Abstract

Abstract We measure power spectrum response functions in the presence of baryonic physical processes using separate universe simulations with the IllustrisTNG galaxy formation model. The response functions describe how the small-scale power spectrum reacts to long-wavelength perturbations and they can be efficiently measured with the separate universe technique by absorbing the effects of the long modes into a modified cosmology. Specifically, we focus on the total first-order matter power spectrum response to an isotropic density fluctuation R1(k, z), which is fully determined by the logarithmic derivative of the non-linear matter power spectrum dlnPm(k, z)/dlnk and the growth-only response function G1(k, z). We find that G1(k, z) is not affected by the baryonic physical processes in the simulations at redshifts z < 3 and on all scales probed (k ≲ 15 h Mpc−1; i.e. length scales $\gtrsim 0.4\, {\rm Mpc}\,h^{-1}$). In practice, this implies that the power spectrum fully specifies the baryonic dependence of its response function. Assuming an idealized lensing survey set-up, we evaluate numerically the baryonic impact on the squeezed-lensing bispectrum and the lensing supersample power spectrum covariance, which are given in terms of responses. Our results show that these higher-order lensing statistics can display varying levels of sensitivity to baryonic effects compared to the power spectrum, with the squeezed bispectrum being the least sensitive. We also show that ignoring baryonic effects on lensing covariances slightly overestimates the error budget (and is therefore conservative from the point of view of parameter error bars) and likely has negligible impact on parameter biases in inference analyses.

Highlights

  • The large-scale distribution of matter in the Universe is one of the best tools to address some of the deepest open problems in fundamental physics

  • We take a number of steps forward in understanding the impact of baryonic effects on higher-order N-point correlation functions by using the response approach to perturbation theory developed by Barreira & Schmidt (2017a,b) as an extension of previous work done by Chiang et al (2014), Wagner et al (2015b), and Chiang et al (2015)

  • Where G1(k, t) is called the growth-only response function that describes effect (iii) above in isolation. This is the only term for which separate universe simulations are needed, with the remainder of the response function R1 being completely specified by the logarithmic derivative of the non-linear matter power spectrum dlnPm(k, t)/dlnk

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Summary

INTRODUCTION

Osato, Shirasaki & Yoshida (2015) investigated the impact of baryonic effects on weak-lensing peaks and Minkowski functionals, which are statistics sensitive to higher-order N-point functions (see Yang et al 2013 and Castro et al 2018 for a study of baryonic effects on the probability distribution function of weak-lensing maps) Studies such as these can provide interesting insights on the physics of non-linear structure formation and are crucial to fully exploit the constraining power of existing and future data sets. We take a number of steps forward in understanding the impact of baryonic effects on higher-order N-point correlation functions by using the response approach to perturbation theory developed by Barreira & Schmidt (2017a,b) as an extension of previous work done by Chiang et al (2014), Wagner et al (2015b), and Chiang et al (2015).

Power spectrum responses
Separate Universe formalism
Separate Universe simulations
RESPONSE MEASUREMENTS
Response of the total matter field
Response of individual mass components
The lensing convergence power spectrum
The lensing convergence squeezed bispectrum
The lensing covariance matrix
Baryonic effects on higher-order lensing statistics
Baryonic effects on parameter inference using weak-lensing data
Findings
SUMMARY AND CONCLUSIONS
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