev G. Manca G. Mancinelli C. Mancuso R. Manera Escalero D. Manuzzi D. Marangotto J. F. Marchand R. Marchevski U. Marconi E. Mariani S. Mariani C. Marin Benito J. Marks A. M. Marshall L. Martel G. Martelli G. Martellotti L. Martinazzoli M. Martinelli D. Martinez Santos F. Martinez Vidal A. Massafferri R. Matev A. Mathad V. Matiunin C. Matteuzzi K. R. Mattioli A. Mauri E. Maurice J. Mauricio P. Mayencourt J. Mazorra de Cos M. Mazurek M. McCann L. Mcconnell T. H. McGrath N. T. McHugh A. McNab R. McNulty B. Meadows G. Meier D. Melnychuk F. M. Meng M. Merk A. Merli L. Meyer Garcia D. Miao H. Miao M. Mikhasenko D. A. Milanes A. Minotti E. Minucci T. Miralles B. Mitreska D. S. Mitzel A. Modak R. A. Mohammed R. D. Moise S. Mokhnenko T. Mombächer M. Monk S. Monteil A. Morcillo Gomez G. Morello M. J. Morello M. P. Morgenthaler A. B. Morris A. G. Morris R. Mountain H. Mu Z. M. Mu E. Muhammad F. Muheim M. Mulder K. Müller F. Muñoz-Rojas R. Murta P. Naik T. Nakada R. Nandakumar T. Nanut I. Nasteva M. Needham N. Neri S. Neubert N. Neufeld P. Neustroev J. Nicolini D. Nicotra E. M. Niel N. Nikitin P. Nogarolli P. Nogga N. S. Nolte C. Normand J. Novoa Fernandez G. Nowak C. Nunez H. N. Nur A. Oblakowska-Mucha V. Obraztsov T. Oeser S. Okamura A. Okhotnikov O. Okhrimenko R. Oldeman F. Oliva M. Olocco C. J. G. Onderwater R. H. O'Neil D. Osthues J. M. Otalora Goicochea P. Owen A. Oyanguren O. Ozcelik F. Paciolla A. Padee K. O. Padeken B. Pagare P. R. Pais T. Pajero A. Palano M. Palutan G. Panshin L. Paolucci A. Papanestis M. Pappagallo L. L. Pappalardo C. Pappenheimer C. Parkes B. Passalacqua G. Passaleva D. Passaro A. Pastore M. Patel J. Patoc C. Patrignani A. Paul C. J. Pawley A. Pellegrino J. Peng M. Pepe Altarelli S. Perazzini D. Pereima H. Pereira Da Costa A. Pereiro Castro P. Perret A. Perro K. Petridis A. Petrolini J. P. Pfaller H. Pham L. Pica M. Piccini B. Pietrzyk G. Pietrzyk D. Pinci F. Pisani M. Pizzichemi V. Placinta M. Plo Casasus T. Poeschl F. Polci M. Poli Lener A. Poluektov N. Polukhina I. Polyakov E. Polycarpo S. Ponce D. Popov S. Poslavskii K. Prasanth C. Prouve V. Pugatch G. Punzi S. Qasim Q. Q. Qian W. Qian N. Qin S. Qu R. Quagliani R. I. Rabadan Trejo J. H. Rademacker M. Rama M. Ramírez García V. Ramos De Oliveira M. Ramos Pernas M. S. Rangel F. Ratnikov G. Raven M. Rebollo De Miguel F. Redi J. Reich F. Reiss Z. Ren P. K. Resmi R. Ribatti G. R. Ricart D. Riccardi S. Ricciardi K. Richardson M. Richardson-Slipper K. Rinnert P. Robbe G. Robertson E. Rodrigues E. Rodriguez Fernandez J. A. Rodriguez Lopez E. Rodriguez Rodriguez J. Roensch A. Rogachev A. Rogovskiy D. L. Rolf P. Roloff V. Romanovskiy M. Romero Lamas A. Romero Vidal G. Romolini F. Ronchetti T. Rong M. Rotondo S. R. Roy M. S. Rudolph T. Ruf M. Ruiz Diaz R. A. Ruiz Fernandez J. Ruiz Vidal A. Ryzhikov J. Ryzka J. J. Saavedra-Arias J. J. Saborido Silva R. Sadek N. Sagidova D. Sahoo N. Sahoo B. Saitta M. Salomoni C. Sanchez Gras I. Sanderswood R. Santacesaria C. Santamarina Rios M. Santimaria L. Santoro E. Santovetti A. Saputi D. Saranin A. S. Sarnatskiy G. Sarpis M. Sarpis C. Satriano A. Satta M. Saur D. Savrina H. Sazak L. G. Scantlebury Smead A. Scarabotto S. Schael S. Scherl M. Schiller H. Schindler M. Schmelling B. Schmidt S. Schmitt H. Schmitz O. Schneider A. Schopper N. Schulte S. Schulte M. H. Schune R. Schwemmer G. Schwering B. Sciascia A. Sciuccati S. Sellam A. Semennikov T. Senger M. Senghi Soares A. Sergi N. Serra L. Sestini A. Seuthe Y. Shang D. M. Shangase M. Shapkin R. S. Sharma I. Shchemerov L. Shchutska T. Shears L. Shekhtman Z. Shen S. Sheng V. Shevchenko B. Shi Q. Shi Y. Shimizu E. Shmanin R. Shorkin J. D. Shupperd R. Silva Coutinho G. Simi S. Simone N. Skidmore T. Skwarnicki M. W. Slater J. C. Smallwood E. Smith K. Smith M. Smith A. Snoch L. Soares Lavra M. D. Sokoloff F. J. P. Soler A. Solomin A. Solovev I. Solovyev R. Song Y. Song Y. Song Y. S. Song F. L. Souza De Almeida B. Souza De Paula E. Spadaro Norella E. Spedicato J. G. Speer E. Spiridenkov P. Spradlin V. Sriskaran F. Stagni M. Stahl S. Stahl S. Stanislaus E. N. Stein O. Steinkamp O. Stenyakin H. Stevens D. Strekalina Y. Su F. Suljik J. Sun L. Sun Y. Sun D. S. Sundfeld Lima W. Sutcliffe P. N. Swallow F. Swystun A. Szabelski T. Szumlak Y. Tan M. D. Tat A. Terentev F. Terzuoli F. Teubert E. Thomas D. J. D. Thompson H. Tilquin V. Tisserand S. T'Jampens M. Tobin L. Tomassetti G. Tonani X. Tong D. Torres Machado L. Toscano D. Y. Tou C. Trippl G. Tuci N. Tuning L. H. Uecker A. Ukleja D. J. Unverzagt E. Ursov A. Usachov A. Ustyuzhanin U. Uwer V. Vagnoni G. Valenti N. Valls Canudas H. Van Hecke E. van Herwijnen C. B. Van Hulse R. Van Laak M. van Veghel G. Vasquez R. Vazquez Gomez P. Vazquez Regueiro C. Vázquez Sierra S. Vecchi J. J. Velthuis M. Veltri A. Venkateswaran M. Vesterinen D. Vico Benet M. Vieites Diaz X. Vilasis-Cardona E. Vilella Figueras A. Villa P. Vincent F. C. Volle D. vom Bruch N. Voropaev K. Vos G. Vouters C. Vrahas J. Wagner J. Walsh E. J. Walton G. Wan C. Wang G. Wang J. Wang J. Wang J. Wang J. Wang M. Wang N. W. Wang R. Wang X. Wang X. Wang X. W. Wang Y. Wang Z. Wang Z. Wang Z. Wang J. A. Ward M. Waterlaat N. K. Watson D. Websdale Y. Wei J. Wendel B. D. C. Westhenry C. White M. Whitehead E. Whiter A. R. Wiederhold D. Wiedner G. Wilkinson M. K. Wilkinson M. Williams M. R. J. Williams R. Williams Z. Williams F. F. Wilson W. Wislicki M. Witek L. Witola C. P. Wong G. Wormser S. A. Wotton H. Wu J. Wu Y. Wu K. Wyllie S. Xian Z. Xiang Y. Xie A. Xu J. Xu L. Xu L. Xu M. Xu Z. Xu Z. Xu Z. Xu D. Yang K. Yang S. Yang X. Yang Y. Yang Z. Yang Z. Yang V. Yeroshenko H. Yeung H. Yin C. Y. Yu J. Yu X. Yuan Y Yuan E. Zaffaroni M. Zavertyaev M. Zdybal C. Zeng M. Zeng C. Zhang D. Zhang J. Zhang L. Zhang S. Zhang S. Zhang Y. Zhang Y. Z. Zhang Y. Zhao A. Zharkova A. Zhelezov S. Z. Zheng X. Z. Zheng Y. Zheng T. Zhou X. Zhou Y. Zhou V. Zhovkovska L. Z. Zhu X. Zhu X. Zhu V. Zhukov J. Zhuo Q. Zou D. Zuliani G. Zunica






















roman




EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN)



pdflatex

        

        


         CERN-EP-2024-200 
  
         LHCb-PAPER-2024-017 
  
         September 4, 2024 

         











  











[Authors are listed at the end of this paper.]







§ ABSTRACT 
  

A comprehensive study of the angular distributions in the bottom-baryon decays → h^-(h=π, K), followed by → h^+ with → or → decays, is performed 
using a data sample of proton-proton collisions corresponding to an integrated luminosity of 9 collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 .
The decay parameters and the associated charge-parity () asymmetries are measured,
with no significant violation observed.
For the first time, the → h^- decay parameters are measured.
The most precise measurements of the decay parameters α, β and γ are obtained for  decays and 
an independent measurement of the decay parameters for the strange-baryon  decay is provided.
The results deepen our understanding of weak decay dynamics in baryon decays.







  Submitted to
  Phys. Rev. Lett.








 . .


































































plain 

arabic










Hadronic weak decays of baryons provide an excellent platform for 
studying baryon decay dynamics and the origin of the asymmetry between matter and antimatter <cit.>.
Among them, the  decay of a spin-half baryon to a spin-half baryon and a pseudoscalar meson is of special interest. 
For this type of decay, three decay parameters, first proposed by Lee and Yang to search for parity violation <cit.>, can be defined as

    α≡2(s^*p)/|s|^2+|p|^2,   β≡2(s^*p)/|s|^2+|p|^2,  γ≡|s|^2-|p|^2/|s|^2+|p|^2 ,

satisfying α^2+β^2+γ^2=1,   where s and p denote the parity-violating S-wave and parity-conserving P-wave amplitudes, respectively.
The interference between the two amplitudes may
generate differences between the differential decay rates of baryons and antibaryons, allowing  -violation phenomena to be probed via  angular analyses <cit.>.
The amount of violation  can be quantified by the asymmetries
A_α=(α+α̅)/(α-α̅) and
R_β=(β+β̅)/(α-α̅), 
where α̅ and β̅ denote the decay parameters of the antibaryons, and should have signs opposite to their baryonic counterparts.
At leading order, these asymmetries are related to the weak and strong phase differences between the S- and P-wave amplitudes, Δϕ and Δδ, via the relations 
A_α=-tanΔδtanΔϕ and
R_β=tanΔϕ <cit.>.


Many phenomenological models have been used to calculate baryon decay parameters.
For some two-body beauty-baryon decays, factorization is assumed to hold in model calculations <cit.>, which predict that  , consistent with the V-A nature of the weak current and maximal parity violation.
For charm-baryon decays, model calculations are complicated by the presence of nonfactorizable contributions and often do not agree with each other <cit.>.
For strange-baryon decays, nonfactorizable  contributions may dominate, making  theoretical calculations even more challenging <cit.>.


Decay parameters have been measured for several  hyperon and charm-baryon decays <cit.>,
while beauty decays are much less explored.
The α parameter of the → decay was recently updated by the  <cit.> and CLAS <cit.> collaborations, which resulted in a significantly larger value compared to the previous world average <cit.>.
The α parameters of several decays were precisely measured by the FOCUS <cit.>,  <cit.> and  <cit.> collaborations,
while the precision of the β and γ measurements  is still very limited <cit.>.
To date, there is no 
decay parameter measurement  for any    decay to a baryon and a pseudoscalar meson, despite the observation of many such  decay modes.
The decay parameter of the → decay  was measured in proton-proton (pp) collisions at the  <cit.>,
together with the  polarization, which is  found to be consistent with zero.
Moreover, the photon polarization of the →γ decay was measured by LHCb <cit.>, suggesting the dominance of left-handed photons. 


In this Letter, the decay parameters and asymmetries of  and    decays are measured through an angular analysis.
Three   decays are analyzed:
→ p, 
→
and → with the subsequent decays → and →π^+π^-.
The decay parameters and associated asymmetries  of the 
,  and  decays are  determined simultaneously.
The analysis is performed using data from pp collisions at center-of-mass energies of =7, 8  and 13, 
corresponding to an integrated luminosity of 9 collected with the detector.  Inclusion of charge-conjugate processes is implied, unless otherwise stated. 


The LHCb detector, designed for the study of particles containing  or  quarks, is a single-arm forward spectrometer covering the pseudorapidity range 2 < η < 5, described in detail in Refs. <cit.>. 
The online event selection for decays is performed by a trigger <cit.>, which consists of a hardware stage followed by a  software stage <cit.>.
The hardware trigger requires a muon with high transverse momentum or a hadron, photon or electron with high transverse energy in the calorimeters.
The software trigger requires a
two-, three- or four-track secondary vertex with a significant displacement from any primary vertex (PV).


Simulated samples of  decays are produced to optimize event selection, study potential backgrounds and model the detector acceptance.
These samples are generated using the software described in Refs. <cit.>. 
The products of each decay in the  cascades are distributed uniformly in the allowed phase space.


In the offline selection, all tracks in the final state are required to have a  large transverse momentum and be inconsistent with being directly produced from any PV.
The and candidates are reconstructed using → and → decays, 
where the final-state tracks are required to form a vertex with a good fit quality that is significantly displaced from any PV, 
and their invariant mass is consistent with the known value <cit.>.
The () candidate is combined with a kaon/pion (proton) track to form the  candidate.
The invariant mass is required to be within ±26 (20) of the known value <cit.> for the → and → (→) decays. The smaller mass region for the → decay is used to suppress the →(→γ) background, where the photon is not reconstructed.
The candidate is formed by combining a candidate with a kaon or pion. 
The  invariant mass, m( h^-), is required to be larger than 5500 to reject background due to partially reconstructed decays.


Two types of background peaking in the signal mass region are identified.
For the first type,  or  mesons are observed in the invariant-mass distributions of the two charged companion tracks of  and  decays.
The second type involves a genuine  () decay reconstructed as the  () decay.
These background candidates are suppressed using information from particle identification (PID) detectors or rejected by specific vetoes in the corresponding mass spectra.
A boosted decision tree (BDT) classifier implemented in the TMVA toolkit <cit.> is then used to  separate the signal from the background of random combinations of final-state particles.
The BDT analysis is performed independently for → p and → h^+ decays.
Each BDT classifier is trained on simulated signal decays and background from data in the high-mass region m( h^-)>5900, 
using a combination of kinematic, topological and isolation variables of the , ,  or  hadrons.
In the final stage of the event selection,
a simultaneous optimization of   the final-state PID and BDT classifier requirements is performed to maximize the figure of merit, N_S^2/(N_S+N_B)^3/2,
chosen to favour a high signal purity with small decay-parameter uncertainties.
Here, 
N_S and N_B represent the signal and background yields in the signal region chosen to be ±32 around the known mass <cit.>, estimated with simulated signal decays and data in the high-mass region.
The invariant mass is calculated with a kinematic fit <cit.> constraining the masses of all intermediate particles to their known values
and the momentum to point back to its best-matched PV.


The invariant-mass distributions of the five significant  cascade decays to 
(), (), (), () and () final states,
where decay products are shown in brackets, 
are shown in Fig. <ref> for candidates passing all selection criteria.
The signal yields of the five decays are determined  to be
(8.635± 0.032)×10^4, (4.16±0.07)×10^3, (2.475±0.017)×10^4, (1.19±0.04)×10^3 and (1.010±0.034)×10^3, respectively, from 
unbinned maximum-likelihood fits performed to the mass distributions.
The signal component is described by a  Hypatia function <cit.> and
the combinatorial background by an exponential function. 
The → decay misidentified as → decay, or vice versa, is also modelled by a Hypatia function,
whose parameters are fixed to those obtained from the simulated samples.
The relative yields of these cross-feed contributions are constrained using relative experimental efficiencies.
For every decay mode, the fit result is used to determine the weight for each candidate <cit.>, applied to subtract the background for the subsequent angular analysis.





The decay parameters are determined by analyzing the angular distributions of the  cascade decays.
The angular variables are calculated with the
invariant mass constrained to the known value <cit.>.
The kinematics of the three-step cascade decays are fully described by five angular variables
Ω≡(θ_0,θ_1,ϕ_1,θ_2,ϕ_2), depicted in Fig. <ref>.
The variable θ_0 is the polar angle between the normal P⃗_z of the production plane formed by the beam and  momenta in the laboratory frame, 
and the  momentum p⃗_ in the  rest frame.
The variable θ_1 (θ_2) is the polar angle between p⃗_ (p⃗_) and p⃗_, where particle momenta are defined in the rest frames of the  () and  baryons, respectively.
The variable ϕ_1 (ϕ_2) is the angle between the () decay plane and the decay plane, spanned by the momenta of their respective decay products.
Similarly, for the two-step cascade decays, , the kinematics are described by three angular variables
Ω≡(θ_0,θ_1,ϕ_1), which are the same as the first three variables of the three-step cascade.





The angular distributions can be expanded through the helicity formalism <cit.>.
Based on previous studies at the LHC <cit.>,
the  baryon is considered to be unpolarized, 
in which case the angular distributions become uniform in θ_0 and ϕ_1.
The impact of  polarization is considered as a source of systematic uncertainty.
The reduced angular distributions are thus expressed as

    d^3Γ/dcosθ_1dcosθ_2dϕ_2∝    (1+cosθ_1
    	+cosθ_2
    	+cosθ_1cosθ_2
       -sinθ_1sinθ_2cosϕ_2
        +sinθ_1sinθ_2sinϕ_2),

for  decays,
and

    dΓ/dcosθ_1∝ 
    	1+cosθ_1,

for decays,
where the subscript of the decay parameters denotes the decaying particle.
The decay parameters in this analysis
are determined from simultaneous unbinned maximum-likelihood fits to the five  () cascade decays,
imposing the constraint  ()^2 + ()^2 + ()^2 = 1. 
The  and parameters are related to the and parameters by 
= √(1 - ()^2) sin, = √(1 - ()^2) cos, 
where is the phase difference between the two helicity amplitudes of the → h^+ decay.
This leads to two equivalent sets of fit parameters for a → h^+ decay.
The fit is performed for each set of parameters independently to directly determine their values and uncertainties.
To test violation, an additional joint fit of and samples is applied with -related fit parameters, which are the asymmetries A_α, R_β, and averages , .
At leading order, the weak and strong phase differences are determined using R_β=tanΔϕ and R'_β=tanΔδ <cit.>.



The logarithm of the likelihood function (logℒ) is constructed as

    logℒ(ν) = ∑_k=1^5(
        𝒞_k 
        ∑_i=1^N_kw_k,i×log[ 𝒫_k(Ω_k^i|ν)]),

where ν is the set of decay parameters, Ω is the set of angular variables,
and 𝒫(Ω|ν)  represents the signal probability density function (PDF).
The subscript k runs over the five   cascade decays, 
and the subscript i runs over all the N_k candidates of the k-th decay.
The weight w_k,i in the logℒ is used to remove the contribution of background candidates <cit.>, while
the constants 𝒞_k≡∑_i∈data_kw_k,i/∑_i∈data_kw_k,i^2 are scale factors needed to correct the obtained statistical uncertainties <cit.>.
The signal PDF 𝒫_k(Ω_k|ν)  is formulated as

    𝒫_k(Ω_k|ν) = ϵ_k(Ω_k) · f_k(Ω⃗_k|ν)/∫dΩ_k ϵ_k(Ω_k) · f_k(Ω⃗_k|ν),

where f_k(Ω⃗_k|ν) represents the angular distribution given in 
Eq. <ref> or <ref>,
and ϵ_k(Ω_k) is the angular acceptance. 
The denominator is calculated numerically using the Monte Carlo integration method <cit.>
beginning with the corresponding simulated signal decays after full selection.
The distributions of the  transverse momentum and pseudorapidity, and the number of
tracks per event in the simulation samples are corrected to match those in data.
In Fig. <ref>, the angular distributions of   and  decays are shown, superimposed by the fit result. 
Distributions for all decays are provided in Ref. <cit.>.
A binned  test between the data and the fit gives a p-value of 28%.





Various sources of systematic uncertainty on the decay parameters are studied.
Possible biases introduced by the angular fit method are evaluated using pseudoexperiments. Mass and angular distributions of pseudosamples are generated according to the baseline fit results, and then the whole fit procedure is repeated to extract decay parameters.
The parameter's systematic uncertainty is taken to be the mean of its pull distribution times its nominal statistical uncertainty.
The method is used to subtract the background, 
hence the choice of the invariant-mass fit model introduces systematic uncertainties.
These are estimated by repeating the invariant-mass fit with alternative fit models,
including alternative descriptions of mass-shape functions and removing the constraints on yields,
then using the corresponding updated weights to determine decay parameters.
As the PID variables in simulation samples are calibrated to match data <cit.>, 
the uncertainty on the calibration procedure introduces systematic uncertainties which are estimated with alternative calibration configurations. 
The limited size of simulation samples introduces an uncertainty on the efficiency propagated to the decay parameters, 
which is estimated with bootstrapped pseudoexperiments <cit.>. 
The influence of the production asymmetry for  baryons and detection asymmetries on the final-state particles <cit.> are taken into account.
Following the prescription of measurements <cit.>,
these asymmetries are introduced in the angular acceptance, 
and the angular fit is repeated to verify their impact on the measurements. 
The polarization of baryons is considered as a source of systematic uncertainty.
The angular fit is repeated with additional terms in the PDF incorporating the transverse polarization measured by  <cit.>
(see appendix for details on this PDF).
The impact of the experimental angular resolution is considered as a systematic uncertainty and found to be negligible.
The spin of the baryon undergoes a precession in the magnetic field of the detector, 
which modifies its angular distribution depending on the decay length <cit.>.
The systematic uncertainty arising from the precession is examined using pseudoexperiments,
and found to be negligible.
A summary of the contributions from the various sources is given in Ref. <cit.>.
The systematic uncertainties from different sources are added in quadrature, 
resulting in totals that are smaller than the statistical uncertainties.








The results are listed in Table <ref> for the α parameters of , and decays, 
and in Table <ref> for the β and γ parameters of → h^+ decays.
The -related parameters are also obtained,
and no violation is found.
This is the first measurement of the parity-violating parameters of two-body decays into a spin-half baryon and a pseudoscalar meson.
The results of the decay parameters  are close to -1, 
suggesting that baryons in → h^- decays are almost fully longitudinally polarized, which corresponds to the V-A nature of weak decays and supports the factorization hypothesis in theoretical calculations <cit.>.
The  decay parameters are consistent with, and more precise than, the  <cit.> and  <cit.> results.
The  parameters are found to significantly deviate from -1, which may suggest that nonfactorizable contributions are substantial in hadronic decays of charm baryons.
The β, γ and Δ parameters of → h^+ decays are precisely measured for the first time, 
and will serve as essential inputs to theoretical models <cit.>.
The weak and strong phase differences are determined to be
Δϕ=0.01± 0.02  and Δδ =-0.448± 0.017  for the → decay,
and Δϕ=-0.03± 0.15  and Δδ =-0.57± 0.19 for the → decay,
where a possible ambiguity of +π rad due to the inverse of tangent function is not included.
The α parameter and the corresponding asymmetry of the → decay in this analysis are consistent with the results <cit.>.


In conclusion, based on pp collision data collected by the experiment, corresponding to an integrated luminosity of 9,
a comprehensive study of the angular distributions in cascade decays
is performed.
The analysis provides the first measurements of the decay parameters for → h^- decays, and the most precise measurements for the  decay parameters.  
The weak and strong phase differences for → h^+ decays are also determined.
The asymmetries are studied between the decay parameters of baryon and antibaryon decays, and no hint of violation is observed.
The results provide valuable insights into the weak decay dynamics of baryons.







§ ACKNOWLEDGEMENTS




We express our gratitude to our colleagues in the CERN
accelerator departments for the excellent performance of the LHC. We
thank the technical and administrative staff at the LHCb
institutes.
We acknowledge support from CERN and from the national agencies:
CAPES, CNPq, FAPERJ and FINEP (Brazil); 
MOST and NSFC (China); 
CNRS/IN2P3 (France); 
BMBF, DFG and MPG (Germany); 
INFN (Italy); 
NWO (Netherlands); 
MNiSW and NCN (Poland); 
MCID/IFA (Romania); 

MICIU and AEI (Spain);
SNSF and SER (Switzerland); 
NASU (Ukraine); 
STFC (United Kingdom); 
DOE NP and NSF (USA).
We acknowledge the computing resources that are provided by CERN, IN2P3
(France), KIT and DESY (Germany), INFN (Italy), SURF (Netherlands),
PIC (Spain), GridPP (United Kingdom), 

CSCS (Switzerland), IFIN-HH (Romania), CBPF (Brazil),
and Polish WLCG (Poland).
We are indebted to the communities behind the multiple open-source
software packages on which we depend.
Individual groups or members have received support from
ARC and ARDC (Australia);
Key Research Program of Frontier Sciences of CAS, CAS PIFI, CAS CCEPP, 
Fundamental Research Funds for the Central Universities, 
and Sci. & Tech. Program of Guangzhou (China);
Minciencias (Colombia);
EPLANET, Marie Skłodowska-Curie Actions, ERC and NextGenerationEU (European Union);
A*MIDEX, ANR, IPhU and Labex P2IO, and Région Auvergne-Rhône-Alpes (France);

AvH Foundation (Germany);
ICSC (Italy); 

Severo Ochoa and María de Maeztu Units of Excellence, GVA, XuntaGal, GENCAT, InTalent-Inditex and Prog.  Atracción Talento CM (Spain);
SRC (Sweden);
the Leverhulme Trust, the Royal Society
 and UKRI (United Kingdom).








§ END MATTER



§ ANGULAR DISTRIBUTIONS


The helicity formalism is employed to describe the angular distributions of the decays in this Letter.
For the decay of a spin-half baryon to a spin-half baryon and a pseudoscalar
meson, two helicity amplitudes are involved with the respective couplings H_±, 
where the subscript represents the sign of the helicity of the final-state spin-half baryon.
The helicity couplings are related to the S-wave (s) and P-wave (p) couplings as s=(H_+ + H_-)/√(2) and p=(H_+-H_-)/√(2).
The decay parameters are defined using the helicity amplitudes as

    α = |H_+|^2 - |H_-|^2/|H_+|^2 + |H_-|^2,  β = √(1 - α^2)sinΔ,  γ = √(1 - α^2)cosΔ,

where Δ = (H_+ / H_-) is the phase angle difference between the two helicity amplitudes.


The angular distribution  is determined by the sum of all possible helicity  amplitudes as 

    dΓ/dΩ∝ |M|^2 = ∑_λ_0, λ'_0, λ_nρ_λ_0, λ'_0 M_λ_0, λ_n M^*_λ'_0, λ_n,

where λ_0^(') and λ_n run over the helicities of the initial and final baryons, ρ_λ_0, λ'_0 is the polarization density matrix of the decaying baryon,
and M_λ_0, λ_n, M^*_λ'_0, λ_n are the amplitude matrix elements.

For the baryon promptly produced  in pp collisions, 
the possible polarization is expected to be perpendicular to the production plane due to parity conservation in strong interactions. 
Defining the polarization axis as the z-axis, and the magnitude of the polarization as P_z, 
the polarization  density matrix is expressed as

    ρ = [ 1 + P_z       0;       0   1-P_z ].







 §.§ Angular distribution for  decays


For decays,
the helicity amplitude is determined as

    M_λ_b, λ_ = ∑_λ_c H^b_λ_c d^1/2_λ_b, λ_c(θ_0) ·
        H^c_λ_ e^iλ_cϕ_1 d^1/2_λ_c, λ_(θ_1),

where d^J_λ, λ'(θ) is the Wigner d-matrix,
λ_b, λ_c and λ_ refer to the helicities of , and baryons, and
H^b_λ_c and H^c_λ_ are the helicity couplings of and decays.
The total amplitude squared is calculated by 

    |M|^2 ∝∑_λ_[ (1 + P_z) · |M_1/2, λ_|^2 + (1 - P_z) · |M_-1/2, λ_|^2],

which leads to

    d^3Γ/dcosθ_0dcosθ_1dϕ_1∝      1+cosθ_1
       +P_z· (cosθ_0+cosθ_0cosθ_1
       -sinθ_0sinθ_1cosϕ_1
       +sinθ_0sinθ_1sinϕ_1),

where ,, are the  decay parameters defined by H_±^b, and
 is the  decay parameter related to H_±^c. 






 §.§ Angular distribution for   decays


For decays,
the relevant  angles are (θ_0, θ_1, ϕ_1, θ_2, ϕ_2), which are defined in Fig. <ref>.
The helicity amplitude is expressed as

    M_λ_b, λ_ = ∑_λ_c H^b_λ_c d^1/2_λ_b, λ_c(θ_0) ·
        H^c_λ_s e^iλ_cϕ_1 d^1/2_λ_c, λ_s(θ_1) ·
        H^s_λ_ e^iλ_sϕ_2 d^1/2_λ_s, λ_(θ_2),

where λ_s refers to the helicity of baryons, and 
H^c_λ_s and H^s_λ_ are the helicity couplings of and decays.
The total amplitude is calculated by Eq. <ref>, which leads to

    d^5Γ/dcosθ_0dcosθ_1dϕ_1dcosθ_2dϕ_2
    ∝     (1+cosθ_1
    	+cosθ_2
    	+cosθ_1cosθ_2
       -sinθ_1sinθ_2cosϕ_2
        +sinθ_1sinθ_2sinϕ_2)
    
    	+P_z   · (cosθ_0
    	+cosθ_0cosθ_1
    	+cosθ_0cosθ_2
       +cosθ_0cosθ_1cosθ_2
    	-sinθ_0sinθ_1cosϕ_1
    	+sinθ_0sinθ_1sinϕ_1
       -cosθ_0sinθ_1sinθ_2cosϕ_2
    	+cosθ_0sinθ_1sinθ_2sinϕ_2
       -sinθ_0sinθ_1cosθ_2cosϕ_1
    	+sinθ_0sinθ_1cosθ_2sinϕ_1
       +sinθ_0sinθ_2cosϕ_1cosϕ_2
        +sinθ_0sinθ_2cosϕ_1sinϕ_2
       +sinθ_0sinθ_2sinϕ_1cosϕ_2
        +sinθ_0sinθ_2sinϕ_1sinϕ_2
       -sinθ_0cosθ_1sinθ_2cosϕ_1cosϕ_2
       +sinθ_0cosθ_1sinθ_2cosϕ_1sinϕ_2
       +sinθ_0cosθ_1sinθ_2sinϕ_1cosϕ_2
       -sinθ_0cosθ_1sinθ_2sinϕ_1sinϕ_2),

where 
 is the  decay parameter related to H_±^s.









tocsectionReferences

LHCb




§ PRL JUSTIFICATION


This letter presents a comprehensive study of parity and charge-parity () violation in decays of bottom, charm and strange baryons using the angular analysis method initially proposed by T.D. Lee and C.N. Yang.  The major results include the first measurement of the decay parameters for → h^+ (h=K,π) decays, the most precise determinations of the decay parameters α,β, γ
for →Λ^0 h^+ (h=K,π) decays, α for → decay
and the associated asymmetries, as well as an independent confirmation of the decay parameter 
α (Λ^0→ pπ^-) measured by the BESIII experiment, which was significantly higher than  the previous world average. 
These results support the factorization hypothesis in theoretical calculations of beauty baryon hadronic decays, and indicate the importance of nonfactorizable contributions in hadronic decays of charm baryons.
This is the first study of its kind at and at a hadron collider, demonstrating ’s great potential to study violation in baryon decays via the angular analysis approach. 




 §.§ Word count


    
  * Text (captions included): 3022
    
  * Math display: 128
    
  * Tables: 188.5
    
  * Figures: 431
    
  * All: 3770












 
Supplemental material


§ SUMMARY OF SYSTEMATIC UNCERTAINTIES

The various sources of systematic uncertainties on the decay parameter measurements, including fit procedure, mass fit model, PID calibration, limited size of simulation samples, production and detection asymmetries and polarization, are summarized in Table <ref>, Table <ref> and Table <ref>.
The total systematic uncertainties correspond to the sum in quadrature of all sources.










§ PROJECTIONS OF ANGULAR DISTRIBUTIONS


Projections of angular distributions and fit results for various decays studied in the Letter are shown in Figs. <ref>, <ref>, <ref>, <ref> and <ref>.














§ CORRELATION MATRICES FOR PARAMETERS


Correlation matrices between decay parameters without accounting for systematic uncertainties are provided in Tables <ref>-<ref>.
The correlation matrix between -related parameters is provided in Table <ref>.















Correlation matrix for the -related parameters.
!


                                                                 

    1.000     -0.033     0.159     -0.013     -0.326     0.030     0.026     -0.153     -0.057     0.018     0.009     -0.025     -0.668     0.025     0.405     0.044 

        1.000     -0.007     0.158     -0.026     -0.326     -0.097     -0.031     -0.022     -0.054     -0.010     -0.014     -0.011     -0.666     -0.032     -0.404 

            1.000     -0.164     -0.077     0.036     -0.017     -0.029     -0.004     -0.009     -0.002     -0.004     -0.214     0.001     -0.101     -0.001 

                1.000     -0.039     -0.078     -0.015     -0.024     -0.004     -0.009     -0.002     -0.003     -0.005     -0.213     -0.000     -0.100 

                    1.000     -0.023     -0.020     -0.531     0.019     -0.007     -0.003     -0.005     0.220     -0.022     -0.122     -0.012 

                        1.000     0.367     0.005     0.018     0.008     0.003     0.005     0.019     0.219     0.009     0.122 

                            1.000     0.043     -0.010     0.004     0.002     0.004     -0.102     -0.015     0.065     0.010 

                                1.000     -0.010     0.001     0.002     0.003     -0.018     0.023     0.065     0.015 

                                    1.000     0.095     -0.077     -0.428     0.038     -0.015     -0.033     -0.017 

                                        1.000     0.147     0.025     0.011     0.036     0.013     0.032 

                                            1.000     0.188     0.006     0.036     0.010     0.010 

                                                1.000     -0.017     0.009     0.013     0.015 

                                                    1.000     -0.005     -0.275     -0.023 

                                                        1.000     0.021     0.273 

                                                            1.000     0.046 

                                                                1.000 








 



LHCb collaboration


R. Aaij^360000-0003-0533-1952,
A.S.W. Abdelmotteleb^550000-0001-7905-0542,
C. Abellan Beteta^49,
F. Abudinén^550000-0002-6737-3528,
T. Ackernley^590000-0002-5951-3498,
A. A.  Adefisoye^670000-0003-2448-1550,
B. Adeva^450000-0001-9756-3712,
M. Adinolfi^530000-0002-1326-1264,
P. Adlarson^800000-0001-6280-3851,
C. Agapopoulou^130000-0002-2368-0147,
C.A. Aidala^810000-0001-9540-4988,
Z. Ajaltouni^11,
S. Akar^640000-0003-0288-9694,
K. Akiba^360000-0002-6736-471X,
P. Albicocco^260000-0001-6430-1038,
J. Albrecht^180000-0001-8636-1621,
F. Alessio^470000-0001-5317-1098,
M. Alexander^580000-0002-8148-2392,
Z. Aliouche^610000-0003-0897-4160,
P. Alvarez Cartelle^540000-0003-1652-2834,
R. Amalric^150000-0003-4595-2729,
S. Amato^30000-0002-3277-0662,
J.L. Amey^530000-0002-2597-3808,
Y. Amhis^13,470000-0003-4282-1512,
L. An^60000-0002-3274-5627,
L. Anderlini^250000-0001-6808-2418,
M. Andersson^490000-0003-3594-9163,
A. Andreianov^420000-0002-6273-0506,
P. Andreola^490000-0002-3923-431X,
M. Andreotti^240000-0003-2918-1311,
D. Andreou^670000-0001-6288-0558,
A. Anelli^29,o0000-0002-6191-934X,
D. Ao^70000-0003-1647-4238,
F. Archilli^35,u0000-0002-1779-6813,
M. Argenton^240009-0006-3169-0077,
S. Arguedas Cuendis^9,470000-0003-4234-7005,
A. Artamonov^420000-0002-2785-2233,
M. Artuso^670000-0002-5991-7273,
E. Aslanides^120000-0003-3286-683X,
R. Ataíde Da Silva^480009-0005-1667-2666,
M. Atzeni^630000-0002-3208-3336,
B. Audurier^140000-0001-9090-4254,
D. Bacher^620000-0002-1249-367X,
I. Bachiller Perea^100000-0002-3721-4876,
S. Bachmann^200000-0002-1186-3894,
M. Bachmayer^480000-0001-5996-2747,
J.J. Back^550000-0001-7791-4490,
P. Baladron Rodriguez^450000-0003-4240-2094,
V. Balagura^140000-0002-1611-7188,
W. Baldini^240000-0001-7658-8777,
L. Balzani^180009-0006-5241-1452,
H.  Bao^70009-0002-7027-021X,
J. Baptista de Souza Leite^590000-0002-4442-5372,
C. Barbero Pretel^45,820009-0001-1805-6219,
M. Barbetti^25,l0000-0002-6704-6914,
I. R. Barbosa^680000-0002-3226-8672,
R.J. Barlow^610000-0002-8295-8612,
M. Barnyakov^230009-0000-0102-0482,
S. Barsuk^130000-0002-0898-6551,
W. Barter^570000-0002-9264-4799,
M. Bartolini^540000-0002-8479-5802,
J. Bartz^670000-0002-2646-4124,
J.M. Basels^160000-0001-5860-8770,
S. Bashir^380000-0001-9861-8922,
G. Bassi^33,r0000-0002-2145-3805,
B. Batsukh^50000-0003-1020-2549,
P. B.  Battista^13,
A. Bay^480000-0002-4862-9399,
A. Beck^550000-0003-4872-1213,
M. Becker^180000-0002-7972-8760,
F. Bedeschi^330000-0002-8315-2119,
I.B. Bediaga^20000-0001-7806-5283,
N. A.  Behling^180000-0003-4750-7872,
S. Belin^450000-0001-7154-1304,
V. Bellee^490000-0001-5314-0953,
K. Belous^420000-0003-0014-2589,
I. Belov^270000-0003-1699-9202,
I. Belyaev^340000-0002-7458-7030,
G. Benane^120000-0002-8176-8315,
G. Bencivenni^260000-0002-5107-0610,
E. Ben-Haim^150000-0002-9510-8414,
A. Berezhnoy^420000-0002-4431-7582,
R. Bernet^490000-0002-4856-8063,
S. Bernet Andres^430000-0002-4515-7541,
A. Bertolin^310000-0003-1393-4315,
C. Betancourt^490000-0001-9886-7427,
F. Betti^570000-0002-2395-235X,
J.  Bex^540000-0002-2856-8074,
Ia. Bezshyiko^490000-0002-4315-6414,
J. Bhom^390000-0002-9709-903X,
M.S. Bieker^180000-0001-7113-7862,
N.V. Biesuz^240000-0003-3004-0946,
P. Billoir^150000-0001-5433-9876,
A. Biolchini^360000-0001-6064-9993,
M. Birch^600000-0001-9157-4461,
F.C.R. Bishop^100000-0002-0023-3897,
A. Bitadze^610000-0001-7979-1092,
A. Bizzeti^0000-0001-5729-5530,
T. Blake^550000-0002-0259-5891,
F. Blanc^480000-0001-5775-3132,
J.E. Blank^180000-0002-6546-5605,
S. Blusk^670000-0001-9170-684X,
V. Bocharnikov^420000-0003-1048-7732,
J.A. Boelhauve^180000-0002-3543-9959,
O. Boente Garcia^140000-0003-0261-8085,
T. Boettcher^640000-0002-2439-9955,
A.  Bohare^570000-0003-1077-8046,
A. Boldyrev^420000-0002-7872-6819,
C.S. Bolognani^770000-0003-3752-6789,
R. Bolzonella^24,k0000-0002-0055-0577,
N. Bondar^420000-0003-2714-9879,
A. Bordelius^470009-0002-3529-8524,
F. Borgato^31,p0000-0002-3149-6710,
S. Borghi^610000-0001-5135-1511,
M. Borsato^29,o0000-0001-5760-2924,
J.T. Borsuk^390000-0002-9065-9030,
S.A. Bouchiba^480000-0002-0044-6470,
M.  Bovill^620009-0006-2494-8287,
T.J.V. Bowcock^590000-0002-3505-6915,
A. Boyer^470000-0002-9909-0186,
C. Bozzi^240000-0001-6782-3982,
A. Brea Rodriguez^480000-0001-5650-445X,
N. Breer^180000-0003-0307-3662,
J. Brodzicka^390000-0002-8556-0597,
A. Brossa Gonzalo^45,55,44,†0000-0002-4442-1048,
J. Brown^590000-0001-9846-9672,
D. Brundu^300000-0003-4457-5896,
E. Buchanan^57,
A. Buonaura^490000-0003-4907-6463,
L. Buonincontri^31,p0000-0002-1480-454X,
A.T. Burke^610000-0003-0243-0517,
C. Burr^470000-0002-5155-1094,
A. Butkevich^420000-0001-9542-1411,
J.S. Butter^540000-0002-1816-536X,
J. Buytaert^470000-0002-7958-6790,
W. Byczynski^470009-0008-0187-3395,
S. Cadeddu^300000-0002-7763-500X,
H. Cai^72,
A. C.  Caillet^15,
R. Calabrese^24,k0000-0002-1354-5400,
S. Calderon Ramirez^90000-0001-9993-4388,
L. Calefice^440000-0001-6401-1583,
S. Cali^260000-0001-9056-0711,
M. Calvi^29,o0000-0002-8797-1357,
M. Calvo Gomez^430000-0001-5588-1448,
P. Camargo Magalhaes^2,y0000-0003-3641-8110,
J. I. Cambon Bouzas^450000-0002-2952-3118,
P. Campana^260000-0001-8233-1951,
D.H. Campora Perez^770000-0001-8998-9975,
A.F. Campoverde Quezada^70000-0003-1968-1216,
S. Capelli^290000-0002-8444-4498,
L. Capriotti^240000-0003-4899-0587,
R. Caravaca-Mora^90000-0001-8010-0447,
A. Carbone^23,i0000-0002-7045-2243,
L. Carcedo Salgado^450000-0003-3101-3528,
R. Cardinale^27,m0000-0002-7835-7638,
A. Cardini^300000-0002-6649-0298,
P. Carniti^29,o0000-0002-7820-2732,
L. Carus^20,
A. Casais Vidal^630000-0003-0469-2588,
R. Caspary^200000-0002-1449-1619,
G. Casse^590000-0002-8516-237X,
J. Castro Godinez^90000-0003-4808-4904,
M. Cattaneo^470000-0001-7707-169X,
G. Cavallero^24,470000-0002-8342-7047,
V. Cavallini^24,k0000-0001-7601-129X,
S. Celani^200000-0003-4715-7622,
D. Cervenkov^620000-0002-1865-741X,
S.  Cesare^28,n0000-0003-0886-7111,
A.J. Chadwick^590000-0003-3537-9404,
I. Chahrour^810000-0002-1472-0987,
M. Charles^150000-0003-4795-498X,
Ph. Charpentier^470000-0001-9295-8635,
E.  Chatzianagnostou^360009-0009-3781-1820,
C.A. Chavez Barajas^590000-0002-4602-8661,
M. Chefdeville^100000-0002-6553-6493,
C. Chen^120000-0002-3400-5489,
S. Chen^50000-0002-8647-1828,
Z. Chen^70000-0002-0215-7269,
A. Chernov^390000-0003-0232-6808,
S. Chernyshenko^510000-0002-2546-6080,
X.  Chiotopoulos^770009-0006-5762-6559,
V. Chobanova^790000-0002-1353-6002,
S. Cholak^480000-0001-8091-4766,
M. Chrzaszcz^390000-0001-7901-8710,
A. Chubykin^420000-0003-1061-9643,
V. Chulikov^420000-0002-7767-9117,
P. Ciambrone^260000-0003-0253-9846,
X. Cid Vidal^450000-0002-0468-541X,
G. Ciezarek^470000-0003-1002-8368,
P. Cifra^470000-0003-3068-7029,
P.E.L. Clarke^570000-0003-3746-0732,
M. Clemencic^470000-0003-1710-6824,
H.V. Cliff^540000-0003-0531-0916,
J. Closier^470000-0002-0228-9130,
C. Cocha Toapaxi^200000-0001-5812-8611,
V. Coco^470000-0002-5310-6808,
J. Cogan^120000-0001-7194-7566,
E. Cogneras^110000-0002-8933-9427,
L. Cojocariu^410000-0002-1281-5923,
P. Collins^470000-0003-1437-4022,
T. Colombo^470000-0002-9617-9687,
M. C.  Colonna^180009-0000-1704-4139,
A. Comerma-Montells^440000-0002-8980-6048,
L. Congedo^220000-0003-4536-4644,
A. Contu^300000-0002-3545-2969,
N. Cooke^580000-0002-4179-3700,
I. Corredoira ^450000-0002-6089-0899,
A. Correia^150000-0002-6483-8596,
G. Corti^470000-0003-2857-4471,
J.J. Cottee Meldrum^53,
B. Couturier^470000-0001-6749-1033,
D.C. Craik^490000-0002-3684-1560,
M. Cruz Torres^2,f0000-0003-2607-131X,
E. Curras Rivera^480000-0002-6555-0340,
R. Currie^570000-0002-0166-9529,
C.L. Da Silva^660000-0003-4106-8258,
S. Dadabaev^420000-0002-0093-3244,
L. Dai^690000-0002-4070-4729,
X. Dai^60000-0003-3395-7151,
E. Dall'Occo^180000-0001-9313-4021,
J. Dalseno^450000-0003-3288-4683,
C. D'Ambrosio^470000-0003-4344-9994,
J. Daniel^110000-0002-9022-4264,
A. Danilina^420000-0003-3121-2164,
P. d'Argent^220000-0003-2380-8355,
A.  Davidson^550009-0002-0647-2028,
J.E. Davies^610000-0002-5382-8683,
A. Davis^610000-0001-9458-5115,
O. De Aguiar Francisco^610000-0003-2735-678X,
C. De Angelis^30,j0009-0005-5033-5866,
F. De Benedetti^470000-0002-7960-3116,
J. de Boer^360000-0002-6084-4294,
K. De Bruyn^760000-0002-0615-4399,
S. De Capua^610000-0002-6285-9596,
M. De Cian^20,470000-0002-1268-9621,
U. De Freitas Carneiro Da Graca^2,b0000-0003-0451-4028,
E. De Lucia^260000-0003-0793-0844,
J.M. De Miranda^20009-0003-2505-7337,
L. De Paula^30000-0002-4984-7734,
M. De Serio^22,g0000-0003-4915-7933,
P. De Simone^260000-0001-9392-2079,
F. De Vellis^180000-0001-7596-5091,
J.A. de Vries^770000-0003-4712-9816,
F. Debernardis^220009-0001-5383-4899,
D. Decamp^100000-0001-9643-6762,
V. Dedu^120000-0001-5672-8672,
S.  Dekkers^10000-0001-9598-875X,
L. Del Buono^150000-0003-4774-2194,
B. Delaney^630009-0007-6371-8035,
H.-P. Dembinski^180000-0003-3337-3850,
J. Deng^80000-0002-4395-3616,
V. Denysenko^490000-0002-0455-5404,
O. Deschamps^110000-0002-7047-6042,
F. Dettori^30,j0000-0003-0256-8663,
B. Dey^750000-0002-4563-5806,
P. Di Nezza^260000-0003-4894-6762,
I. Diachkov^420000-0001-5222-5293,
S. Didenko^420000-0001-5671-5863,
S. Ding^670000-0002-5946-581X,
L. Dittmann^200009-0000-0510-0252,
V. Dobishuk^510000-0001-9004-3255,
A. D.  Docheva^580000-0002-7680-4043,
C. Dong^40000-0003-3259-6323,
A.M. Donohoe^210000-0002-4438-3950,
F. Dordei^300000-0002-2571-5067,
A.C. dos Reis^20000-0001-7517-8418,
A. D.  Dowling^670009-0007-1406-3343,
W. Duan^700000-0003-1765-9939,
P. Duda^780000-0003-4043-7963,
M.W. Dudek^390000-0003-3939-3262,
L. Dufour^470000-0002-3924-2774,
V. Duk^320000-0001-6440-0087,
P. Durante^470000-0002-1204-2270,
M. M. Duras^780000-0002-4153-5293,
J.M. Durham^660000-0002-5831-3398,
O. D.  Durmus^750000-0002-8161-7832,
A. Dziurda^390000-0003-4338-7156,
A. Dzyuba^420000-0003-3612-3195,
S. Easo^560000-0002-4027-7333,
E. Eckstein^17,
U. Egede^10000-0001-5493-0762,
A. Egorychev^420000-0001-5555-8982,
V. Egorychev^420000-0002-2539-673X,
S. Eisenhardt^570000-0002-4860-6779,
E. Ejopu^610000-0003-3711-7547,
L. Eklund^800000-0002-2014-3864,
M. Elashri^640000-0001-9398-953X,
J. Ellbracht^180000-0003-1231-6347,
S. Ely^600000-0003-1618-3617,
A. Ene^410000-0001-5513-0927,
E. Epple^640000-0002-6312-3740,
J. Eschle^670000-0002-7312-3699,
S. Esen^200000-0003-2437-8078,
T. Evans^610000-0003-3016-1879,
F. Fabiano^30,j0000-0001-6915-9923,
L.N. Falcao^20000-0003-3441-583X,
Y. Fan^70000-0002-3153-430X,
B. Fang^720000-0003-0030-3813,
L. Fantini^32,q,470000-0002-2351-3998,
M. Faria^480000-0002-4675-4209,
K.   Farmer^570000-0003-2364-2877,
D. Fazzini^29,o0000-0002-5938-4286,
L. Felkowski^780000-0002-0196-910X,
M. Feng^5,70000-0002-6308-5078,
M. Feo^18,470000-0001-5266-2442,
A. Fernandez Casani^460000-0003-1394-509X,
M. Fernandez Gomez^450000-0003-1984-4759,
A.D. Fernez^650000-0001-9900-6514,
F. Ferrari^230000-0002-3721-4585,
F. Ferreira Rodrigues^30000-0002-4274-5583,
M. Ferrillo^490000-0003-1052-2198,
M. Ferro-Luzzi^470009-0008-1868-2165,
S. Filippov^420000-0003-3900-3914,
R.A. Fini^220000-0002-3821-3998,
M. Fiorini^24,k0000-0001-6559-2084,
K.L. Fischer^620009-0000-8700-9910,
D.S. Fitzgerald^810000-0001-6862-6876,
C. Fitzpatrick^610000-0003-3674-0812,
F. Fleuret^140000-0002-2430-782X,
M. Fontana^230000-0003-4727-831X,
L. F.  Foreman^610000-0002-2741-9966,
R. Forty^470000-0003-2103-7577,
D. Foulds-Holt^540000-0001-9921-687X,
M. Franco Sevilla^650000-0002-5250-2948,
M. Frank^470000-0002-4625-559X,
E. Franzoso^24,k0000-0003-2130-1593,
G. Frau^610000-0003-3160-482X,
C. Frei^470000-0001-5501-5611,
D.A. Friday^610000-0001-9400-3322,
J. Fu^70000-0003-3177-2700,
Q. Fuehring^18,540000-0003-3179-2525,
Y. Fujii^10000-0002-0813-3065,
T. Fulghesu^150000-0001-9391-8619,
E. Gabriel^360000-0001-8300-5939,
G. Galati^220000-0001-7348-3312,
M.D. Galati^360000-0002-8716-4440,
A. Gallas Torreira^450000-0002-2745-7954,
D. Galli^23,i0000-0003-2375-6030,
S. Gambetta^570000-0003-2420-0501,
M. Gandelman^30000-0001-8192-8377,
P. Gandini^280000-0001-7267-6008,
B.  Ganie^610009-0008-7115-3940,
H. Gao^70000-0002-6025-6193,
R. Gao^620009-0004-1782-7642,
Y. Gao^80000-0002-6069-8995,
Y. Gao^60000-0003-1484-0943,
Y. Gao^8,
M. Garau^30,j0000-0002-0505-9584,
L.M. Garcia Martin^480000-0003-0714-8991,
P. Garcia Moreno^440000-0002-3612-1651,
J. García Pardiñas^470000-0003-2316-8829,
K. G.  Garg^80000-0002-8512-8219,
L. Garrido^440000-0001-8883-6539,
C. Gaspar^470000-0002-8009-1509,
R.E. Geertsema^360000-0001-6829-7777,
L.L. Gerken^180000-0002-6769-3679,
E. Gersabeck^610000-0002-2860-6528,
M. Gersabeck^610000-0002-0075-8669,
T. Gershon^550000-0002-3183-5065,
S. G.  Ghizzo^27,m,
Z. Ghorbanimoghaddam^53,
L. Giambastiani^31,p0000-0002-5170-0635,
F. I. Giasemis^15,e0000-0003-0622-1069,
V. Gibson^540000-0002-6661-1192,
H.K. Giemza^400000-0003-2597-8796,
A.L. Gilman^620000-0001-5934-7541,
M. Giovannetti^260000-0003-2135-9568,
A. Gioventù^440000-0001-5399-326X,
L. Girardey^610000-0002-8254-7274,
P. Gironella Gironell^440000-0001-5603-4750,
C. Giugliano^24,k0000-0002-6159-4557,
M.A. Giza^390000-0002-0805-1561,
E.L. Gkougkousis^600000-0002-2132-2071,
F.C. Glaser^13,200000-0001-8416-5416,
V.V. Gligorov^15,470000-0002-8189-8267,
C. Göbel^680000-0003-0523-495X,
E. Golobardes^430000-0001-8080-0769,
D. Golubkov^420000-0001-6216-1596,
A. Golutvin^60,42,470000-0003-2500-8247,
A. Gomes^2,a,†0009-0005-2892-2968,
S. Gomez Fernandez^440000-0002-3064-9834,
F. Goncalves Abrantes^620000-0002-7318-482X,
M. Goncerz^390000-0002-9224-914X,
G. Gong^40000-0002-7822-3947,
J. A. Gooding^180000-0003-3353-9750,
I.V. Gorelov^420000-0001-5570-0133,
C. Gotti^290000-0003-2501-9608,
J.P. Grabowski^170000-0001-8461-8382,
L.A. Granado Cardoso^470000-0003-2868-2173,
E. Graugés^440000-0001-6571-4096,
E. Graverini^48,s0000-0003-4647-6429,
L. Grazette^550000-0001-7907-4261,
G. Graziani^0000-0001-8212-846X,
A. T. Grecu^410000-0002-7770-1839,
L.M. Greeven^360000-0001-5813-7972,
N.A. Grieser^640000-0003-0386-4923,
L. Grillo^580000-0001-5360-0091,
S. Gromov^420000-0002-8967-3644,
C.  Gu^140000-0001-5635-6063,
M. Guarise^240000-0001-8829-9681,
L.  Guerry^110009-0004-8932-4024,
M. Guittiere^130000-0002-2916-7184,
V. Guliaeva^420000-0003-3676-5040,
P. A. Günther^200000-0002-4057-4274,
A.-K. Guseinov^480000-0002-5115-0581,
E. Gushchin^420000-0001-8857-1665,
Y. Guz^6,42,470000-0001-7552-400X,
T. Gys^470000-0002-6825-6497,
K. Habermann^170009-0002-6342-5965,
T. Hadavizadeh^10000-0001-5730-8434,
C. Hadjivasiliou^650000-0002-2234-0001,
G. Haefeli^480000-0002-9257-839X,
C. Haen^470000-0002-4947-2928,
J. Haimberger^470000-0002-3363-7783,
M. Hajheidari^47,
G.  Hallett^550009-0005-1427-6520,
M.M. Halvorsen^470000-0003-0959-3853,
P.M. Hamilton^650000-0002-2231-1374,
J. Hammerich^590000-0002-5556-1775,
Q. Han^80000-0002-7958-2917,
X. Han^200000-0001-7641-7505,
S. Hansmann-Menzemer^200000-0002-3804-8734,
L. Hao^70000-0001-8162-4277,
N. Harnew^620000-0001-9616-6651,
M. Hartmann^130009-0005-8756-0960,
S. Hashmi^380000-0003-2714-2706,
J. He^7,c0000-0002-1465-0077,
F. Hemmer^470000-0001-8177-0856,
C. Henderson^640000-0002-6986-9404,
R.D.L. Henderson^1,550000-0001-6445-4907,
A.M. Hennequin^470009-0008-7974-3785,
K. Hennessy^590000-0002-1529-8087,
L. Henry^480000-0003-3605-832X,
J. Herd^600000-0001-7828-3694,
P. Herrero Gascon^200000-0001-6265-8412,
J. Heuel^160000-0001-9384-6926,
A. Hicheur^30000-0002-3712-7318,
G. Hijano Mendizabal^49,
D. Hill^480000-0003-2613-7315,
S.E. Hollitt^180000-0002-4962-3546,
J. Horswill^610000-0002-9199-8616,
R. Hou^80000-0002-3139-3332,
Y. Hou^110000-0001-6454-278X,
N. Howarth^59,
J. Hu^20,
J. Hu^700000-0002-8227-4544,
W. Hu^60000-0002-2855-0544,
X. Hu^40000-0002-5924-2683,
W. Huang^70000-0002-1407-1729,
W. Hulsbergen^360000-0003-3018-5707,
R.J. Hunter^550000-0001-7894-8799,
M. Hushchyn^420000-0002-8894-6292,
D. Hutchcroft^590000-0002-4174-6509,
D. Ilin^420000-0001-8771-3115,
P. Ilten^640000-0001-5534-1732,
A. Inglessi^420000-0002-2522-6722,
A. Iniukhin^420000-0002-1940-6276,
A. Ishteev^420000-0003-1409-1428,
K. Ivshin^420000-0001-8403-0706,
R. Jacobsson^470000-0003-4971-7160,
H. Jage^160000-0002-8096-3792,
S.J. Jaimes Elles^46,730000-0003-0182-8638,
S. Jakobsen^470000-0002-6564-040X,
E. Jans^360000-0002-5438-9176,
B.K. Jashal^460000-0002-0025-4663,
A. Jawahery^65,470000-0003-3719-119X,
V. Jevtic^180000-0001-6427-4746,
E. Jiang^650000-0003-1728-8525,
X. Jiang^5,70000-0001-8120-3296,
Y. Jiang^70000-0002-8964-5109,
Y. J.  Jiang^60000-0002-0656-8647,
M. John^620000-0002-8579-844X,
A.  John Rubesh Rajan^210000-0002-9850-4965,
D. Johnson^520000-0003-3272-6001,
C.R. Jones^540000-0003-1699-8816,
T.P. Jones^550000-0001-5706-7255,
S. Joshi^400000-0002-5821-1674,
B. Jost^470009-0005-4053-1222,
J.  Juan Castella^540009-0009-5577-1308,
N. Jurik^470000-0002-6066-7232,
I. Juszczak^390000-0002-1285-3911,
D. Kaminaris^480000-0002-8912-4653,
S. Kandybei^500000-0003-3598-0427,
M.  Kane^57 0009-0006-5064-966X,
Y. Kang^40000-0002-6528-8178,
C. Kar^110000-0002-6407-6974,
M. Karacson^470009-0006-1867-9674,
D. Karpenkov^420000-0001-8686-2303,
A. Kauniskangas^480000-0002-4285-8027,
J.W. Kautz^640000-0001-8482-5576,
F. Keizer^470000-0002-1290-6737,
M. Kenzie^540000-0001-7910-4109,
T. Ketel^360000-0002-9652-1964,
B. Khanji^670000-0003-3838-281X,
A. Kharisova^420000-0002-5291-9583,
S. Kholodenko^33,470000-0002-0260-6570,
G. Khreich^130000-0002-6520-8203,
T. Kirn^160000-0002-0253-8619,
V.S. Kirsebom^29,o0009-0005-4421-9025,
O. Kitouni^630000-0001-9695-8165,
S. Klaver^370000-0001-7909-1272,
N. Kleijne^33,r0000-0003-0828-0943,
K. Klimaszewski^400000-0003-0741-5922,
M.R. Kmiec^400000-0002-1821-1848,
S. Koliiev^510009-0002-3680-1224,
L. Kolk^180000-0003-2589-5130,
A. Konoplyannikov^420009-0005-2645-8364,
P. Kopciewicz^38,470000-0001-9092-3527,
P. Koppenburg^360000-0001-8614-7203,
M. Korolev^420000-0002-7473-2031,
I. Kostiuk^360000-0002-8767-7289,
O. Kot^51,
S. Kotriakhova^0000-0002-1495-0053,
A. Kozachuk^420000-0001-6805-0395,
P. Kravchenko^420000-0002-4036-2060,
L. Kravchuk^420000-0001-8631-4200,
M. Kreps^550000-0002-6133-486X,
P. Krokovny^420000-0002-1236-4667,
W. Krupa^670000-0002-7947-465X,
W. Krzemien^400000-0002-9546-358X,
O.K. Kshyvanskyi^51,
J. Kubat^20,
S. Kubis^780000-0001-8774-8270,
M. Kucharczyk^390000-0003-4688-0050,
V. Kudryavtsev^420009-0000-2192-995X,
E. Kulikova^420009-0002-8059-5325,
A. Kupsc^800000-0003-4937-2270,
B. K.  Kutsenko^120000-0002-8366-1167,
D. Lacarrere^470009-0005-6974-140X,
P.  Laguarta Gonzalez^440009-0005-3844-0778,
A. Lai^300000-0003-1633-0496,
A. Lampis^300000-0002-5443-4870,
D. Lancierini^540000-0003-1587-4555,
C. Landesa Gomez^450000-0001-5241-8642,
J.J. Lane^10000-0002-5816-9488,
R. Lane^530000-0002-2360-2392,
G. Lanfranchi^260000-0002-9467-8001,
C. Langenbruch^200000-0002-3454-7261,
J. Langer^180000-0002-0322-5550,
O. Lantwin^420000-0003-2384-5973,
T. Latham^550000-0002-7195-8537,
F. Lazzari^33,s0000-0002-3151-3453,
C. Lazzeroni^520000-0003-4074-4787,
R. Le Gac^120000-0002-7551-6971,
H.  Lee^590009-0003-3006-2149,
R. Lefèvre^110000-0002-6917-6210,
A. Leflat^420000-0001-9619-6666,
S. Legotin^420000-0003-3192-6175,
M. Lehuraux^550000-0001-7600-7039,
E. Lemos Cid^470000-0003-3001-6268,
O. Leroy^120000-0002-2589-240X,
T. Lesiak^390000-0002-3966-2998,
B. Leverington^200000-0001-6640-7274,
A. Li^40000-0001-5012-6013,
C.  Li^120000-0002-3554-5479,
H. Li^700000-0002-2366-9554,
K. Li^80000-0002-2243-8412,
L. Li^610000-0003-4625-6880,
P. Li^470000-0003-2740-9765,
P.-R. Li^710000-0002-1603-3646,
Q.  Li^5,70009-0004-1932-8580,
S. Li^80000-0001-5455-3768,
T. Li^5,d0000-0002-5241-2555,
T. Li^700000-0002-5723-0961,
Y. Li^8,
Y. Li^50000-0003-2043-4669,
Z. Lian^40000-0003-4602-6946,
X. Liang^670000-0002-5277-9103,
S. Libralon^460009-0002-5841-9624,
C. Lin^70000-0001-7587-3365,
T. Lin^560000-0001-6052-8243,
R. Lindner^470000-0002-5541-6500,
V. Lisovskyi^480000-0003-4451-214X,
R. Litvinov^30,470000-0002-4234-435X,
F. L.  Liu^10009-0002-2387-8150,
G. Liu^700000-0001-5961-6588,
K. Liu^710000-0003-4529-3356,
S. Liu^5,70000-0002-6919-227X,
W.  Liu^8,
Y. Liu^570000-0003-3257-9240,
Y. Liu^71,
Y. L.  Liu^600000-0001-9617-6067,
A. Lobo Salvia^440000-0002-2375-9509,
A. Loi^300000-0003-4176-1503,
J. Lomba Castro^450000-0003-1874-8407,
T. Long^540000-0001-7292-848X,
J.H. Lopes^30000-0003-1168-9547,
A. Lopez Huertas^440000-0002-6323-5582,
S. López Soliño^450000-0001-9892-5113,
Q. Lu^140000-0002-6598-1941,
C. Lucarelli^25,l0000-0002-8196-1828,
D. Lucchesi^31,p0000-0003-4937-7637,
M. Lucio Martinez^770000-0001-6823-2607,
V. Lukashenko^36,510000-0002-0630-5185,
Y. Luo^60009-0001-8755-2937,
A. Lupato^31,h0000-0003-0312-3914,
E. Luppi^24,k0000-0002-1072-5633,
K. Lynch^210000-0002-7053-4951,
X.-R. Lyu^70000-0001-5689-9578,
G. M.  Ma^40000-0001-8838-5205,
R. Ma^70000-0002-0152-2412,
S. Maccolini^180000-0002-9571-7535,
F. Machefert^130000-0002-4644-5916,
F. Maciuc^410000-0001-6651-9436,
B.  Mack^670000-0001-8323-6454,
I. Mackay^620000-0003-0171-7890,
L. M.  Mackey^670000-0002-8285-3589,
L.R. Madhan Mohan^540000-0002-9390-8821,
M. J.  Madurai^520000-0002-6503-0759,
A. Maevskiy^420000-0003-1652-8005,
D. Magdalinski^360000-0001-6267-7314,
D. Maisuzenko^420000-0001-5704-3499,
M.W. Majewski^38,
J.J. Malczewski^390000-0003-2744-3656,
S. Malde^620000-0002-8179-0707,
L. Malentacca^47,
A. Malinin^420000-0002-3731-9977,
T. Maltsev^420000-0002-2120-5633,
G. Manca^30,j0000-0003-1960-4413,
G. Mancinelli^120000-0003-1144-3678,
C. Mancuso^28,13,n0000-0002-2490-435X,
R. Manera Escalero^440000-0003-4981-6847,
D. Manuzzi^230000-0002-9915-6587,
D. Marangotto^28,n0000-0001-9099-4878,
J.F. Marchand^100000-0002-4111-0797,
R. Marchevski^480000-0003-3410-0918,
U. Marconi^230000-0002-5055-7224,
E. Mariani^15,
S. Mariani^470000-0002-7298-3101,
C. Marin Benito^440000-0003-0529-6982,
J. Marks^200000-0002-2867-722X,
A.M. Marshall^530000-0002-9863-4954,
L.  Martel^620000-0001-8562-0038,
G. Martelli^32,q0000-0002-6150-3168,
G. Martellotti^340000-0002-8663-9037,
L. Martinazzoli^470000-0002-8996-795X,
M. Martinelli^29,o0000-0003-4792-9178,
D. Martinez Santos^450000-0002-6438-4483,
F. Martinez Vidal^460000-0001-6841-6035,
A. Massafferri^20000-0002-3264-3401,
R. Matev^470000-0001-8713-6119,
A. Mathad^470000-0002-9428-4715,
V. Matiunin^420000-0003-4665-5451,
C. Matteuzzi^670000-0002-4047-4521,
K.R. Mattioli^140000-0003-2222-7727,
A. Mauri^600000-0003-1664-8963,
E. Maurice^140000-0002-7366-4364,
J. Mauricio^440000-0002-9331-1363,
P. Mayencourt^480000-0002-8210-1256,
J. Mazorra de Cos^460000-0003-0525-2736,
M. Mazurek^400000-0002-3687-9630,
M. McCann^600000-0002-3038-7301,
L. Mcconnell^210009-0004-7045-2181,
T.H. McGrath^610000-0001-8993-3234,
N.T. McHugh^580000-0002-5477-3995,
A. McNab^610000-0001-5023-2086,
R. McNulty^210000-0001-7144-0175,
B. Meadows^640000-0002-1947-8034,
G. Meier^180000-0002-4266-1726,
D. Melnychuk^400000-0003-1667-7115,
F. M.  Meng^40009-0004-1533-6014,
M. Merk^36,770000-0003-0818-4695,
A. Merli^480000-0002-0374-5310,
L. Meyer Garcia^650000-0002-2622-8551,
D. Miao^5,70000-0003-4232-5615,
H. Miao^70000-0002-1936-5400,
M. Mikhasenko^740000-0002-6969-2063,
D.A. Milanes^730000-0001-7450-1121,
A. Minotti^29,o0000-0002-0091-5177,
E. Minucci^670000-0002-3972-6824,
T. Miralles^110000-0002-4018-1454,
B. Mitreska^180000-0002-1697-4999,
D.S. Mitzel^180000-0003-3650-2689,
A. Modak^560000-0003-1198-1441,
R.A. Mohammed^620000-0002-3718-4144,
R.D. Moise^160000-0002-5662-8804,
S. Mokhnenko^420000-0002-1849-1472,
T. Mombächer^470000-0002-5612-979X,
M. Monk^55,10000-0003-0484-0157,
S. Monteil^110000-0001-5015-3353,
A. Morcillo Gomez^450000-0001-9165-7080,
G. Morello^260000-0002-6180-3697,
M.J. Morello^33,r0000-0003-4190-1078,
M.P. Morgenthaler^200000-0002-7699-5724,
A.B. Morris^470000-0002-0832-9199,
A.G. Morris^120000-0001-6644-9888,
R. Mountain^670000-0003-1908-4219,
H. Mu^40000-0001-9720-7507,
Z. M.  Mu^60000-0001-9291-2231,
E. Muhammad^550000-0001-7413-5862,
F. Muheim^570000-0002-1131-8909,
M. Mulder^760000-0001-6867-8166,
K. Müller^490000-0002-5105-1305,
F. Muñoz-Rojas^90000-0002-4978-602X,
R. Murta^600000-0002-6915-8370,
P. Naik^590000-0001-6977-2971,
T. Nakada^480009-0000-6210-6861,
R. Nandakumar^560000-0002-6813-6794,
T. Nanut^470000-0002-5728-9867,
I. Nasteva^30000-0001-7115-7214,
M. Needham^570000-0002-8297-6714,
N. Neri^28,n0000-0002-6106-3756,
S. Neubert^170000-0002-0706-1944,
N. Neufeld^470000-0003-2298-0102,
P. Neustroev^42,
J. Nicolini^18,130000-0001-9034-3637,
D. Nicotra^770000-0001-7513-3033,
E.M. Niel^480000-0002-6587-4695,
N. Nikitin^420000-0003-0215-1091,
P. Nogarolli^30009-0001-4635-1055,
P. Nogga^17,
N.S. Nolte^630000-0003-2536-4209,
C. Normand^530000-0001-5055-7710,
J. Novoa Fernandez^450000-0002-1819-1381,
G. Nowak^640000-0003-4864-7164,
C. Nunez^810000-0002-2521-9346,
H. N.  Nur^580000-0002-7822-523X,
A. Oblakowska-Mucha^380000-0003-1328-0534,
V. Obraztsov^420000-0002-0994-3641,
T. Oeser^160000-0001-7792-4082,
S. Okamura^24,k0000-0003-1229-3093,
A. Okhotnikov^42,
O. Okhrimenko^510000-0002-0657-6962,
R. Oldeman^30,j0000-0001-6902-0710,
F. Oliva^570000-0001-7025-3407,
M. Olocco^180000-0002-6968-1217,
C.J.G. Onderwater^770000-0002-2310-4166,
R.H. O'Neil^570000-0002-9797-8464,
D. Osthues^18,
J.M. Otalora Goicochea^30000-0002-9584-8500,
P. Owen^490000-0002-4161-9147,
A. Oyanguren^460000-0002-8240-7300,
O. Ozcelik^570000-0003-3227-9248,
F. Paciolla^33,v0000-0002-6001-600X,
A.  Padee^400000-0002-5017-7168,
K.O. Padeken^170000-0001-7251-9125,
B. Pagare^550000-0003-3184-1622,
P.R. Pais^200009-0005-9758-742X,
T. Pajero^470000-0001-9630-2000,
A. Palano^220000-0002-6095-9593,
M. Palutan^260000-0001-7052-1360,
G. Panshin^420000-0001-9163-2051,
L. Paolucci^550000-0003-0465-2893,
A. Papanestis^560000-0002-5405-2901,
M. Pappagallo^22,g0000-0001-7601-5602,
L.L. Pappalardo^24,k0000-0002-0876-3163,
C. Pappenheimer^640000-0003-0738-3668,
C. Parkes^610000-0003-4174-1334,
B. Passalacqua^240000-0003-3643-7469,
G. Passaleva^250000-0002-8077-8378,
D. Passaro^33,r0000-0002-8601-2197,
A. Pastore^220000-0002-5024-3495,
M. Patel^600000-0003-3871-5602,
J. Patoc^620009-0000-1201-4918,
C. Patrignani^23,i0000-0002-5882-1747,
A.  Paul^670009-0006-7202-0811,
C.J. Pawley^770000-0001-9112-3724,
A. Pellegrino^360000-0002-7884-345X,
J.  Peng^5,70009-0005-4236-4667,
M. Pepe Altarelli^260000-0002-1642-4030,
S. Perazzini^230000-0002-1862-7122,
D. Pereima^420000-0002-7008-8082,
H.  Pereira Da Costa^660000-0002-3863-352X,
A. Pereiro Castro^450000-0001-9721-3325,
P. Perret^110000-0002-5732-4343,
A. Perro^470000-0002-1996-0496,
K. Petridis^530000-0001-7871-5119,
A. Petrolini^27,m0000-0003-0222-7594,
J. P.  Pfaller^640009-0009-8578-3078,
H. Pham^670000-0003-2995-1953,
L. Pica^33,r0000-0001-9837-6556,
M. Piccini^320000-0001-8659-4409,
B. Pietrzyk^100000-0003-1836-7233,
G. Pietrzyk^130000-0001-9622-820X,
D. Pinci^340000-0002-7224-9708,
F. Pisani^470000-0002-7763-252X,
M. Pizzichemi^29,o,470000-0001-5189-230X,
V. Placinta^410000-0003-4465-2441,
M. Plo Casasus^450000-0002-2289-918X,
T. Poeschl^470000-0003-3754-7221,
F. Polci^15,470000-0001-8058-0436,
M. Poli Lener^260000-0001-7867-1232,
A. Poluektov^120000-0003-2222-9925,
N. Polukhina^420000-0001-5942-1772,
I. Polyakov^470000-0002-6855-7783,
E. Polycarpo^30000-0002-4298-5309,
S. Ponce^470000-0002-1476-7056,
D. Popov^70000-0002-8293-2922,
S. Poslavskii^420000-0003-3236-1452,
K. Prasanth^570000-0001-9923-0938,
C. Prouve^450000-0003-2000-6306,
V. Pugatch^510000-0002-5204-9821,
G. Punzi^33,s0000-0002-8346-9052,
S.  Qasim^490000-0003-4264-9724,
Q. Q.  Qian^60000-0001-6453-4691,
W. Qian^70000-0003-3932-7556,
N. Qin^40000-0001-8453-658X,
S. Qu^40000-0002-7518-0961,
R. Quagliani^470000-0002-3632-2453,
R.I. Rabadan Trejo^550000-0002-9787-3910,
J.H. Rademacker^530000-0003-2599-7209,
M. Rama^330000-0003-3002-4719,
M.  Ramírez García^810000-0001-7956-763X,
V. Ramos De Oliveira^680000-0003-3049-7866,
M. Ramos Pernas^550000-0003-1600-9432,
M.S. Rangel^30000-0002-8690-5198,
F. Ratnikov^420000-0003-0762-5583,
G. Raven^370000-0002-2897-5323,
M. Rebollo De Miguel^460000-0002-4522-4863,
F. Redi^28,h0000-0001-9728-8984,
J. Reich^530000-0002-2657-4040,
F. Reiss^610000-0002-8395-7654,
Z. Ren^70000-0001-9974-9350,
P.K. Resmi^620000-0001-9025-2225,
R. Ribatti^480000-0003-1778-1213,
G. R.  Ricart^14,820000-0002-9292-2066,
D. Riccardi^33,r0009-0009-8397-572X,
S. Ricciardi^560000-0002-4254-3658,
K. Richardson^630000-0002-6847-2835,
M. Richardson-Slipper^570000-0002-2752-001X,
K. Rinnert^590000-0001-9802-1122,
P. Robbe^130000-0002-0656-9033,
G. Robertson^580000-0002-7026-1383,
E. Rodrigues^590000-0003-2846-7625,
E. Rodriguez Fernandez^450000-0002-3040-065X,
J.A. Rodriguez Lopez^730000-0003-1895-9319,
E. Rodriguez Rodriguez^450000-0002-7973-8061,
J. Roensch^18,
A. Rogachev^420000-0002-7548-6530,
A. Rogovskiy^560000-0002-1034-1058,
D.L. Rolf^470000-0001-7908-7214,
P. Roloff^470000-0001-7378-4350,
V. Romanovskiy^420000-0003-0939-4272,
M. Romero Lamas^450000-0002-1217-8418,
A. Romero Vidal^450000-0002-8830-1486,
G. Romolini^240000-0002-0118-4214,
F. Ronchetti^480000-0003-3438-9774,
T. Rong^60000-0002-5479-9212,
M. Rotondo^260000-0001-5704-6163,
S. R.  Roy^200000-0002-3999-6795,
M.S. Rudolph^670000-0002-0050-575X,
M. Ruiz Diaz^200000-0001-6367-6815,
R.A. Ruiz Fernandez^450000-0002-5727-4454,
J. Ruiz Vidal^80,z0000-0001-8362-7164,
A. Ryzhikov^420000-0002-3543-0313,
J. Ryzka^380000-0003-4235-2445,
J. J. Saavedra-Arias^90000-0002-2510-8929,
J.J. Saborido Silva^450000-0002-6270-130X,
R. Sadek^140000-0003-0438-8359,
N. Sagidova^420000-0002-2640-3794,
D. Sahoo^750000-0002-5600-9413,
N. Sahoo^520000-0001-9539-8370,
B. Saitta^30,j0000-0003-3491-0232,
M. Salomoni^29,o,470009-0007-9229-653X,
C. Sanchez Gras^360000-0002-7082-887X,
I. Sanderswood^460000-0001-7731-6757,
R. Santacesaria^340000-0003-3826-0329,
C. Santamarina Rios^450000-0002-9810-1816,
M. Santimaria^26,470000-0002-8776-6759,
L. Santoro ^20000-0002-2146-2648,
E. Santovetti^350000-0002-5605-1662,
A. Saputi^24,470000-0001-6067-7863,
D. Saranin^420000-0002-9617-9986,
A. Sarnatskiy^760009-0007-2159-3633,
G. Sarpis^570000-0003-1711-2044,
M. Sarpis^610000-0002-6402-1674,
C. Satriano^34,t0000-0002-4976-0460,
A. Satta^350000-0003-2462-913X,
M. Saur^60000-0001-8752-4293,
D. Savrina^420000-0001-8372-6031,
H. Sazak^160000-0003-2689-1123,
F. Sborzacchi^47,260009-0004-7916-2682,
L.G. Scantlebury Smead^620000-0001-8702-7991,
A. Scarabotto^180000-0003-2290-9672,
S. Schael^160000-0003-4013-3468,
S. Scherl^590000-0003-0528-2724,
M. Schiller^580000-0001-8750-863X,
H. Schindler^470000-0002-1468-0479,
M. Schmelling^190000-0003-3305-0576,
B. Schmidt^470000-0002-8400-1566,
S. Schmitt^160000-0002-6394-1081,
H. Schmitz^17,
O. Schneider^480000-0002-6014-7552,
A. Schopper^470000-0002-8581-3312,
N. Schulte^180000-0003-0166-2105,
S. Schulte^480009-0001-8533-0783,
M.H. Schune^130000-0002-3648-0830,
R. Schwemmer^470009-0005-5265-9792,
G. Schwering^160000-0003-1731-7939,
B. Sciascia^260000-0003-0670-006X,
A. Sciuccati^470000-0002-8568-1487,
S. Sellam^450000-0003-0383-1451,
A. Semennikov^420000-0003-1130-2197,
T. Senger^490009-0006-2212-6431,
M. Senghi Soares^370000-0001-9676-6059,
A. Sergi^27,m,470000-0001-9495-6115,
N. Serra^490000-0002-5033-0580,
L. Sestini^310000-0002-1127-5144,
A. Seuthe^180000-0002-0736-3061,
Y. Shang^60000-0001-7987-7558,
D.M. Shangase^810000-0002-0287-6124,
M. Shapkin^420000-0002-4098-9592,
R. S.  Sharma^670000-0003-1331-1791,
I. Shchemerov^420000-0001-9193-8106,
L. Shchutska^480000-0003-0700-5448,
T. Shears^590000-0002-2653-1366,
L. Shekhtman^420000-0003-1512-9715,
Z. Shen^60000-0003-1391-5384,
S. Sheng^5,70000-0002-1050-5649,
V. Shevchenko^420000-0003-3171-9125,
B. Shi^70000-0002-5781-8933,
Q. Shi^70000-0001-7915-8211,
Y. Shimizu^130000-0002-4936-1152,
E. Shmanin^420000-0002-8868-1730,
R. Shorkin^420000-0001-8881-3943,
J.D. Shupperd^670009-0006-8218-2566,
R. Silva Coutinho^670000-0002-1545-959X,
G. Simi^31,p0000-0001-6741-6199,
S. Simone^22,g0000-0003-3631-8398,
N. Skidmore^550000-0003-3410-0731,
T. Skwarnicki^670000-0002-9897-9506,
M.W. Slater^520000-0002-2687-1950,
J.C. Smallwood^620000-0003-2460-3327,
E. Smith^630000-0002-9740-0574,
K. Smith^660000-0002-1305-3377,
M. Smith^600000-0002-3872-1917,
A. Snoch^360000-0001-6431-6360,
L. Soares Lavra^570000-0002-2652-123X,
M.D. Sokoloff^640000-0001-6181-4583,
F.J.P. Soler^580000-0002-4893-3729,
A. Solomin^42,530000-0003-0644-3227,
A. Solovev^420000-0002-5355-5996,
I. Solovyev^420000-0003-4254-6012,
R. Song^10000-0002-8854-8905,
Y. Song^480000-0003-0256-4320,
Y. Song^40000-0003-1959-5676,
Y. S.  Song^60000-0003-3471-1751,
F.L. Souza De Almeida^670000-0001-7181-6785,
B. Souza De Paula^30009-0003-3794-3408,
E. Spadaro Norella^27,m0000-0002-1111-5597,
E. Spedicato^230000-0002-4950-6665,
J.G. Speer^180000-0002-6117-7307,
E. Spiridenkov^42,
P. Spradlin^580000-0002-5280-9464,
V. Sriskaran^470000-0002-9867-0453,
F. Stagni^470000-0002-7576-4019,
M. Stahl^470000-0001-8476-8188,
S. Stahl^470000-0002-8243-400X,
S. Stanislaus^620000-0003-1776-0498,
E.N. Stein^470000-0001-5214-8865,
O. Steinkamp^490000-0001-7055-6467,
O. Stenyakin^42,
H. Stevens^180000-0002-9474-9332,
D. Strekalina^420000-0003-3830-4889,
Y. Su^70000-0002-2739-7453,
F. Suljik^620000-0001-6767-7698,
J. Sun^300000-0002-6020-2304,
L. Sun^720000-0002-0034-2567,
Y. Sun^650000-0003-4933-5058,
D. Sundfeld^20000-0002-5147-3698,
W. Sutcliffe^49,
P.N. Swallow^520000-0003-2751-8515,
F. Swystun^540009-0006-0672-7771,
A. Szabelski^400000-0002-6604-2938,
T. Szumlak^380000-0002-2562-7163,
Y. Tan^40000-0003-3860-6545,
M.D. Tat^620000-0002-6866-7085,
A. Terentev^420000-0003-2574-8560,
F. Terzuoli^33,v,470000-0002-9717-225X,
F. Teubert^470000-0003-3277-5268,
E. Thomas^470000-0003-0984-7593,
D.J.D. Thompson^520000-0003-1196-5943,
H. Tilquin^600000-0003-4735-2014,
V. Tisserand^110000-0003-4916-0446,
S. T'Jampens^100000-0003-4249-6641,
M. Tobin^5,470000-0002-2047-7020,
L. Tomassetti^24,k0000-0003-4184-1335,
G. Tonani^28,n,470000-0001-7477-1148,
X. Tong^60000-0002-5278-1203,
D. Torres Machado^20000-0001-7030-6468,
L. Toscano^180009-0007-5613-6520,
D.Y. Tou^40000-0002-4732-2408,
C. Trippl^430000-0003-3664-1240,
G. Tuci^200000-0002-0364-5758,
N. Tuning^360000-0003-2611-7840,
L.H. Uecker^200000-0003-3255-9514,
A. Ukleja^380000-0003-0480-4850,
D.J. Unverzagt^200000-0002-1484-2546,
E. Ursov^420000-0002-6519-4526,
A. Usachov^370000-0002-5829-6284,
A. Ustyuzhanin^420000-0001-7865-2357,
U. Uwer^200000-0002-8514-3777,
V. Vagnoni^230000-0003-2206-311X,
G. Valenti^230000-0002-6119-7535,
N. Valls Canudas^470000-0001-8748-8448,
H. Van Hecke^660000-0001-7961-7190,
E. van Herwijnen^600000-0001-8807-8811,
C.B. Van Hulse^45,x0000-0002-5397-6782,
R. Van Laak^480000-0002-7738-6066,
M. van Veghel^360000-0001-6178-6623,
G. Vasquez^490000-0002-3285-7004,
R. Vazquez Gomez^440000-0001-5319-1128,
P. Vazquez Regueiro^450000-0002-0767-9736,
C. Vázquez Sierra^450000-0002-5865-0677,
S. Vecchi^240000-0002-4311-3166,
J.J. Velthuis^530000-0002-4649-3221,
M. Veltri^25,w0000-0001-7917-9661,
A. Venkateswaran^480000-0001-6950-1477,
M. Vesterinen^550000-0001-7717-2765,
D.  Vico Benet^620009-0009-3494-2825,
M. Vieites Diaz^470000-0002-0944-4340,
X. Vilasis-Cardona^430000-0002-1915-9543,
E. Vilella Figueras^590000-0002-7865-2856,
A. Villa^230000-0002-9392-6157,
P. Vincent^150000-0002-9283-4541,
F.C. Volle^520000-0003-1828-3881,
D. vom Bruch^120000-0001-9905-8031,
N. Voropaev^420000-0002-2100-0726,
K. Vos^770000-0002-4258-4062,
G. Vouters^10,470009-0008-3292-2209,
C. Vrahas^570000-0001-6104-1496,
J. Wagner^180000-0002-9783-5957,
J. Walsh^330000-0002-7235-6976,
E.J. Walton^1,550000-0001-6759-2504,
G. Wan^60000-0003-0133-1664,
C. Wang^200000-0002-5909-1379,
G. Wang^80000-0001-6041-115X,
J. Wang^60000-0001-7542-3073,
J. Wang^50000-0002-6391-2205,
J. Wang^40000-0002-3281-8136,
J. Wang^720000-0001-6711-4465,
M. Wang^280000-0003-4062-710X,
N. W.  Wang^70000-0002-6915-6607,
R. Wang^530000-0002-2629-4735,
X. Wang^8,
X. Wang^700000-0002-2399-7646,
X. W.  Wang^600000-0001-9565-8312,
Y. Wang^60009-0003-2254-7162,
Z. Wang^130000-0002-5041-7651,
Z. Wang^40000-0003-0597-4878,
Z. Wang^280000-0003-4410-6889,
J.A. Ward^55,10000-0003-4160-9333,
M. Waterlaat^47,
N.K. Watson^520000-0002-8142-4678,
D. Websdale^600000-0002-4113-1539,
Y. Wei^60000-0001-6116-3944,
J. Wendel^790000-0003-0652-721X,
B.D.C. Westhenry^530000-0002-4589-2626,
C. White^540009-0002-6794-9547,
M. Whitehead^580000-0002-2142-3673,
E. Whiter^520009-0003-3902-8123,
A.R. Wiederhold^550000-0002-1023-1086,
D. Wiedner^180000-0002-4149-4137,
G. Wilkinson^620000-0001-5255-0619,
M.K. Wilkinson^640000-0001-6561-2145,
M. Williams^630000-0001-8285-3346,
M.R.J. Williams^570000-0001-5448-4213,
R. Williams^540000-0002-2675-3567,
Z.  Williams^530009-0009-9224-4160,
F.F. Wilson^560000-0002-5552-0842,
W. Wislicki^400000-0001-5765-6308,
M. Witek^390000-0002-8317-385X,
L. Witola^200000-0001-9178-9921,
C.P. Wong^660000-0002-9839-4065,
G. Wormser^130000-0003-4077-6295,
S.A. Wotton^540000-0003-4543-8121,
H. Wu^670000-0002-9337-3476,
J. Wu^80000-0002-4282-0977,
Y. Wu^60000-0003-3192-0486,
Z. Wu^70000-0001-6756-9021,
K. Wyllie^470000-0002-2699-2189,
S. Xian^70,
Z. Xiang^50000-0002-9700-3448,
Y. Xie^80000-0001-5012-4069,
A. Xu^330000-0002-8521-1688,
J. Xu^70000-0001-6950-5865,
L. Xu^40000-0003-2800-1438,
L. Xu^40000-0002-0241-5184,
M. Xu^550000-0001-8885-565X,
Z. Xu^110000-0002-7531-6873,
Z. Xu^70000-0001-9558-1079,
Z. Xu^50000-0001-9602-4901,
D. Yang^0009-0002-2675-4022,
K.  Yang^600000-0001-5146-7311,
S. Yang^70000-0003-2505-0365,
X. Yang^60000-0002-7481-3149,
Y. Yang^27,m0000-0002-8917-2620,
Z. Yang^60000-0003-2937-9782,
Z. Yang^650000-0003-0572-2021,
V. Yeroshenko^130000-0002-8771-0579,
H. Yeung^610000-0001-9869-5290,
H. Yin^80000-0001-6977-8257,
C. Y.  Yu^60000-0002-4393-2567,
J. Yu^690000-0003-1230-3300,
X. Yuan^50000-0003-0468-3083,
Y Yuan^5,70009-0000-6595-7266,
E. Zaffaroni^480000-0003-1714-9218,
M. Zavertyaev^190000-0002-4655-715X,
M. Zdybal^390000-0002-1701-9619,
F. Zenesini^23,i0009-0001-2039-9739,
C.  Zeng^5,70009-0007-8273-2692,
M. Zeng^40000-0001-9717-1751,
C. Zhang^60000-0002-9865-8964,
D. Zhang^80000-0002-8826-9113,
J. Zhang^70000-0001-6010-8556,
L. Zhang^40000-0003-2279-8837,
S. Zhang^690000-0002-9794-4088,
S. Zhang^620000-0002-2385-0767,
Y. Zhang^60000-0002-0157-188X,
Y. Z.  Zhang^40000-0001-6346-8872,
Y. Zhao^200000-0002-8185-3771,
A. Zharkova^420000-0003-1237-4491,
A. Zhelezov^200000-0002-2344-9412,
S. Z.  Zheng^60009-0001-4723-095X,
X. Z.  Zheng^40000-0001-7647-7110,
Y. Zheng^70000-0003-0322-9858,
T. Zhou^60000-0002-3804-9948,
X. Zhou^80009-0005-9485-9477,
Y. Zhou^70000-0003-2035-3391,
V. Zhovkovska^550000-0002-9812-4508,
L. Z.  Zhu^70000-0003-0609-6456,
X. Zhu^40000-0002-9573-4570,
X. Zhu^80000-0002-4485-1478,
V. Zhukov^160000-0003-0159-291X,
J. Zhuo^460000-0002-6227-3368,
Q. Zou^5,70000-0003-0038-5038,
D. Zuliani^31,p0000-0002-1478-4593,
G. Zunica^480000-0002-5972-6290.



^1School of Physics and Astronomy, Monash University, Melbourne, Australia

^2Centro Brasileiro de Pesquisas Físicas (CBPF), Rio de Janeiro, Brazil

^3Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil

^4Center for High Energy Physics, Tsinghua University, Beijing, China

^5Institute Of High Energy Physics (IHEP), Beijing, China

^6School of Physics State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China

^7University of Chinese Academy of Sciences, Beijing, China

^8Institute of Particle Physics, Central China Normal University, Wuhan, Hubei, China

^9Consejo Nacional de Rectores  (CONARE), San Jose, Costa Rica

^10Université Savoie Mont Blanc, CNRS, IN2P3-LAPP, Annecy, France

^11Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France

^12Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France

^13Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France

^14Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France

^15LPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3, Paris, France

^16I. Physikalisches Institut, RWTH Aachen University, Aachen, Germany

^17Universität Bonn - Helmholtz-Institut für Strahlen und Kernphysik, Bonn, Germany

^18Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany

^19Max-Planck-Institut für Kernphysik (MPIK), Heidelberg, Germany

^20Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany

^21School of Physics, University College Dublin, Dublin, Ireland

^22INFN Sezione di Bari, Bari, Italy

^23INFN Sezione di Bologna, Bologna, Italy

^24INFN Sezione di Ferrara, Ferrara, Italy

^25INFN Sezione di Firenze, Firenze, Italy

^26INFN Laboratori Nazionali di Frascati, Frascati, Italy

^27INFN Sezione di Genova, Genova, Italy

^28INFN Sezione di Milano, Milano, Italy

^29INFN Sezione di Milano-Bicocca, Milano, Italy

^30INFN Sezione di Cagliari, Monserrato, Italy

^31INFN Sezione di Padova, Padova, Italy

^32INFN Sezione di Perugia, Perugia, Italy

^33INFN Sezione di Pisa, Pisa, Italy

^34INFN Sezione di Roma La Sapienza, Roma, Italy

^35INFN Sezione di Roma Tor Vergata, Roma, Italy

^36Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands

^37Nikhef National Institute for Subatomic Physics and VU University Amsterdam, Amsterdam, Netherlands

^38AGH - University of Krakow, Faculty of Physics and Applied Computer Science, Kraków, Poland

^39Henryk Niewodniczanski Institute of Nuclear Physics  Polish Academy of Sciences, Kraków, Poland

^40National Center for Nuclear Research (NCBJ), Warsaw, Poland

^41Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest-Magurele, Romania

^42Affiliated with an institute covered by a cooperation agreement with CERN

^43DS4DS, La Salle, Universitat Ramon Llull, Barcelona, Spain

^44ICCUB, Universitat de Barcelona, Barcelona, Spain

^45Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain

^46Instituto de Fisica Corpuscular, Centro Mixto Universidad de Valencia - CSIC, Valencia, Spain

^47European Organization for Nuclear Research (CERN), Geneva, Switzerland

^48Institute of Physics, Ecole Polytechnique  Fédérale de Lausanne (EPFL), Lausanne, Switzerland

^49Physik-Institut, Universität Zürich, Zürich, Switzerland

^50NSC Kharkiv Institute of Physics and Technology (NSC KIPT), Kharkiv, Ukraine

^51Institute for Nuclear Research of the National Academy of Sciences (KINR), Kyiv, Ukraine

^52School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom

^53H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom

^54Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom

^55Department of Physics, University of Warwick, Coventry, United Kingdom

^56STFC Rutherford Appleton Laboratory, Didcot, United Kingdom

^57School of Physics and Astronomy, University of Edinburgh, Edinburgh, United Kingdom

^58School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom

^59Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom

^60Imperial College London, London, United Kingdom

^61Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom

^62Department of Physics, University of Oxford, Oxford, United Kingdom

^63Massachusetts Institute of Technology, Cambridge, MA, United States

^64University of Cincinnati, Cincinnati, OH, United States

^65University of Maryland, College Park, MD, United States

^66Los Alamos National Laboratory (LANL), Los Alamos, NM, United States

^67Syracuse University, Syracuse, NY, United States

^68Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Rio de Janeiro, Brazil, associated to ^3

^69School of Physics and Electronics, Hunan University, Changsha City, China, associated to ^8

^70Guangdong Provincial Key Laboratory of Nuclear Science, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Institute of Quantum Matter, South China Normal University, Guangzhou, China, associated to ^4

^71Lanzhou University, Lanzhou, China, associated to ^5

^72School of Physics and Technology, Wuhan University, Wuhan, China, associated to ^4

^73Departamento de Fisica , Universidad Nacional de Colombia, Bogota, Colombia, associated to ^15

^74Ruhr Universitaet Bochum, Fakultaet f. Physik und Astronomie, Bochum, Germany, associated to ^18

^75Eotvos Lorand University, Budapest, Hungary, associated to ^47

^76Van Swinderen Institute, University of Groningen, Groningen, Netherlands, associated to ^36

^77Universiteit Maastricht, Maastricht, Netherlands, associated to ^36

^78Tadeusz Kosciuszko Cracow University of Technology, Cracow, Poland, associated to ^39

^79Universidade da Coruña, A Coruna, Spain, associated to ^43

^80Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden, associated to ^58

^81University of Michigan, Ann Arbor, MI, United States, associated to ^67

^82Département de Physique Nucléaire (DPhN), Gif-Sur-Yvette, France

^aUniversidade de Brasília, Brasília, Brazil

^bCentro Federal de Educacão Tecnológica Celso Suckow da Fonseca, Rio De Janeiro, Brazil

^cHangzhou Institute for Advanced Study, UCAS, Hangzhou, China

^dSchool of Physics and Electronics, Henan University , Kaifeng, China

^eLIP6, Sorbonne Université, Paris, France

^fUniversidad Nacional Autónoma de Honduras, Tegucigalpa, Honduras

^gUniversità di Bari, Bari, Italy

^hUniversità di Bergamo, Bergamo, Italy

^iUniversità di Bologna, Bologna, Italy

^jUniversità di Cagliari, Cagliari, Italy

^kUniversità di Ferrara, Ferrara, Italy

^lUniversità di Firenze, Firenze, Italy

^mUniversità di Genova, Genova, Italy

^nUniversità degli Studi di Milano, Milano, Italy

^oUniversità degli Studi di Milano-Bicocca, Milano, Italy

^pUniversità di Padova, Padova, Italy

^qUniversità  di Perugia, Perugia, Italy

^rScuola Normale Superiore, Pisa, Italy

^sUniversità di Pisa, Pisa, Italy

^tUniversità della Basilicata, Potenza, Italy

^uUniversità di Roma Tor Vergata, Roma, Italy

^vUniversità di Siena, Siena, Italy

^wUniversità di Urbino, Urbino, Italy

^xUniversidad de Alcalá, Alcalá de Henares , Spain

^yFacultad de Ciencias Fisicas, Madrid, Spain

^zDepartment of Physics/Division of Particle Physics, Lund, Sweden

^†Deceased





