Gauge fixing for gravity-coupled theories and the super-Higgs effect beyond the unitary gauge

1986 ◽  
Vol 273 (2) ◽  
pp. 366-386 ◽  
Author(s):  
Laurent Baulieu ◽  
Antoine Georges ◽  
Stephane Ouvry
1992 ◽  
Vol 07 (31) ◽  
pp. 7775-7786
Author(s):  
L. ROZANSKY

Green’s function of Schrödinger equation is represented as a time-reparametrization invariant path integral. Unitary gauge fixing enables us to get the WKB preexponential factor without calculating determinants of operators containing derivatives.


2014 ◽  
Vol 29 (29) ◽  
pp. 1450170 ◽  
Author(s):  
Bum-Hoon Lee ◽  
Shahin Mamedov ◽  
Chanyong Park

Using the AdS/CFT correspondence, we investigate a nucleon mass splitting and pion–nucleon coupling in the isospin medium. We find that there exists a nucleon mass splitting which is exactly given by the half of the meson mass splitting because nucleon has the half isospin charge of the charged mesons. In addition, we also investigate the pion–nucleon and four pion interactions which requires the modification of the known Abelian-type unitary gauge fixing because of the non-Abelian structure of the isospin medium. After finding the non-Abelian unitary gauge fixing, we find that in the isospin medium the couplings only for π0 π0 π+ π- and π0 π0π0 π0 of four pion interactions shift, while there is no pion–nucleon coupling splitting in spite of the nucleon's and meson's mass splittings.


1993 ◽  
Vol 08 (35) ◽  
pp. 3317-3323 ◽  
Author(s):  
WON-TAE KIM ◽  
HYEONJOON SHIN ◽  
JAE KWAN KIM

The statistics-changing phase transition in terms of the spontaneous symmetry breaking is examined by studying anomalous angular momenta in symmetric and broken phases. We show that the zero-momentum mode of charged degree of freedom cannot be eliminated through the unitary gauge fixing even though the excited modes can be done in any vacuum phase, and the statistics-changing phase transition is impossible in the Chern-Simons Higgs theory.


2020 ◽  
Vol 2020 (12) ◽  
Author(s):  
Andreas Ekstedt ◽  
Johan Löfgren

Abstract The electroweak phase transition broke the electroweak symmetry. Perturbative methods used to calculate observables related to this phase transition suffer from severe problems such as gauge dependence, infrared divergences, and a breakdown of perturbation theory. In this paper we develop robust perturbative tools for dealing with phase transitions. We argue that gauge and infrared problems are absent in a consistent power-counting. We calculate the finite temperature effective potential to two loops for general gauge-fixing parameters in a generic model. We demonstrate gauge invariance, and perform numerical calculations for the Standard Model in Fermi gauge.


1995 ◽  
Vol 456 (1-2) ◽  
pp. 442-472 ◽  
Author(s):  
Géza Fülöp ◽  
Robert Marnelius
Keyword(s):  

2012 ◽  
Vol 27 (13) ◽  
pp. 1250075 ◽  
Author(s):  
MIR FAIZAL

In this paper, we will study perturbative quantum gravity on supermanifolds with both noncommutativity and non-anticommutativity of spacetime coordinates. We shall first analyze the BRST and the anti-BRST symmetries of this theory. Then we will also analyze the effect of shifting all the fields of this theory in background field method. We will construct a Lagrangian density which apart from being invariant under the extended BRST transformations is also invariant under on-shell extended anti-BRST transformations. This will be done by using the Batalin–Vilkovisky (BV) formalism. Finally, we will show that the sum of the gauge-fixing term and the ghost term for this theory can be elegantly written down in superspace with a two Grassmann parameter.


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