22 research outputs found
Observation of Two New Excited Ξb0 States Decaying to Λb0 K-π+
- Author
- Aaij R
- Abdelmotteleb ASW
- Abrantes FG
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barbetti M
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bashir S
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Beteta CA
- Betti F
- Bezshyiko I
- Bhasin S
- Bhom J
- Bian L
- Bieker MS
- Bifani S
- Billoir P
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Bjorn M
- Blago MP
- Blake T
- Blanc F
- Blusk S
- Bobulska D
- Boelhauve JA
- Boettcher T
- Boldyrev A
- Bondar A
- Bondar N
- Borghi S
- Borisyak M
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brodski M
- Brodzicka J
- Brundu D
- Buonaura A
- Buonincontri L
- Burke AT
- Burr C
- Bursche A
- Butkevich A
- Butter JS
- Buytaert J
- Byczynski W
- Cadeddu S
- Cai H
- Calabrese R
- Calefice L
- Cali S
- Calladine R
- Calvi M
- Campana P
- Canudas NV
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- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carli I
- Carniti P
- Cartelle PA
- Carus L
- Casasus MP
- Casse G
- Castro AP
- Castro JL
- Cattaneo M
- Cavallero G
- Cazon BRG
- Celani S
- Cerasoli J
- Cervenkov D
- Chadwick AJ
- Chapman MG
- Charles M
- Charpentier P
- Chatzikonstantinidis G
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
- Cicala MF
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Cobbledick JL
- Coco V
- Coelho JAB
- Cogan J
- Cogneras E
- Cojocariu L
- Collins P
- Colombo T
- Congedo L
- Contu A
- Cooke N
- Coombs G
- Corredoira I
- Corti G
- Coutinho RS
- Couturier B
- Craik DC
- Crkovska J
- Currie R
- D'Ambrosio C
- D'Argent P
- Da Silva CL
- Dadabaev S
- Dai L
- Dall'Occo E
- Dalseno J
- Danilina A
- Davies JE
- Davis A
- De Almeida FLS
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Paula BS
- De Paula L
- De Serio M
- De Simone D
- De Simone P
- de Vries JA
- Dean CT
- Decamp D
- Dedu V
- Del Buono L
- Delaney B
- Dembinski HP
- Dendek A
- Denysenko V
- Derkach D
- Deschamps O
- Desse F
- Dettori F
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- Di Cicco A
- Di Nezza P
- Diaz LC
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- Dijkstra H
- Dobishuk V
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- Kitouni O
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- Kmiec MR
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- Morello G
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- Regueiro PV
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- Wislicki W
- Witek M
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- Wotton SA
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- Wyllie K
- Xiang Z
- Xiao D
- Xie Y
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- Xu M
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- Yao Y
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- Yin H
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- Yushchenko O
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu X
- Zhu X
- Zhu Z
- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Two narrow resonant states are observed in the Λb0K-π+ mass spectrum using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the LHCb experiment and corresponding to an integrated luminosity of 6 fb-1. The minimal quark content of the Λb0K-π+ system indicates that these are excited Ξb0 baryons. The masses of the Ξb(6327)0 and Ξb(6333)0 states are m[Ξb(6327)0]=6327.28-0.21+0.23±0.12±0.24 and m[Ξb(6333)0]=6332.69-0.18+0.17±0.03±0.22 MeV, respectively, with a mass splitting of Δm=5.41-0.27+0.26±0.12 MeV, where the uncertainties are statistical, systematic, and due to the Λb0 mass measurement. The measured natural widths of these states are consistent with zero, with upper limits of Γ[Ξb(6327)0]<2.20(2.56) and Γ[Ξb(6333)0]<1.60(1.92) MeV at a 90% (95%) credibility level. The significance of the two-peak hypothesis is larger than nine (five) Gaussian standard deviations compared to the no-peak (one-peak) hypothesis. The masses, widths, and resonant structure of the new states are in good agreement with the expectations for a doublet of 1D Ξb0 resonances
Search for dijet resonances in 7 TeV pp collisions at CMS
- Author
- Abbaneo D
- Abbiendi G
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- Zoeller MH
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2010 APSA search for narrow resonances in the dijet mass spectrum is performed using data corresponding to an integrated luminosity of 2.9 pb-1 collected by the CMS experiment at the Large Hadron Collider. Upper limits at the 95% confidence level are presented on the product of the resonance cross section, branching fraction into dijets, and acceptance, separately for decays into quark-quark, quark-gluon, or gluon-gluon pairs. The data exclude new particles predicted in the following models at the 95% confidence level: string resonances, with mass less than 2.50 TeV, excited quarks, with mass less than 1.58 TeV, and axigluons, colorons, and E6 diquarks, in specific mass intervals. This extends previously published limits on these models.This work is supported by FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
Search for Dijet Resonances in 7 TeV pp Collisions at CMS (vol 105, 211801, 2010)
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- Abbiendi G
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- Abdullin S
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- AMER PHYSICAL SOC
- Publication date
- 13/01/2011
- Field of study
Publisher’s Note: Search for Dijet Resonances in 7 TeV pp Collisions at CMS [Phys. Rev. Lett. 105, 211801 (2010)
High-power single-stage single-crystal Yb:YAG fiber amplifier for radially polarized ultrashort laser pulses
- Author
- A Loescher
- A Voss
- B Weichelt
- Christof Pruss
- D Sangla
- F Lesparre
- François Balembois
- Frederik Schaal
- Frieder Beirow
- JMO Lin Di
- Julien Didierjean
- M Eckerle
- M Endo
- M Meier
- MA Ahmed
- MA Ahmed
- Marwan Abdou Ahmed
- Matthieu Perrier
- Michael Eckerle
- Nicolas Aubry
- Patrick Georges
- Q Zhan
- R Dorn
- R Weber
- T Moser
- Thomas Graf
- Thomas Kämpfe
- Tom Dietrich
- VG Niziev
- Wolfgang Osten
- Xavier Délen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the lifetimes of promptly produced Omega(0)(c) and Xi(9)(c) baryons
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- Abdelmotteleb ASW
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- Hollitt SE
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- Hu J
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- Huang X
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- Hushchyn M
- Hutchcroft D
- Hynds D
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- Idzik M
- Ilin D
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- Ishteev A
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- Jawahery A
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- Jezabek M
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- Jones CR
- Jones TP
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- Jurik N
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- Kandybei S
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- Karacson M
- Karpov M
- Keizer F
- Kenzie M
- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Kleijne N
- Klimaszewski K
- Kmiec MR
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- Konoplyannikov A
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- Koppenburg P
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- Kostiuk I
- Kot O
- Kotriakhova S
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- Krawczyk RD
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- Kress F
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- Kuindersma HS
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- Nguyen-Mau C
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- Obraztsov V
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- Oldeman R
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- Ossowska A
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- Zheng Y
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- Zonneveld JB
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- Zunica G
- Publication venue
- Publication date
- 01/01/2022
- Field of study
A measurement of the lifetimes of the Omega(0)(c) and Xi(0)(c) baryons is reported using proton-proton collision data at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4 fb(-1) collected by the LHCb experiment. The Omega(0)(c) and Xi(0)(c) baryons are produced directly from proton interactions and reconstructed in the pK(-)K(-)pi(+) final state. The Omega(0)(c) lifetime is measured to be 276.5 +/- 13.4 +/- 4.4 +/- 0.7 fs, and the Xi(0)(c) lifetime is measured to be 148.0 +/- 2.3 +/- 2.2 +/- 0.2 fs, where the first uncertainty is statistical, the second systematic, and the third due to the uncertainty on the D-0 lifetime. These results confirm previous LHCb measurements based on semileptonic beauty-hadron decays, which disagree with earlier results of a four times shorter Omega(c)0 lifetime, and provide the single most precise measurement of the Omega(0 )(c)lifetime. (C) 2021 Science China Press. Published by Elsevier B.V. and Science China Press
Tests of Lepton Universality Using B-0 -> K(S)(0)l(+) l(-) and B+ -> K*(+)l(+)l(-) Decays
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- Aaij R
- Abdelmotteleb ASW
- Abrantes FG
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- Stenyakin O
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- Suljik F
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- Swientek K
- Szabelski A
- Szumlak T
- Szymanski M
- T'Jampens S
- Taneja S
- Tanner AR
- Tat MD
- Terentev A
- Teubert F
- Thomas E
- Thompson DJD
- Thomson KA
- Tilquin H
- Tisserand V
- Tobin M
- Tomassetti L
- Tong X
- Torreira AG
- Torres MC
- Tou DY
- Trejo RIR
- Trifonova E
- Trilov SM
- Trippl C
- Tuci G
- Tully A
- Tuning N
- Ukleja A
- Unverzagt DJ
- Ursov E
- Usachov A
- Ustyuzhanin A
- Uwer U
- Vagner A
- Vagnoni V
- Valassi A
- Valenti G
- van Beuzekom M
- Van Dijk M
- Van Hecke H
- van Herwijnen E
- van Veghel M
- Vecchi S
- Velthuis JJ
- Veltri M
- Venkateswaran A
- Veronesi M
- Vesterinen M
- Vidal AC
- Vidal AR
- Vidal FM
- Vidal JR
- Vidal XC
- Vieira D
- Viemann H
- Vilasis-Cardona X
- Villa A
- Vincent P
- Volle FC
- Vom Bruch D
- Vorobyev A
- Vorobyev V
- Voropaev N
- Vos K
- Waldi R
- Walsh J
- Wang C
- Wang J
- Wang J
- Wang J
- Wang J
- Wang M
- Wang R
- Wang Y
- Wang Z
- Wang Z
- Wang Z
- Ward JA
- Watson NK
- Weber SG
- Websdale D
- Weisser C
- Westhenry BDC
- White DJ
- Whitehead M
- Wiederhold AR
- Wiedner D
- Wilkinson G
- Wilkinson M
- Williams I
- Williams M
- Williams MRJ
- Wilson FF
- Wislicki W
- Witek M
- Witola L
- Wormser G
- Wotton SA
- Wu H
- Wyllie K
- Xiang Z
- Xiao D
- Xie Y
- Xu A
- Xu J
- Xu L
- Xu M
- Xu Q
- Xu Z
- Xu Z
- Yang D
- Yang S
- Yang Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu X
- Zhu X
- Zhu Z
- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Tests of lepton universality in B-0 -> K(S)(0)l(+)l(-) and B+ -> K*(+)l(+)l(-) decays where l is either an electron or a muon are presented. The differential branching fractions of B-0 -> K(S)(0)e(+)e(-) and B+ -> K*(+)e(+)e(-) decays are measured in intervals of the dilepton invariant mass squared. The measurements are performed using proton-proton collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 9 fb(-1). The results are consistent with the standard model and previous tests of lepton universality in related decay modes. The first observation of B-0 -> K(S)(0)e(+)e(-) and B+ -> K*(+)e(+)e(-) decays is reported
Measurement of prompt charged-particle production in pp collisions at root s=13 TeV
- Author
- Aaij R
- Abrantes FG
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Alasfar L
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Arribas JMFT
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Becker M
- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Beteta CA
- Betti F
- Bezshyiko I
- Bhasin S
- Bhom J
- Bian L
- Bieker MS
- Bifani S
- Billoir P
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Bjorn M
- Blago MP
- Blake T
- Blanc F
- Blusk S
- Bobulska D
- Boelhauve JA
- Boettcher T
- Boldyrev A
- Bondar A
- Bondar N
- Borghi S
- Borisyak M
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brodski M
- Brodzicka J
- Brundu D
- Buonaura A
- Burr C
- Bursche A
- Butkevich A
- Butter JS
- Buytaert J
- Byczynski W
- Cadeddu S
- Cai H
- Calabrese R
- Calefice L
- Cali S
- Calladine R
- Calvi M
- Campana P
- Canudas NV
- Capelli S
- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carli I
- Carniti P
- Cartelle PA
- Carus L
- Casasus MP
- Casse G
- Castro JL
- Cattaneo M
- Cavallero G
- Cazon BRG
- Celani S
- Cerasoli J
- Chadwick AJ
- Chapman MG
- Charles M
- Charpentier P
- Chatzikonstantinidis G
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
- Cicala MF
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Cobbledick JL
- Coco V
- Coelho JAB
- Cogan J
- Cogneras E
- Cojocariu L
- Collins P
- Colombo T
- Congedo L
- Contu A
- Cooke N
- Coombs G
- Corti G
- Coutinho RS
- Couturier B
- Craik DC
- Crkovska J
- Currie R
- D'Ambrosio C
- D'Argent P
- Da Silva CL
- Dadabaev S
- Dall'Occo E
- Dalseno J
- Danilina A
- Davis A
- De Almeida FLS
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Paula BS
- De Paula L
- De Serio M
- De Simone D
- De Simone P
- de Vries JA
- Dean CT
- Decamp D
- Del Buono L
- Delaney B
- Dembinski HP
- Dendek A
- Denysenko V
- Derkach D
- Deschamps O
- Desse F
- Dettori F
- Dey B
- Di Cicco A
- Di Nezza P
- Diaz LC
- Diaz MV
- Didenko S
- Dijkstra H
- Dobishuk V
- Donohoe AM
- Dordei F
- dos Reis AC
- Douglas L
- Dovbnya A
- Downes AG
- Dreimanis K
- Dudek MW
- Dufour L
- Duk V
- Durante P
- Durham JM
- Dutta D
- Dziurda A
- Dzyuba A
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Ek-In S
- Eklund L
- Ely S
- Ene A
- Epple E
- Escher S
- Eschle J
- Esen S
- Evans T
- Falabella A
- Fan J
- Fan Y
- Fang B
- Farry S
- Fazzini D
- Feo M
- Fernandez SG
- Fernez AD
- Ferrari F
- Ferrillo M
- Ferro-Luzzi M
- Figueras EV
- Filippov S
- Fini RA
- Fiorini M
- Firlej M
- Fischer KM
- Fitzgerald DS
- Fitzpatrick C
- Fiutowski T
- Fkiaras A
- Fleuret F
- Fontana M
- Fontanelli F
- Forty R
- Francisco OD
- Frank M
- Franzoso E
- Frau G
- Frei C
- Friday DA
- Fu J
- Fuehring Q
- Funk W
- Gabriel E
- Gaintseva T
- Galli D
- Gambetta S
- Gan Y
- Gandelman M
- Gandini P
- Gao Y
- Garau M
- Garcia LM
- Garcia OB
- Garrido L
- Gaspar C
- Geertsema RE
- Gerick D
- Gerken LL
- Gersabeck E
- Gersabeck M
- Gershon T
- Gerstel D
- Ghez P
- Gibson V
- Giemza HK
- Giovannetti M
- Gioventu A
- Gironell PG
- Giubega L
- Giugliano C
- Gizdov K
- Gkougkousis EL
- Gligorov VV
- Gobel C
- Goicochea JMO
- Golobardes E
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
- Gomez RV
- Goncerz M
- Gong G
- Gonzalo AB
- Gonzalo DS
- Gorbounov P
- Gorelov IV
- Gotti C
- Govorkova E
- Grabowski JP
- Grammatico T
- Gras CS
- Grauges E
- Graverini E
- Graziani G
- Grecu A
- Greeven LM
- Griffith P
- Grillo L
- Gromov S
- Gu C
- Guarise M
- Gunther PA
- Gushchin E
- Guth A
- Guz Y
- Gys T
- Hadavizadeh T
- Haefeli G
- Haen C
- Haimberger J
- Halewood-leagas T
- Hamilton PM
- Hammerich JP
- Han Q
- Han X
- Hancock TH
- Hansmann-Menzemer S
- Harnew N
- Harrison T
- Hasse C
- Hatch M
- He J
- Hecker M
- Heijhoff K
- Heinicke K
- Hennequin AM
- Hennessy K
- Henry L
- Heuel J
- Hicheur A
- Hill D
- Hilton M
- Hollitt SE
- Hu J
- Hu J
- Hu W
- Hu X
- Huang W
- Huang X
- Hulsbergen W
- Hunter RJ
- Hushchyn M
- Hutchcroft D
- Hynds D
- Ibis P
- Idzik M
- Ilin D
- Ilten P
- Inglessi A
- Ishteev A
- Ivshin K
- Jacobsson R
- Jakobsen S
- Jans E
- Jashal BK
- Jawahery A
- Jevtic V
- Jezabek M
- Jiang F
- John M
- Johnson D
- Jones CR
- Jones TP
- Jost B
- Jurik N
- Kandybei S
- Kang Y
- Karacson M
- Karpov M
- Keizer F
- Kenzie M
- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Klimaszewski K
- Koliiev S
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
- Korolev M
- Kostiuk I
- Kot O
- Kotriakhova S
- Kravchenko P
- Kravchuk L
- Krawczyk RD
- Kreps M
- Kress F
- Kretzschmar S
- Krokovny P
- Krupa W
- Krzemien W
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- Kuindersma HS
- Kunde GJ
- Kvaratskheliya T
- Lacarrere D
- Lafferty G
- Lai A
- Lamas MR
- Lampis A
- Lancierini D
- Lane JJ
- Lane R
- Lanfranchi G
- Langenbruch C
- Langer J
- Lantwin O
- Latham T
- Lavra LS
- Lazzari F
- Le Gac R
- Lee SH
- Lefevre R
- Leflat A
- Legotin S
- Leite JB
- Lener MP
- Leroy O
- Lesiak T
- Leverington B
- Li H
- Li L
- Li P
- Li S
- Li Y
- Li Y
- Li Z
- Liang X
- Lima VF
- Lin T
- Lindner R
- Lisovskyi V
- Litvinov R
- Liu G
- Liu H
- Liu S
- Loi A
- Longstaff I
- Lopes JH
- Lopes LF
- Lopez JAR
- Lovell GH
- Lu Y
- Lucchesi D
- Luchuk S
- Lukashenko V
- Luo Y
- Lupato A
- Luppi E
- Lupton O
- Lusiani A
- Lyu X
- Ma L
- Ma R
- Maccolini S
- Machado DT
- Machefert F
- Maciuc F
- Macko V
- Mackowiak P
- Maddrell-Mander S
- Madejczyk O
- Maev O
- Maevskiy A
- Magalhaes PC
- Maisuzenko D
- Majewski MW
- Malczewski JJ
- Malde S
- Malecki B
- Malinin A
- Maltsev T
- Malygina H
- Manca G
- Mancinelli G
- Manuzzi D
- Marangotto D
- Maratas J
- Marchand JF
- Marconi U
- Mariani S
- Marinangeli M
- Marks J
- Maronas LD
- Marshall AM
- Marshall PJ
- Martellotti G
- Martin LMG
- Martinazzoli L
- Martinelli M
- Martinez ML
- Massafferri A
- Materok M
- Matev R
- Mathad A
- Mathe Z
- Matiunin V
- Matteuzzi C
- Mattioli KR
- Mauri A
- Maurice E
- Mauricio J
- Mazurek M
- McCann M
- Mcconnell L
- Mcgrath TH
- McNab A
- McNulty R
- Mead JV
- Meadows B
- Meier G
- Meinert N
- Melnychuk D
- Meloni S
- Merk M
- Merli A
- Mikhasenko M
- Milanes DA
- Millard E
- Milovanovic M
- Minard MN
- Minotti A
- Minzoni L
- Mitchell SE
- Mitreska B
- Mitzel DS
- Modden A
- Mohammed RA
- Mohan LRM
- Moise RD
- Mombacher T
- Monroy IA
- Monteil S
- Morandin M
- Morello G
- Morello MJ
- Moreno PG
- Moron J
- Morris AB
- Morris AG
- Mountain R
- Mu H
- Muheim F
- Mulder M
- Muller D
- Muller K
- Murphy CH
- Murray D
- Muzzetto P
- Naik P
- Nakada T
- Nandakumar R
- Nanut T
- Nasteva I
- Needham M
- Neri I
- Neri N
- Neubert S
- Neufeld N
- Newcombe R
- Nguyen TD
- Nguyen-Mau C
- Niel EM
- Nieswand S
- Nikitin N
- Nolte NS
- Norella ES
- Normand C
- Nunez C
- O'Hanlon DP
- O'neil RH
- Oblakowska-Mucha A
- Obraztsov V
- Oldeman R
- Olivares ME
- Onderwater CJG
- Ossowska A
- Ovsiannikova T
- Owen P
- Oyanguren A
- Pagare B
- Pais PR
- Pajero T
- Palano A
- Palutan M
- Pan Y
- Panshin G
- Papanestis A
- Pappagallo M
- Pappalardo LL
- Pappenheimer C
- Pardinas JG
- Parker W
- Parkes C
- Parkinson CJ
- Passalacqua B
- Passaleva G
- Pastore A
- Patel M
- Patrignani C
- Pawley CJ
- Pearce A
- Pellegrino A
- Perazzini S
- Pereima D
- Pernas MR
- Perret P
- Petric M
- Petridis K
- Petrolini A
- Petrov A
- Petrucci S
- Petruzzo M
- Pham TTH
- Philippov A
- Pica L
- Piccini M
- Pietrzyk B
- Pietrzyk G
- Pili M
- Pinci D
- Pisani F
- Placinta V
- Plana BG
- Plews J
- Polci F
- Poliakova M
- Poluektov A
- Polukhina N
- Polyakov I
- Polycarpo E
- Pomery GJ
- Ponce S
- Popov D
- Popov S
- Poslavskii S
- Prasanth K
- Prieto AF
- Promberger L
- Prouve C
- Pugatch V
- Pullen H
- Punzi G
- Qi H
- Qian W
- Qin J
- Qin N
- Quagliani R
- Quezada AFC
- Quintana B
- Raab NV
- Rachwal B
- Rademacker JH
- Rama M
- Rangel MS
- Ratnikov F
- Raven G
- Reboud M
- Redi F
- Regueiro PV
- Reiss F
- Ren Z
- Renaudin V
- Resmi PK
- Ribatti R
- Ricciardi S
- Rinnert K
- Rios CS
- Robbe P
- Robertson G
- Rodrigues AB
- Rodrigues E
- Rodrigues FF
- Rodriguez AB
- Rodriguez PB
- Rollings A
- Roloff P
- Romanovskiy V
- Rosales FAG
- Roth JD
- Rotondo M
- Rudolph MS
- Ruf T
- Ryzhikov A
- Ryzka J
- Sagidova N
- Sahoo N
- Saitta B
- Salomoni M
- Santacesaria R
- Santimaria M
- Santos DM
- Santovetti E
- Saranin D
- Sarpis G
- Sarpis M
- Sarti A
- Satriano C
- Satta A
- Saur M
- Savrina D
- Sazak H
- Scarabotto A
- Schael S
- Schiller M
- Schindler H
- Schmelling M
- Schmidt B
- Schneider O
- Schopper A
- Schubiger M
- Schulte S
- Schune MH
- Schwemmer R
- Sciascia B
- Sellam S
- Semennikov A
- Sergi A
- Serra N
- Sestini L
- Seuthe A
- Sevilla MF
- Seyfert P
- Shang Y
- Shangase DM
- Shapkin M
- Shchemerov I
- Shchutska L
- Shears T
- Shekhtman L
- Shen Z
- Shevchenko V
- Shields EB
- Shmanin E
- Shupperd JD
- Siddi BG
- Sierra CV
- Silva JJS
- Simi G
- Simone S
- Skidmore N
- Skwarnicki T
- Slater MW
- Slazyk I
- Smallwood JC
- Smead LGS
- Smeaton JG
- Smetkina A
- Smith E
- Smith M
- Snoch A
- Soares M
- Soares MS
- Sobral CMC
- Sokoloff MD
- Sole SF
- Soler FJP
- Solovev A
- Solovyev I
- Spaan B
- Spradlin P
- Stagni F
- Stahl M
- Stahl S
- Stefko P
- Steinkamp O
- Stenyakin O
- Stevens H
- Stone S
- Stramaglia ME
- Straticiuc M
- Strekalina D
- Suljik F
- Sun J
- Sun L
- Sun Y
- Svihra P
- Swallow PN
- Swientek K
- Szabelski A
- Szumlak T
- Szymanski M
- T'Jampens S
- Taneja S
- Tanner AR
- Terentev A
- Teubert F
- Thomas E
- Thomson KA
- Tisserand V
- Tobin M
- Tomassetti L
- Torreira AG
- Torres MC
- Tou DY
- Tran MT
- Trejo RIR
- Trifonova E
- Trippl C
- Tuci G
- Tully A
- Tuning N
- Ukleja A
- Unverzagt DJ
- Ursov E
- Usachov A
- Ustyuzhanin A
- Uwer U
- Vagner A
- Vagnoni V
- Valassi A
- Valenti G
- van Beuzekom M
- Van Dijk M
- van Herwijnen E
- Van Hulse CB
- van Veghel M
- Vecchi S
- Velthuis JJ
- Veltri M
- Venkateswaran A
- Veronesi M
- Vesterinen M
- Vidal AC
- Vidal AR
- Vidal FM
- Vidal JR
- Vidal XC
- Vieira D
- Viemann H
- Vilasis-Cardona X
- Villa A
- Vincent P
- Vom Bruch D
- Vorobyev A
- Vorobyev V
- Voropaev N
- Vos K
- Waldi R
- Walsh J
- Wang C
- Wang J
- Wang J
- Wang J
- Wang J
- Wang M
- Wang R
- Wang Y
- Wang Z
- Wang Z
- Wark HM
- Watson NK
- Weber SG
- Websdale D
- Weisser C
- Westhenry BDC
- White DJ
- Whitehead M
- Wiedner D
- Wilkinson G
- Wilkinson M
- Williams I
- Williams M
- Williams MRJ
- Wilson FF
- Wislicki W
- Witek M
- Witola L
- Wormser G
- Wotton SA
- Wu H
- Wyllie K
- Xiang Z
- Xiao D
- Xie Y
- Xu A
- Xu J
- Xu L
- Xu M
- Xu Q
- Xu Z
- Xu Z
- Yang D
- Yang S
- Yang Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang Y
- Zhang Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou X
- Zhou Y
- Zhu X
- Zhu Z
- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
The differential cross-section of prompt inclusive production of long-lived charged particles in proton-proton collisions is measured using a data sample recorded by the LHCb experiment at a centre-of-mass energy of root s = 13 TeV. The data sample, collected with an unbiased trigger, corresponds to an integrated luminosity of 5.4 nb(-1). The differential cross-section is measured as a function of transverse momentum and pseudorapidity in the ranges P-T is an element of [80, 10 000) MeV/c and eta is an element of [2.0, 4.8) and is determined separately for positively and negatively charged particles. The results are compared with predictions from various hadronic-interaction models
Measurement of the photon polarization in Lambda(0)(b) -> Lambda gamma decays
- Author
- Aaij R
- Abdelmotteleb ASW
- Abrantes FG
- Abudinen F
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barbetti M
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bashir S
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
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- Zeng M
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- Zhelezov A
- Zheng Y
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- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2022
- Field of study
The photon polarization in b→sγ transitions is measured for the first time in radiative b-baryon decays exploiting the unique spin structure of Λb0→Λγ decays. A data sample corresponding to an integrated luminosity of 6 fb-1 collected by the LHCb experiment in pp collisions at a center-of-mass energy of 13 TeV is used. The photon polarization is measured to be αγ=0.82-0.26-0.13+0.17+0.04, where the first uncertainty is statistical and the second systematic. This result is in agreement with the Standard Model prediction and previous measurements in b-meson decays. Charge-parity breaking effects are studied for the first time in this observable and found to be consistent with CP symmetry
Measurement of the Nuclear Modification Factor and Prompt Charged Particle Production in p-Pb and pp Collisions at root s(NN )=5 TeV
- Author
- Aaij R
- Abrantes FG
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bassi G
- Batsukh B
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- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Beteta CA
- Betti F
- Bezshyiko I
- Bhasin S
- Bhom J
- Bian L
- Bieker MS
- Bifani S
- Billoir P
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Bjorn M
- Blago MP
- Blake T
- Blanc F
- Blusk S
- Bobulska D
- Boelhauve JA
- Boettcher T
- Boldyrev A
- Bondar A
- Bondar N
- Borghi S
- Borisyak M
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brodski M
- Brodzicka J
- Brundu D
- Buonaura A
- Burke AT
- Burr C
- Bursche A
- Butkevich A
- Butter JS
- Buytaert J
- Byczynski W
- Cadeddu S
- Cai H
- Calabrese R
- Calefice L
- Cali S
- Calladine R
- Calvi M
- Campana P
- Canudas NV
- Capelli S
- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carli I
- Carniti P
- Cartelle PA
- Carus L
- Casasus MP
- Casse G
- Castro JL
- Cattaneo M
- Cavallero G
- Cazon BRG
- Celani S
- Cerasoli J
- Chadwick AJ
- Chapman MG
- Charles M
- Charpentier P
- Chatzikonstantinidis G
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
- Cicala MF
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Cobbledick JL
- Coco V
- Coelho JAB
- Cogan J
- Cogneras E
- Cojocariu L
- Collins P
- Colombo T
- Congedo L
- Contu A
- Cooke N
- Coombs G
- Corredoira I
- Corti G
- Coutinho RS
- Couturier B
- Craik DC
- Crkovska J
- Currie R
- D'Ambrosio C
- D'Argent P
- Da Silva CL
- Dadabaev S
- Dai L
- Dall'Occo E
- Dalseno J
- Danilina A
- Davies JE
- Davis A
- De Almeida FLS
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Paula BS
- De Paula L
- De Serio M
- De Simone D
- De Simone P
- de Vries JA
- Dean CT
- Decamp D
- Del Buono L
- Delaney B
- Dembinski HP
- Dendek A
- Denysenko V
- Derkach D
- Deschamps O
- Desse F
- Dettori F
- Dey B
- Di Cicco A
- Di Nezza P
- Diaz LC
- Diaz MV
- Didenko S
- Dijkstra H
- Dobishuk V
- Donohoe AM
- Dordei F
- dos Reis AC
- Douglas L
- Dovbnya A
- Downes AG
- Dreimanis K
- Dudek MW
- Dufour L
- Duk V
- Durante P
- Durham JM
- Dutta D
- Dziurda A
- Dzyuba A
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Ek-In S
- Eklund L
- Ely S
- Ene A
- Epple E
- Escher S
- Eschle J
- Esen S
- Evans T
- Falabella A
- Fan J
- Fan Y
- Fang B
- Farry S
- Fazzini D
- Feo M
- Fernandez SG
- Fernez AD
- Ferrari F
- Ferrillo M
- Ferro-Luzzi M
- Figueras EV
- Filippov S
- Fini RA
- Fiorini M
- Firlej M
- Fischer KM
- Fitzgerald DS
- Fitzpatrick C
- Fiutowski T
- Fkiaras A
- Fleuret F
- Fontana M
- Fontanelli F
- Forty R
- Francisco OD
- Frank M
- Franzoso E
- Frau G
- Frei C
- Friday DA
- Fu J
- Fuehring Q
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- Zdybal M
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- Zhelezov A
- Zheng Y
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- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2022
- Field of study
The production of prompt charged particles in proton-lead collisions and in proton-proton collisions at the nucleon-nucleon center-of-mass energy root s(NN) = 5 TeV is studied at LHCb as a function of pseudorapidity (eta) and transverse momentum (p(T) ) with respect to the proton beam direction. The nuclear modification factor for charged particles is determined as a function of eta between -4.8 < eta < -2.5 (backward region) and 2.0 < eta < 4.8 (forward region), and p(T) between 0.2 < p(T) < 8.0 GeV/c. The results show a suppression of charged particle production in proton-lead collisions relative to proton-proton collisions in the forward region and an enhancement in the backward region for p(T) larger than 1.5 GeV/c. This measurement constrains nuclear PDFs and saturation models at previously unexplored values of the parton momentum fraction down to 10(-6)
Branching Fraction Measurements of the Rare B-s(0) -> phi mu(+)mu(-) and B-s(0)-> f(2)' (1525)mu(+)mu(-) Decays
- Author
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- Abrantes FG
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- Aidala CA
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- Gioventu A
- Gironell PG
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- Gligorov VV
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- Greeven LM
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- Grillo L
- Gromov S
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- Guarise M
- Gunther PA
- Gushchin E
- Guth A
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- Hadavizadeh T
- Haefeli G
- Haen C
- Haimberger J
- Halewood-leagas T
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- Hancock TH
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- Harnew N
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- Hasse C
- Hatch M
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- Hecker M
- Heijhoff K
- Heinicke K
- Hennequin AM
- Hennessy K
- Henry L
- Heuel J
- Hicheur A
- Hill D
- Hilton M
- Hollitt SE
- Hu J
- Hu J
- Hu W
- Hu X
- Huang W
- Huang X
- Hulsbergen W
- Hunter RJ
- Hushchyn M
- Hutchcroft D
- Hynds D
- Ibis P
- Idzik M
- Ilin D
- Ilten P
- Inglessi A
- Ishteev A
- Ivshin K
- Jacobsson R
- Jakobsen S
- Jans E
- Jashal BK
- Jawahery A
- Jevtic V
- Jezabek M
- Jiang F
- John M
- Johnson D
- Jones CR
- Jones TP
- Jost B
- Jurik N
- Kandybei S
- Kang Y
- Karacson M
- Karpov M
- Keizer F
- Kenzie M
- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Klimaszewski K
- Koliiev S
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
- Korolev M
- Kostiuk I
- Kot O
- Kotriakhova S
- Kravchenko P
- Kravchuk L
- Krawczyk RD
- Kreps M
- Kress F
- Kretzschmar S
- Krokovny P
- Krupa W
- Krzemien W
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- Kuindersma HS
- Kunde GJ
- Kvaratskheliya T
- Lacarrere D
- Lafferty G
- Lai A
- Lamas MR
- Lampis A
- Lancierini D
- Lane JJ
- Lane R
- Lanfranchi G
- Langenbruch C
- Langer J
- Lantwin O
- Latham T
- Lavra LS
- Lazzari F
- Le Gac R
- Lee SH
- Lefevre R
- Leflat A
- Legotin S
- Leite JB
- Lener MP
- Leroy O
- Lesiak T
- Leverington B
- Li H
- Li L
- Li P
- Li S
- Li Y
- Li Y
- Li Z
- Liang X
- Lima VF
- Lin T
- Lindner R
- Lisovskyi V
- Litvinov R
- Liu G
- Liu H
- Liu S
- Loi A
- Longstaff I
- Lopes JH
- Lopes LF
- Lopez JAR
- Lovell GH
- Lu Y
- Lucchesi D
- Luchuk S
- Lukashenko V
- Luo Y
- Lupato A
- Luppi E
- Lupton O
- Lusiani A
- Lyu X
- Ma L
- Ma R
- Maccolini S
- Machado DT
- Machefert F
- Maciuc F
- Macko V
- Mackowiak P
- Maddrell-Mander S
- Madejczyk O
- Maev O
- Maevskiy A
- Magalhaes PC
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- Matteuzzi C
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- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
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- Zhang Y
- Zharkova A
- Zhelezov A
- Zheng Y
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- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
The branching fraction of the rare Bs0→φμ+μ- decay is measured using data collected by the LHCb experiment at center-of-mass energies of 7, 8, and 13 TeV, corresponding to integrated luminosities of 1, 2, and 6 fb-1, respectively. The branching fraction is reported in intervals of q2, the square of the dimuon invariant mass. In the q2 region between 1.1 and 6.0 GeV2/c4, the measurement is found to lie 3.6 standard deviations below a standard model prediction based on a combination of light cone sum rule and lattice QCD calculations. In addition, the first observation of the rare Bs0→f2′(1525)μ+μ- decay is reported with a statistical significance of 9 standard deviations and its branching fraction is determined