通过超大质量黑洞的强引力透镜观测德能型暗物质晕的可观测特征以及来自 EHT 观测的约束条件

IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS
Amna Ali , Niyaz Uddin Molla , Sushant G. Ghosh , Ammuthavali Ramasamya , Ujjal Debnath
{"title":"通过超大质量黑洞的强引力透镜观测德能型暗物质晕的可观测特征以及来自 EHT 观测的约束条件","authors":"Amna Ali ,&nbsp;Niyaz Uddin Molla ,&nbsp;Sushant G. Ghosh ,&nbsp;Ammuthavali Ramasamya ,&nbsp;Ujjal Debnath","doi":"10.1016/j.dark.2025.101859","DOIUrl":null,"url":null,"abstract":"<div><div>We investigate strong gravitational lensing by black holes influenced by a Dehnen-type dark matter halo, characterized by an additional parameter, the core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, and the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, alongside the black hole mass <span><math><mi>M</mi></math></span>. Our findings reveal that, for a fixed value of the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, key parameters such as the unstable photon orbit radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, critical impact parameter <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, angular position <span><math><msub><mrow><mi>θ</mi></mrow><mrow><mi>∞</mi></mrow></msub></math></span>, and angular separation <span><math><mi>S</mi></math></span> increase with the growing value of the core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, while the relative magnitude <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi><mi>a</mi><mi>g</mi></mrow></msub></math></span> decreases. Conversely, for a fixed value of <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, parameters including the unstable photon orbit radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, critical impact parameter <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, strong deflection angle <span><math><msub><mrow><mi>α</mi></mrow><mrow><mi>D</mi></mrow></msub></math></span>, angular position <span><math><msub><mrow><mi>θ</mi></mrow><mrow><mi>∞</mi></mrow></msub></math></span>, angular separation <span><math><mi>S</mi></math></span>, relative magnitude <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi><mi>a</mi><mi>g</mi></mrow></msub></math></span>, and the outermost Einstein ring <span><math><msubsup><mrow><mi>θ</mi></mrow><mrow><mn>1</mn></mrow><mrow><mi>E</mi></mrow></msubsup></math></span> increase with the growing value of the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>. For Sgr A*, the outermost Einstein ring <span><math><msubsup><mrow><mi>θ</mi></mrow><mrow><mn>1</mn></mrow><mrow><mi>E</mi></mrow></msubsup></math></span> is larger than in the case of M87*. We have calculated the time delay between two relativistic images by utilizing various supermassive black holes in nearby galaxies. It is found that the time delay under the influence of a Dehnen-type dark matter halo (<span><math><mrow><mo>∼</mo><mn>33</mn><mo>.</mo><mn>7584</mn></mrow></math></span> min) is suppressed compared to the case of a Schwarzschild black hole (<span><math><mrow><mo>∼</mo><mn>38</mn><mo>.</mo><mn>7682</mn></mrow></math></span> min), as in the case of NGC 2778. Finally, we constrain the central density parameter of the dark matter halo, <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, for a fixed core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, using observational data from the Event Horizon Telescope collaboration for the supermassive black holes <span><math><mrow><mi>M</mi><mn>8</mn><msup><mrow><mn>7</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span> and <span><math><mrow><mi>S</mi><mi>g</mi><mi>r</mi><msup><mrow><mi>A</mi></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span>. The dark matter halo parameter <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span> is constrained to the range <span><math><mrow><mn>2</mn><mo>.</mo><mn>06</mn><mo>≤</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>≤</mo><mn>2</mn><mo>.</mo><mn>67</mn></mrow></math></span> for <span><math><mrow><mi>M</mi><mn>8</mn><msup><mrow><mn>7</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span> and <span><math><mrow><mn>1</mn><mo>.</mo><mn>9</mn><mo>≤</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>≤</mo><mn>2</mn><mo>.</mo><mn>26</mn></mrow></math></span> for <span><math><mrow><mi>S</mi><mi>g</mi><mi>r</mi><msup><mrow><mi>A</mi></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span>. Our results suggest that black holes enveloped by a Dehnen-type dark matter halo align with EHT observations, making it a promising candidate for explaining the surrounding environment of black holes.</div></div>","PeriodicalId":48774,"journal":{"name":"Physics of the Dark Universe","volume":"48 ","pages":"Article 101859"},"PeriodicalIF":6.4000,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Observable signature of Dehnen-type dark matter halos via strong gravitational lensing by supermassive black holes and constraints from EHT observations\",\"authors\":\"Amna Ali ,&nbsp;Niyaz Uddin Molla ,&nbsp;Sushant G. Ghosh ,&nbsp;Ammuthavali Ramasamya ,&nbsp;Ujjal Debnath\",\"doi\":\"10.1016/j.dark.2025.101859\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We investigate strong gravitational lensing by black holes influenced by a Dehnen-type dark matter halo, characterized by an additional parameter, the core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, and the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, alongside the black hole mass <span><math><mi>M</mi></math></span>. Our findings reveal that, for a fixed value of the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, key parameters such as the unstable photon orbit radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, critical impact parameter <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, angular position <span><math><msub><mrow><mi>θ</mi></mrow><mrow><mi>∞</mi></mrow></msub></math></span>, and angular separation <span><math><mi>S</mi></math></span> increase with the growing value of the core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, while the relative magnitude <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi><mi>a</mi><mi>g</mi></mrow></msub></math></span> decreases. Conversely, for a fixed value of <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, parameters including the unstable photon orbit radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, critical impact parameter <span><math><msub><mrow><mi>u</mi></mrow><mrow><mi>m</mi></mrow></msub></math></span>, strong deflection angle <span><math><msub><mrow><mi>α</mi></mrow><mrow><mi>D</mi></mrow></msub></math></span>, angular position <span><math><msub><mrow><mi>θ</mi></mrow><mrow><mi>∞</mi></mrow></msub></math></span>, angular separation <span><math><mi>S</mi></math></span>, relative magnitude <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>m</mi><mi>a</mi><mi>g</mi></mrow></msub></math></span>, and the outermost Einstein ring <span><math><msubsup><mrow><mi>θ</mi></mrow><mrow><mn>1</mn></mrow><mrow><mi>E</mi></mrow></msubsup></math></span> increase with the growing value of the dark matter central density <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>. For Sgr A*, the outermost Einstein ring <span><math><msubsup><mrow><mi>θ</mi></mrow><mrow><mn>1</mn></mrow><mrow><mi>E</mi></mrow></msubsup></math></span> is larger than in the case of M87*. We have calculated the time delay between two relativistic images by utilizing various supermassive black holes in nearby galaxies. It is found that the time delay under the influence of a Dehnen-type dark matter halo (<span><math><mrow><mo>∼</mo><mn>33</mn><mo>.</mo><mn>7584</mn></mrow></math></span> min) is suppressed compared to the case of a Schwarzschild black hole (<span><math><mrow><mo>∼</mo><mn>38</mn><mo>.</mo><mn>7682</mn></mrow></math></span> min), as in the case of NGC 2778. Finally, we constrain the central density parameter of the dark matter halo, <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, for a fixed core radius <span><math><msub><mrow><mi>r</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span>, using observational data from the Event Horizon Telescope collaboration for the supermassive black holes <span><math><mrow><mi>M</mi><mn>8</mn><msup><mrow><mn>7</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span> and <span><math><mrow><mi>S</mi><mi>g</mi><mi>r</mi><msup><mrow><mi>A</mi></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span>. The dark matter halo parameter <span><math><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span> is constrained to the range <span><math><mrow><mn>2</mn><mo>.</mo><mn>06</mn><mo>≤</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>≤</mo><mn>2</mn><mo>.</mo><mn>67</mn></mrow></math></span> for <span><math><mrow><mi>M</mi><mn>8</mn><msup><mrow><mn>7</mn></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span> and <span><math><mrow><mn>1</mn><mo>.</mo><mn>9</mn><mo>≤</mo><msub><mrow><mi>ρ</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mi>M</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>≤</mo><mn>2</mn><mo>.</mo><mn>26</mn></mrow></math></span> for <span><math><mrow><mi>S</mi><mi>g</mi><mi>r</mi><msup><mrow><mi>A</mi></mrow><mrow><mo>∗</mo></mrow></msup></mrow></math></span>. Our results suggest that black holes enveloped by a Dehnen-type dark matter halo align with EHT observations, making it a promising candidate for explaining the surrounding environment of black holes.</div></div>\",\"PeriodicalId\":48774,\"journal\":{\"name\":\"Physics of the Dark Universe\",\"volume\":\"48 \",\"pages\":\"Article 101859\"},\"PeriodicalIF\":6.4000,\"publicationDate\":\"2025-02-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physics of the Dark Universe\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2212686425000548\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ASTRONOMY & ASTROPHYSICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics of the Dark Universe","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2212686425000548","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0

摘要

我们研究了受dehnen型暗物质晕影响的黑洞的强引力透镜效应,其特征是核心半径rs和暗物质中心密度ρs,以及黑洞质量m。我们的研究结果表明,对于固定值的暗物质中心密度ρs,关键参数如不稳定光子轨道半径rm,临界撞击参数um,角位置θ∞,角距S随岩心半径rs的增大而增大,相对震级减小。相反,当rs值一定时,不稳定光子轨道半径rm、临界撞击参数um、强偏转角αD、角位置θ∞、角间距S、相对星等rg、最外层爱因斯坦环θ 1e等参数随着暗物质中心密度ρs值的增大而增大。对于人马座A*来说,最外层的爱因斯坦环θ1E比M87*大。我们利用邻近星系的各种超大质量黑洞计算了两个相对论性图像之间的时间延迟。研究发现,与史瓦西黑洞(~ 38.7682 min)相比,在dehnen型暗物质晕影响下的时间延迟(~ 33.7584 min)被抑制,如NGC 2778的情况。最后,我们利用事件视界望远镜合作项目对超大质量黑洞M87∗和SgrA∗的观测数据,对固定核心半径rs的暗物质晕的中心密度参数ρs进行了约束。暗物质晕参数ρs在M87∗的2.06≤ρsM2≤2.67和SgrA∗的1.9≤ρsM2≤2.26的范围内被约束。我们的研究结果表明,被dehnen型暗物质晕包围的黑洞与EHT观测结果一致,使其成为解释黑洞周围环境的有希望的候选者。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Observable signature of Dehnen-type dark matter halos via strong gravitational lensing by supermassive black holes and constraints from EHT observations
We investigate strong gravitational lensing by black holes influenced by a Dehnen-type dark matter halo, characterized by an additional parameter, the core radius rs, and the dark matter central density ρs, alongside the black hole mass M. Our findings reveal that, for a fixed value of the dark matter central density ρs, key parameters such as the unstable photon orbit radius rm, critical impact parameter um, angular position θ, and angular separation S increase with the growing value of the core radius rs, while the relative magnitude rmag decreases. Conversely, for a fixed value of rs, parameters including the unstable photon orbit radius rm, critical impact parameter um, strong deflection angle αD, angular position θ, angular separation S, relative magnitude rmag, and the outermost Einstein ring θ1E increase with the growing value of the dark matter central density ρs. For Sgr A*, the outermost Einstein ring θ1E is larger than in the case of M87*. We have calculated the time delay between two relativistic images by utilizing various supermassive black holes in nearby galaxies. It is found that the time delay under the influence of a Dehnen-type dark matter halo (33.7584 min) is suppressed compared to the case of a Schwarzschild black hole (38.7682 min), as in the case of NGC 2778. Finally, we constrain the central density parameter of the dark matter halo, ρs, for a fixed core radius rs, using observational data from the Event Horizon Telescope collaboration for the supermassive black holes M87 and SgrA. The dark matter halo parameter ρs is constrained to the range 2.06ρsM22.67 for M87 and 1.9ρsM22.26 for SgrA. Our results suggest that black holes enveloped by a Dehnen-type dark matter halo align with EHT observations, making it a promising candidate for explaining the surrounding environment of black holes.
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来源期刊
Physics of the Dark Universe
Physics of the Dark Universe ASTRONOMY & ASTROPHYSICS-
CiteScore
9.60
自引率
7.30%
发文量
118
审稿时长
61 days
期刊介绍: Physics of the Dark Universe is an innovative online-only journal that offers rapid publication of peer-reviewed, original research articles considered of high scientific impact. The journal is focused on the understanding of Dark Matter, Dark Energy, Early Universe, gravitational waves and neutrinos, covering all theoretical, experimental and phenomenological aspects.
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