×
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

Ratio of a strange quark mass ms to up or down quark mass mu,d predicted by a quark propagator in the frameworkof the chiral perturbation theory

  • Based on the fully dressed quark propagator and chiral perturbation theory, we study the ratio of the strange quark mass ms to up or down quark mass mu,d. The ratio is related to the determination of quark masses which are fundamental input parameters of QCD Lagrangian in the Standard Model of particle physics and can not be directly measured since the quark is confined within a hadron. An accurate determination of these QCD free parameters is extremely important for both phenomenological and theoretical applications. We begin with a brief introduction to the non-perturbation QCD theory, and then study the mass ratio in the framework of the chiral perturbation theory (χ PT) with a parameterized fully dressed quark propagator which describes confining fully dressed quark propagation and is analytic everywhere in the finite complex p2-plane and has no Lehmann representation so there are no quark production thresholds in any theoretical calculations of observable data. Our prediction for the ratio ms/mu,d is consistent with other model predictions such as Lattice QCD, instanton model, QCD sum rules and the empirical values used widely in the literature. As a by-product of this study, our theoretical results, together with other predictions of physical quantities that used this quark propagator in our previous publications, clearly show that the parameterized form of the fully dressed quark propagator is an applicable and reliable approximation to the solution of the Dyson-Schwinger Equation of quark propagator in the QCD.
      PCAS:
  • 加载中
  • [1] 't Hooft G. Phys. Rev. Lett., 1976, 37: 8; Witten E. Nucl. Phys. B, 1979, 156: 269; Veneziano G. Nucl. Phys. B, 1979, 159: 213[2] Herwijnen E V, Williams P G. Phys. Rev. D, 1981, 24: 240[3] Herwijnen E V, Williams P G. Nucl. Phys. B, 1982, 196: 109[4] Gasser J, Leutwyler H. Phys. Rept. C, 1982, 87: 77[5] Gell-Mann M, Oakes R J, Renner B. Phys. Rev., 1968, 175: 2195[6] Gunion J F, McNamee P C, Scadron M D. Nucl. Phys. B, 1977, 123: 445; Caser S, Testa M. Phys. Lett. B, 1976, 61: 267[7] Roberts C D, Williams A G. Prog. Part. Nucl. Phys., 2004, 33: 477; ZHOU Li-Juan, WU Qing, PAN Ji-Huan et al. Commun. Theor. Phys., 2006, 46: 101[8] Gasser J, Leutwyler H. Nucl. Phys. B, 1985, 250: 465; Gasser J, Leutwyler H. Phys. Lett. B, 1983, 125: 321; Ann. of Phys., 1984, 158: 142[9] Colangelo G, Gasser J, Rusetsky A. Eur. Phys. J. C, 2009, 59: 777 (arXiv:0811.0775 [hep-ph]); Bissegger M, Fuhrer A, Gasser J et al. Nucl. Phys. B, 2009, 806: 178 (arXiv:0807.0515 [hep-ph])[10] Weinberg S. Trans. New York Acad. Sci., 1977, 38: 185[11] Georgi H. Weak Interactions and Modern Particle Theory. Menlo Park, California: Addison-Wesley Publishing Company, Inc., 1984[12] Bazavov A et al. (MILC collaboration). PoS, C D, 2009, 09: 007 (arXiv:0910.2966 [hep-ph])[13] Kisslinger L S, Meissner T. Phys. Rev. C, 1998, 58: 1528; Roberts C D, Cahill R T, Sevior M E et al. Phys. Rev. D, 1994, 49: 125[14] Roberts C D. Prog. Part. Nucl. Phys., 2000, 45: 511; Cahill R T, Roberts C D. Phys. Rev. D, 1985, 32: 2419; Cahill R T. Nucl. Phys. A, 1992, 543: 63C; Tandy P C. Prog. Part. Nucl. Phys., 1997, 39: 117 (arXiv:nucl-th/9705018); ZHOU Li-Juan, MA Wei-Xing. Commun. Theor. Phys., 2006, 45: 675[15] MA Wei-Xing, SHEN Peng-Nian, ZHOU Li-Juan. Commun. Theor. Phys., 2002, 38: 571[16] GU Yun-Ting, QIN Song-Mei, ZHOU Li-Juan et al. Commun. Theor. Phys., 2008, 50: 1205[17] Groom D E (Particle Data Group). Eur. Phys. J. C, 2000, 15: 1[18] Jamin M, Munz M, CERN- TH.7435/94, TUM-T31-78/94[19] Dominguez C A. Nucl. Phys. Proc. (Suppl.), 1998, 66: 486[20] Weinberg S. in Festschrift for I. I. Rabi. edited by MOTZ L (1978)[21] Kaiser R. The η and η' at large Nc. Diploma work, University of Bern, 1997; Leutwyler H. Nucl. Phys. Proc. (Suppl.), 1998, 64: 223
  • 加载中

Get Citation
PENG Jin-Song, ZHOU Li-Juan, MENG Cheng-Ju, PAN Ji-Huan, MA Wei-Xing and YUAN Tong-Quan. Ratio of a strange quark mass ms to up or down quark mass mu,d predicted by a quark propagator in the frameworkof the chiral perturbation theory[J]. Chinese Physics C, 2013, 37(4): 043101. doi: 10.1088/1674-1137/37/4/043101
PENG Jin-Song, ZHOU Li-Juan, MENG Cheng-Ju, PAN Ji-Huan, MA Wei-Xing and YUAN Tong-Quan. Ratio of a strange quark mass ms to up or down quark mass mu,d predicted by a quark propagator in the frameworkof the chiral perturbation theory[J]. Chinese Physics C, 2013, 37(4): 043101.  doi: 10.1088/1674-1137/37/4/043101 shu
Milestone
Received: 2012-04-13
Revised: 2012-11-20
Article Metric

Article Views(2338)
PDF Downloads(409)
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:

Ratio of a strange quark mass ms to up or down quark mass mu,d predicted by a quark propagator in the frameworkof the chiral perturbation theory

Abstract: Based on the fully dressed quark propagator and chiral perturbation theory, we study the ratio of the strange quark mass ms to up or down quark mass mu,d. The ratio is related to the determination of quark masses which are fundamental input parameters of QCD Lagrangian in the Standard Model of particle physics and can not be directly measured since the quark is confined within a hadron. An accurate determination of these QCD free parameters is extremely important for both phenomenological and theoretical applications. We begin with a brief introduction to the non-perturbation QCD theory, and then study the mass ratio in the framework of the chiral perturbation theory (χ PT) with a parameterized fully dressed quark propagator which describes confining fully dressed quark propagation and is analytic everywhere in the finite complex p2-plane and has no Lehmann representation so there are no quark production thresholds in any theoretical calculations of observable data. Our prediction for the ratio ms/mu,d is consistent with other model predictions such as Lattice QCD, instanton model, QCD sum rules and the empirical values used widely in the literature. As a by-product of this study, our theoretical results, together with other predictions of physical quantities that used this quark propagator in our previous publications, clearly show that the parameterized form of the fully dressed quark propagator is an applicable and reliable approximation to the solution of the Dyson-Schwinger Equation of quark propagator in the QCD.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return