Fractional polarization of extragalactic sources in the 500 deg2 SPTpol survey
- Univ. of Melbourne, Parkville, VIC (Australia)
- Univ. of Melbourne, Parkville, VIC (Australia)
- Cardiff Univ., Cardiff (United Kingdom)
- Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States); Univ. of Chicago, IL (United States)
- Univ. of Illinois at Urbana-Champaign, IL (United States)
- National Inst. of Standards and Technology (NIST), Boulder, CO (United States)
- Univ. of California, Berkeley, CA (United States)
- Univ. of Chicago, IL (United States); Argonne National Lab. (ANL), Argonne, IL (United States)
- Univ. of KwaZulu-Natal, Durban (South Africa)
- Univ. of Chicago, IL (United States)
- California Inst. of Technology (CalTech), Pasadena, CA (United States)
- Univ. of Chicago, IL (United States); California Inst. of Technology (CalTech), Pasadena, CA (United States)
- Univ. of California, Berkeley, CA (United States); Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
- McGill Univ., Montreal, QC (Canada); Canadian Inst. for Advanced Research, Toronto, ON (Canada)
- Univ. of Colorado, Boulder, CO (United States)
- Univ. of Chicago, IL (United States); Harvey Mudd College, Claremont, CA (United States)
- Univ. of California, Berkeley, CA (United States); European Southern Observatory, Garching (Germany)
- McGill Univ., Montreal, QC (Canada)
- Univ. of Illinois at Urbana-Champaign, IL (United States); Canadian Inst. for Advanced Research, Toronto, ON (Canada)
- SLAC National Accelerator Lab., Menlo Park, CA (United States); Stanford Univ., CA (United States)
- Univ. of California, Davis, CA (United States)
- National Inst. of Standards and Technology (NIST), Boulder, CO (United States); SLAC National Accelerator Lab., Menlo Park, CA (United States)
- Univ. of Arizona, Tucson, AZ (United States)
- Univ. of Michigan, Ann Arbor, MI (United States)
- Ludwig Maximilian Univ., Munich (Germany); Max Planck Inst. for Extraterrestrial Physics, Garching (Germany)
- Univ. of Illinois at Urbana-Champaign, IL (United States); Univ. of Toronto, ON (Canada)
- Argonne National Lab. (ANL), Argonne, IL (United States)
- Univ. of Minnesota, Minneapolis, MN (United States)
- Case Western Reserve Univ., Cleveland, OH (United States)
- Univ. of Chicago, IL (United States); School of the Art Inst. of Chicago, Chicago, IL (United States)
- Univ. of California, Berkeley, CA (United States); Univ. of Chicago, IL (United States)
- McGill Univ., Montreal, QC (Canada); Three-Speed Logic, Inc., Vancouver, B.C. (Canada)
- Case Western Reserve Univ., Cleveland, OH (United States); California Inst. of Technology (CalTech), Pasadena, CA (United States). Jet Propulsion Lab. (JPL)
- Harvard-Smithsonian Center for Astrophysics, Cambridge, MA (United States)
- Stanford Univ., CA (United States)
- Univ. of Chicago, IL (United States); NASA Goddard Space Flight Center (GSFC), Greenbelt, MD (United States)
- Cardiff Univ. Cardiff (United Kingdom)
- Univ. of Toronto, ON (Canada)
- Univ. of Maryland Baltimore County (UMBC), Baltimore, MD (United States)
- Univ. of California, Los Angeles, CA (United States)
- Univ. of Chicago, IL (United States); California Inst. of Technology (CalTech), Pasadena, CA (United States). Jet Propulsion Lab. (JPL)
We study the polarization properties of extragalactic sources at 95 and 150 GHz in the SPTpol 500 deg2 survey. We estimate the polarized power by stacking maps at known source positions, and correct for noise bias by subtracting the mean polarized power at random positions in the maps. We show that the method is unbiased using a set of simulated maps with similar noise properties to the real SPTpol maps. We find a flux-weighted mean-squared polarization fraction $$\langle$$p2$$\rangle$$ = [8.9 ± 1.1] × 10-4 at 95 GHz and [6.9 ± 1.1] × 10-4 at 150 GHz for the full sample. This is consistent with the values obtained for a subsample of active galactic nuclei. For dusty sources, we find 95 percent upper limits of $$\langle$$p2$$\rangle$$95 < 16.9 × 10-3 and $$\langle$$p2$$\rangle$$150 < 2.6 × 10-3. We find no evidence that the polarization fraction depends on the source flux or observing frequency. The 1σ upper limit on measured mean-squared polarization fraction at 150 GHz implies that extragalactic foregrounds will be subdominant to the CMB E and B mode polarization power spectra out to at least ℓ ≲ 5700 (ℓ ≲ 4700) and ℓ ≲ 5300 (ℓ ≲ 3600), respectively, at 95 (150) GHz.
- Research Organization:
- Argonne National Laboratory (ANL), Argonne, IL (United States); Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States); SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States). National Energy Research Scientific Computing Center (NERSC)
- Sponsoring Organization:
- USDOE Office of Science (SC), High Energy Physics (HEP); National Science Foundation (NSF); Kavli Foundation; Gordon and Betty Moore Foundation; Australian Research Council (ARC)
- Contributing Organization:
- SPT
- Grant/Contract Number:
- AC02-07CH11359; AC02-05CH11231; AC02-76SF00515; PHY-1125897; GBMF 947; PLR-1248097
- OSTI ID:
- 1607541
- Alternate ID(s):
- OSTI ID: 1556975; OSTI ID: 1634014; OSTI ID: 1737589
- Report Number(s):
- arXiv:1907.02156; FERMILAB-PUB-19-386-AE; oai:inspirehep.net:1742660
- Journal Information:
- Monthly Notices of the Royal Astronomical Society, Vol. 490, Issue 4; ISSN 0035-8711
- Publisher:
- Royal Astronomical SocietyCopyright Statement
- Country of Publication:
- United States
- Language:
- English
Web of Science
Similar Records
Measurements of Sub-degree B-mode Polarization in the Cosmic Microwave Background from 100 Square Degrees of SPTpol Data
Measurements of the Temperature and E-mode Polarization of the CMB from 500 Square Degrees of SPTpol Data