An updated study of Y production and polarizationat the Tevatron and LHC

  • Following the nonrelativistic QCD factorization scheme, by taking the latest available measurements of χbJ(3P) into consideration, we present an updated study on the yield and polarization of Y(1S, 2S, 3S) hadroproduction, and the fractions of χbJ(mP) feed-down in Y(nS) production at QCD next-to-leading order. In the fitting, three schemes are applied with different choices of χbJ(mP) feed-down ratios and NRQCD factorization scale. The results can explain the measurements of yield very well. The polarization puzzle to (3S) is now solved by considering the χbJ(3P) feed-down contributions. The ratio of σ[χb2(1P)]/σ[χb1(1P)] measured by the CMS experiment can also be reproduced in our prediction. Among the different schemes, the results show little difference, but there are sizeable differences for the fitted long-distance color-octet matrix elements. This may bring large uncertainties when the values are applied in theoretical predictions for other experiments such as those at ee, ep colliders.
      PCAS:
  • 加载中
  • [1] Braaten E, Fleming S. Phys. Rev. Lett., 1995, 74: 3327-3330
    [2] Bodwin G T, Braaten E, Lepage G P. Phys. Rev. D, 1995, 51: 1125-1171
    [3] Campbell J M, Maltoni F, Tramontano F. Phys. Rev. Lett., 2007, 98: 252002
    [4] GONG Bin, WANG Jian-Xiong. Phys. Rev. Lett., 2008, 100: 232001
    [5] KANG Zhong-Bo, QIU Jian-Wei, Sterman G. Phys. Rev. Lett., 2012, 108: 102002
    [6] GONG Bin, LI Xue-Qian, WANG Jian-Xiong. Phys. Lett. B, 2009, 673: 197-200
    [7] MA Yan-Qing, WANG Kai, CHAO Kuang-Ta. Phys. Rev. D, 2011, 83: 111503
    [8] Butenschoen M, Kniehl B A. Phys. Rev. Lett., 2012, 108: 172002
    [9] CHAO Kuang-Ta, MA Yan-Qing, SHAO Hua-Sheng et al. Phys. Rev. Lett., 2012, 108: 242004
    [10] GONG Bin, WAN Lu-Ping, WANG Jian-Xiong et al. Phys. Rev. Lett., 2013, 110: 042002
    [11] Aaij R et al. (LHCb collaboration). arXiv: 1409.3612
    [12] Butenschoen M, HE Zhi-Guo, Kniehl B A. Phys. Rev. Lett., 2014, 114: 092004
    [13] HAN Hao, MA Yan-Qing, MENG Ce et al. Phys. Rev. Lett., 2015, 114: 092005
    [14] ZHANG Hong-Fei, SUN Zhan, SANG Wen-Long et al. Phys. Rev. Lett., 2014, 114: 092006
    [15] GONG Bin, WANG Jian-Xiong, ZHANG Hong-Fei. Phys. Rev. D, 2011, 83: 114021
    [16] WANG Kai, MA Yan-Qing, CHAO Kuang-Ta. Phys. Rev. D, 2012, 85: 114003
    [17] GONG Bin, WAN Lu-Ping, WANG Jian-Xiong et al. Phys. Rev. Lett., 2014, 112(3): 032001
    [18] Aaij R et al. (LHCb collaboration). JHEP, 2014, 1410: 88
    [19] Aaij R et al. (LHCb collaboration). Eur. Phys. J. C, 2014, 74(10): 3092
    [20] Khachatryan V et al. (CMS collaboration). arXiv: 1409. 5761
    [21] Beneke M, Kramer M, Vanttinen M. Phys. Rev. D, 1998, 57: 4258-4274
    [22] WANG Jian-Xiong. Nucl. Instrum. Methods A, 2004, 534: 241-245
    [23] WAN Lu-Ping, WANG Jian-Xiong. Comput. Phys. Commun, 2014, 185: 2939-2949
    [24] Pumplin J, Stump D R, Huston J et al. JHEP, 2002, 0207: 012
    [25] Beringer J et al. (Particle Data Group collaboration). Phys. Rev. D, 2012, 86: 010001
    [26] Eichten E J, Quigg C. Phys. Rev. D, 1995, 52: 1726-1728
    [27] Acosta D et al. (CDF collaboration). Phys. Rev. Lett., 2002, 88: 161802
    [28] Aaij R et al. (LHCb collaboration). Eur. Phys. J. C, 2012, 72: 2025
    [29] Khachatryan V et al. (CMS collaboration). Phys. Rev. D, 2011, 83: 112004
    [30] Aad G et al. (ATLAS collaboration). Phys. Rev. D, 2013, 87(5): 052004
    [31] Aaltonen T et al. (CDF collaboration). Phys. Rev. Lett., 2012, 108: 151802
    [32] Chatrchyan S et al. (CMS collaboration). Phys. Rev. Lett., 2013, 110(8): 081802
    [33] HAN Hao, MA Yan-Qing, MENG Ce et al. arXiv:1410.8537
    [34] WANG Jian-Xiong, ZHANG Hong-Fei. J. Phys. G, 2015, 42(2): 025004
    [35] JIA Lan, YU Ling, ZHANG Hong-Fei. arXiv: 1410.4032
  • 加载中

Get Citation
FENG Yu, GONG Bin, WAN Lu-Ping and WANG Jian-Xiong. An updated study of Y production and polarizationat the Tevatron and LHC[J]. Chinese Physics C, 2015, 39(12): 123102. doi: 10.1088/1674-1137/39/12/123102
FENG Yu, GONG Bin, WAN Lu-Ping and WANG Jian-Xiong. An updated study of Y production and polarizationat the Tevatron and LHC[J]. Chinese Physics C, 2015, 39(12): 123102.  doi: 10.1088/1674-1137/39/12/123102 shu
Milestone
Received: 2015-03-31
Revised: 2015-07-08
Fund

    Supported by National Nature Science Foundation of China (11475183) and Youth Innovation Promotion Association of CAS (2014010)

Article Metric

Article Views(1569)
PDF Downloads(46)
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:

An updated study of Y production and polarizationat the Tevatron and LHC

    Corresponding author: FENG Yu,
    Corresponding author: GONG Bin,
    Corresponding author: WAN Lu-Ping,
    Corresponding author: WANG Jian-Xiong,
  • 1. Institute of High Energy Physics, Chinese Academy of Sciences, P.O.Box 918(4), Beijing 100049, China
Fund Project:  Supported by National Nature Science Foundation of China (11475183) and Youth Innovation Promotion Association of CAS (2014010)

Abstract: Following the nonrelativistic QCD factorization scheme, by taking the latest available measurements of χbJ(3P) into consideration, we present an updated study on the yield and polarization of Y(1S, 2S, 3S) hadroproduction, and the fractions of χbJ(mP) feed-down in Y(nS) production at QCD next-to-leading order. In the fitting, three schemes are applied with different choices of χbJ(mP) feed-down ratios and NRQCD factorization scale. The results can explain the measurements of yield very well. The polarization puzzle to (3S) is now solved by considering the χbJ(3P) feed-down contributions. The ratio of σ[χb2(1P)]/σ[χb1(1P)] measured by the CMS experiment can also be reproduced in our prediction. Among the different schemes, the results show little difference, but there are sizeable differences for the fitted long-distance color-octet matrix elements. This may bring large uncertainties when the values are applied in theoretical predictions for other experiments such as those at ee, ep colliders.

    HTML

Reference (35)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return