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Effects of long-wavelength fluctuations in large galaxy surveys

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arxiv 1809.03637 v2 pith:SJYMS6W4 submitted 2018-09-10 astro-ph.CO

classification astro-ph.CO
keywords gpchvolumecomputationaleffectsbox-sizedarklargematter
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In order to capture as much information as possible large galaxy surveys have been increasing their volume and redshift depth. To face this challenge theory has responded by making cosmological simulations of huge computational volumes with equally increasing the number of dark matter particles and supercomputing resources. Thus, it is taken for granted that the ideal situation is when a single computational box encompasses the whole effective volume of the observational survey, e.g., ~50 Gpch^3 for the DESI and Euclid surveys. Here we study the effects of missing long-waves in a finite volume using several relevant statistics: the abundance of dark matter halos, the PDF, the correlation function and power spectrum, and covariance matrices. Finite volume effects can substantially modify the results if the computational volumes are less than ~(500Mpch)^3. However, the effects become extremely small and practically can be ignored when the box-size exceeds ~1Gpch^3. We find that the average power spectra of dark matter fluctuations show remarkable lack of dependence on the computational box-size with less than 0.1% differences between 1Gpch and 4Gpch boxes. No measurable differences are expected for the halo mass functions for these volumes. The covariance matrices are scaled trivially with volume, and small corrections due to super-sample modes can be added. We conclude that there is no need to make those extremely large simulations when a box-size of 1-1.5Gpch is sufficient to fulfil most of the survey science requirements.

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  1. Super sample covariance and the volume scaling of galaxy survey covariance matrices

    astro-ph.CO 2024-11 conditional novelty 5.0 of 10

    Covariance matrices from small-volume simulations can be rescaled to match large-volume ones at the 3% level using a new bin-centering correction, provided the large-scale power spectrum is known.

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