{"title":"用帕代近似和最新的 Pantheon+ 样本测试宇宙各向异性","authors":"J.P. Hu, J. Hu, X. Jia, B. Gao, F.Y. Wang","doi":"10.1051/0004-6361/202450342","DOIUrl":null,"url":null,"abstract":"Cosmography can be used to constrain the kinematics of the Universe in a model-independent way. In this work, we attempt to combine the Pad$ e $ approximations with the latest Pantheon+ sample to test the cosmological principle. Based on the Pad$ e $ approximations, we first applied cosmographic constraints to different-order polynomials including third-order (Pad$ e $), fourth-order (Pad$ e $), and fifth-order (Pad$ e $) ones. The statistical analyses show that the Pad$ e $ polynomial has the best performance. Its best fits are $H_ $ = 72.53pm 0.28 km s$^ $ Mpc$^ $, $q_ $, and $j_ $. By further fixing $j_ $ = 1.00, it can be found that the Pad$ e $ polynomial can describe the Pantheon+ sample better than the regular Pad$ e $ polynomial and the usual cosmological models (including the Lambda CDM, $w$CDM, CPL, and $R_h$ = ct models). Based on the Pad$ e $ ($j_ $ = 1) polynomial and the hemisphere comparison method, we tested the cosmological principle and found the preferred directions of cosmic anisotropy, such as (l, b) = (304.6$^ circ circ $) and (311.1$^ circ circ $) for $q_ $ and $H_ $, respectively. These two directions are consistent with each other at a $1 confidence level, but the corresponding results of statistical isotropy analyses including isotropy and isotropy with real positions are quite different. The statistical significance of $ is stronger than that of $q_ $; that is, 4.75sigma and 4.39sigma for isotropy and isotropy with real positions, respectively. Reanalysis with fixed $q_ = -0.55$ (corresponds to $ m $ = 0.30) gives similar results. Overall, our model-independent results provide clear indications of a possible cosmic anisotropy, which must be taken seriously. Further testing is needed to better understand this signal.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"11 3","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Testing cosmic anisotropy with Padé approximations and the latest Pantheon+ sample\",\"authors\":\"J.P. Hu, J. Hu, X. Jia, B. Gao, F.Y. Wang\",\"doi\":\"10.1051/0004-6361/202450342\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Cosmography can be used to constrain the kinematics of the Universe in a model-independent way. In this work, we attempt to combine the Pad$ e $ approximations with the latest Pantheon+ sample to test the cosmological principle. Based on the Pad$ e $ approximations, we first applied cosmographic constraints to different-order polynomials including third-order (Pad$ e $), fourth-order (Pad$ e $), and fifth-order (Pad$ e $) ones. The statistical analyses show that the Pad$ e $ polynomial has the best performance. Its best fits are $H_ $ = 72.53pm 0.28 km s$^ $ Mpc$^ $, $q_ $, and $j_ $. By further fixing $j_ $ = 1.00, it can be found that the Pad$ e $ polynomial can describe the Pantheon+ sample better than the regular Pad$ e $ polynomial and the usual cosmological models (including the Lambda CDM, $w$CDM, CPL, and $R_h$ = ct models). Based on the Pad$ e $ ($j_ $ = 1) polynomial and the hemisphere comparison method, we tested the cosmological principle and found the preferred directions of cosmic anisotropy, such as (l, b) = (304.6$^ circ circ $) and (311.1$^ circ circ $) for $q_ $ and $H_ $, respectively. These two directions are consistent with each other at a $1 confidence level, but the corresponding results of statistical isotropy analyses including isotropy and isotropy with real positions are quite different. The statistical significance of $ is stronger than that of $q_ $; that is, 4.75sigma and 4.39sigma for isotropy and isotropy with real positions, respectively. Reanalysis with fixed $q_ = -0.55$ (corresponds to $ m $ = 0.30) gives similar results. Overall, our model-independent results provide clear indications of a possible cosmic anisotropy, which must be taken seriously. 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引用次数: 0
摘要
宇宙学可以用来以一种与模型无关的方式约束宇宙运动学。在这项工作中,我们尝试将Pad$ e $近似与最新的Pantheon+样本相结合,来检验宇宙学原理。在Pad$ e $近似的基础上,我们首先将宇宙学约束应用于不同阶的多项式,包括三阶(Pad$ e $)、四阶(Pad$ e $)和五阶(Pad$ e $)多项式。统计分析显示,Pad$ e $ 多项式的性能最好。通过进一步固定$j_ $ = 1.00,可以发现Pad$ e $多项式对Pantheon+样本的描述优于常规的Pad$ e $多项式和通常的宇宙学模型(包括Lambda CDM、$w$CDM、CPL和$R_h$ = ct模型)。基于Pad$ e $ ($j_ $ = 1)多项式和半球比较法,我们检验了宇宙学原理,发现了宇宙各向异性的优选方向,如(l, b) = (304.6$^ circ circ $)和(311.1$^ circ circ $)分别为$q_ $和$H_ $。这两个方向在 1 美元的置信水平下是一致的,但包括各向同性和实位各向同性在内的统计各向同性分析的相应结果却大相径庭。$ 的统计显著性强于 $q_ $;即各向同性和实位各向同性的统计显著性分别为 4.75sigma 和 4.39sigma。用固定的 $q_ = -0.55$(相当于 $ m $ = 0.30)重新分析也得到了类似的结果。总之,我们与模型无关的结果清楚地表明了可能存在的宇宙各向异性,必须认真对待。要更好地理解这一信号,还需要进一步的测试。
Testing cosmic anisotropy with Padé approximations and the latest Pantheon+ sample
Cosmography can be used to constrain the kinematics of the Universe in a model-independent way. In this work, we attempt to combine the Pad$ e $ approximations with the latest Pantheon+ sample to test the cosmological principle. Based on the Pad$ e $ approximations, we first applied cosmographic constraints to different-order polynomials including third-order (Pad$ e $), fourth-order (Pad$ e $), and fifth-order (Pad$ e $) ones. The statistical analyses show that the Pad$ e $ polynomial has the best performance. Its best fits are $H_ $ = 72.53pm 0.28 km s$^ $ Mpc$^ $, $q_ $, and $j_ $. By further fixing $j_ $ = 1.00, it can be found that the Pad$ e $ polynomial can describe the Pantheon+ sample better than the regular Pad$ e $ polynomial and the usual cosmological models (including the Lambda CDM, $w$CDM, CPL, and $R_h$ = ct models). Based on the Pad$ e $ ($j_ $ = 1) polynomial and the hemisphere comparison method, we tested the cosmological principle and found the preferred directions of cosmic anisotropy, such as (l, b) = (304.6$^ circ circ $) and (311.1$^ circ circ $) for $q_ $ and $H_ $, respectively. These two directions are consistent with each other at a $1 confidence level, but the corresponding results of statistical isotropy analyses including isotropy and isotropy with real positions are quite different. The statistical significance of $ is stronger than that of $q_ $; that is, 4.75sigma and 4.39sigma for isotropy and isotropy with real positions, respectively. Reanalysis with fixed $q_ = -0.55$ (corresponds to $ m $ = 0.30) gives similar results. Overall, our model-independent results provide clear indications of a possible cosmic anisotropy, which must be taken seriously. Further testing is needed to better understand this signal.