scholarly journals Erratum to: Axion stars in the infrared limit

2016 ◽  
Vol 2016 (11) ◽  
Author(s):  
Joshua Eby ◽  
Peter Suranyi ◽  
Cenalo Vaz ◽  
L. C. R. Wijewardhana
Keyword(s):  
2014 ◽  
Vol 23 (08) ◽  
pp. 1450068 ◽  
Author(s):  
O. Goldoni ◽  
M. F. A. da Silva ◽  
G. Pinheiro ◽  
R. Chan

In this paper, we have studied nonstationary radiative spherically symmetric spacetime, in general covariant theory (U(1) extension) of Hořava–Lifshitz (HL) gravity without the projectability condition and in the infrared (IR) limit. The Newtonian prepotential φ was assumed null. We have shown that there is not the analogue of the Vaidya's solution in the Hořava–Lifshitz Theory (HLT), as we know in the General Relativity Theory (GRT). Therefore, we conclude that the gauge field A should interact with the null radiation field of the Vaidya's spacetime in the HLT.


2012 ◽  
Vol 86 (8) ◽  
Author(s):  
Mohammed Mia ◽  
Fang Chen ◽  
Keshav Dasgupta ◽  
Paul Franche ◽  
Sachindeo Vaidya

1994 ◽  
Vol 336 (3-4) ◽  
pp. 381-387 ◽  
Author(s):  
Antti J Niemi ◽  
V.V Sreedhar
Keyword(s):  

1977 ◽  
Vol 16 (8) ◽  
pp. 2424-2429 ◽  
Author(s):  
N. Caderni ◽  
V. De Cosmo ◽  
R. Fabbri ◽  
B. Melchiorri ◽  
F. Melchiorri ◽  
...  

2001 ◽  
Vol 16 (11) ◽  
pp. 2125-2130
Author(s):  
M. SIMIONATO

I study a class of Wilsonian formulations of non-Abelian gauge theories in algebraic noncovariant gauges where the Wilsonian infrared cutoff Λ is inserted as a mass term for the propagating fields. In this way the Ward-Takahashi identities are preserved to all scales. Nevertheless the BRS-invariance in broken and the theory is gauge-dependent and unphysical at Λ≠ 0. Then I discuss the infrared limit Λ→0. I show that the singularities of the axial gauge choice are avoided in planar gauge and in light-cone gauge. Finally the rectangular Wilson loop of size 2L×2T is evaluated at lowest order in perturbation theory and a noncommutativity between the limits Λ→0 and T→∞ is pointed out.


2008 ◽  
Vol 23 (27n30) ◽  
pp. 2352-2355 ◽  
Author(s):  
Y. NAKAGAWA ◽  
A. NAKAMURA ◽  
T. SAITO ◽  
H. TOKI

We investigate the Gribov-Zwanziger scenario in Coulomb gauge QCD using a SU(3) quenched lattice gauge simulation. The ghost propagator diverges in the infrared limit stronger than the free ghost propagator, and the ghost degree of freedom plays a central role in the confinement mechanism in the Coulomb gauge. The infrared divergent ghost dressing function results in the confining color-Coulomb instantaneous interaction. The equal-time transverse gluon propagator is suppressed in the infrared region. Therefore, in the Coulomb gauge, the instantaneous interaction mediated by time-like gluons is responsible for the confining force, and the would-be physical gluons are confined in hadrons.


Author(s):  
Ikfal Hanafi ◽  
Thamrin Thamrin
Keyword(s):  

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