In order to generate mass for an abelian spin-1 vector field while preserving gauge invariance we couple it to a symmetric tensor. The derivative coupling includes up to three derivatives. We show that unitarity, causality and absence of Stueckelberg (compensating) fields single out a unique model up to trivial field redefinitions. The model contains one massive and one massless spin-1 particle. It is shown by means of a master action to be dual to the direct sum of a Maxwell plus a Maxwell-Proca theory.Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq
The generic form of space-time dynamics as a classical gauge field theory has recently been derived,...
AbstractIn this paper we consider frame-like formulation for mixed symmetry spin-tensors correspondi...
Massive spin-one particles have been described by means of an antisymmetric second-rank tensor field...
In the topologically massive BF model (TMBF) the photon becomes massive via coupling to an antisymme...
AbstractIn the topologically massive BF model (TMBF) the photon becomes massive via coupling to an a...
A `covariant' field that transforms like a relativistic field operator is required to be a linear co...
Starting with a description of massive spin-2 particles in D = 4 in terms of a mixed symmetry tensor...
We present the most general ghost-free classical Lagrangian containing first-order derivatives and d...
We analyse the properties of massless (bose or fermi) particles with spin j;;;; I that have non-vani...
407-410Lorentz condition in Maxwell’s eleclromagnetic theory implies that transverse photon of spin...
In light of recent progress in ghost-free theories of massive gravity and multi-gravity, we reconsid...
Nontrivial translation matrices occur for spin (A,B)+(C,D) with |A-C| = |B-D| = 1/2, necessarily ass...
The four-dimensional theory of a 1-form abelian gauge field A coupled to a 2-form (antisymmetric ten...
We show how implementing invariance under divergence-free gauge transformations leads to a remarkabl...
Gauge field theory with rank-one field Tμ is a quantum field theory that describes the interaction o...
The generic form of space-time dynamics as a classical gauge field theory has recently been derived,...
AbstractIn this paper we consider frame-like formulation for mixed symmetry spin-tensors correspondi...
Massive spin-one particles have been described by means of an antisymmetric second-rank tensor field...
In the topologically massive BF model (TMBF) the photon becomes massive via coupling to an antisymme...
AbstractIn the topologically massive BF model (TMBF) the photon becomes massive via coupling to an a...
A `covariant' field that transforms like a relativistic field operator is required to be a linear co...
Starting with a description of massive spin-2 particles in D = 4 in terms of a mixed symmetry tensor...
We present the most general ghost-free classical Lagrangian containing first-order derivatives and d...
We analyse the properties of massless (bose or fermi) particles with spin j;;;; I that have non-vani...
407-410Lorentz condition in Maxwell’s eleclromagnetic theory implies that transverse photon of spin...
In light of recent progress in ghost-free theories of massive gravity and multi-gravity, we reconsid...
Nontrivial translation matrices occur for spin (A,B)+(C,D) with |A-C| = |B-D| = 1/2, necessarily ass...
The four-dimensional theory of a 1-form abelian gauge field A coupled to a 2-form (antisymmetric ten...
We show how implementing invariance under divergence-free gauge transformations leads to a remarkabl...
Gauge field theory with rank-one field Tμ is a quantum field theory that describes the interaction o...
The generic form of space-time dynamics as a classical gauge field theory has recently been derived,...
AbstractIn this paper we consider frame-like formulation for mixed symmetry spin-tensors correspondi...
Massive spin-one particles have been described by means of an antisymmetric second-rank tensor field...