Tuning and validation of hadronic event generator for R value measurements in the tau-charm region

  • To measure the R value in an energy scan experiment with e+e- collisions, precise calculation of initial state radiation is required in the event generators. We present an event generator for this consideration, which incorporates initial state radiation effects up to second order accuracy. The radiative correction factor is calculated using the totally hadronic Born cross section. The measured exclusive processes are generated according to their cross sections, while the unknown processes are generated using the LUND Area Law model, and its parameters are tuned with data collected at √s=3.65 GeV. The optimized values are validated with data in the range √s=2.2324-3.671 GeV. These optimized parameters are universally valid for event generation below the DD threshold.
      PCAS:
    • 13.66.Jn(Precision measurements in e?e+ interactions)
    • 02.70.Uu(Applications of Monte Carlo methods)
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    [39] C. Z. Yuan et al (Belle Collaboration),Phys. Rev. D 77: 011105(2008); arXiv: 0709.2565
    [40] C. Z. Yuan et al (Belle Collaboration), Phys. Rev. D, 77: 011105(2008)[arXiv: 0709.2565]
    [41] D. Cronin-Hennessy et al (CLEO Collaboration), Phys. Rev. D, 80: 072001(2009)
    [42] Pang Cai-Ying and Ping Rong-Gang, Chin. Phys. Letts., 24: 1411(2007)
    [43] M. Bahr et al, Eur. Phys. J. C, 58: 639(2008)
    [44] T. Sjostrand, S. Mrenna, and P. Skands, J. High Energy Phys., 0605: 026(2006)[hep-ph/0603175]
    [45] M. Ablikim et al, Nucl. Instrum. Methods A 614: 345(2010)
    [46] A. Buckley, H. Hoeth, H. Lacker et al, Eur. Phys. J. C, 65: 331(2010)
    [47] M. Althoff et al (TASSO Collaboration), Z. Phys. C, 26: 157(1984)
    [48] W. Braunschweig et al (TASSO Collaboration), Z. Phys. C, 41: 359(1988)
    [49] D. Buskulic et al (ALEPH Collaboration), Z. Phys. C, 55: 209(1992)
    [50] R. Barate et al (ALEPH Collaboration), Phys. Rep., 294: 1(1998)
    [51] K. Hamacher, M. Weierstall, hep-ex/9511011(1995)
    [52] P. Abreu et al (DELPHI Collaboration), Z. Phys. C, 73: 11(1996)
    [53] P. Abreu, W. Adam, and T. Adye et al, Z. Phys. C, 73: 11(1996)
    [54] F. James, CERN-D-506(1994); F. James and M. Roos, Comput. Phys. Commun., 10: 343(1975)
    [55] M. Ablikim et al, Phys. Lett. B, 677: 239(2009)
    [56] Z. Y. Deng et al, High Energy Physics and Nuclear Physics, 30: 371(2006) (in Chinese)
    [57] S. Jadach, B. F. L. Ward, and Z. Was, Phys. Rev. D, 63: 113009(2001); B. F. L. Ward, S. Jadach, and Z. Was, Nucl. Phys. B, Proc. Suppl. 116:73(2003)
    [58] Piotr Golonka and Zbigniew Was, Eur. Phys. J. C, 45: 97(2006)
  • [1] B. Pietrzyk, Nucl. Phys. B (Pro. Suppl.), 162: 18(2006); F. Jegerlehner, Nucl. Phys. B (Pro. Suppl.), 162: 22(2006)[hep-ph/0608329]; F. Ambrosino et al, Eur. Phys. J. C, 50: 729(2007)[hep-ex/0603056]
    [2] J. Z. Bai et al(BES Collaboration), Phy. Rev. Lett.88: 101802(2002)[hep-ex/0102003]
    [3] H. Burkhardt and B. Pietrzyk, Phys. Lett., B513: 46(2001); F. Jegerlehner, J. Phys. G, 29: 101(2003)
    [4] V. P. Druzhinin et al, Rev. Mod. Phys., 83: 1545(2011); M. R. Whalley, J. Phys. G, 29: A1(2003)
    [5] R. G. Ping, Chin. Phys. C, 32: 599(2008)
    [6] Kuang-Ta Zhao and Yifang Wang, Int. J. Mod. Phys. A, 24: Supp. 1(2009); Bo Andersson and Haiming Hu, arXiv:hep-ph/9910285; Haiming Hu and An Tai, arXiv:hep-ex/0106017
    [7] V. N. Baier and V. S. Khoze, Nucl. Phys. B, 65: 381(1973); D. R. Yennie, S. C. Frautschi and H. Suura, Ann. Phys., 13: 379(1961)
    [8] E. A. Kuraev and V. S. Fadin, Sov. J. Nucl. Phys., 41: 466(1985)
    [9] G. Montagna, O. Nicrosini, F. Piccinini, Phys. Lett. B, 406: 243(1997)
    [10] K. A. Olive et al (Particle Data Group), Chin. Phys. C, 38: 1(2014)
    [11] G. Bonneau and F. Martin, Nucl. Phys. B, 27: 381(1971)
    [12] S. Actis et al, Eur. Phys. J. C, 66: 585(2010)
    [13] S. Eidelman and F. Jegerlehner, Z. Phys. C, 67: 585(1995)[hep-ph/9502298]; F. Jegerlehner, Nucl. Phys. Proc. Suppl., 162: 22(2006)[hep-ph/0608329]; F. Jegerlehner, Nucl. Phys. Proc. Suppl., 135: 181(2008); F. Jegerlehner, Nucl. Phys. Proc. Suppl., 126: 325(2004)[hep-ph/0310234]; F. Jegerlehner, hep-ph/0308117(2003)
    [14] B Aubert et al (Babar Collaboration), Phys. Rev. D, 73: 012005(2006)
    [15] A. Anotnelli et al, Nucl. Phys. B, 517: 3(1998)
    [16] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 76: 092006(2007)
    [17] J. P. Lees et al (Babar Collaboration), Phys. Rev. D, 86: 032013(2012)
    [18] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 70: 072004(2004)
    [19] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 77: 092002(2008)
    [20] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 71: 052001(2005)
    [21] V. P. Druzhinin (Babar Collaboration), arXiv:0710.3455
    [22] J. P. Lees et al (Babar Collaboration), arXiv:1103.3001
    [23] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 76: 012008(2007)
    [24] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 76: 092005(2007)
    [25] B. Aubert et al (Babar Collaboration), Phys. Rev. D, 73: 052003(2007)
    [26] M. R. Whalley, J. Phys. G, 29: A1(2003)
    [27] M. Ablikim et al (BES III Collaboration), Submitted to Phys. Lett. B.
    [28] T. K. Pedlar et al (CLEO Collaboration), Phys. Rev. Lett., 95: 261803(2005); Kamal K Seth et al, arXiv: 1210.1596
    [29] G. Pakhlova et al (Belle Collaboration), Phys. Rev. D, 77: 011103(2008)
    [30] G. Pakhlova et al (Belle Collaboration), Phys. Rev. Lett., 98: 092001(2007)[arXiv: hep-ex/0608018]
    [31] G. Pakhlova et al (Belle Collaboration), Phys.Rev.Lett., 100: 062001(2008)[arXiv: 0708.0082]
    [32] G. Pakhlova et al (Belle Collaboration), Phys. Rev. D, 80: 091101(2009)[arXiv: 0908.0231]
    [33] G. Pakhlova et al (Belle Collaboration), Phys. Rev. Lett., 101: 172001(2008)[arXiv: 0807.4458]
    [34] X. L. Wang et al (Belle Collaboration), Phys. Rev. D, 87: 051101(2013);
    [35] C. Z. Yuan et al (Belle Collaboration), Phys. Rev. Lett., 99: 182004(2007)[arXiv:0707.2541]
    [36] X. L. Wang et al (Belle Collaboration), Phys. Rev. Lett., 99:142002(2007)[arXiv:0707.3699]
    [37] M. Ablikim et al (BESIII Collaboration),Phys. Rev. Lett. 111: 242001(2013)
    [38] M. Ablikim et al (BESIII Collaboration),Phys. Rev. Lett. 113: 212002(2014)
    [39] C. Z. Yuan et al (Belle Collaboration),Phys. Rev. D 77: 011105(2008); arXiv: 0709.2565
    [40] C. Z. Yuan et al (Belle Collaboration), Phys. Rev. D, 77: 011105(2008)[arXiv: 0709.2565]
    [41] D. Cronin-Hennessy et al (CLEO Collaboration), Phys. Rev. D, 80: 072001(2009)
    [42] Pang Cai-Ying and Ping Rong-Gang, Chin. Phys. Letts., 24: 1411(2007)
    [43] M. Bahr et al, Eur. Phys. J. C, 58: 639(2008)
    [44] T. Sjostrand, S. Mrenna, and P. Skands, J. High Energy Phys., 0605: 026(2006)[hep-ph/0603175]
    [45] M. Ablikim et al, Nucl. Instrum. Methods A 614: 345(2010)
    [46] A. Buckley, H. Hoeth, H. Lacker et al, Eur. Phys. J. C, 65: 331(2010)
    [47] M. Althoff et al (TASSO Collaboration), Z. Phys. C, 26: 157(1984)
    [48] W. Braunschweig et al (TASSO Collaboration), Z. Phys. C, 41: 359(1988)
    [49] D. Buskulic et al (ALEPH Collaboration), Z. Phys. C, 55: 209(1992)
    [50] R. Barate et al (ALEPH Collaboration), Phys. Rep., 294: 1(1998)
    [51] K. Hamacher, M. Weierstall, hep-ex/9511011(1995)
    [52] P. Abreu et al (DELPHI Collaboration), Z. Phys. C, 73: 11(1996)
    [53] P. Abreu, W. Adam, and T. Adye et al, Z. Phys. C, 73: 11(1996)
    [54] F. James, CERN-D-506(1994); F. James and M. Roos, Comput. Phys. Commun., 10: 343(1975)
    [55] M. Ablikim et al, Phys. Lett. B, 677: 239(2009)
    [56] Z. Y. Deng et al, High Energy Physics and Nuclear Physics, 30: 371(2006) (in Chinese)
    [57] S. Jadach, B. F. L. Ward, and Z. Was, Phys. Rev. D, 63: 113009(2001); B. F. L. Ward, S. Jadach, and Z. Was, Nucl. Phys. B, Proc. Suppl. 116:73(2003)
    [58] Piotr Golonka and Zbigniew Was, Eur. Phys. J. C, 45: 97(2006)
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2. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Study of e+e- →π+π-π0 at s from 2.00 to 3.08 GeV at BESIII[J]. Physical Review D, 2024, 110(3): 032005. doi: 10.1103/PhysRevD.110.032005
3. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Measurements of Normalized Differential Cross Sections of Inclusive η Production in e+e- Annihilation at Energy from 2.0000 to 3.6710 GeV[J]. Physical Review Letters, 2024, 133(2): 021901. doi: 10.1103/PhysRevLett.133.021901
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8. de Mori, F.. R-value measurements at BESIII[J]. Nuovo Cimento della Societa Italiana di Fisica C, 2024, 47(4): e243. doi: 10.1393/ncc/i2024-24243-4
9. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Study of e+e- →ηφ at center-of-mass energies from 3.773 to 4.600 GeV[J]. Physical Review D, 2023, 108(11): 112011. doi: 10.1103/PhysRevD.108.112011
10. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Measurement of the cross sections for e+e- →ηπ+π- at center-of-mass energies between 2.00 and 3.08 GeV[J]. Physical Review D, 2023, 108(11): L111101. doi: 10.1103/PhysRevD.108.L111101
11. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Measurement of Energy-Dependent Pair-Production Cross Section and Electromagnetic Form Factors of a Charmed Baryon[J]. Physical Review Letters, 2023, 131(19): 191901. doi: 10.1103/PhysRevLett.131.191901
12. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Study of the e+e − → π + π − ω process at center-of-mass energies between 4.0 and 4.6 GeV[J]. Journal of High Energy Physics, 2023, 2023(8): 159. doi: 10.1007/JHEP08(2023)159
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14. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Measurements of Normalized Differential Cross Sections of Inclusive π0 and KS0 Production in e+e- Annihilation at Energies from 2.2324 to 3.6710 GeV[J]. Physical Review Letters, 2023, 130(23): 231901. doi: 10.1103/PhysRevLett.130.231901
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16. Zhou, L.. Measurement of R value at BESIII[J]. Nuclear and Particle Physics Proceedings, 2022. doi: 10.1016/j.nuclphysbps.2022.09.034
17. Ablikim, M., Achasov, M.N., Adlarson, P. et al. Cross section measurements of the processes e + e − → ωπ 0 and ωη at center-of-mass energies between 3.773 and 4.701 GeV[J]. Journal of High Energy Physics, 2022, 2022(7): 64. doi: 10.1007/JHEP07(2022)064
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25. Irshad, M.. Status of Measurement of R value at BESIII[J]. Proceedings of Science, 2021.
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28. Hu, H.. The status of R value measurement at BESIII[J]. Nuclear and Particle Physics Proceedings, 2017. doi: 10.1016/j.nuclphysbps.2017.03.045
Get Citation
Rong-Gang Ping, Xi-An Xiong, Lei Xia, Zhen Gao, Ying-Tian Li, Xing-Yu Zhou, Bing-Xin Zhang, Bo Zheng, Wen-Biao Yan, Hai-Ming Hu and Guang-Shun Huang. Tuning and validation of hadronic event generator for R value measurements in the tau-charm region[J]. Chinese Physics C, 2016, 40(11): 113002. doi: 10.1088/1674-1137/40/11/113002
Rong-Gang Ping, Xi-An Xiong, Lei Xia, Zhen Gao, Ying-Tian Li, Xing-Yu Zhou, Bing-Xin Zhang, Bo Zheng, Wen-Biao Yan, Hai-Ming Hu and Guang-Shun Huang. Tuning and validation of hadronic event generator for R value measurements in the tau-charm region[J]. Chinese Physics C, 2016, 40(11): 113002.  doi: 10.1088/1674-1137/40/11/113002 shu
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Received: 2016-05-10
Revised: 2016-07-13
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    Supported by National Natural Science Foundation of China (11175146, 11375205, 11575077, 11335008, 11565006), Large Science Setup of Joint Foundation (10979059), and 100 Talents Program of CAS

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Tuning and validation of hadronic event generator for R value measurements in the tau-charm region

    Corresponding author: Rong-Gang Ping,
    Corresponding author: Bo Zheng,
  • 1.  Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
  • 2.  University of Science and Technology of China, Hefei 230026, China
  • 3.  University of South China, Hengyang, 421001, China
Fund Project:  Supported by National Natural Science Foundation of China (11175146, 11375205, 11575077, 11335008, 11565006), Large Science Setup of Joint Foundation (10979059), and 100 Talents Program of CAS

Abstract: To measure the R value in an energy scan experiment with e+e- collisions, precise calculation of initial state radiation is required in the event generators. We present an event generator for this consideration, which incorporates initial state radiation effects up to second order accuracy. The radiative correction factor is calculated using the totally hadronic Born cross section. The measured exclusive processes are generated according to their cross sections, while the unknown processes are generated using the LUND Area Law model, and its parameters are tuned with data collected at √s=3.65 GeV. The optimized values are validated with data in the range √s=2.2324-3.671 GeV. These optimized parameters are universally valid for event generation below the DD threshold.

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