180 research outputs found
HIV-1 Protease and Reverse Transcriptase Control the Architecture of Their Nucleocapsid Partner
- Author
- A Apolloni
- A Billich
- A Fassati
- A Kotov
- B Liu
- B Muller
- BM Forshey
- BM Forshey
- BM Lee
- C Beloin
- D Lener
- DJ Dismuke
- Dominique Coulaud
- E Le Cam
- Eric Le Cam
- G Krishnamoorthy
- G Mirambeau
- Gilles Mirambeau
- H al-Ghusein
- H de Rocquigny
- Isabelle Borde
- J Benjamin
- J Dubochet
- J Guo
- J Lanman
- J Lehmann-Che
- J Shi
- JA Briggs
- JA Briggs
- JA Thomas
- JG Levin
- Josette Jeusset
- K Gao
- K Luo
- K Wiegers
- K Zhu
- L Bannwarth
- L Hameau
- L Kleiman
- Laurence Hameau
- M Cruceanu
- M Dettenhofer
- M Hsu
- M Joanicot
- M Li
- M Nijhuis
- M Prabu-Jeyabalan
- M Shehu-Xhilaga
- M Shehu-Xhilaga
- M Wisniewski
- M Yamashita
- Martin Egli
- Michèle Reboud-Ravaux
- MK Hill
- MV Nermut
- N Arhel
- N Sheng
- N Sheng
- P Charneau
- P Zhu
- R Khan
- RJ Fisher
- RM Anthony
- Robert J. Gorelick
- S Carteau
- S Henriet
- S Iordanskiy
- S Lyonnais
- S Lyonnais
- S Nisole
- SC Pettit
- SC Pettit
- SJ Schultz
- Sophie Lafosse
- Sébastien Lyonnais
- Tobias Restle
- W Fu
- X Veaute
- Y Jenkins
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2007
- Field of study
The HIV-1 nucleocapsid is formed during protease (PR)-directed viral maturation, and is transformed into pre-integration complexes following reverse transcription in the cytoplasm of the infected cell. Here, we report a detailed transmission electron microscopy analysis of the impact of HIV-1 PR and reverse transcriptase (RT) on nucleocapsid plasticity, using in vitro reconstitutions. After binding to nucleic acids, NCp15, a proteolytic intermediate of nucleocapsid protein (NC), was processed at its C-terminus by PR, yielding premature NC (NCp9) followed by mature NC (NCp7), through the consecutive removal of p6 and p1. This allowed NC co-aggregation with its single-stranded nucleic-acid substrate. Examination of these co-aggregates for the ability of RT to catalyse reverse transcription showed an effective synthesis of double-stranded DNA that, remarkably, escaped from the aggregates more efficiently with NCp7 than with NCp9. These data offer a compelling explanation for results from previous virological studies that focused on i) Gag processing leading to nucleocapsid condensation, and ii) the disappearance of NCp7 from the HIV-1 pre-integration complexes. We propose that HIV-1 PR and RT, by controlling the nucleocapsid architecture during the steps of condensation and dismantling, engage in a successive nucleoprotein-remodelling process that spatiotemporally coordinates the pre-integration steps of HIV-1. Finally we suggest that nucleoprotein remodelling mechanisms are common features developed by mobile genetic elements to ensure successful replication
Utilização da terapia ultra-sônica de baixa intensidade na redução da lipodistrofia ginecóide: uma terapia segura ou risco cardiovascular transitório? Um estudo pré-clínico
- Author
- Araújo M
- Barnett SB
- Barroso SG
- Coakley WT
- Dyson M
- Dyson M
- Gonçalves WLS
- Guedes DP
- Guirro
- Guirro EC
- Hogan RD
- Jones BA
- João Paulo Cirqueira
- Kornowski R
- Lener DJ
- Lip GY
- Luciana Saloto Soares
- Lyon CJ
- Margareth Ribeiro Moysés
- Moysés MR
- Moysés MR
- Nazaré Souza Bissoli
- Nedvidkova J
- Riggs PN
- Robertson VJ
- Rossi ABR
- Safanova I
- Santos RL
- Schlking P
- Shenoy U
- Stewart HD
- Vaezy S
- Vague J
- Vague J
- Washington Luiz S. Gonçalves
- Yamamoto Y
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Observation and branching fraction measurement of the decay Ξb- → Λ0 bπ -
- Author
- Aaij R
- Abdelmotteleb ASW
- Abellan Beteta C
- Abudinen F
- Ackernley T
- Adeva B
- Adinolfi M
- Adlarson P
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Ajaltouni Z
- Akar S
- Akiba K
- Albicocco P
- Albrecht J
- Alessio F
- Alexander M
- Alfonso Albero A
- Aliouche Z
- Alvarez Cartelle P
- Amalric R
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andersson M
- Andreianov A
- Andreola P
- Andreotti M
- Andreou D
- Ao D
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Atzeni M
- Audurier B
- Bacher D
- Bachiller Perea I
- Bachmann S
- Bachmayer M
- Back JJ
- Bailly reyre A
- Baladron Rodriguez P
- Balagura V
- Baldini W
- Baptista de Souza Leite J
- Barbetti M
- Barbosa IR
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga IB
- Beiter A
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Benane G
- Bencivenni G
- Berezhnoy A
- Bernet Andres S
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Betti F
- Bex J
- Bezshyiko I
- Bhom J
- Bian L
- Bieker MS
- Biesuz NV
- Billoir P
- Biolchini A
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Blago MP
- Blake T
- Blanc F
- Blank JE
- Blusk S
- Bobulska D
- Bocharnikov V
- Boelhauve JA
- Boente Garcia O
- Boettcher T
- Bohare A
- Boldyrev A
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- Borgato F
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- Borsuk JT
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- Brodzicka J
- Brossa Gonzalo A
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- Brundu D
- Buonaura A
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- Burke AT
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- Chrzaszcz M
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- Wilkinson MK
- Williams I
- Williams M
- Williams MRJ
- Williams R
- Wilson FF
- Wislicki W
- Witek M
- Witola L
- Wong CP
- Wormser G
- Wotton SA
- Wu H
- Wu J
- Wu Y
- Wyllie K
- Xian S
- Xiang Z
- Xie Y
- Xu A
- Xu J
- Xu L
- Xu M
- Xu Z
- Yang D
- Yang S
- Yang X
- Yang Y
- Yang Z
- Yeroshenko V
- Yeung H
- Yin H
- Yu CY
- Yu J
- Yuan X
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zeng M
- Zhang C
- Zhang D
- Zhang J
- Zhang L
- Zhang S
- Zhang Y
- Zhao Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu LZ
- Zhu X
- Zhu Z
- Zhukov V
- Zhuo J
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
Precision measurement of CP violation in the penguin-mediated decay Bs0→ϕϕ
- Author
- Aaij R
- Abdelmotteleb ASW
- Abellan Beteta C
- Abudinén F
- Ackernley T
- Adeva B
- Adinolfi M
- Adlarson P
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Ajaltouni Z
- Akar S
- Akiba K
- Albicocco P
- Albrecht J
- Alessio F
- Alexander M
- Alfonso Albero A
- Aliouche Z
- Alvarez Cartelle P
- Amalric R
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andersson M
- Andreianov A
- Andreotti M
- Andreou D
- Ao D
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Atzeni M
- Audurier B
- Bachiller Perea IB
- Bachmann S
- Bachmayer M
- Back JJ
- Bailly-Reyre A
- Baladron Rodriguez P
- Balagura V
- Baldini W
- Baptista de Souza Leite J
- Barbetti M
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bassi G
- Batozskaya V
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga IB
- Beiter A
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Benane G
- Bencivenni G
- Berezhnoy A
- Bernet Andres S
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Betti F
- Bezshyiko Ia
- Bhom J
- Bian L
- Bieker MS
- Biesuz NV
- Billoir P
- Biolchini A
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Blago MP
- Blake T
- Blanc F
- Blank JE
- Blusk S
- Bobulska D
- Bocharnikov VB
- Boelhauve JA
- Boente Garcia O
- Boettcher T
- Boldyrev A
- Bolognani CS
- Bolzonella R
- Bondar N
- Borgato F
- Borghi S
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brea Rodriguez A
- Breer N
- Brodzicka J
- Brossa Gonzalo A
- Brown 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
- Calvi M
- Calvo Gomez M
- Campana P
- Campora Perez DH
- Campoverde Quezada AF
- Capelli S
- Capriotti L
- Carbone A
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- Cardini A
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- Casais Vidal A
- Caspary R
- Casse G
- Cattaneo M
- Cavallero G
- Cavallini V
- Celani S
- Cerasoli J
- Cervenkov D
- Chadwick AJ
- Chahrour IC
- Chapman MG
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- Charpentier Ph
- Chavez Barajas CA
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chernyshenko S
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
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- Kot O
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- Lee SH
- Leflat A
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- Lesiak T
- Leverington B
- LHCb Collaboration
- Li A
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- Westhenry BDC
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- Wilson FF
- Wislicki W
- Witek M
- Witola L
- Wong CP
- Wormser G
- Wotton SA
- Wu H
- Wu J
- Wu Y
- Wyllie K
- Xiang Z
- Xie Y
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- Xu L
- Xu L
- Xu M
- Xu Q
- Xu Z
- Xu Z
- Xu Z
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- Yang Y
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- Yeroshenko V
- Yeung H
- Yin H
- Yu J
- Yuan X
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zeng M
- Zhang C
- Zhang D
- Zhang JZ
- Zhang L
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zhao Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu X
- Zhu X
- Zhu Z
- Zhukov V
- Zhuo J
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
A flavor-tagged time-dependent angular analysis of the decay
Bs0→ϕϕ is performed using pp collision data collected
by the LHCb experiment at % at s=13 TeV, the center-of-mass energy of
13 TeV, corresponding to an integrated luminosity of 6 fb^{-1}. The
CP-violating phase and direct CP-violation parameter are measured
to be ϕssˉs=−0.042±0.075±0.009 rad and
∣λ∣=1.004±0.030±0.009, respectively, assuming the same values
for all polarization states of the ϕϕ system. In these results, the
first uncertainties are statistical and the second systematic. These parameters
are also determined separately for each polarization state, showing no evidence
for polarization dependence. The results are combined with previous LHCb
measurements using pp collisions at center-of-mass energies of 7 and 8 TeV,
yielding ϕssˉs=−0.074±0.069 rad and ∣lambda∣=1.009±0.030. This is the most precise study of time-dependent CP violation
in a penguin-dominated B meson decay. The results are consistent with
CP symmetry and with the Standard Model predictions.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2023-001.html (LHCb
public pages
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
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- Yao Y
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- Yin H
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- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
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- Zharkova A
- Zhelezov A
- Zheng Y
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- Zhovkovska V
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- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- 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
Measurement of the Λb0→Λ(1520)μ+μ− differential branching fraction
- Author
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- Craik DC
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- d'Argent P
- Da Silva CL
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- Westhenry BDC
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- Wislicki W
- Witek M
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- Wong CP
- Wormser G
- Wotton SA
- Wu H
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- Wyllie K
- Xiang Z
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- Yeomans LE
- Yeroshenko V
- Yeung H
- Yin H
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- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zeng M
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- Zhang S
- Zhang Y
- Zhang Y
- Zhao Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
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- Zhu X
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- Zhu Z
- Zhukov V
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
The branching fraction of the rare decay Λb0→Λ(1520)μ+μ− is measured for the first time, in the squared dimuon mass
intervals, q2, excluding the J/ψ and ψ(2S) regions. The data
sample analyzed was collected by the LHCb experiment at center-of-mass energies
of 7, 8, and 13 TeV, corresponding to a total integrated luminosity of $9\
\mathrm{fb}^{-1}.Theresultinthehighestq^{2}interval,q^{2} >15.0\
\mathrm{GeV}^2/c^4$, where theoretical predictions have the smallest model
dependence, agrees with the predictions.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-050.html (LHCb
public pages
Search for beautiful tetraquarks in the <i>ϒ</i>(1<i>S</i>)μ<sup>+</sup>μ<sup>−</sup> invariant-mass spectrum
- Author
- A Ali
- A Esposito
- A. A. Alves
- A. Alfonso Albero
- A. Artamonov
- A. B. Morris
- A. B. Rodrigues
- A. Baranov
- A. Bay
- A. Beiter
- A. Berezhnoy
- A. Bertolin
- A. Birnkraut
- A. Bizzeti
- A. Bondar
- A. Brossa Gonzalo
- A. Buonaura
- A. Bursche
- A. C. dos Reis
- A. Camboni
- A. Carbone
- A. Cardini
- A. Chubykin
- A. Comerma-Montells
- A. Contu
- A. Crocombe
- A. Danilina
- A. Davis
- A. Dendek
- A. Di Canto
- A. Dosil Suárez
- A. Dovbnya
- A. Dziurda
- A. Dzyuba
- A. Ene
- A. Falabella
- A. Fernandez Prieto
- A. Gallas Torreira
- A. Golutvin
- A. Gomes
- A. Grecu
- A. Heister
- A. Hicheur
- A. Jawahery
- A. K. Kuonen
- A. Lai
- A. Leflat
- A. Loi
- A. Lupato
- A. Lusiani
- A. Malinin
- A. Massafferri
- A. Mathad
- A. Mauri
- A. Mazurov
- A. McNab
- A. Merli
- A. Mogini
- A. Mödden
- A. Nandi
- A. Nogay
- A. Oblakowska-Mucha
- A. Ossowska
- A. Oyanguren
- A. Palano
- A. Papanestis
- A. Pastore
- A. Pearce
- A. Pellegrino
- A. Petrolini
- A. Petrov
- A. Piucci
- A. Poluektov
- A. Popov
- A. Puig Navarro
- A. Robert
- A. Rogozhnikov
- A. Rollings
- A. Romero Vidal
- A. Sarti
- A. Satta
- A. Schopper
- A. Sciubba
- A. Semennikov
- A. Sergi
- A. Seuthe
- A. Stocchi
- A. Tayduganov
- A. Trisovic
- A. Tsaregorodtsev
- A. Tully
- A. Ukleja
- A. Usachov
- A. Ustyuzhanin
- A. Vagner
- A. Valassi
- A. Venkateswaran
- A. Vitkovskiy
- A. Vollhardt
- A. Vorobyev
- A. Weiden
- A. Xu
- A. Zhelezov
- AV Berezhnoy
- B. Adeva
- B. Audurier
- B. Batsukh
- B. Couturier
- B. Delaney
- B. Dey
- B. G. Siddi
- B. Garcia Plana
- B. Hamilton
- B. Jost
- B. Khanji
- B. Leverington
- B. Malecki
- B. Maurin
- B. Meadows
- B. Pietrzyk
- B. Quintana
- B. R. Gruberg Cazon
- B. Rachwal
- B. Saitta
- B. Sanmartin Sedes
- B. Schmidt
- B. Sciascia
- B. Souza De Paula
- B. Spaan
- B. Storaci
- B. Voneki
- C Hughes
- C. A. Aidala
- C. Betancourt
- C. Bozzi
- C. Burr
- C. Chen
- C. D’Ambrosio
- C. Fitzpatrick
- C. Frei
- C. Färber
- C. Gaspar
- C. Gotti
- C. Gu
- C. Göbel
- C. H. Murphy
- C. Hadjivasiliou
- C. Haen
- C. Hasse
- C. J. G. Onderwater
- C. Joram
- C. Khurewathanakul
- C. L. Da Silva
- C. Langenbruch
- C. Lazzeroni
- C. M. Costa Sobral
- C. Marin Benito
- C. Matteuzzi
- C. Meaux
- C. Nguyen-Mau
- C. Parkes
- C. Patrignani
- C. Potterat
- C. Prouve
- C. R. Jones
- C. Remon Alepuz
- C. Sanchez Gras
- C. Sanchez Mayordomo
- C. Santamarina Rios
- C. Satriano
- C. T. Dean
- C. Vázquez Sierra
- C. Weisser
- D. A. Milanes
- D. Berninghoff
- D. Bobulska
- D. Brundu
- D. C. Craik
- D. Chamont
- D. Decamp
- D. Derkach
- D. Dutta
- D. Fazzini
- D. Galli
- D. Gascon
- D. Gerick
- D. Gerstel
- D. Golubkov
- D. H. Campora Perez
- D. Hill
- D. Hutchcroft
- D. Hynds
- D. Johnson
- D. Lacarrere
- D. Lancierini
- D. Loh
- D. Lucchesi
- D. Maisuzenko
- D. Marangotto
- D. Martinez Santos
- D. Melnychuk
- D. Murray
- D. Müller
- D. P. O’Hanlon
- D. Pereima
- D. Pinci
- D. Popov
- D. R. Ward
- D. S. Mitzel
- D. Savrina
- D. Tonelli
- D. Vieira
- D. Websdale
- D. Xiao
- D. Y. Tou
- D. Zhang
- DJ Lange
- E. Aslanides
- E. Ben-Haim
- E. Bertholet
- E. Buchanan
- E. Cogneras
- E. Dall’Occo
- E. Gabriel
- E. Gersabeck
- E. Govorkova
- E. Graugés
- E. Graverini
- E. Gushchin
- E. Jans
- E. Khairullin
- E. Luppi
- E. Maurice
- E. Michielin
- E. Millard
- E. Polycarpo
- E. Price
- E. Rodrigues
- E. S. Sepulveda
- E. Santovetti
- E. Shmanin
- E. Smith
- E. Thomas
- E. Tournefier
- E. van Herwijnen
- F-K Guo
- F. Alessio
- F. Archilli
- F. Baryshnikov
- F. Bedeschi
- F. Betti
- F. Blanc
- F. Bossu
- F. Da Cunha Marinho
- F. Desse
- F. Dettori
- F. Dordei
- F. F. Wilson
- F. Ferrari
- F. Ferreira Rodrigues
- F. Fleuret
- F. Fontanelli
- F. J. P. Soler
- F. Jiang
- F. Keizer
- F. Kress
- F. Lemaitre
- F. Lionetto
- F. Machefert
- F. Maciuc
- F. Martinez Vidal
- F. Meier
- F. Muheim
- F. Pisani
- F. Polci
- F. Ratnikov
- F. Redi
- F. Reiss
- F. Stagni
- F. Teubert
- G. A. Cowan
- G. Alkhazov
- G. Andreassi
- G. Bencivenni
- G. Carboni
- G. Casse
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- V. Tisserand
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- V. Volkov
- V. Vorobyev
- V. Zhukov
- W Chen
- W. Baldini
- W. Barter
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- W. C. Zhang
- W. Funk
- W. Hu
- W. Huang
- W. Hulsbergen
- W. Krupa
- W. Krzemien
- W. Kucewicz
- W. Parker
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- X. Cid Vidal
- X. Han
- X. Liang
- X. Liu
- X. Lyu
- X. Vilasis-Cardona
- X. Yuan
- X. Zhu
- Y. Amhis
- Y. Gan
- Y. Gao
- Y. Shcheglov
- Y. Wang
- Y. Xie
- Y. Yao
- Y. Zhang
- Y. Zheng
- Yu. Guz
- Z-G Wang
- Z. Ajaltouni
- Z. C. Huard
- Z. Li
- Z. Mathe
- Z. Ren
- Z. Tang
- Z. Wang
- Z. Xu
- Z. Xu
- Z. Yang
- Z. Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
International audienceThe ϒ(1S)μ+μ− invariant-mass distribution is investigated for a possible exotic meson state composed of two b quarks and two b quarks, Xbbbb . The analysis is based on a data sample of pp collisions recorded with the LHCb detector at centre-of-mass energies s=7 , 8 and 13 TeV, corresponding to an integrated luminosity of 6.3 fb−1. No significant excess is found, and upper limits are set on the product of the production cross-section and the branching fraction as functions of the mass of the Xbbbb state. The limits are set in the fiducial volume where all muons have pseudorapidity in the range [2.0, 5.0], and the Xbbbb state has rapidity in the range [2.0, 4.5] and transverse momentum less than 15 GeV/c
Measurement of the CKM angle γ using<i> B</i><sup>±</sup> → <i>DK</i><sup>±</sup> with D → K <sub>S</sub> <sup>0</sup> π<sup>+</sup>π<sup>−</sup>, K <sub>S</sub> <sup>0</sup> K<sup>+</sup>K<sup>−</sup> decays
- Author
- A Bondar
- A Bondar
- A. A. Alves
- A. Alfonso Albero
- A. Artamonov
- A. B. Morris
- A. B. Rodrigues
- A. Baranov
- A. Bay
- A. Beiter
- A. Berezhnoy
- A. Bertolin
- A. Birnkraut
- A. Bizzeti
- A. Bondar
- A. Buonaura
- A. Bursche
- A. C. dos Reis
- A. Camboni
- A. Carbone
- A. Cardini
- A. Chubykin
- A. Comerma-Montells
- A. Contu
- A. Crocombe
- A. Danilina
- A. Davis
- A. Dendek
- A. Di Canto
- A. Dosil Suárez
- A. Dovbnya
- A. Dziurda
- A. Dzyuba
- A. Ene
- A. Falabella
- A. Fernandez Prieto
- A. Gallas Torreira
- A. Golutvin
- A. Gomes
- A. Grecu
- A. Heister
- A. Hicheur
- A. Jawahery
- A. K. Kuonen
- A. Lai
- A. Leflat
- A. Loi
- A. Lupato
- A. Lusiani
- A. Malinin
- A. Massafferri
- A. Mathad
- A. Mauri
- A. Mazurov
- A. McNab
- A. Merli
- A. Mogini
- A. Nandi
- A. Nogay
- A. Oblakowska-Mucha
- A. Ossowska
- A. Oyanguren
- A. Palano
- A. Papanestis
- A. Pastore
- A. Pearce
- A. Pellegrino
- A. Petrolini
- A. Petrov
- A. Piucci
- A. Poluektov
- A. Popov
- A. Puig Navarro
- A. Robert
- A. Rogozhnikov
- A. Rollings
- A. Romero Vidal
- A. Sarti
- A. Satta
- A. Schopper
- A. Sciubba
- A. Semennikov
- A. Sergi
- A. Tayduganov
- A. Trisovic
- A. Tsaregorodtsev
- A. Tully
- A. Ukleja
- A. Usachov
- A. Ustyuzhanin
- A. Vagner
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- B. Leverington
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- B. Maurin
- B. Meadows
- B. Pietrzyk
- B. Quintana
- B. R. Gruberg Cazon
- B. Rachwal
- B. Saitta
- B. Sanmartin Sedes
- B. Schmidt
- B. Sciascia
- B. Souza De Paula
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- C. A. Aidala
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- DJ Lange
- E. Aslanides
- E. Ben-Haim
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- F James
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- I Belyaev
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- X. Cid Vidal
- X. Han
- X. Liang
- X. Liu
- X. Lyu
- X. Vilasis-Cardona
- X. Yuan
- X. Zhu
- Y Freund
- Y Grossman
- Y. Amhis
- Y. Gao
- Y. Shcheglov
- Y. Wang
- Y. Xie
- Y. Yao
- Y. Zhang
- Y. Zheng
- Yu. Guz
- Z. Ajaltouni
- Z. C. Huard
- Z. Li
- Z. Mathe
- Z. Ren
- Z. Tang
- Z. Wang
- Z. Xu
- Z. Xu
- Z. Yang
- Z. Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
A binned Dalitz plot analysis of B±→DK± decays, with D→KS0π+π− and D→KS0K+K−, is used to perform a
measurement of the CP-violating observables x± and y±, which are
sensitive to the Cabibbo-Kobayashi-Maskawa angle γ. The analysis is
performed without assuming any D decay model, through the use of information
on the strong-phase variation over the Dalitz plot from the CLEO collaboration.
Using a sample of proton-proton collision data collected with the LHCb
experiment in 2015 and 2016, and corresponding to an integrated luminosity of
2.0fb−1, the values of the CP violation parameters are found to
be x−=(9.0±1.7±0.7±0.4)×10−2, y−=(2.1±2.2±0.5±1.1)×10−2, x+=(−7.7±1.9±0.7±0.4)×10−2, and y+=(−1.0±1.9±0.4±0.9)×10−2. The first
uncertainty is statistical, the second is systematic, and the third is due to
the uncertainty on the strong-phase measurements. These values are used to
obtain \gamma = \left(87\,^{+11}_{-12}\right)^\circ, rB=0.086−0.014+0.013, and δB=(101±11)∘, where rB is the ratio
between the suppressed and favoured B-decay amplitudes and δB is the
corresponding strong-interaction phase difference. This measurement is combined
with the result obtained using 2011 and 2012 data collected with the \lhcb
experiment, to give \gamma = \left(80\,^{+10}_{\,-9}\right)^\circ, rB=0.080±0.011, and δB=(110±10)∘.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2018-017.html.
Version 2 includes minor changes made during journal revie
Angular Analysis of the B+ -> K*(+)mu(+) mu(-) Decay
- Author
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- Pawley CJ
- Pearce A
- Pellegrino A
- Perazzini S
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- Pernas M Ramos
- Perret P
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- Sellam S
- Semennikov A
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- Shields EB
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- Shupperd JD
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- Sierra C Vazquez
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- Skiba I
- Skidmore N
- Skwarnicki T
- Slater MW
- Smallwood JC
- Smead LG Scantlebury
- Smeaton JG
- Smetkina A
- Smith E
- Smith M
- Snoch A
- Soares M
- Soares M Senghi
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- Sokoloff MD
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- Soler FJP
- Solovev A
- Solovyev I
- Spaan B
- Spradlin P
- Stagni F
- Stahl M
- Stahl S
- Stefko P
- Steinkamp O
- Stemmle S
- Stenyakin O
- Stevens H
- Stone S
- Stramaglia ME
- Straticiuc M
- Strekalina D
- Strokov S
- 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
- Teubert F
- Thomas E
- Thomson KA
- Tilley MJ
- Tisserand V
- Tobin M
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- Torres M Cruz
- Tou DY
- Traill M
- Tran MT
- Trejo RI Rabadan
- Trifonova E
- Trippl C
- Tuci G
- Tully A
- Tuning N
- Ukleja A
- Unverzagt DJ
- Usachov A
- Ustyuzhanin A
- Uwer U
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- Vagnoni V
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- Valenti G
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- van Herwijnen E
- Van Hulse CB
- van Veghel M
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- Vazquez Regueiro P
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- Veltri M
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- Vesterinen M
- Vieira D
- Viemann H
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- Vincent P
- Vitali G
- Vollhardt A
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- Vorobyev A
- Vorobyev V
- Voropaev N
- Waldi R
- Walsh J
- Wang C
- Wang J
- Wang J
- Wang J
- Wang J
- Wang M
- Wang R
- Wang Y
- 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 Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zarebski KA
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang Y
- Zhang Y
- Zhelezov A
- Zheng Y
- Zhou X
- Zhou Y
- Zhu X
- Zhukov V
- Zonneveld JB
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
We present an angular analysis of the
B
+
→
K
*
+
(
→
K
0
S
π
+
)
μ
+
μ
−
decay using
9
fb
−
1
of
p
p
collision data collected with the LHCb experiment. For the first time, the full set of
C
P
-averaged angular observables is measured in intervals of the dimuon invariant mass squared. Local deviations from standard model predictions are observed, similar to those in previous LHCb analyses of the isospin-partner
B
0
→
K
*
0
μ
+
μ
−
decay. The global tension is dependent on which effective couplings are considered and on the choice of theory nuisance parameters
Recommended from our members
Study of the ψ2(3823) and χc1(3872) states in B+→(Jψπ+π−)K+ decays
- Author
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- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba K Carvalho
- Albero A Alfonso
- Albrecht J
- Alepuz C Remon
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- Aliouche Z
- Alkhazov G
- Almeida FL Souza De
- Altarelli M Pepe
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- Amhis Y
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- Andreassi G
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- Arzymatov K
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- Basels JM
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- Batsukh B
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- Bellee V
- Belous K
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito C Marin
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- Berninghoff D
- Bernstein HC
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- Bertholet E
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- Beuzekom M van
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- Karacson M
- Kariuki JM
- Kazeev N
- Kecke M
- Keizer F
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- Khanji B
- Kharisova A
- Kim KE
- Kirn T
- Kirsebom VS
- Kitouni O
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- Koliiev S
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
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- Kostiuk I
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- Pappalardo LL
- Pappenheimer C
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- Parkes C
- Parkinson CJ
- Passaleva G
- Pastore A
- Patel M
- Patrignani C
- Paula B Souza De
- Paula L De
- Pearce A
- Pellegrino A
- Perazzini S
- Pereima D
- Perez DH Campora
- Pernas M Ramos
- Perret P
- Petridis K
- Petrolini A
- Petrov A
- Petrucci S
- Petruzzo M
- Philippov A
- Pica L
- Pietrzyk B
- Pietrzyk G
- Pili M
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- Polukhina N
- Polyakov I
- Polycarpo E
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- Poslavskii S
- Prasanth K
- Prieto A Fernandez
- Promberger L
- Prouve C
- Pugatch V
- Pullen H
- Punzi G
- Qian W
- Qin J
- Quagliani R
- Quezada AF Campoverde
- Quintana B
- Raab NV
- Rachwal B
- Rademacker JH
- Rama M
- Rangel MS
- Ratnikov F
- Raven G
- Reboud M
- Redi F
- Regueiro P Vazquez
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- Renaudin V
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- Ricciardi S
- Richards DS
- Rinnert K
- Rios C Santamarina
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- Robertson G
- Rodrigues AB
- Rodrigues E
- Rodrigues F Ferreira
- Rodriguez A Brea
- Rodriguez P Baladron
- Roehrken M
- Rollings A
- Romanovskiy V
- Rosales FA Garcia
- Roth JD
- Rotondo M
- Rudolph MS
- Ruf T
- Ryzhikov A
- Ryzka J
- Sagidova N
- Sahoo N
- Saitta B
- Santacesaria R
- Santimaria M
- Santos D Martinez
- Santovetti E
- Sarpis G
- Sarpis M
- Sarti A
- Satriano C
- Satta A
- Saur M
- Savrina D
- Sazak H
- Schael S
- Schellenberg M
- Schiller M
- Schindler H
- Schmelling M
- Schmelzer T
- Schmidt B
- Schneider O
- Schopper A
- Schreiner HF
- Schubiger M
- Schulte S
- Schune MH
- Schwemmer R
- Sciascia B
- Sciubba A
- Sellam S
- Semennikov A
- Sergi A
- Serio M De
- Serra N
- Serrano J
- Sestini L
- Seuthe A
- Sevilla M Franco
- Seyfert P
- Shangase DM
- Shapkin M
- Shchutska L
- Shears T
- Shekhtman L
- Shevchenko V
- Shields EB
- Shmanin E
- Shupperd JD
- Siddi BG
- Sierra C Vázquez
- Silva CL Da
- Silva JJ Saborido
- Simi G
- Simone D De
- Simone P De
- Simone S
- Skiba I
- Skidmore N
- Skwarnicki T
- Slater MW
- Smallwood JC
- Smead LG Scantlebury
- Smeaton JG
- Smetkina A
- Smith E
- Smith M
- Snoch A
- Soares M
- Sobral CM Costa
- Sokoloff MD
- Sole S Ferreres
- Soler FJP
- Solovev A
- Solovyev I
- Spaan B
- Spradlin P
- Stagni F
- Stahl M
- Stahl S
- Stefko P
- Steinkamp O
- Stemmle S
- Stenyakin O
- Stevens H
- Stone S
- Stracka S
- Stramaglia ME
- Straticiuc M
- Strekalina D
- Strokov S
- 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
- Tang Z
- Tekampe T
- Teubert F
- Thomas E
- Thomson KA
- Tilley MJ
- Tisserand V
- Tobin M
- Tolk S
- Tomassetti L
- Torreira A Gallas
- Torres M Cruz
- Tou DY
- Traill M
- Tran MT
- Trejo RI Rabadan
- Trifonova E
- Trippl C
- Tsaregorodtsev A
- Tuci G
- Tully A
- Tuning N
- Ukleja A
- Unverzagt DJ
- Usachov A
- Ustyuzhanin A
- Uwer U
- Vagner A
- Vagnoni V
- Valassi A
- Valenti G
- Vecchi S
- Veghel M van
- Velthuis JJ
- Veltri M
- Venkateswaran A
- Veronesi M
- Vesterinen M
- Vidal A Casais
- Vidal A Romero
- Vidal F Martinez
- Vidal J Ruiz
- Vidal X Cid
- Vieira D
- Viemann H
- Vilasis-Cardona X
- Vincent P
- Vitali G
- Vitkovskiy A
- Vollhardt A
- Vorobyev A
- Vorobyev V
- Voropaev N
- Vries JA de
- Waldi R
- Walsh J
- Wang J
- Wang J
- Wang J
- Wang J
- Wang M
- Wang R
- Wang Y
- Wang Z
- Ward DR
- 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
- Xing H
- Xu A
- Xu J
- Xu L
- Xu M
- Xu Q
- Xu Z
- Yang D
- Yang Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zarebski KA
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang Y
- Zhelezov A
- Zheng Y
- Zhou X
- Zhou Y
- Zhu X
- Zhukov V
- Zonneveld JB
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- JHEP
- Publication date
- 26/08/2021
- Field of study
The decays B+→J/ψπ+π−K+ are studied using a data
set corresponding to an integrated luminosity of 9fb−1 collected with the
LHCb detector in proton-proton collisions between 2011 and 2018. Precise
measurements of the ratios of branching fractions with the intermediate
ψ2(3823), χc1(3872) and ψ(2S) states are reported. The decay
of B+→ψ2(3823)K+ with ψ2(3823)→Jψπ+π− is observed for the first time with a significance of 5.1
standard deviations. The mass differences between the ψ2(3823),
χc1(3872) and ψ(2S) states are measured to be mχc1(3872)−mψ2(3823)mψ2(3823)−mψ(2S)mχc1(3872)−mψ(2S)===47.50±0.53±0.13MeV/c2,137.98±0.53±0.14MeV/c2,185.49±0.06±0.03MeV/c2, resulting in the
most precise determination of the χc1(3782) mass. The width of the
ψ2(3823) state is found to be below 5.2MeV at 90\% confidence level. The
Breit-Wigner width of the χc1(3872) state is measured to be Γχc1(3872)BW=0.96−0.18+0.19±0.21MeV, which is inconsistent with zero by 5.5 standard deviations
- …