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The Aemulus Project. II. Emulating the Halo Mass Function

Thomas McClintockDepartment of Physics, University of Arizona, Tuscon, AZ 85721, USAEduardo RozoDepartment of Physics, University of Arizona, Tuscon, AZ 85721, USAM. R. BeckerCivis Analytics, Chicago, IL 60607, USAJoseph DeRoseDepartment of Particle Physics and Astrophysics, SLAC National Accelerator Laboratory, Stanford, CA 94305, USAYao-Yuan MaoDepartment of Physics and Astronomy and the Pittsburgh Particle Physics, Astrophysics and Cosmology Center (PITT PACC), University of Pittsburgh, Pittsburgh, PA 15260, USASean McLaughlinDepartment of Particle Physics and Astrophysics, SLAC National Accelerator Laboratory, Stanford, CA 94305, USAJeremy L. TinkerCenter for Cosmology and Particle Physics, Department of Physics, New York University, 4 Washington Place, New York, NY 10003, USAR.H. WechslerDepartment of Particle Physics and Astrophysics, SLAC National Accelerator Laboratory, Stanford, CA 94305, USAZhongxu ZhaiCenter for Cosmology and Particle Physics, Department of Physics, New York University, 4 Washington Place, New York, NY 10003, USA
2019en
ABI

Abstract

Abstract Existing models for the dependence of the halo mass function on cosmological parameters will become a limiting source of systematic uncertainty for cluster cosmology in the near future. We present a halo mass function emulator and demonstrate improved accuracy relative to state-of-the-art analytic models. In this work, mass is defined using an overdensity criteria of 200 relative to the mean background density. Our emulator is constructed from the Aemulus simulations, a suite of 40 N -body simulations with snapshots from z = 3 to z = 0. These simulations cover the flat w CDM parameter space allowed by recent cosmic microwave background, baryon acoustic oscillation and SNe Ia results, varying the parameters w , Ω m , Ω b , σ 8 , N eff , n s , and H 0 . We validate our emulator using five realizations of seven different cosmologies, for a total of 35 test simulations. These test simulations were not used in constructing the emulator, and were run with fully independent initial conditions. We use our test simulations to characterize the modeling uncertainty of the emulator, and introduce a novel way of marginalizing over the associated systematic uncertainty. We confirm nonuniversality in our halo mass function emulator as a function of both cosmological parameters and redshift. Our emulator achieves better than 1% precision over much of the relevant parameter space, and we demonstrate that the systematic uncertainty in our emulator will remain a negligible source of error for cluster abundance studies through at least the LSST Year 1 data set.

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Cited by 40 references
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