@article{eb6192b7d2424a89b77eb830242055ad,
title = "First Constraints on the Epoch of Reionization Using the Non-Gaussianity of the Kinematic Sunyaev-Zel'dovich Effect from the South Pole Telescope and Herschel-SPIRE Observations",
abstract = "We report results from an analysis aimed at detecting the trispectrum of the kinematic Sunyaev-Zel'dovich (kSZ) effect by combining data from the South Pole Telescope (SPT) and Herschel-SPIRE experiments over a 100 deg2 field. The SPT observations combine data from the previous and current surveys, namely SPTpol and SPT-3G, to achieve depths of 4.5, 3, and 16 μK-arcmin in bands centered at 95, 150, and 220 GHz. For SPIRE, we include data from the 600 and 857 GHz bands. We reconstruct the velocity-induced large-scale correlation of the small-scale kSZ signal with a quadratic estimator that uses two cosmic microwave background (CMB) temperature maps, constructed by optimally combining data from all the frequency bands. We reject the null hypothesis of a zero trispectrum at 10.3σ level. However, the measured trispectrum contains contributions from both the kSZ and other undesired components, such as CMB lensing and astrophysical foregrounds, with kSZ being sub-dominant. We use the agora simulations to estimate the expected signal from CMB lensing and astrophysical foregrounds. After accounting for the contributions from CMB lensing and foreground signals, we do not detect an excess kSZ-only trispectrum and use this nondetection to set constraints on reionization. By applying a prior based on observations of the Gunn-Peterson trough, we obtain an upper limit on the duration of reionization of Δzre,50<4.5 (95\% confidence level). We find these constraints are fairly robust to foregrounds assumptions. This trispectrum measurement is independent of, but consistent with, Planck's optical depth measurement. This result is the first constraint on the epoch of reionization using the non-Gaussian nature of the kSZ signal.",
author = "\{(SPT-3G and SPTpol Collaboration)\} and S. Raghunathan and Ade, \{P. A.R.\} and Anderson, \{A. J.\} and B. Ansarinejad and M. Archipley and Austermann, \{J. E.\} and L. Balkenhol and Beall, \{J. A.\} and K. Benabed and Bender, \{A. N.\} and Benson, \{B. A.\} and F. Bianchini and Bleem, \{L. E.\} and J. Bock and Bouchet, \{F. R.\} and L. Bryant and E. Camphuis and Carlstrom, \{J. E.\} and Cecil, \{T. W.\} and Chang, \{C. L.\} and P. Chaubal and Chiang, \{H. C.\} and Chichura, \{P. M.\} and Chou, \{T. L.\} and R. Citron and A. Coerver and Crawford, \{T. M.\} and Crites, \{A. T.\} and A. Cukierman and C. Daley and Dibert, \{K. R.\} and Dobbs, \{M. A.\} and A. Doussot and D. Dutcher and W. Everett and C. Feng and Ferguson, \{K. R.\} and K. Fichman and A. Foster and S. Galli and J. Gallicchio and Gambrel, \{A. E.\} and Gardner, \{R. W.\} and F. Ge and George, \{E. M.\} and N. Goeckner-Wald and R. Gualtieri and Holder, \{G. P.\} and F. Menanteau and Vieira, \{J. D.\}",
note = "We thank all the three anonymous referees for their detailed and valuable feedback that has helped in shaping the manuscript better. S.R. acknowledges support by the Illinois Survey Science Fellowship from the Center for AstroPhysical Surveys at the National Center for Supercomputing Applications. This work made use of the following computing resources: Illinois Campus Cluster, a computing resource that is operated by the Illinois Campus Cluster Program (ICCP) in conjunction with the National Center for Supercomputing Applications (NCSA) and which is supported by funds from the University of Illinois at Urbana-Champaign; the computational and storage services associated with the Hoffman2 Shared Cluster provided by UCLA Institute for Digital Research and Education's Research Technology Group; and the computing resources provided on Crossover, a high-performance computing cluster operated by the Laboratory Computing Resource Center at Argonne National Laboratory. The South Pole Telescope program is supported by the National Science Foundation (NSF) through grant OPP-1852617. Partial support is also provided by the Kavli Institute of Cosmological Physics at the University of Chicago. Work at Argonne National Lab is supported by UChicago Argonne LLC, Operator of Argonne National Laboratory (Argonne). Argonne, a U.S. Department of Energy Office of Science Laboratory, is operated under Contract No. DE-AC02-06CH11357. We thank all the three anonymous referees for their detailed and valuable feedback that has helped in shaping the manuscript better. S.\textbackslash{}u2009R. acknowledges support by the Illinois Survey Science Fellowship from the Center for AstroPhysical Surveys at the National Center for Supercomputing Applications. This work made use of the following computing resources: Illinois Campus Cluster, a computing resource that is operated by the Illinois Campus Cluster Program (ICCP) in conjunction with the National Center for Supercomputing Applications (NCSA) and which is supported by funds from the University of Illinois at Urbana-Champaign; the computational and storage services associated with the Hoffman2 Shared Cluster provided by UCLA Institute for Digital Research and Education\textbackslash{}u2019s Research Technology Group; and the computing resources provided on Crossover, a high-performance computing cluster operated by the Laboratory Computing Resource Center at Argonne National Laboratory. The South Pole Telescope program is supported by the National Science Foundation (NSF) through grant OPP-1852617. Partial support is also provided by the Kavli Institute of Cosmological Physics at the University of Chicago. Work at Argonne National Lab is supported by UChicago Argonne LLC, Operator of Argonne National Laboratory (Argonne). Argonne, a U.S. Department of Energy Office of Science Laboratory, is operated under Contract No. DE-AC02-06CH11357.",
year = "2024",
month = sep,
day = "20",
doi = "10.1103/PhysRevLett.133.121004",
language = "English (US)",
volume = "133",
journal = "Physical review letters",
issn = "0031-9007",
publisher = "American Physical Society",
number = "12",
}