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《中国物理C》(英文)编辑部
2024年10月30日

Heavy quarkonia spectra and their decays in a relativistic quark model

  • Using the phenomenological relativistic harmonic model (RHM) for quarks, we have obtained the masses of S wave charmonium and bottomonium states. The full Hamiltonian used in the investigation has Lorentz scalar plus vector confinement potential, along with the confined one gluon exchange potential (COGEP). A good agreement with the experimental masses for the ground and the radially excited states is obtained both for the triplet and singlet S wave mesons. The decay properties of the ground state charmonium and bottomonium are investigated.
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  • [1] Nakamura K et al. (Particle Data Group). J. Phys. G: Nucl. Part. Phys., 2010, 37: 0750212 Amsler C et al. (Particle Data Group). Phy. Lett. B, 2008, 667: 13 Gromes D. Nucl. Phys. B, 1977, 130: 184 Greenberg O. W. Ann. Rev. Nucl. Part. Sci., 1978 28: 3275 Bhaduri R K, Cohler L E, Nogami Y. Nuovo Cim. A, 1981, 65: 3766 Godfrey S, Isgur N. Phys. Rev. D, 1985, 32: 1897 Silvestre-Brac B, Gignoux C. Phys. Rev. D, 1985, 32: 7438 Vijayakumar K B, Hanumaiah B, Pepin S. Eur. Phys. J. A, 2004, 19: 2479 Eichten E, Godfrey S, Mahlke H, Rosner J L. Rev. Mod. Phys., 2008, 80: 1161; arXiiv: hep-ph/0701208v310 Appelquist T, Politzer H D. Phys. Rev. Lett., 1975, 34: 4311 Kwong W, Rosner J L, Quigg C. Annu. Rev. Nucl. Part. Sci., 1987, 37: 32512 Kwong W, Mackenzie P B. Phys. Rev. D, 1988, 37: 321013 Suaya R, Townsend J. Phys. Rev. D, 1977, 16: 334614 Bergstrom L, Snellman H, Tengstrand G. Phys. Lett. B, 1979, 82: 41915 LI Z P, Close F E, Barnes T. Phys. Rev. D, 1991, 43: 216116 Gupta S N, Johnson J M. Phys. Rev. D, 1996, 54: 2075; arXiv:hep-ph/960634917 Khadkikar S B, Gupta S K. Phys. Lett. B, 1983, 124: 52318 Vinodkumar P C, Vijay Kumar K B, Khadkikar S B. Pramana-J. Phys., 1992, 39: 4719 Khadkikar S B, Vinodkumar P C. Pramana-J. Phys., 1987, 29: 3920 Khadkikar S B, Vijaya Kumar K B. Phys. Lett. B, 1991, 254: 32021 Vijaya Kumar K B, Khadkikar S B. Nucl. Phys. A, 1993, 556: 39622 Fishbane P M et al. Phys. Rev. D, 1983, 27: 243323 Gartenhaus G, Schwartz C. Phys. Rev., 1957, 108: 48224 Khadkikar S B. Pramana-J. Phys., 1985, 24: 6325 Feynman R P, Kislinger M, Ravndal F. Phys. Rev. D, 1976, 3: 270626 Monteiro A P, Vijaya Kumar K. B. Commun. Theor. Phys., 2010, 53: 32527 Lakhina O, Swanson E S. Phys. Rev. D, 2006, 74: 01401228 Van Royen R, Weisskpof V F. Nuovo Cim. A, 1967, 50: 61729 Laverty J T, Radford S F, Repko W W. 2009, arXiv: hepph/0901.3917v330 Kwong W, Mackenzie P B, Rosenfeld R, Rosner J L. Phys. Rev. D, 1988, 37: 321031 Aubert J J et al. Phys. Rev. Lett., 1974, 33: 1401
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Bhaghyesh, K. B. Vijaya Kumar and Antony Prakash Monteiro. Heavy quarkonia spectra and their decays in a relativistic quark model[J]. Chinese Physics C, 2011, 35(11): 997-1003. doi: 10.1088/1674-1137/35/11/003
Bhaghyesh, K. B. Vijaya Kumar and Antony Prakash Monteiro. Heavy quarkonia spectra and their decays in a relativistic quark model[J]. Chinese Physics C, 2011, 35(11): 997-1003.  doi: 10.1088/1674-1137/35/11/003 shu
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Received: 2011-01-06
Revised: 2011-02-17
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Heavy quarkonia spectra and their decays in a relativistic quark model

Abstract: Using the phenomenological relativistic harmonic model (RHM) for quarks, we have obtained the masses of S wave charmonium and bottomonium states. The full Hamiltonian used in the investigation has Lorentz scalar plus vector confinement potential, along with the confined one gluon exchange potential (COGEP). A good agreement with the experimental masses for the ground and the radially excited states is obtained both for the triplet and singlet S wave mesons. The decay properties of the ground state charmonium and bottomonium are investigated.

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