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《中国物理C》(英文)编辑部
2024年10月30日

LATTICE FORMULATION OF THE PURE GAUGE FIELDS ON COSET SPACE

  • In this paper we construct a lattice formulation of the pure gauge fields on a coset space in the cases of a group G with non-trivial topological property and of a chiral group G, and present a local gauge invariant action of a quark system on a four-dimensional Euclidean space lattice, which has the continuum limit as usual. For non-chiral group with trivial topological property, it is shown that the coset pure gauge fields have no influence on the confinement properties of the confinement properties of the quark system by calculating lattice current-current propagator when the coset pure gauge fields remain manifest.
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  • [1] 周光召、杜东生、阮图南, Scientia Sinica, 22(1979), 37.[2] 周光召, Scientia Sinica, 23(1980), 431[3] Zhou Guang-Zhao, Ruan Tu-nan, Journal of CUST, 11(1981), 15, Proceedings of the 1980 Guangzhou Conference on Theoretical Particle Physics, p. 902.[4] K .G. Wilson, Phys. Rev., D10(1974), 2445.
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RUAN Tu-Nan, JING Si-Cong and LIU Zu-Wei. LATTICE FORMULATION OF THE PURE GAUGE FIELDS ON COSET SPACE[J]. Chinese Physics C, 1983, 7(5): 550-559.
RUAN Tu-Nan, JING Si-Cong and LIU Zu-Wei. LATTICE FORMULATION OF THE PURE GAUGE FIELDS ON COSET SPACE[J]. Chinese Physics C, 1983, 7(5): 550-559. shu
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Received: 1900-01-01
Revised: 1900-01-01
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LATTICE FORMULATION OF THE PURE GAUGE FIELDS ON COSET SPACE

    Corresponding author: RUAN Tu-Nan,

Abstract: In this paper we construct a lattice formulation of the pure gauge fields on a coset space in the cases of a group G with non-trivial topological property and of a chiral group G, and present a local gauge invariant action of a quark system on a four-dimensional Euclidean space lattice, which has the continuum limit as usual. For non-chiral group with trivial topological property, it is shown that the coset pure gauge fields have no influence on the confinement properties of the confinement properties of the quark system by calculating lattice current-current propagator when the coset pure gauge fields remain manifest.

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