scholarly journals The light-front gauge-invariant energy-momentum tensor

2015 ◽  
Vol 2015 (8) ◽  
Author(s):  
Cédric Lorcé
1986 ◽  
Vol 33 (4) ◽  
pp. 1162-1165 ◽  
Author(s):  
Hans Georg Embacher ◽  
Gebhard Grübl ◽  
Rainer Patek

2000 ◽  
Vol 15 (32) ◽  
pp. 1991-2005 ◽  
Author(s):  
A. B. PESTOV ◽  
BIJAN SAHA

The gauge symmetry inherent in the concept of manifold has been discussed. Within the scope of this symmetry the linear connection or displacement field can be considered as a natural gauge field on the manifold. The gauge-invariant equations for the displacement field have been derived. It has been shown that the energy–momentum tensor of this field conserves and hence the displacement field can be treated as one that transports energy and gravitates. To show the existence of the solutions of the field equations, we have derived the general form of the displacement field in Minkowski space–time which is invariant under rotation and space and time inversion. With this ansatz we found spherically-symmetric solutions of the equations in question.


Author(s):  
T. S. Chang

The relativistic field theories of elementary particles are extended to cases where the field equations are derived from Lagrangians containing all derivatives of the field quantities. Expressions for the current, the energy-momentum tensor, the angular-momentum tensor, and the symmetrized energy-momentum tensor are given. When the field interacts with an electromagnetic field, we introduce a subtraction procedure, by which all the above expressions are made gauge-invariant. The Hamiltonian formulation of the equations of motion in a gauge-invariant form is also given.After considering the Lagrangian L as a scalar in a general relativity transformation and thus a function of gμν and their derivatives, the functional derivative ofwith respect to gμν (x) at a point where the space time is flat is worked out. It is shown that this differs from the symmetrized energy-momentum tensor given in the above sections by a term which vanishes when certain operators Sij are antisymmetrical or when the Lagrangian contains the first derivatives of the field quantities only and whose divergence to either μ or ν vanishes.


2021 ◽  
Vol 103 (9) ◽  
Author(s):  
M. Costa ◽  
I. Karpasitis ◽  
T. Pafitis ◽  
G. Panagopoulos ◽  
H. Panagopoulos ◽  
...  

Author(s):  
Michele Maggiore

Decomposition of the perturbations over FRW into scalar, vector and tensor perturbations. Physical and unphysical degrees of freedom. Gauge-invariant metric perturbations, Bardeen variables. Gauge-invariant perturbations of the energy-momentum tensor


2004 ◽  
Vol 19 (32) ◽  
pp. 5615-5624 ◽  
Author(s):  
J. M. GRIMSTRUP ◽  
B. KLOIBÖCK ◽  
L. POPP ◽  
M. SCHWEDA ◽  
M. WICKENHAUSER ◽  
...  

We discuss the different possibilities of constructing the various energy–momentum tensors for noncommutative gauge field models. We use Jackiw's method in order to get symmetric and gauge invariant stress tensors — at least for commutative gauge field theories. The noncommutative counterparts are analyzed with the same methods. The issues for the noncommutative cases are worked out.


2002 ◽  
Vol 11 (08) ◽  
pp. 1209-1225 ◽  
Author(s):  
MASSIMO GIOVANNINI

A gauge invariant theory of gravitational fluctuations of brane-world model is presented. Without resorting to any specific gauge choice, a general method is presented in order to disentangle the fluctuations of the energy–momentum tensor of the brane from the fluctuations of the metric. The employed procedure is gauge-invariant at every step. As an application of the formalism we address the localization of metric fluctuations on scalar branes breaking spontaneously five-dimensional Poincaré invariance is addressed. Assuming that the four-dimensional Planck mass is finite and that the geometry is regular, it is demonstrated that the vector and scalar fluctuations of the metric are not localized on the brane.


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