I=1/2 low-lying mesons in lattice QCD

  • Using a conventional constituent-quark model, I=1/2 scalar κ, vector K*(892), and axial vector K1 mesons are studied in the asqtad-improved staggered fermion with wall-source and point-sink interpolators. The mass ratio of mκ/mK*(892) is numerically confirmed to apparently vary with quark mass, and the experimental ordering mK*(892) > mκ holds elegantly when the light u/d quark masses are sufficiently small, while the valence strange quark mass is fixed to its physical value. We also get reasonable signals for the K1 meson suggested by the SCALAR Collaboration from lattice QCD. The computations are conducted with the MILC Nf=3 flavor gauge configurations at three lattice spacings: a≈ 0.15, 0.12, and 0.09 fm.
      PCAS:
  • 加载中
  • [1] Olive K et al. (Particle Data Group collaboration). Chin. Phys. C, 2014, 38: 090001[2] Bugg D. Phys. Rev. D, 2010, 81: 014002[3] Aitala M et al. Phys. Rev. Lett., 2002, 89: 121801; Ablikim M et al. Phys. Lett. B, 2011, 698: 183; Ablikim M et al. Phys. Lett. B, 2010, 693: 88[4] Alde D et al. Phys. Lett. B, 1997, 397: 350[5] Bonvicini G et al. Phys. Rev. D, 2008, 78: 052001[6] Ablikim M et al. Phys. Lett. B, 2006, 633: 681; Boito D, Escribano R, Jamin M. J. High Energy Phys., 2010, 1009: 031; Mitchell R et al. Phys. Rev. D, 2009, 79: 072008; Aubert B et al. Phys. Rev. D, 2007, 76: 012008[7] Bernard C et al. Phys. Rev. D, 2001, 64: 054506; Aubin C et al. Phys. Rev. D, 2004, 70: 094505[8] Aoki S et al. Phys. Rev. D, 2003, 67: 034503[9] Prelovsek S et al. Phys. Rev. D, 2013, 88: 054508[10] FU Z, FU K. Phys. Rev. D, 2012, 86: 094507[11] Kunihiro T et al. Phys. Rev. D, 2004, 70: 034504[12] Wada H et al. Phys. Lett. B, 2007, 652: 250[13] Kunihiro T et al. EPJ Web Conf., 2010, 3: 03010[14] Nakamura A. eConf: C0402171[15] Sekiguchi M et al. Conf. Proc. C, 2011, 110613: 117[16] Nebreda J, Peláez J. Phys. Rev. D, 2010, 81: 054035[17] FU Zi-Wen, DeTar C. Chin. Phys. C, 2011, 35: 1079; FU Zi-Wen. Chin. Phys. C, 2012, 36: 489; FU Z. Int. J. Mod. Phys. A, 2013, 28: 1350059; FU Zi-Wen. Chin. Phys. C, 2014, 38, 063102[18] Aubin C et al. Phys. Rev. D, 2004, 70: 094505[19] Daum C et al. (ACCMOR collaboration). Nucl. Phys. B, 1981, 187: 1[20] Kunihiro T et al. PoS LATTICE, 2006, 2005: 034[21] Kunihiro T et al. Acta Phys. Polon. B, 2007, 38: 491[22] Beveren E, Rupp G. Eur. Phys. J. A, 2007, 31: 468[23] Golterman M. Nucl. Phys. B, 1986, 273: 663[24] Bernard C et al. Phys. Rev. D, 2007, 76: 094504; FU Z. J. High Energy Phys., 2012, 1207: 142; FU Zi-Wen, DeTar C. Chin. Phys. C, 2011, 35: 896; FU Zi-Wen. Chin. Phys. Lett., 2011, 28: 081202; FU Z. Phys. Rev. D, 2013, 87: 074501; FU Zi-Wen. Commun. Theor. Phys., 2012, 57: 78[25] Geng L S et al. Phys. Rev. D, 2007, 75: 014017[26] Bazavov A et al. Rev. Mod. Phys., 2010, 82: 1349[27] Bernard C et al. Phys. Rev. D, 2011, 83: 034503[28] Aubin C et al. (MILC collaboration). Phys. Rev. D, 2004, 70: 114501[29] Jeltema T, Sher M. Phys. Rev. D, 2000, 61: 017301; Hanhart C, Pelaez J, Rios G. Phys. Rev. Lett., 2008, 100: 152001[30] Roca L, Oset E. Phys. Rev. D, 2012, 85: 054507[31] Alford M, Jaffe R. Nucl. Phys. B, 2000, 578: 367[32] Prelovsek S et al. Phys. Rev. D, 2010, 82: 094507; Prelovsek S, Mohler D. Phys. Rev. D, 2009, 79: 014503[33] Loan M, LUO Z, Lam Y. Eur. Phys. J. C, 2008, 57: 579[34] Alexandrou C et al. J. High Energy Phys., 2013, 1304: 137[35] Wagner M et al. (ETM collaboration). Acta Phys. Polon. Supp., 2013, 6(3): 847[36] GUO F et al. Phys. Rev. D, 2013, 88: 074506[37] Wagner M et al. (ETM collaboration). PoS LATTICE, 2014, 2013: 258; Abdel-Rehim A et al. arXiv: hep-lat/1410.8757[38] FU Z. Eur. Phys. J. C, 2012, 72: 2159; FU Zi-Wen. Commun. Theor. Phys., 2014, 61: 75[39] FU Z. J. High Energy Phys., 2012, 1201: 017; FU Z. Phys. Rev. D, 2012, 85: 014506; FU Z. Phys. Rev. D, 2012, 85: 074501
  • 加载中

Get Citation
FU Zi-Wen. I=1/2 low-lying mesons in lattice QCD[J]. Chinese Physics C, 2015, 39(8): 083101. doi: 10.1088/1674-1137/39/8/083101
FU Zi-Wen. I=1/2 low-lying mesons in lattice QCD[J]. Chinese Physics C, 2015, 39(8): 083101.  doi: 10.1088/1674-1137/39/8/083101 shu
Milestone
Received: 2014-12-05
Revised: 2015-02-05
Article Metric

Article Views(1686)
PDF Downloads(288)
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:

I=1/2 low-lying mesons in lattice QCD

    Corresponding author: FU Zi-Wen,

Abstract: Using a conventional constituent-quark model, I=1/2 scalar κ, vector K*(892), and axial vector K1 mesons are studied in the asqtad-improved staggered fermion with wall-source and point-sink interpolators. The mass ratio of mκ/mK*(892) is numerically confirmed to apparently vary with quark mass, and the experimental ordering mK*(892) > mκ holds elegantly when the light u/d quark masses are sufficiently small, while the valence strange quark mass is fixed to its physical value. We also get reasonable signals for the K1 meson suggested by the SCALAR Collaboration from lattice QCD. The computations are conducted with the MILC Nf=3 flavor gauge configurations at three lattice spacings: a≈ 0.15, 0.12, and 0.09 fm.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return