CWRU PAT Coffee Agenda

Tuesdays 10:30 - 11:30 | Fridays 11:30 - 12:30

+2 Weinberg Soft Theorems from Weinberg Adiabatic Modes.

oxg34 +1 aam80 +1

+1 Electromagnetic Counterparts to Black Hole Mergers Detected by LIGO.

sxk1031 +1

+1 Tests of general relativity with GW150914.

oxg34 +1 qxc76 +1 aam80 +1 jtd55 +1

+1 Local Conformal Symmetry: the Missing Symmetry Component for Space and Time

cad96 +1

+1 Practical Introduction to Clustering Data.

cjc5 +1

+1 Gravitational Wave Detection in the Introductory Lab.

jtd55 +1

+1 Fermi GBM Observations of LIGO Gravitational Wave event GW150914.

jtd55 +1 aam80 +1

+1 First Search for a Dark Matter Annual Modulation Signal with NaI(Tl) in the Southern Hemisphere by DM-Ice17.

cjc5 +1

+1 Singularities, horizons, firewalls, and local conformal symmetry.

qxc76 +1 bump  

+1 Testing Gravity with Gravitational Wave Source Counts.

oxg34 +1 aam80 +1 jtd55 +1 jbm120 +1

0 Inhomogeneous Anisotropic Cosmology.

bump   sxz353 +1 jbm120 +1

Showing votes from 2016-02-16 11:30 to 2016-02-19 12:30 | Next meeting is Friday May 8th, 11:30 am.

users

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astro-ph.CO

  • Weinberg Soft Theorems from Weinberg Adiabatic Modes.- [PDF] - [Article]

    Mehrdad Mirbabayi, Marko Simonović
     

    Soft theorems for the scattering of low energy photons and gravitons and cosmological consistency conditions on the squeezed-limit correlation functions are both understood to be consequences of invariance under large gauge transformations. We apply the same method used in cosmology -- based on the identification of an infinite set of "adiabatic modes" and the corresponding conserved currents -- to derive flat space soft theorems for electrodynamics and gravity. We discuss how the recent derivations based on the asymptotic symmetry groups (BMS) can be continued to a finite size sphere surrounding the scattering event, when the soft photon or graviton has a finite momentum. We give a finite distance derivation of the antipodal matching condition previously imposed between future and past null infinities, and explain why all but one radiative degrees of freedom decouple in the soft limit. In contrast to earlier works on BMS, we work with adiabatic modes which correspond to large gauge transformations that are $r$-dependent.

astro-ph.HE

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astro-ph.GA

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astro-ph.IM

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gr-qc

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hep-ph

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hep-th

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hep-ex

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quant-ph

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other

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