CWRU PAT Coffee Agenda

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

+2 Born-Infeld Gravity with a Massless Graviton in Four Dimensions

jtd55 +2

+2 Did LIGO detect dark matter?.

kxp265 +1 cad96 +1

+1 Constraints on the Early and Late Integrated Sachs-Wolfe effects from Planck 2015 Cosmic Microwave Background Anisotropies angular power spectra. - [UPDATED]

cjc5 +1

+1 Photon Mass Limits from Fast Radio Bursts.

jtd55 +1

+1 A Repeating Fast Radio Burst.

jtd55 +1

+1 Localization and broadband follow-up of the gravitational-wave transient GW150914.

jtd55 +1

+1 Did GW150914 produce a rotating gravastar?.

jtd55 +1

+1 Strong field gravitational lensing by a charged Galileon black hole.

jtd55 +1

+1 Constraints on modified gravity from Planck 2015: when the health of your theory makes the difference.

jtd55 +1

+1 Black Holes and Abelian Symmetry Breaking.

qxc76 +1

+1 Topological Induced Gravity.

qxc76 +1

+1 Gravitational Wave Memory In dS$_{4+2n}$ and 4D Cosmology.

kxp265 +1

0 Inflation in pure gravity with only massless spin-2 fields.

kxp265 -1 oxg34 +1

Showing votes from 2016-03-01 11:30 to 2016-03-04 12:30 | Next meeting is Tuesday May 5th, 10:30 am.

users

  • No papers in this section today!

astro-ph.CO

  • Constraints on the Early and Late Integrated Sachs-Wolfe effects from Planck 2015 Cosmic Microwave Background Anisotropies angular power spectra.- [PDF] - [Article] - [UPDATED]

    Giovanni Cabass, Martina Gerbino, Elena Giusarma, Alessandro Melchiorri, Luca Pagano, Laura Salvati
     

    The Integrated Sachs-Wolfe (ISW) effect predicts additional anisotropies in the Cosmic Microwave Background due to time variation of the gravitational potential when the expansion of the universe is not matter dominated. The ISW effect is therefore expected in the early universe, due to the presence of relativistic particles at recombination, and in the late universe, when dark energy starts to dominate the expansion. Deviations from the standard picture can be parameterized by $A_{e\text{ISW}}$ and $A_{l\text{ISW}}$, which rescale the overall amplitude of the early and late ISW effects. Analyzing the most recent CMB temperature spectra from the Planck 2015 release, we detect the presence of the early ISW at high significance with $A_{e\mathrm{ISW}} = 1.06\pm0.04$ at 68% CL and an upper limit for the late ISW of $A_{l\mathrm{ISW}} < 1.1$ at 95% CL. The inclusion of the recent polarization data from the Planck experiment results in $A_{e\mathrm{ISW}} = 0.999\pm0.028$ at 68% CL, in better agreement with the value $A_{e\mathrm{ISW}} = 1$ of a standard cosmology. When considering the recent detections of the late ISW coming from correlations between CMB temperature anisotropies and weak lensing, a value of $A_{l\mathrm{ISW}}=0.85\pm0.21$ is predicted at 68% CL, showing a $4\sigma$ evidence. We discuss the stability of our result in the case of an extra relativistic energy component parametrized by the effective neutrino number $N_\mathrm{eff}$ and of a CMB lensing amplitude $A_\mathrm{L}$.

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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