Impact factor of Chinese Physics C is 3.6 in 2023 Impact factor of Chinese Physics C is 3.6 in 2022 2021 Impact Factor 2.944
Advanced Search
×
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
Chinese Physics C> 2017, Vol. 41> Issue(12) : 124101 DOI: 10.1088/1674-1137/41/12/124101

On the chiral covariant approach to ρρ scattering

  • 1.

      School of Physics and Nuclear Energy Engineering &

  • 2.

      Physics Department, The George Washington University, Washington, DC 20052, USA

  • 3.

      Departamento de Fí

  • We examine in detail a recent work (D. Gülmez, U. G. Meißner and J. A. Oller, Eur. Phys. J. C, 77:460 (2017)), where improvements to make ρρ scattering relativistically covariant are made. The paper has the remarkable conclusion that the J=2 state disappears with a potential which is much more attractive than for J=0, where a bound state is found. We trace this abnormal conclusion to the fact that an "on-shell" factorization of the potential is done in a region where this potential is singular and develops a large discontinuous and unphysical imaginary part. A method is developed, evaluating the loops with full ρ propagators, and we show that they do not develop singularities and do not have an imaginary part below threshold. With this result for the loops we define an effective potential, which when used with the Bethe-Salpeter equation provides a state with J=2 around the energy of the f2(1270). In addition, the coupling of the state to ρρ is evaluated and we find that this coupling and the T matrix around the energy of the bound state are remarkably similar to those obtained with a drastic approximation used previously, in which the q2 terms of the propagators of the exchanged ρ mesons are dropped, once the cut-off in the ρρ loop function is tuned to reproduce the bound state at the same energy.
      PCAS:
  • 加载中

  • References

    [1] J. A. Oller and E. Oset, Nucl. Phys. A, 620:438(1997) Erratum:[Nucl. Phys. A, 652:407(1999)]
    [2] N. Kaiser, Eur. Phys. J. A, 3:307(1998).
    [3] M. P. Locher, V. E. Markushin, and H. Q. Zheng, Eur. Phys. J. C, 4:317(1998)
    [4] J. Nieves and E. Ruiz Arriola, Phys. Lett. B, 455:30(1999)
    [5] T. Waas, N. Kaiser, and W. Weise, Phys. Lett. B, 379:34(1996)
    [6] E. Oset and A. Ramos, Nucl. Phys. A, 635:99(1998)
    [7] J. A. Oller and U. G. Meiner, Phys. Lett. B, 500:263(2001)
    [8] C. Garcia-Recio, J. Nieves, E. Ruiz Arriola, and M. J. Vicente Vacas, Phys. Rev. D, 67:076009(2003)
    [9] T. Hyodo, S. I. Nam, D. Jido, and A. Hosaka, Phys. Rev. C, 68:018201(2003)
    [10] J. A. Oller, E. Oset, and A. Ramos, Prog. Part. Nucl. Phys., 45:157(2000)
    [11] R. Molina, D. Nicmorus, and E. Oset, Phys. Rev. D, 78:114018(2008)
    [12] L. S. Geng and E. Oset, Phys. Rev. D, 79:074009(2009)
    [13] H. Nagahiro, J. Yamagata-Sekihara, E. Oset, S. Hirenzaki, and R. Molina, Phys. Rev. D, 79:114023(2009)
    [14] E. Oset, L. S. Geng, and R. Molina, J. Phys. Conf. Ser., 348:012004(2012)
    [15] D. Glmez, U. G. Meiner, and J. A. Oller, Eur. Phys. J. C, 77(7):460(2017) arXiv:1611.00168[hep-ph]
    [16] S. Weinberg, Phys. Rev., 130:776(1963); S. Weinberg, Phys. Rev. B, 137:672(1965)
    [17] V. Baru, J. Haidenbauer, C. Hanhart, Y. Kalashnikova, and A. E. Kudryavtsev, Phys. Lett. B, 586:53(2004)
    [18] D. Gamermann, J. Nieves, E. Oset and E. Ruiz Arriola, Phys. Rev. D, 81:014029(2010)
    [19] E. Klempt and A. Zaitsev, Phys. Rept., 454:1(2007)
    [20] V. Crede and C. A. Meyer, Prog. Part. Nucl. Phys., 63:74(2009)
    [21] J. J. Xie and E. Oset, Eur. Phys. J. A, 51:111(2015)
    [22] J. J. Xie, E. Oset, and L. S. Geng, Phys. Rev. C, 93(2):025202(2016)
    [23] M. Bando, T. Kugo, S. Uehara, K. Yamawaki, and T. Yanagida, Phys. Rev. Lett., 54:1215(1985)
    [24] M. Bando, T. Kugo, and K. Yamawaki, Phys. Rept., 164:217(1988)
    [25] U. G. Meiner, Phys. Rept., 161:213(1988)
    [26] S. Weinberg, Physica A, 96:327(1979)
    [27] J. Gasser and H. Leutwyler, Annals Phys., 158:142(1984)
    [28] S. Scherer, Adv. Nucl. Phys., 27:277(2003)
    [29] G. Ecker, J. Gasser, H. Leutwyler, A. Pich, and E. de Rafael, Phys. Lett. B, 223:425(1989)
    [30] G. F. Chew and S. Mandelstam, Phys. Rev., 119:467(1960)
    [31] J. A. Oller and E. Oset, Phys. Rev. D, 60:074023(1999)
    [32] J. R. Pelaez, Phys. Rept., 658:1(2016)
    [33] E. E. Salpeter and H. A. Bethe, Phys. Rev., 84:1232(1951)
    [34] T. Regge, Nuovo Cim., 14:951(1959)
    [35] T. Regge, Nuovo Cim., 18:947(1960)
    [36] M. M. Brisudova, L. Burakovsky, J. T. Goldman, and A. Szczepaniak, Phys. Rev. D, 67:094016(2003)
    [37] A. V. Barnes, D. J. Mellema, A. V. Tollestrup, R. L. Walker, O. I. Dahl, R. A. Johnson, R. W. Kenney, and M. Pripstein, Phys. Rev. Lett., 37:76(1976)
    [38] H. Navelet and P. R. Stevens, Nucl. Phys. B, 118:475(1977)
    [39] M. Guidal, J. M. Laget, and M. Vanderhaeghen, Nucl. Phys. A, 627:645(1997)
    [40] N. I. Kochelev, M. Battaglieri, and R. De Vita, Phys. Rev. C, 80:025201(2009)
    [41] C. R. Ji, R. Kaminski, L. Lesniak, A. Szczepaniak, and R. Williams, Phys. Rev. C, 58:1205(1998)
    [42] M. Battaglieri et al (CLAS Collaboration), Phys. Rev. D, 80:072005(2009)
    [43] J. Yamagata-Sekihara, J. Nieves, and E. Oset, Phys. Rev. D, 83:014003(2011)

  • Access

    加载中

Get Citation
Li-Sheng Geng, Raquel Molina and Eulogio Oset. On the chiral covariant approach to ρρ scattering[J]. Chinese Physics C, 2017, 41(12): 124101. doi: 10.1088/1674-1137/41/12/124101
Li-Sheng Geng, Raquel Molina and Eulogio Oset. On the chiral covariant approach to ρρ scattering[J]. Chinese Physics C, 2017, 41(12): 124101.  doi: 10.1088/1674-1137/41/12/124101 shu
Milestone
Received: 2017-06-05
Revised: 2017-08-31
Fund

    Supported by National Natural Science Foundation of China (11375024, 11522539), the Spanish Ministerio de Economia y Competitividad and European FEDER funds (FIS2011-28853-C02-01, FIS2011-28853-C02-02, FIS2014-57026-REDT, FIS2014-51948-C2-1-P, FIS2014-51948-C2-2-P), the Generalitat Valenciana in the program Prometeo Ⅱ-2014/068, We acknowledge the support of the European Community-Research Infrastructure Integrating Activity Study of Strongly Interacting Matter (acronym HadronPhysics3, Grant Agreement n. 283286) under the Seventh Framework Programme of the EU

Article Metric

Article Views(1604)
PDF Downloads(37)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
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:

On the chiral covariant approach to ρρ scattering

    Corresponding author: Li-Sheng Geng,
  • 1.  School of Physics and Nuclear Energy Engineering &
  • 2.  Physics Department, The George Washington University, Washington, DC 20052, USA
  • 3.  Departamento de Fí
  • Received Date: 2017-06-05
  • Accepted Date: 2017-08-31
  • Available Online: 2017-12-05
Fund Project:  Supported by National Natural Science Foundation of China (11375024, 11522539), the Spanish Ministerio de Economia y Competitividad and European FEDER funds (FIS2011-28853-C02-01, FIS2011-28853-C02-02, FIS2014-57026-REDT, FIS2014-51948-C2-1-P, FIS2014-51948-C2-2-P), the Generalitat Valenciana in the program Prometeo Ⅱ-2014/068, We acknowledge the support of the European Community-Research Infrastructure Integrating Activity Study of Strongly Interacting Matter (acronym HadronPhysics3, Grant Agreement n. 283286) under the Seventh Framework Programme of the EU

Abstract: We examine in detail a recent work (D. Gülmez, U. G. Meißner and J. A. Oller, Eur. Phys. J. C, 77:460 (2017)), where improvements to make ρρ scattering relativistically covariant are made. The paper has the remarkable conclusion that the J=2 state disappears with a potential which is much more attractive than for J=0, where a bound state is found. We trace this abnormal conclusion to the fact that an "on-shell" factorization of the potential is done in a region where this potential is singular and develops a large discontinuous and unphysical imaginary part. A method is developed, evaluating the loops with full ρ propagators, and we show that they do not develop singularities and do not have an imaginary part below threshold. With this result for the loops we define an effective potential, which when used with the Bethe-Salpeter equation provides a state with J=2 around the energy of the f2(1270). In addition, the coupling of the state to ρρ is evaluated and we find that this coupling and the T matrix around the energy of the bound state are remarkably similar to those obtained with a drastic approximation used previously, in which the q2 terms of the propagators of the exchanged ρ mesons are dropped, once the cut-off in the ρρ loop function is tuned to reproduce the bound state at the same energy.

    HTML

Reference (43)

目录

Link
IOPScience
SCOAP3
arXiv
Chinese Physical Society
Journal information
Introduction
Editorial Board
Others
Subscribe
Contact us
QQ: 1307685413
Tel: +86-010-88235947
Fax: +86-010-88233126
E-mail: cpc@ihep.ac.cn

  • CPC Website

  • IOP Website

  • CPC WeChat

Copyright © Institute of High Energy Physics, Chinese Academy of Sciences, 19B Yuquan Road, Beijing 100049, China 京ICP备05002789号-1

Supported by: Beijing Renhe Information Technology Co. Ltd  E-mail: info@rhhz.net

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return