A gauge field theory of fermionic continuous-spin particles

被引：38

作者：

Bekaert, X. ^{[1
,2
]}

Najafizadeh, M. ^{[1
,3
]}

Setare, M. R. ^{[3
]}

机构：

[1] Univ Tours, Federat Rech Denis Poisson 2964, Unite Mixte Rech 7350, Lab Math & Phys Theor,CNRS, Parc Grandmont, F-37200 Tours, France

[2] Inst for Basic Sci Korea, BW Lee Ctr Fields Grav & Strings, Daejeon, South Korea

[3] Univ Kurdistan, Dept Phys, Fac Sci, Sanandaj 6617715177, Iran

来源：

PHYSICS LETTERS B | 2016年 / 760卷

基金：

俄罗斯科学基金会;

关键词：

Continuous spin particle; Poincare group representation; Higher spin theory; MASSLESS FIELDS; REPRESENTATIONS;

D O I：

10.1016/j.physletb.2016.07.005

中图分类号：

P1 [天文学];

学科分类号：

0704 ;

摘要：

In this letter, we suggest a local covariant action for a gauge field theory of fermionic Continuous-Spin Particles (CSPs). The action is invariant under gauge transformations without any constraint on both the gauge field and the gauge transformation parameter. The Fang-Fronsdal equations for a tower of massless fields with all half-integer spins arise as a particular limit of the equation of motion of fermionic CSPs. (C) 2016 The Authors. Published by Elsevier B.V.

引用

页码：320 / 323

页数：4

共 17 条

[1]

Bekaert X, 2006, J HIGH ENERGY PHYS

[2]

Borgmann V., 1984, P NATL ACAD SCI USA, V34, P211

[3] Continuous spin representations of the Poincare and super-Poincare groups [J].