×
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

Spectra of charmed and bottom baryons with hyperfine interaction

  • Up to now, the excited charmed and bottom baryon states have still not been well studied experimentally or theoretically. In this paper, we predict the mass of Ωb*, the only L=0 baryon state which has not been observed, to be 6069.2 MeV. The spectra of charmed and bottom baryons with the orbital angular momentum L=1 are studied in two popular constituent quark models, the Goldstone boson exchange (GBE) model and the one gluon exchange (OGE) hyperfine interaction model. Inserting the latest experimental data from the "Review of Particle Physics", we find that in the GBE model, there exist some multiplets (∑c(b), Ξ'c(b) and Ωc(b)) in which the total spin of the three quarks in their lowest energy states is 3/2, but in the OGE model there is no such phenomenon. This is the most important difference between the GBE and OGE models. These results can be tested in the near future. We suggest more efforts to study the excited charmed and bottom baryons both theoretically and experimentally, not only for the abundance of baryon spectra, but also for determining which hyperfine interaction model best describes nature.
      PCAS:
  • 加载中
  • [1] L. A. Copley, N. Isgur, and G. Karl, Phys. Rev. D, 20:768(1979)
    [2] L. Y. Glozman and D. O. Riska, Phys. Rept., 268:263(1996)
    [3] L. Y. Glozman and D. O. Riska, Nucl. Phys. A, 603:326(1996)
    [4] N. Isgur and G. Karl, Phys. Rev. D, 19:2653(1979)
    [5] N. Isgur and G. Karl, Phys. Rev. D, 18:4187(1978)
    [6] K. Maltman and N. Isgur, Phys. Rev. D, 22:1701(1980)
    [7] N. Mathur, Y. Chen, S. J. Dong, T. Draper, I. Horvath, F. X. Lee, K. F. Liu, and J. B. Zhang, Phys. Lett. B, 605:137(2005)
    [8] K. A. Olive et al (Particle Data Group Collaboration), Chin. Phys. C, 38:090001(2014)
    [9] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 109:172003(2012)
    [10] R. Aaij et al (LHCb Collaboration), Phys. Rev. Lett., 114:062004(2015)
    [11] R. Mizuk et al (Belle Collaboration), Phys. Rev. Lett., 94:122002(2005)
    [12] B. Aubert et al (BaBar Collaboration), Phys. Rev. D, 78:112003(2008)
    [13] A. De Rujula, H. Georgi, and S. L. Glashow, Phys. Rev. D, 12:147(1975)
    [14] S. Godfrey and N. Isgur, Phys. Rev. D, 32:189(1985)
    [15] J. Q. Chen, Group Representation Theory for Physicists, (Singapore:World Scientific, 1989)
    [16] Zhong-Qi Ma, Group Theory in Physics (in Chinese) (Beijing:Science Press, 1998)
    [17] F. E. Close, An Introduction to Quarks and Partons, (New York:Academic Press 1979)
    [18] N. Isgur and G. Karl, Phys. Lett. B 72:109(1977)
    [19] N. Isgur and G. Karl, Phys. Rev. D, 20:1191(1979)
    [20] S. Capstick and W. Roberts, Prog. Part. Nucl. Phys., 45:S241(2000)
    [21] V. Borka Jovanovic, S. R. Ignjatovic, D. Borka, and P. Jovanovic, Phys. Rev. D, 82:117501(2010)
    [22] F. Buisseret, N. Matagne, and C. Semay, Phys. Rev. D, 85:036010(2012)
    [23] S. Capstick and N. Isgur, Phys. Rev. D, 34:2809(1986)
    [24] V. Borka Jovanovic and D. Borka, Rom. J. Phys., 57:803(2012)
    [25] M. Karliner and J. L. Rosner, Phys. Rev. D, 90(9):094007(2014)
    [26] D. Ebert, R. N. Faustov, and V. O. Galkin, Phys. Rev. D, 84:014025(2011)
    [27] Z. Shah, K. Thakkar, A. Kumar Rai, and P. C. Vinodkumar, Eur. Phys. J. A, 52(10):313(2016)
    [28] Z. Shah, K. Thakkar, A. K. Rai, and P. C. Vinodkumar, Chin. Phys. C, 40(12):123102(2016)
    [29] K. L. Wang, L. Y. Xiao, X. H. Zhong, and Q. Zhao, arXiv:1703.09130[hep-ph]
    [30] B. Chen and X. Liu, arXiv:1704.02583[hep-ph]
  • 加载中

Get Citation
Zhen-Yang Wang, Jing-Juan Qi, Xin-Heng Guo and Ke-Wei Wei. Spectra of charmed and bottom baryons with hyperfine interaction[J]. Chinese Physics C, 2017, 41(9): 093103. doi: 10.1088/1674-1137/41/9/093103
Zhen-Yang Wang, Jing-Juan Qi, Xin-Heng Guo and Ke-Wei Wei. Spectra of charmed and bottom baryons with hyperfine interaction[J]. Chinese Physics C, 2017, 41(9): 093103.  doi: 10.1088/1674-1137/41/9/093103 shu
Milestone
Received: 2017-02-10
Revised: 2017-05-12
Fund

    Supported by National Natural Science Foundation of China (11175020, 11575023, U1204115)

Article Metric

Article Views(1604)
PDF Downloads(28)
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:

Spectra of charmed and bottom baryons with hyperfine interaction

    Corresponding author: Zhen-Yang Wang,
    Corresponding author: Jing-Juan Qi,
    Corresponding author: Xin-Heng Guo,
    Corresponding author: Ke-Wei Wei,
  • 1.  College of Nuclear Science and Technology, Beijing Normal University, Beijing 100875, China
  • 2.  College of Physics and Electrical Engineering, Anyang Normal University, Anyang 455000, China
Fund Project:  Supported by National Natural Science Foundation of China (11175020, 11575023, U1204115)

Abstract: Up to now, the excited charmed and bottom baryon states have still not been well studied experimentally or theoretically. In this paper, we predict the mass of Ωb*, the only L=0 baryon state which has not been observed, to be 6069.2 MeV. The spectra of charmed and bottom baryons with the orbital angular momentum L=1 are studied in two popular constituent quark models, the Goldstone boson exchange (GBE) model and the one gluon exchange (OGE) hyperfine interaction model. Inserting the latest experimental data from the "Review of Particle Physics", we find that in the GBE model, there exist some multiplets (∑c(b), Ξ'c(b) and Ωc(b)) in which the total spin of the three quarks in their lowest energy states is 3/2, but in the OGE model there is no such phenomenon. This is the most important difference between the GBE and OGE models. These results can be tested in the near future. We suggest more efforts to study the excited charmed and bottom baryons both theoretically and experimentally, not only for the abundance of baryon spectra, but also for determining which hyperfine interaction model best describes nature.

    HTML

Reference (30)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return