A Measurement of the Cosmic Microwave Background Gravitational Lensing Potential and its Power Spectrum from 500 Square Degrees of SPTpol Data

Weak gravitational lensing by large-scale structure in the universe causes deflections in the paths of cosmic microwave background (CMB) photons. This effect introduces statistical anisotropy in the observed CMB temperature and polarization fields. The signature of lensing can be used to reconstruct...

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Bibliographic Details
Main Author: Mocanu, Laura Monica
Format: Text
Language:English
Published: The University of Chicago 2019
Subjects:
Online Access:https://doi.org/10.6082/uchicago.1437
http://knowledge.uchicago.edu/record/1437
Description
Summary:Weak gravitational lensing by large-scale structure in the universe causes deflections in the paths of cosmic microwave background (CMB) photons. This effect introduces statistical anisotropy in the observed CMB temperature and polarization fields. The signature of lensing can be used to reconstruct the projected gravitational lensing potential with a quadratic estimator technique; this provides a measure of the integrated mass distribution out to the surface of last scattering, sourced primarily from redshifts between 0.1 and 5. The power spectrum of the lensing potential encodes information about the geometry of the universe and the growth of structure and can be used to place constraints on the sum of neutrino masses and dark energy. High signal-to-noise mass maps from CMB lensing are also powerful for cross-correlating with other tracers of large-scale structure and for delensing the CMB in search for primordial gravitational waves. This thesis describes a high signal-to-noise reconstruction of the CMB gravitational lensing potential and a measurement of its power spectrum using data from 500 \sqdeg of sky observed between 2012 and 2015 with the polarization-sensitive receiver SPTpol, installed on the South Pole Telescope (SPT). We find the ratio of the lensing spectrum to a theoretical $\Lambda$CDM model to be $A_{\rm \mv}=0.94 \pm 0.05 {\rm\, (stat.)} \pm 0.04 {\rm\, (sys.)}$. This measurement represents a $17.1 \sigma$ constraint on the lensing amplitude and a $41 \sigma$ detection of lensing effects.