×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《中国物理C》(英文)编辑部
2024年10月30日

Study of the production of Λb0 and B0 hadrons in pp collisions and first measurement of the Λb0→J/ψpK- branching fraction

  • The product of the Λb0(B0) di erential production cross-section and the branching fraction of the decay Λb0→J/ψpK- (B0→J/ψpK*(892)0) is measured as a function of the beauty hadron transverse momentum, pT, and rapidity, y. The kinematic region of the measurements is pT <20 GeV/c and 2.0< y< 4.5. The measurements use a data sample corresponding to an integrated luminosity of 3fb-1 collected by the LHCb detector in pp collisions at centre-of-mass energies √s= 7 TeV in 2011 and √s= 8 TeV in 2012. Based on previous LHCb results of the fragmentation fraction ratio, fΛb0/fd, the branching fraction of the decay Λb0→J/ψpK- is measured to be
    Bb0→J/ψpK-)=(3.17±0.04±0.07±0.34-0.28+0.45)×10-4,
    where the rst uncertainty is statistical, the second is systematic, the third is due to the uncertainty on the branching fraction of the decay B0→J/ψpK*(892)0, and the fourth is due to the knowledge of fΛb0/fd. The sum of the asymmetries in the production and decay between Λb0 and Λb0 is also measured as a function of pT and y. The previously published branching fraction of Λb0→J/ψpπ-, relative to that of Λb0→J/ψpK-, is updated. The branching fractions of Λb0→Pc+(→J/ψp)K- are determined.
      PCAS:
  • 加载中
  • [1] Y. Oh, C. M. Ko, S. H. Lee, and S. Yasui, Phys. Rev. C, 79:044905 (2009)
    [2] S. H. Lee et al, Phys. Rev. Lett., 100: 222301 (2008)
    [3] W. S. Lockman et al, Phys. Lett. B, 85: 443 (1979)
    [4] P. Chauvat et al (R608 Collaboration), Phys. Lett. B, 199: 304(1987)
    [5] S. Chatrchyan et al (CMS Collaboration), Phys. Lett. B, 714:136 (2012)
    [6] J. L. Rosner, Phys. Rev. D, 90: 014023 (2014)
    [7] R. Aaij et al (LHCb Collaboration), Phys. Rev. D, 85: 032008(2012)
    [8] R. Aaij et al (LHCb Collaboration), JHEP, 08: 143 (2014)
    [9] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 111:102003 (2013)
    [10] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 115:072001 (2015)
    [11] R. Aaij et al (LHCb Collaboration), JHEP, 07: 103 (2014)
    [12] K. Abe et al (Belle Collaboration), Phys. Lett. B, 538: 11(2002)
    [13] A. A. Alves Jr. et al (LHCb Collaboration), JINST, 3: S08005(2008)
    [14] R. Aaij et al (LHCb Collaboration), Int. J. Mod. Phys. A, 30:1530022 (2015)
    [15] R. Aaij et al, JINST, 9: P09007 (2014)
    [16] R. Arink et al, JINST, 9: P01002 (2014)
    [17] M. Adinolfi et al, Eur. Phys. J. C, 73: 2431 (2013)
    [18] A. A. Alves Jr. et al, JINST, 8: P02022 (2013)
    [19] R. Aaij et al, JINST, 8: P04022 (2013)
    [20] K. A. Olive et al (Particle Data Group), Chin. Phys. C, 38:090001 (2014)
    [21] T. Sjstrand, S. Mrenna, and P. Skands, JHEP, 05: 026 (2006)
    [22] T. Sjstrand, S. Mrenna, and P. Skands, Comput. Phys. Commun.,178: 852 (2008)
    [23] I. Belyaev et al, J. Phys. Conf. Ser., 331: 032047 (2011)
    [24] D. J. Lange, Nucl. Instrum. Methods A, 462: 152 (2001)
    [25] P. Golonka and Z. Was, Eur. Phys. J. C, 45: 97 (2006)
    [26] J. Allison et al (Geant4 Collaboration), IEEE Trans. Nucl. Sci.,53: 270 (2006)
    [27] S. Agostinelli et al (Geant4 Collaboration), Nucl. Instrum.Methods A, 506: 250 (2003)
    [28] M. Clemencic et al, J. Phys. Conf. Ser., 331: 032023 (2011)
    [29] L. Breiman, J. H. Friedman, R. A. Olshen, and C. J. Stone, Classification and regression trees (Belmont, California, USA: Wadsworth international group, 1984)
    [30] B. P. Roe et al, Nucl. Instrum. Methods A, 543: 577 (2005)
    [31] R. E. Schapire and Y. Freund, Jour. Comp. and Syst. Sc., 55:119 (1997)
    [32] A. Hoecker et al, PoS, ACAT: 040 (2007)
    [33] R. Fruhwirth, Nucl. Instrum. Methods A, 262: 444 (1987)
    [34] M. Needham and J. Van Tilburg, LHCb -2007-020
    [35] M. Needham, LHCb -2007-129
    [36] R. Aaij et al (LHCb Collaboration), JINST, 9: P12005 (2014)
    [37] W. D. Hulsbergen, Nucl. Instrum. Methods A, 552: 566 (2005)
    [38] R. Aaij et al (LHCb Collaboration), JHEP, 08: 117 (2013)
    [39] R. Aaij et al (LHCb Collaboration), Phys. Rev. D, 88: 052002(2013)
    [40] M. Pivk and F. R. Le Diberder, Nucl. Instrum. Methods A,555: 356 (2005)
    [41] R. Aaij et al (LHCb Collaboration), JHEP, 07: 041 (2014)
    [42] D. Martnez Santos and F. Dupertuis, Nucl. Instrum. MethodsA, 764: 150 (2014)
    [43] R. Aaij et al (LHCb Collaboration), JINST, 10: P02007 (2015)
    [44] C. Tsallis, J. Statist. Phys., 52: 479 (1988)
    [45] C. Tsallis, Braz. J. Phys., 29: 1 (1999)
    [46] A. A. Bylinkin and O. I. Piskounova, arXiv:1501.07706
    [47] G. D. Lafferty and T. R. Wyatt, Nucl. Instrum. Methods A,355: 541 (1995)
    [48] M. Cacciari, M. Greco, and P. Nason, JHEP, 05: 007 (1998)
    [49] M. Cacciari, S. Frixione, and P. Nason, JHEP, 03: 006 (2001)
    [50] M. Cacciari et al, JHEP, 10: 137 (2012)
    [51] J. L. Rosner, Phys. Rev. D, 86: 014011 (2012)
  • 加载中

Get Citation
R. Aaij and   et al  (LHCb Collaboration). Study of the production of Λb0 and B0 hadrons in pp collisions and first measurement of the Λb0→J/ψpK- branching fraction[J]. Chinese Physics C, 2016, 40(1): 011001. doi: 10.1088/1674-1137/40/1/011001
R. Aaij and   et al  (LHCb Collaboration). Study of the production of Λb0 and B0 hadrons in pp collisions and first measurement of the Λb0→J/ψpK- branching fraction[J]. Chinese Physics C, 2016, 40(1): 011001.  doi: 10.1088/1674-1137/40/1/011001 shu
Milestone
Received: 2015-09-01
Fund

    Supported by CERN and national agencies: CAPES, CNPq, FAPERJ and FINEP (Brazil)

    NSFC (China)

    CNRS/IN2P3 (France)

    BMBF, DFG, HGF and MPG (Germany)

    INFN (Italy)

    FOM and NWO (The Netherlands)

    MNiSW and NCN (Poland)

    MEN/IFA (Romania)

    MinES and FANO (Russia)

    MinECo (Spain)

    SNSF and SER (Switzerland)

    NASU (Ukraine)

    STFC (United Kingdom)

    NSF (USA). The Tier1 computing centres are supported by IN2P3 (France), KIT and BMBF (Germany), INFN (Italy), NWO and SURF (The Netherlands), PIC (Spain), GridPP (United Kingdom). Individual groups or members have received support from EPLANET, Marie Sklodowska-Curie Actions and ERC (European Union), Conseil generalde Haute-Savoie, Labex ENIGMASS and OCEVU, Region Auvergne (France), RFBR (Russia), XuntaGal and GENCAT (Spain), Royal Society and Royal Commission for the Exhibition of 1851 (United Kingdom).

Article Metric

Article Views(1702)
PDF Downloads(90)
Cited by(0)
Policy on re-use
To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Study of the production of Λb0 and B0 hadrons in pp collisions and first measurement of the Λb0→J/ψpK- branching fraction

Fund Project:  Supported by CERN and national agencies: CAPES, CNPq, FAPERJ and FINEP (Brazil) NSFC (China) CNRS/IN2P3 (France) BMBF, DFG, HGF and MPG (Germany) INFN (Italy) FOM and NWO (The Netherlands) MNiSW and NCN (Poland) MEN/IFA (Romania) MinES and FANO (Russia) MinECo (Spain) SNSF and SER (Switzerland) NASU (Ukraine) STFC (United Kingdom) NSF (USA). The Tier1 computing centres are supported by IN2P3 (France), KIT and BMBF (Germany), INFN (Italy), NWO and SURF (The Netherlands), PIC (Spain), GridPP (United Kingdom). Individual groups or members have received support from EPLANET, Marie Sklodowska-Curie Actions and ERC (European Union), Conseil generalde Haute-Savoie, Labex ENIGMASS and OCEVU, Region Auvergne (France), RFBR (Russia), XuntaGal and GENCAT (Spain), Royal Society and Royal Commission for the Exhibition of 1851 (United Kingdom).

Abstract: The product of the Λb0(B0) di erential production cross-section and the branching fraction of the decay Λb0→J/ψpK- (B0→J/ψpK*(892)0) is measured as a function of the beauty hadron transverse momentum, pT, and rapidity, y. The kinematic region of the measurements is pT <20 GeV/c and 2.0< y< 4.5. The measurements use a data sample corresponding to an integrated luminosity of 3fb-1 collected by the LHCb detector in pp collisions at centre-of-mass energies √s= 7 TeV in 2011 and √s= 8 TeV in 2012. Based on previous LHCb results of the fragmentation fraction ratio, fΛb0/fd, the branching fraction of the decay Λb0→J/ψpK- is measured to be
Bb0→J/ψpK-)=(3.17±0.04±0.07±0.34-0.28+0.45)×10-4,
where the rst uncertainty is statistical, the second is systematic, the third is due to the uncertainty on the branching fraction of the decay B0→J/ψpK*(892)0, and the fourth is due to the knowledge of fΛb0/fd. The sum of the asymmetries in the production and decay between Λb0 and Λb0 is also measured as a function of pT and y. The previously published branching fraction of Λb0→J/ψpπ-, relative to that of Λb0→J/ψpK-, is updated. The branching fractions of Λb0→Pc+(→J/ψp)K- are determined.

    HTML

Reference (51)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return