scholarly journals Redshift and gauge choice

2020 ◽  
Vol 102 (12) ◽  
Author(s):  
Harald Skarke
Keyword(s):  
1997 ◽  
Vol 55 (11) ◽  
pp. 6730-6742 ◽  
Author(s):  
Kenneth Bernstein ◽  
Giuseppe Di Cecio ◽  
Richard W. Haymaker

2020 ◽  
Vol 2020 (12) ◽  
Author(s):  
ChunJun Cao ◽  
Xiao-Liang Qi ◽  
Brian Swingle ◽  
Eugene Tang

Abstract Using the tensor Radon transform and related numerical methods, we study how bulk geometries can be explicitly reconstructed from boundary entanglement entropies in the specific case of AdS3/CFT2. We find that, given the boundary entanglement entropies of a 2d CFT, this framework provides a quantitative measure that detects whether the bulk dual is geometric in the perturbative (near AdS) limit. In the case where a well-defined bulk geometry exists, we explicitly reconstruct the unique bulk metric tensor once a gauge choice is made. We then examine the emergent bulk geometries for static and dynamical scenarios in holography and in many-body systems. Apart from the physics results, our work demonstrates that numerical methods are feasible and effective in the study of bulk reconstruction in AdS/CFT.


2001 ◽  
Vol 33 (11) ◽  
pp. 2075-2079 ◽  
Author(s):  
A. Edery ◽  
A. A. Méthot ◽  
M. B. Paranjape

1992 ◽  
Vol 07 (17) ◽  
pp. 4053-4071 ◽  
Author(s):  
M. HUQ

We have considered a superparticle action consisting of an infinite tower of Siegel superparticle actions plus a term breaking all the twisted N=2 supersymmetries down to the required N=1 supersymmetry. With appropriate gauge choice we arrive at a quadratic gauge-fixed action, which naturally possesses an infinite sequence of twisted N=2 supersymmetries, but the BRST operator picks out the correct physical states for the Brink-Casalbuoni-Schwarz superparticle.


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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