{"title":"宇宙学中重建光速的随机方法","authors":"Cheng-Yu Zhang, Wei Hong, Yu-Chen Wang, Tong-Jie Zhang","doi":"arxiv-2409.03248","DOIUrl":null,"url":null,"abstract":"The Varying Speed of Light (VSL) model describes how the speed of light in a\nvacuum changes with cosmological redshift. Despite numerous models, there is\nlittle observational evidence for this variation. While the speed of light can\nbe accurately measured by physical means, cosmological methods are rarely used.\nPrevious studies quantified the speed of light at specific redshifts using\nGaussian processes and reconstructed the redshift-dependent function $c(z)$. It\nis crucial to quantify the speed of light across varying redshifts. We use the\nlatest data on angular diameter distances $D_A(z)$ and Hubble parameters $H(z)$\nfrom baryon acoustic oscillation (BAO) and cosmic chronometer measurements in\nthe redshift interval $z\\in[0.07,1.965]$. The speed of light $c(z)$ is\ndetermined using Gaussian and deep Gaussian processes to reconstruct $H(z)$,\n$D_A(z)$, and $D^{\\prime}_A(z)$. Furthermore, we conduct comparisons across\nthree distinct models, encompassing two renowned VSL models. We get the result\nof the parameters constraints in the models (1) for the ``$c$-c\" model,\n$c_0=29492.6 \\pm^{6.2}_{5.3} \\mathrm{~km} \\mathrm{~s}^{-1}$. (2) For the\n``$c$-cl\" model, $c_0=29665.5 \\pm^{11.2}_{11.4}\\mathrm{~km} \\mathrm{~s}^{-1}$\nand $n=0.05535 \\pm^{0.00008}_{0.00007}$. (3) For the ``$c$-CPL\" model,\n$c_0=29555.7 \\pm^{13.3}_{13.2} \\mathrm{~km} \\mathrm{~s}^{-1}$ and $n=-0.0607\n\\pm 0.0001$. Based on our findings, it may be inferred that Barrow's classical\nVSL model is not a suitable fit for our data. In contrast, the widely\nrecognized Chevallier-Polarski-Linder (CPL) VSL model, under some\ncircumstances, as well as the universal ``c is constant\" model, demonstrate a\nsatisfactory ability to account for our findings.","PeriodicalId":501207,"journal":{"name":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","volume":"396 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Stochastic Approach to Reconstructing the Speed of Light in Cosmology\",\"authors\":\"Cheng-Yu Zhang, Wei Hong, Yu-Chen Wang, Tong-Jie Zhang\",\"doi\":\"arxiv-2409.03248\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The Varying Speed of Light (VSL) model describes how the speed of light in a\\nvacuum changes with cosmological redshift. Despite numerous models, there is\\nlittle observational evidence for this variation. While the speed of light can\\nbe accurately measured by physical means, cosmological methods are rarely used.\\nPrevious studies quantified the speed of light at specific redshifts using\\nGaussian processes and reconstructed the redshift-dependent function $c(z)$. It\\nis crucial to quantify the speed of light across varying redshifts. We use the\\nlatest data on angular diameter distances $D_A(z)$ and Hubble parameters $H(z)$\\nfrom baryon acoustic oscillation (BAO) and cosmic chronometer measurements in\\nthe redshift interval $z\\\\in[0.07,1.965]$. The speed of light $c(z)$ is\\ndetermined using Gaussian and deep Gaussian processes to reconstruct $H(z)$,\\n$D_A(z)$, and $D^{\\\\prime}_A(z)$. Furthermore, we conduct comparisons across\\nthree distinct models, encompassing two renowned VSL models. We get the result\\nof the parameters constraints in the models (1) for the ``$c$-c\\\" model,\\n$c_0=29492.6 \\\\pm^{6.2}_{5.3} \\\\mathrm{~km} \\\\mathrm{~s}^{-1}$. (2) For the\\n``$c$-cl\\\" model, $c_0=29665.5 \\\\pm^{11.2}_{11.4}\\\\mathrm{~km} \\\\mathrm{~s}^{-1}$\\nand $n=0.05535 \\\\pm^{0.00008}_{0.00007}$. (3) For the ``$c$-CPL\\\" model,\\n$c_0=29555.7 \\\\pm^{13.3}_{13.2} \\\\mathrm{~km} \\\\mathrm{~s}^{-1}$ and $n=-0.0607\\n\\\\pm 0.0001$. Based on our findings, it may be inferred that Barrow's classical\\nVSL model is not a suitable fit for our data. In contrast, the widely\\nrecognized Chevallier-Polarski-Linder (CPL) VSL model, under some\\ncircumstances, as well as the universal ``c is constant\\\" model, demonstrate a\\nsatisfactory ability to account for our findings.\",\"PeriodicalId\":501207,\"journal\":{\"name\":\"arXiv - PHYS - Cosmology and Nongalactic Astrophysics\",\"volume\":\"396 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-05\",\"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-2409.03248\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Cosmology and Nongalactic Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03248","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A Stochastic Approach to Reconstructing the Speed of Light in Cosmology
The Varying Speed of Light (VSL) model describes how the speed of light in a
vacuum changes with cosmological redshift. Despite numerous models, there is
little observational evidence for this variation. While the speed of light can
be accurately measured by physical means, cosmological methods are rarely used.
Previous studies quantified the speed of light at specific redshifts using
Gaussian processes and reconstructed the redshift-dependent function $c(z)$. It
is crucial to quantify the speed of light across varying redshifts. We use the
latest data on angular diameter distances $D_A(z)$ and Hubble parameters $H(z)$
from baryon acoustic oscillation (BAO) and cosmic chronometer measurements in
the redshift interval $z\in[0.07,1.965]$. The speed of light $c(z)$ is
determined using Gaussian and deep Gaussian processes to reconstruct $H(z)$,
$D_A(z)$, and $D^{\prime}_A(z)$. Furthermore, we conduct comparisons across
three distinct models, encompassing two renowned VSL models. We get the result
of the parameters constraints in the models (1) for the ``$c$-c" model,
$c_0=29492.6 \pm^{6.2}_{5.3} \mathrm{~km} \mathrm{~s}^{-1}$. (2) For the
``$c$-cl" model, $c_0=29665.5 \pm^{11.2}_{11.4}\mathrm{~km} \mathrm{~s}^{-1}$
and $n=0.05535 \pm^{0.00008}_{0.00007}$. (3) For the ``$c$-CPL" model,
$c_0=29555.7 \pm^{13.3}_{13.2} \mathrm{~km} \mathrm{~s}^{-1}$ and $n=-0.0607
\pm 0.0001$. Based on our findings, it may be inferred that Barrow's classical
VSL model is not a suitable fit for our data. In contrast, the widely
recognized Chevallier-Polarski-Linder (CPL) VSL model, under some
circumstances, as well as the universal ``c is constant" model, demonstrate a
satisfactory ability to account for our findings.