Berry's phase and chiral anomalies

被引:3
作者
Fujikawa, Kazuo [1 ]
Umetsu, Koichiro [2 ]
机构
[1] RIKEN, Interdisciplinary Theoret & Math Sci Program iTHEM, Wako 3510198, Japan
[2] Nihon Univ, Coll Sci & Technol & Jr Coll, Lab Phys, Chiba 2748501, Japan
关键词
Berry's phase; Chiral anomaly; Anomalous Hall effect; Non-commutative geometry; Non-canonical system; Novel effects in nuclear physics; EXACTLY MASSLESS QUARKS; TRANSPORT PHENOMENA; MAGNETIC MONOPOLES; ADIABATIC THEOREM; GAUGE-THEORIES; LATTICE; FERMIONS; FIELD; FORMULATION; SYMMETRY;
D O I
10.1016/j.ppnp.2022.103992
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The basic materials of Berry's phase and chiral anomalies are presented to appreciate the phenomena related to those notions recently discussed in the literature. As for Berry's phase, a general survey of the subject including the anomalous Hall effect is presented using both Lagrangian and Hamiltonian formalisms. The canonical Hamiltonian formalism of the Born-Oppenheimer approximation, when applied to the anomalous Hall effect, can incorporate the gauge symmetry of Berry's connection but unable to incorporate the completely independent gauge symmetry of the electromagnetic vector potential simultaneously. Thus the Nernst effect is not realized in the canonical formalism. Transformed to the Lagrangian formalism with a time-derivative term allowed, the Born-Oppenheimer approximation can incorporate the electromagnetic vector potential simultaneously with Berry's connection, but the consistent canonical property is lost and thus becomes classical. The Lagrangian formalism can thus incorporate both gauge symmetries simultaneously but spoils the basic quantum symmetries, and thus results in classical anomalous Poisson brackets and the classical Nernst effect as in the conventional formalism. These properties are taken as the bases of the applications of Berry's phase to the anomalous Hall effect in the present review. As for chiral anomalies, we present basic materials by the path integral formulation with an emphasis on fermions on the lattice. A chiral fermion defined by gamma(5) on the lattice does not contain the chiral anomaly for the non-vanishing lattice spacing a not equal 0. Each species doubler separately does not contain a well-defined chiral anomaly either, since each species doubler defined in a part of the Brillouin zone is not a local field for a not equal 0. The idea of a spectral flow on the lattice does not lead to an anomaly for each species doubler separately but rather to a pair production in a general sense. We also mention that a specific construction called the Ginsparg-Wilson fermion, which is free of species doublers, may practically be useful in the theoretical analysis of an Abelian massless Dirac fermion in condensed matter physics. We discuss a limited number of representative applications of Berry's phase and chiral anomalies in nuclear physics and related fields to illustrate the use of these two basic notions presented in this article. (c) 2022 Elsevier B.V. All rights reserved.
引用
收藏
页数:63
相关论文
共 105 条
[1]   ENERGY BANDS IN THE PRESENCE OF AN EXTERNAL FORCE FIELD .2. ANOMALOUS VELOCITIES [J].
ADAMS, EN ;
BLOUNT, EI .
JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS, 1959, 10 (04) :286-303
[2]   AXIAL-VECTOR VERTEX IN SPINOR ELECTRODYNAMICS [J].
ADLER, SL .
PHYSICAL REVIEW, 1969, 177 (5P2) :2426-&
[3]  
Adler SL., 1970, Perturbation Theory Anomalies
[4]   PHASE-CHANGE DURING A CYCLIC QUANTUM EVOLUTION [J].
AHARONOV, Y ;
ANANDAN, J .
PHYSICAL REVIEW LETTERS, 1987, 58 (16) :1593-1596
[5]   SIGNIFICANCE OF ELECTROMAGNETIC POTENTIALS IN THE QUANTUM THEORY [J].
AHARONOV, Y ;
BOHM, D .
PHYSICAL REVIEW, 1959, 115 (03) :485-491
[6]   Simulating dynamically assisted production of Dirac pairs in gapped graphene monolayers [J].
Akal, I. ;
Egger, R. ;
Mueller, C. ;
Villalba-Chavez, S. .
PHYSICAL REVIEW D, 2019, 99 (01)
[7]   GRAVITATIONAL ANOMALIES [J].
ALVAREZGAUME, L ;
WITTEN, E .
NUCLEAR PHYSICS B, 1984, 234 (02) :269-330
[8]   THE AXIAL ANOMALY AND THE LATTICE DIRAC SEA [J].
AMBJORN, J ;
GREENSITE, J ;
PETERSON, C .
NUCLEAR PHYSICS B, 1983, 221 (02) :381-408
[9]   REGULARIZED FUNCTIONAL INTEGRAL FOR FERMIONS AND ANOMALIES [J].
ANDRIANOV, A ;
BONORA, L ;
GAMBOASARAVI, R .
PHYSICAL REVIEW D, 1982, 26 (10) :2821-2826
[10]  
[Anonymous], 2004, Path integrals and quantum anomalies, DOI DOI 10.1103/PhysRevB.92.075205