2021
DOI: 10.1093/mnras/stab473
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Measuring the tidal response of structure formation: anisotropic separate universe simulations using treepm

Abstract: We present anisotropic ‘separate universe’ simulations which modify the N-body code gadget4 in order to represent a large-scale tidal field through an anisotropic expansion factor. These simulations are used to measure the linear, quasi-linear and nonlinear response of the matter power spectrum to a spatially uniform trace-free tidal field up to wavenumber k = 7 h Mpc−1. Together with the response to a large-scale overdensity measured in previous work, this completely describes the nonlinear matter bispectrum … Show more

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Cited by 25 publications
(38 citation statements)
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“…[20] followed this approach using several realizations of gravity-only simulations with sizes ranging between L box = 1000Mpc/h and L box = 2400Mpc/h, but these simulation volumes are currently numerically prohibitive with galaxy formation models like IllustrisTNG. Methods based on separate universe simulations [9,25,[85][86][87][88][89][90][91][92] do not strictly require large simulation volumes, but estimates of b 1 and b 2 still involve re-running the simulations for cosmological parameters that mimic different values of the long-wavelength overdensity. The same is true for separate universe simulations with tidal fields [89][90][91][92], although these have not yet been performed with galaxy formation simulations.…”
Section: Discussionmentioning
confidence: 99%
“…[20] followed this approach using several realizations of gravity-only simulations with sizes ranging between L box = 1000Mpc/h and L box = 2400Mpc/h, but these simulation volumes are currently numerically prohibitive with galaxy formation models like IllustrisTNG. Methods based on separate universe simulations [9,25,[85][86][87][88][89][90][91][92] do not strictly require large simulation volumes, but estimates of b 1 and b 2 still involve re-running the simulations for cosmological parameters that mimic different values of the long-wavelength overdensity. The same is true for separate universe simulations with tidal fields [89][90][91][92], although these have not yet been performed with galaxy formation simulations.…”
Section: Discussionmentioning
confidence: 99%
“…and are solved alongside the N-body equations of motion (31) by computing the tidal tensor T. One caveat with the GDE approach is that the evolution of D xq is determined not by the force but by the tidal field-which contains one higher spatial derivative of the potential than the force-and therefore is significantly less regular than the force field (see the detailed discussion and analysis in Stu ¨cker et al (2021c) who have also studied the stream density evolution in virialised halos, based on a novel low-noise force calculation). This approach thus requires larger softening to achieve converged answers than a usual N-body simulation, and possibly cannot be shown to converge in the limit of infinite density caustics.…”
Section: Tracking Deformation In Phase Space-the Gde Approachmentioning
confidence: 99%
“…More realistically, a given volume will also be exposed to anisotropic deformation due to a large-scale tidal field. Schmidt et al (2018) (see also Stu ¨cker et al 2021c;Masaki et al 2020;Akitsu et al 2020) have demonstrated that such a global anisotropy can be accounted for by a modification of the force calculation in numerical simulations. These simulations have been used to study the role of largescale tidal fields in the abundance and shape of dark matter halos and the response of the anisotropic power spectrum, and will be very useful also for studies of coherent alignment effects of haloes and galaxies which are important to understand intrinsic alignments in weak gravitational lensing.…”
Section: Separate Universe Simulationsmentioning
confidence: 99%
“…where 𝐺 1 and 𝐺 𝐾 are so-called growth-only response functions, which can be measured very efficiently in the nonlinear regime of structure formation using separate universe simulations. In this paper, we use the measurements of 𝐺 1 from Wagner et al (2015) and the measurements of 𝐺 𝐾 from Schmidt et al (2018) (see also Stücker et al (2021)); the time and scale-dependence of the resulting 𝑅 1 (𝑘, 𝜏), 𝑅 𝐾 (𝑘, 𝜏) functions can be seen alongside one another in Fig. 1 of Barreira et al 2018.…”
Section: Response Approach To the Squeezed Matter Bispectrummentioning
confidence: 99%