An exclusive event generator for e+e- scan experiments

  • An exclusive event generator is designed for e+e- scan experiments, including initial state radiation effects up to the second order correction. The generator is coded within the framework of BesEvtGen. There are seventy hadronic decay modes available, with effective center-of-mass energy coverage from the two pion mass threshold up to about 6 GeV. The accuracy achieved for the initial state radiation correction reaches the level achieved by the KKMC generator. The uncertainty associated with the calculation of the correction factor to the initial state radiation is dominated by the measurements of the energy-dependent Born cross section.
      PCAS:
  • 加载中
  • [1] Pietrzyk B. Nucl. Phys. B (Pro. Suppl.), 2006, 162: 18; Jegerlehner F. Nucl. Phys. B (Pro. Suppl.), 2006, 162: 22 (hep-ph/0608329); Ambrosino F et al. Eur. Phys. J. C, 2007, 50: 729 (hep-ex/0603056)[2] BAI J Z et al. (BES collaboration). Phys. Rev. Lett., 2002, 88: 101802 (hep-ex/0102003)[3] Burkhardt H, Pietrzyk B. Phys. Lett. B, 2001, 513: 46; Jegerlehner F. J. Phys. G, 2003, 29: 101[4] Druzhinin V P et al. Rev. Mod. Phys., 2011, 83: 1545; Whalley M R. J. Phys. G, 2003, 29: A1; Acits S et al. Eur. Phys. J. C, 2010, 66: 585[5] Aubert B et al. (BABAR collaboration). Phys. Rev. Lett., 2005, 95: 142001; Coan T E et al. (CLEO collaboration). Phys. Rev. Lett., 2006, 96: 162003; YUAN C Z et al. (Belle collaboration). Phys. Rev. Lett., 2007, 99: 182004[6] WANG X L et al. (Belle collaboration). Phys. Rev. Lett., 2007, 99: 142002[7] Ablikim M et al. (BESⅡ collaboration). Phys. Rev. Lett., 2013, 110: 252001[8] LIU Z Q et al. (Belle collaboration). Phys. Rev. Lett., 2013, 110: 252002[9] XIAO T, Dobbs S, A. Tomaradze, Kamal K. Seth. arXiv:1304.3036[10] Actis S, Arbuzov A et al. Eur. Phys. J. C, 2010, 66: 585[11] Balossini G, Calame C M C, Montagna G, Nicrosini O, Piccinini F. Nucl. Phys. B, 2006, 758: 227[12] Rodrigo G, Czyz H, Kuhn J H. arXiv:hep-ph/0205097[13] Jadach S, Ward B F L, Was Z. Comput. Phys. Commun., 2000, 130: 260[14] Cronin-Hennessy D et al. (CLEO collaboration). Phys. Rev. D, 2009, 80: 072001[15] Baier V N, Khoze V S. Nucl. Phys. B, 1973, 65: 381; Yennie D R, Frautschi S C, Suura H. Ann. Phys., 1961, 13: 379[16] Nicrosini Q, Trentadue L. Nucl. Phys. B, 1989, 318: 1[17] Kuraev E A, Fadin V S. Sov. J. Nucl. Phys., 1985, 41: 466[18] Montagna G, Nicrosini O, Piccinini F. Phys. Lett. B, 1997, 406: 243[19] Beringer J et al. Phys. Rev. D, 2012, 86: 010001[20] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2006, 73: 012005[21] Anotnelli A et al. Nucl. Phys. B, 1998, 517: 3[22] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2007, 76: 092005[23] Lees J P et al. (Babar collaboration). Phys. Rev. D, 2012, 86: 032013[24] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2004, 70: 072004[25] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2008, 77: 092002[26] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2005, 71: 052001[27] Druzhinin V P et al. (Babar collaboration). arXiv:0710.3455[28] Lees J P et al. (Babar collaboration). arXiv:1103.3001[29] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2007, 76: 012008[30] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2007, 76: 092005[31] Aubert B et al. (Babar collaboration). Phys. Rev. D, 2007, 73: 052003[32] Whalley M R. J. Phys. G, 2003, 29, A1-A33[33] Pedlar T K et al. (CLEO collaboration). Phys. Rev. Lett. 2005, 95: 261803; Seth K K et al. arXiv: 1210.1596[34] Pakhlova G et al. (Belle collaboration). Phys. Rev. D, 2008, 77: 011103[35] Pakhlova G et al. (Belle collaboration). Phys. Rev. Lett., 2007, 98: 092001 (arXiv: hep-ex/0608018)[36] Pakhlova G et al. (Belle collaboration). Phys.Rev. Lett., 2008, 100: 062001 (arXiv: 0708.0082)[37] Pakhlova G et al. (Belle collaboration). Phys. Rev. D, 2009, 80: 091101 (arXiv: 0908.0231)[38] Pakhlova G et al. (Belle collaboration). Phys. Rev. Lett., 2008, 101: 172001 (arXiv: 0807.4458)[39] WANG X L et al. (Belle collaboration). Phys. Rev. D, 2013, 87: 051101;[40] YUAN C Z et al. (Belle collaboration). Phys. Rev. Lett., 2007, 99: 182004 ( arXiv:0707.2541)[41] WANG X L et al. (Belle collaboration). Phys. Rev. Lett., 2007, 99: 142002 ( arXiv:0707.3699)[42] YUAN C Z et al. (Belle collaboration). Phys. Rev. D, 2008, 77: 011105 (arXiv: 0709.2565)[43] Cronin-Hennessy D et al. (CLEO collaboration). Phys. Rev. D, 2009, 80: 072001[44] PING R G. Chinese Phys. C (HEP NP), 2008, 32: 599[45] Jadach S, Ward B F L, Was Z. Phys. Rev. D, 2001, 63: 113009; Ward B F L, Jadach S, Was Z. Nucl. Phys. B, Proc. Suppl., 2003, 116: 73[46] PING R G. 2013 BESⅡ-doc-162-v18[47] Piotr Golonka, Zbigniew Was. Eur. Phys. J. C, 2006, 45: 97
  • 加载中

Get Citation
PING Rong-Gang. An exclusive event generator for e+e- scan experiments[J]. Chinese Physics C, 2014, 38(8): 083001. doi: 10.1088/1674-1137/38/8/083001
PING Rong-Gang. An exclusive event generator for e+e- scan experiments[J]. Chinese Physics C, 2014, 38(8): 083001.  doi: 10.1088/1674-1137/38/8/083001 shu
Milestone
Received: 2013-12-09
Revised: 2014-04-18
Article Metric

Article Views(1580)
PDF Downloads(225)
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 exclusive event generator for e+e- scan experiments

    Corresponding author: PING Rong-Gang,
  • 1. Institute of High Energy Physics, Chinese Academy of Sciences, P. O. Box 918(1), Beijing 100049, China

Abstract: An exclusive event generator is designed for e+e- scan experiments, including initial state radiation effects up to the second order correction. The generator is coded within the framework of BesEvtGen. There are seventy hadronic decay modes available, with effective center-of-mass energy coverage from the two pion mass threshold up to about 6 GeV. The accuracy achieved for the initial state radiation correction reaches the level achieved by the KKMC generator. The uncertainty associated with the calculation of the correction factor to the initial state radiation is dominated by the measurements of the energy-dependent Born cross section.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return