Distribution of stress tensor around static quark-anti-quark from Yang-Mills gradient flow

被引:28
作者
Yanagihara, Ryosuke [1 ]
Iritani, Takumi [2 ]
Kitazawa, Masakiyo [1 ,3 ]
Asakawa, Masayuki [1 ]
Hatsuda, Tetsuo [2 ,4 ]
机构
[1] Osaka Univ, Dept Phys, Toyonaka, Osaka 5600043, Japan
[2] RIKEN, RIKEN Nishina Ctr, Wako, Saitama 3510198, Japan
[3] KEK, Inst Particle & Nucl Studies, KEK Theory Ctr, J PARC Branch, 203-1 Shirakata, Tokai, Ibaraki 3191106, Japan
[4] RIKEN, RIKEN Interdisciplinary Theoret & Math Sci Progra, Wako, Saitama 3510198, Japan
关键词
Lattice gauge theory; Strong interaction; Gradient flow; Stress tensor; FLUX TUBES; STRING TENSION; CONFINEMENT;
D O I
10.1016/j.physletb.2018.09.067
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The spatial distribution of the stress tensor around the quark-anti-quark (Q (Q) over bar) pair in SU(3) lattice gauge theory is studied. The Yang-Mills gradient flow plays a crucial role to make the stress tensor well-defined and derivable from the numerical simulations on the lattice. The resultant stress tensor with a decomposition into local principal axes shows, for the first time, the detailed structure of the flux tube along the longitudinal and transverse directions in a gauge invariant manner. The linear confining behavior of the Q (Q) over bar potential at long distances is derived directly from the integral of the local stress tensor. (C) 2018 The Authors. Published by Elsevier B.V.
引用
收藏
页码:210 / 214
页数:5
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