{"title":"Accurate simulations of reionization using the reduced speed of light approximation","authors":"Christopher Cain","doi":"arxiv-2409.11467","DOIUrl":null,"url":null,"abstract":"The reduced speed of light approximation has been employed to speed up\nradiative transfer simulations of reionization by a factor of $\\gtrsim 5-10$.\nHowever, it has been shown to cause significant errors in the HI-ionizing\nbackground near reionization's end in simulations of representative\ncosmological volumes. This can bias inferences on the galaxy ionizing\nemissivity required to match observables, such as the Ly$\\alpha$ forest. In\nthis work, we show that using a reduced speed of light is, to a good\napproximation, equivalent to re-scaling the global ionizing emissivity in a\nredshift-dependent way. We derive this re-scaling and show that it can be used\nto ``correct'' the emissivity in reduced speed of light simulations. This\napproach of re-scaling the emissivity after the simulation has been run is\nuseful in contexts where the emissivity is a free parameter. We test our method\nby running full speed of light simulations using these re-scaled emissivities\nand comparing them with their reduced speed of light counterparts. We find that\nfor reduced speeds of light $\\tilde{c} \\geq 0.2$, the 21 cm power spectrum at\n$0.1 \\leq k /[h{\\rm Mpc}^{-1}] \\leq 0.2$ and key Ly$\\alpha$ forest observables\nagree to within $20\\%$ throughout reionization, and often better than $10\\%$.\nPosition-dependent time-delay effects cause inaccuracies in reionization's\nmorphology on large scales that produce errors up to a factor of $2$ for\n$\\tilde{c} \\leq 0.1$. Our method enables a factor of $5$ speedup of radiative\ntransfer simulations of reionization in situations where the emissivity can be\ntreated as a free parameter.","PeriodicalId":501207,"journal":{"name":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","volume":"37 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11467","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The reduced speed of light approximation has been employed to speed up
radiative transfer simulations of reionization by a factor of $\gtrsim 5-10$.
However, it has been shown to cause significant errors in the HI-ionizing
background near reionization's end in simulations of representative
cosmological volumes. This can bias inferences on the galaxy ionizing
emissivity required to match observables, such as the Ly$\alpha$ forest. In
this work, we show that using a reduced speed of light is, to a good
approximation, equivalent to re-scaling the global ionizing emissivity in a
redshift-dependent way. We derive this re-scaling and show that it can be used
to ``correct'' the emissivity in reduced speed of light simulations. This
approach of re-scaling the emissivity after the simulation has been run is
useful in contexts where the emissivity is a free parameter. We test our method
by running full speed of light simulations using these re-scaled emissivities
and comparing them with their reduced speed of light counterparts. We find that
for reduced speeds of light $\tilde{c} \geq 0.2$, the 21 cm power spectrum at
$0.1 \leq k /[h{\rm Mpc}^{-1}] \leq 0.2$ and key Ly$\alpha$ forest observables
agree to within $20\%$ throughout reionization, and often better than $10\%$.
Position-dependent time-delay effects cause inaccuracies in reionization's
morphology on large scales that produce errors up to a factor of $2$ for
$\tilde{c} \leq 0.1$. Our method enables a factor of $5$ speedup of radiative
transfer simulations of reionization in situations where the emissivity can be
treated as a free parameter.