TY - JOUR
T1 - Evidence for the kinematic Sunyaev-Zel'dovich effect with the Atacama Cosmology Telescope and velocity reconstruction from the Baryon Oscillation Spectroscopic Survey
AU - ACTPol Collaboration
AU - Schaan, Emmanuel
AU - Ferraro, Simone
AU - Vargas-Magaña, Mariana
AU - Smith, Kendrick M.
AU - Ho, Shirley
AU - Aiola, Simone
AU - Battaglia, Nicholas
AU - Bond, J. Richard
AU - De Bernardis, Francesco
AU - Calabrese, Erminia
AU - Cho, Hsiao Mei
AU - Devlin, Mark J.
AU - Dunkley, Joanna
AU - Gallardo, Patricio A.
AU - Hasselfield, Matthew
AU - Henderson, Shawn
AU - Hill, J. Colin
AU - Hincks, Adam D.
AU - Hlozek, Renée
AU - Hubmayr, Johannes
AU - Hughes, John P.
AU - Irwin, Kent D.
AU - Koopman, Brian
AU - Kosowsky, Arthur
AU - Li, Dale
AU - Louis, Thibaut
AU - Lungu, Marius
AU - Madhavacheril, Mathew
AU - Maurin, Loïc
AU - McMahon, Jeffrey John
AU - Moodley, Kavilan
AU - Naess, Sigurd
AU - Nati, Federico
AU - Newburgh, Laura
AU - Niemack, Michael D.
AU - Page, Lyman A.
AU - Pappas, Christine G.
AU - Partridge, Bruce
AU - Schmitt, Benjamin L.
AU - Sehgal, Neelima
AU - Sherwin, Blake D.
AU - Sievers, Jonathan L.
AU - Spergel, David N.
AU - Staggs, Suzanne T.
AU - Van Engelen, Alexander
AU - Wollack, Edward J.
N1 - Funding Information:
We thank Marcelo Alvarez, Neal Dalal, Tommaso Giannantonio, Oliver Hahn, Andrey Kravtsov, Guilhem Lavaux, Hironao Miyatake, Hyunbae Park, Hiranya Peiris, Ue-Li Pen, Bjoern Soergel, Naonori Sugiyama and Simon White for very useful discussions. This work was supported by the U.S. National Science Foundation (NSF) through Grants No. AST-0408698 and No. AST-0965625 for the ACT project, as well as Grants No. PHY-0855887 and No. PHY-1214379. Funding was also provided by Princeton University, the University of Pennsylvania, Cornell University and a Canada Foundation for Innovation (CFI) award to the University of British Columbia. ACT operates in the Parque Astronomico Atacama in northern Chile under the auspices of the Comision Nacional de Investigacion Cientifica y Tecnologica de Chile (CONICYT). Computations were performed on the GPC supercomputer at the SciNet HPC Consortium. SciNet is funded by the CFI under the auspices of Compute Canada, the Government of Ontario, the Ontario Research Fund-Research Excellence; and the University of Toronto. Colleagues at RadioSky provide logistical support and keep operations in Chile running smoothly. We also thank the Mishrahi Fund and the Wilkinson Fund for their generous support of the project. E.S., S.F. and D.N.S. are supported by NSF Grant No. AST1311756 and NASA Grant No. NNX12AG72G. Research at Perimeter Institute is supported by the Government of Canada through Industry Canada and by the Province of Ontario through the Ministry of Research and Innovation. K.M.S. was supported by an NSERC Discovery grant. S.H. is supported in part by DOE-ASC Award No. DOE-DESC0011114, NASA Grant No. 12-EUCLID11-0004, and NSF Grants No. AST1517593 and No. AST1412966. N.B. acknowledges support from the Lyman Spitzer fellowship. M.N. and F.D.B. acknowledge support from NSF Grants No. AST-1454881 and No. AST-1517049. The development of multichroic detectors and lenses was supported by NASA Grants No. NNX13AE56G and No. NNX14AB58G. C.M. acknowledges support from NASA Grant No. NNX12AM32H. Funding from ERC Grant No. 259505 supports S.N., J.D., E.C., and T.L. H.T. is supported by NASA Grant No. ATP NNX14AB57G, DOE Award No. DE-SC0011114, and NSF Grant No. AST-1312991. B.S. and B.K. are funded by NASA Space Technology research fellowships. R.D. received funding from the CONICYT Grants No. QUIMAL-120001 and No. FONDECYT-1141113. This research used resources of the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Award No. DE-AC02-05CH11231. Funding for SDSS-III has been provided by the Alfred P. Sloan Foundation, the Participating Institutions, the National Science Foundation, and the U.S. Department of Energy Office of Science. The SDSS-III web site is . SDSS-III is managed by the Astrophysical Research Consortium for the Participating Institutions of the SDSS-III Collaboration including the University of Arizona, the Brazilian Participation Group, Brookhaven National Laboratory, Carnegie Mellon University, University of Florida, the French Participation Group, the German Participation Group, Harvard University, the Instituto de Astrofisica de Canarias, the Michigan State/Notre Dame/JINA Participation Group, Johns Hopkins University, Lawrence Berkeley National Laboratory, Max Planck Institute for Astrophysics, Max Planck Institute for Extraterrestrial Physics, New Mexico State University, New York University, Ohio State University, Pennsylvania State University, University of Portsmouth, Princeton University, the Spanish Participation Group, University of Tokyo, University of Utah, Vanderbilt University, University of Virginia, University of Washington, and Yale University.
Publisher Copyright:
© 2016 American Physical Society.
PY - 2016/4/11
Y1 - 2016/4/11
N2 - We use microwave temperature maps from two seasons of data from the Atacama Cosmology Telescope at 146 GHz, together with the "Constant Mass" CMASS galaxy sample from the Baryon Oscillation Spectroscopic Survey to measure the kinematic Sunyaev-Zel'dovich (kSZ) effect over the redshift range z=0.4-0.7. We use galaxy positions and the continuity equation to obtain a reconstruction of the line-of-sight velocity field. We stack the microwave temperature at the location of each halo, weighted by the corresponding reconstructed velocity. We vary the size of the aperture photometry filter used, thus probing the free electron profile of these halos from within the virial radius out to three virial radii, on the scales relevant for investigating the missing baryons problem. The resulting best fit kSZ model is preferred over the no-kSZ hypothesis at 3.3 and 2.9σ for two independent velocity reconstruction methods, using 25,537 galaxies over 660 square degrees. The data suggest that the baryon profile is shallower than the dark matter in the inner regions of the halos probed here, potentially due to energy injection from active galactic nucleus or supernovae. Thus, by constraining the gas profile on a wide range of scales, this technique will be useful for understanding the role of feedback in galaxy groups and clusters. The effect of foregrounds that are uncorrelated with the galaxy velocities is expected to be well below our signal, and residual thermal Sunyaev-Zel'dovich contamination is controlled by masking the most massive clusters. Finally, we discuss the systematics involved in converting our measurement of the kSZ amplitude into the mean free electron fraction of the halos in our sample.
AB - We use microwave temperature maps from two seasons of data from the Atacama Cosmology Telescope at 146 GHz, together with the "Constant Mass" CMASS galaxy sample from the Baryon Oscillation Spectroscopic Survey to measure the kinematic Sunyaev-Zel'dovich (kSZ) effect over the redshift range z=0.4-0.7. We use galaxy positions and the continuity equation to obtain a reconstruction of the line-of-sight velocity field. We stack the microwave temperature at the location of each halo, weighted by the corresponding reconstructed velocity. We vary the size of the aperture photometry filter used, thus probing the free electron profile of these halos from within the virial radius out to three virial radii, on the scales relevant for investigating the missing baryons problem. The resulting best fit kSZ model is preferred over the no-kSZ hypothesis at 3.3 and 2.9σ for two independent velocity reconstruction methods, using 25,537 galaxies over 660 square degrees. The data suggest that the baryon profile is shallower than the dark matter in the inner regions of the halos probed here, potentially due to energy injection from active galactic nucleus or supernovae. Thus, by constraining the gas profile on a wide range of scales, this technique will be useful for understanding the role of feedback in galaxy groups and clusters. The effect of foregrounds that are uncorrelated with the galaxy velocities is expected to be well below our signal, and residual thermal Sunyaev-Zel'dovich contamination is controlled by masking the most massive clusters. Finally, we discuss the systematics involved in converting our measurement of the kSZ amplitude into the mean free electron fraction of the halos in our sample.
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U2 - 10.1103/PhysRevD.93.082002
DO - 10.1103/PhysRevD.93.082002
M3 - Article
AN - SCOPUS:84963682853
SN - 2470-0010
VL - 93
JO - Physical Review D
JF - Physical Review D
IS - 8
M1 - 082002
ER -