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Related papers: Bulk-to-bulk photon propagator in AdS

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We derive the scaling dimension of antisymmetric tensor operators in the boundary theory of the AdS/CFT correspondence using a functional integral representation of the boundary-to-boundary propagators of their dual fields in the bulk. We…

High Energy Physics - Theory · Physics 2013-09-10 Joshua W. Powell

To explore how rigid rotation affects the thermodynamic properties of free relativistic bosons, we employ the standard imaginary time formalism of thermal field theory to calculate the free propagator of complex scalar fields under…

High Energy Physics - Phenomenology · Physics 2024-11-20 E. Siri , N. Sadooghi

We construct a bulk spacetime from a boundary CFT, $O(N)$ free scalar model, at finite temperature using a smearing technique, called a conformal flow. The bulk metric is constructed as an information metric associated with the boundary…

High Energy Physics - Theory · Physics 2023-08-03 Sinya Aoki , János Balog , Kiyoharu Kawana , Kengo Shimada

The BSSN and standard gauge equations are written in covariant form with respect to spatial coordinate transformations. The BSSN variables are defined as tensors with no density weights. This allows us to evolve a given set of initial data…

General Relativity and Quantum Cosmology · Physics 2009-07-30 J. David Brown

We discuss the equivalence of the standard covariant expressions and light-front expressions of the three fundamental one loop Feynman diagrams of Quantum Electrodynamics viz. vertex correction, fermion self-energy and vacuum polarization…

High Energy Physics - Theory · Physics 2020-04-01 Deepesh Bhamre , Anuradha Misra , Vivek Kumar Singh

Gauge covariance properties of the scalar propagator in spinless/scalar quantum electrodynamics (SQED) are explored in the light of the corresponding Landau-Khalatnikov-Fradkin transformation (LKFT). These transformations are non…

In the framework of gauge invariant approach involving Stueckelberg and auxiliary fields, totally symmetric arbitrary spin anomalous conformal current and shadow field in flat space-time of dimension greater than or equal to four are…

High Energy Physics - Theory · Physics 2013-05-30 R. R. Metsaev

We study electromagnetically charged dilatonic black brane solutions in arbitrary dimensions with flat transverse spaces, that are asymptotically AdS. This class of solutions includes spacetimes which possess a bulk region where the metric…

High Energy Physics - Theory · Physics 2015-05-28 Per Berglund , Jishnu Bhattacharyya , David Mattingly

We show that the spectrum of the SYK model can be interpreted as that of a 3D scalar coupled to gravity. The scalar has a mass which is at the Breitenholer-Freedman bound of AdS$_2$, and subject to a delta function potential at the center…

High Energy Physics - Theory · Physics 2017-09-20 Sumit R. Das , Antal Jevicki , Kenta Suzuki

We investigate the large distance behavior of the electric and magnetic propagators of hot SU(2) gauge theory in different gauges using lattice simulations of the full 4d theory and the effective, dimensionally reduced 3d theory. Comparison…

High Energy Physics - Lattice · Physics 2009-09-25 A. Cucchieri , F. Karsch , P. Petreczky

Employing methods introduced by Schwinger in quantum electrodynamics, we compute the propagator for a non-Abelian gauge field in a plane wave background field. In the long distance limit a mass-like term for the gauge field is induced by…

High Energy Physics - Theory · Physics 2019-05-01 D. G. C. McKeon

We generalize a recent ``AdS S-matrix" formulation for interacting massive scalars on AdS spacetimes to the case of massive vector fields. This method relies on taking the infinite radius limit for scattering processes perturbatively, which…

High Energy Physics - Theory · Physics 2024-12-30 Nabamita Banerjee , Amogh Neelkanth Desai , Karan Fernandes , Arpita Mitra , Tabasum Rahnuma

The locality of bulk physics at distances below the AdS length is one of the remarkable aspects of AdS/CFT duality, and one of the least tested. It requires that the AdS radius be large compared to the Planck length and the string length.…

High Energy Physics - Theory · Physics 2009-11-13 Idse Heemskerk , Joao Penedones , Joseph Polchinski , James Sully

We derive the photon propagator in light-shell gauge, which was first introduced in the context of light-shell effective theory.

High Energy Physics - Phenomenology · Physics 2016-05-11 Howard Georgi , Greg Kestin , Aqil Sajjad

We analyze different BRST invariant solutions for the introduction of a mass term in Yang-Mills (YM) theories. First, we analyze the non-local composite gauge-invariant field $A^h_{\mu}(x)$, which can be localized by the Stueckelberg-like…

High Energy Physics - Theory · Physics 2023-10-11 D. M. van Egmond

We study gluon propagator in Landau gauge with lattice QCD, where we use an improved lattice action. The calculation of gluon propagator is performed on lattices with the lattice spacing from 0.40 fm to 0.24 fm and with the lattice volume…

High Energy Physics - Lattice · Physics 2009-10-31 J. P. Ma

We construct propagators in Euclidean AdS(d+1) space-time for massive p-forms and massive symmetric tensors.

High Energy Physics - Theory · Physics 2009-10-31 Asad Naqvi

Temporal offsets between Gamma-Ray Bursts (GRBs) and high-energy neutrinos provide a useful probe of propagation effects in extreme astrophysical environments. We investigate whether such offsets can be generated by photon propagation…

High Energy Physics - Phenomenology · Physics 2026-04-21 M. M. Chaichian , B. A. Couto e Silva , B. L. Sánchez-Vega

We comment on the recent attempt by M. Franz et al [1] to further justify their earlier calculation of the gauge-invariant electron propagator in the context of the QED_3 theory of the pseudogap phase in cuprates [2]. First, we use the…

Strongly Correlated Electrons · Physics 2007-05-23 D. V. Khveshchenko

Field quantization in 5D flat and warped space-times with Z$_2$-parity is comparatively examined. We carefully and closely derive 5D position/momentum(P/M) propagators. Their characteristic behaviours depend on the 4D (real world) momentum…

High Energy Physics - Theory · Physics 2008-11-26 S. Ichinose , A. Murayama
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