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

FENG Yu; GONG Bin; WAN Lu-Ping; WANG Jian-Xiong

doi:10.1088/1674-1137/39/12/123102

Chinese Physics C> 2015, Vol. 39> Issue(12) : 123102 DOI: 10.1088/1674-1137/39/12/123102

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

1.
Institute of High Energy Physics, Chinese Academy of Sciences, P.O.Box 918(4), Beijing 100049, China

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Abstract：
Following the nonrelativistic QCD factorization scheme, by taking the latest available measurements of χ_bJ(3P) into consideration, we present an updated study on the yield and polarization of Y(1S, 2S, 3S) hadroproduction, and the fractions of χ_bJ(mP) feed-down in Y(nS) production at QCD next-to-leading order. In the fitting, three schemes are applied with different choices of χ_bJ(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 χ_bJ(3P) feed-down contributions. The ratio of σ[χ_b2(1P)]/σ[χ_b1(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.
- non-relativistic quantum chromodynamics ,
- next-to-leading order ,
- Y ,
- bJ feed-down contributions ,
- polarization

References

[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

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[15]	CHU Shao-Xia , HOU De-Fu , REN Hai-Cang . On the Next-leading order Heavy-Quark Potential from AdS/CFT. Chinese Physics C, 2010, 34(9): 1355-1359. doi: 10.1088/1674-1137/34/9/041
[16]	E. Prencipe . X Y Z particles at BABAR. Chinese Physics C, 2010, 34(6): 644-649. doi: 10.1088/1674-1137/34/6/006
[17]	LI Hsiang-Nan . Next-to-leading-order calculation in k_T factorization. Chinese Physics C, 2009, 33(6): 463-468. doi: 10.1088/1674-1137/33/6/012
[18]	Deng Jingkang , Shang Rencheng , Zhu Shengjiang , Xu Wang , Zhang Juping , Jin Qingzhen , Zhu Henian , Xia Shaojian , Yan Yonglian , Guo Yanan . Study on Beam Polarization and the Design of a Polarimeter in BEPC. Chinese Physics C, 1997, 21(S3): 85-93.
[19]	Shen Qixing , Yu Hong . The Polarization States of the Gluon and the Glueball Interpretation of the ξ (2230). Chinese Physics C, 1991, 15(S2): 153-157.
[20]	Ge Liangxiao , Zhuo Yizhong . Non-Relativistic BUU Equation. Chinese Physics C, 1989, 13(S3): 289-302.

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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

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Received: 2015-03-31
Revised: 2015-07-08

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

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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

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

Received Date: 2015-03-31

Accepted Date: 2015-07-08

Available Online: 2015-12-20

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 χ_bJ(3P) into consideration, we present an updated study on the yield and polarization of Y(1S, 2S, 3S) hadroproduction, and the fractions of χ_bJ(mP) feed-down in Y(nS) production at QCD next-to-leading order. In the fitting, three schemes are applied with different choices of χ_bJ(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 χ_bJ(3P) feed-down contributions. The ratio of σ[χ_b2(1P)]/σ[χ_b1(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.

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

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