The boundary of cosmic filaments
ABSTRACT For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by constructing stacked galaxy number density profiles around the filament spines. We find that the slope of the profile changes with distance t...
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Published in | Monthly notices of the Royal Astronomical Society Vol. 532; no. 4; pp. 4604 - 4615 |
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Main Authors | , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
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Oxford University Press
01.08.2024
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Abstract | ABSTRACT
For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by constructing stacked galaxy number density profiles around the filament spines. We find that the slope of the profile changes with distance to the filament spine, reaching its minimum at approximately 1 Mpc at $z=0$ in both state-of-the-art hydrodynamical simulations and observational data. This can be taken as the average value of the filament radius. Furthermore, we note that the average filament radius rapidly decreases from $z=4$ to 1, and then slightly increases. Moreover, we find that the radius of the filament depends on the length of the filament, the distance from the connected clusters, and the masses of the clusters. These results suggest a two-phase formation scenario of cosmic filaments. The filaments experienced rapid contraction before $z=1$, but their density distribution has remained roughly stable since then. The subsequent mass transport along the filaments to the connected clusters is likely to have contributed to the formation of the clusters themselves. |
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AbstractList | ABSTRACT
For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by constructing stacked galaxy number density profiles around the filament spines. We find that the slope of the profile changes with distance to the filament spine, reaching its minimum at approximately 1 Mpc at $z=0$ in both state-of-the-art hydrodynamical simulations and observational data. This can be taken as the average value of the filament radius. Furthermore, we note that the average filament radius rapidly decreases from $z=4$ to 1, and then slightly increases. Moreover, we find that the radius of the filament depends on the length of the filament, the distance from the connected clusters, and the masses of the clusters. These results suggest a two-phase formation scenario of cosmic filaments. The filaments experienced rapid contraction before $z=1$, but their density distribution has remained roughly stable since then. The subsequent mass transport along the filaments to the connected clusters is likely to have contributed to the formation of the clusters themselves. For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by constructing stacked galaxy number density profiles around the filament spines. We find that the slope of the profile changes with distance to the filament spine, reaching its minimum at approximately 1 Mpc at $z=0$ in both state-of-the-art hydrodynamical simulations and observational data. This can be taken as the average value of the filament radius. Furthermore, we note that the average filament radius rapidly decreases from $z=4$ to 1, and then slightly increases. Moreover, we find that the radius of the filament depends on the length of the filament, the distance from the connected clusters, and the masses of the clusters. These results suggest a two-phase formation scenario of cosmic filaments. The filaments experienced rapid contraction before $z=1$, but their density distribution has remained roughly stable since then. The subsequent mass transport along the filaments to the connected clusters is likely to have contributed to the formation of the clusters themselves. |
Author | Wang, Peng Libeskind, Noam I Wang, Wei Pakmor, Rüdiger Guo, Hong Springel, Volker Kannan, Rahul Galárraga-Espinosa, Daniela Yu, Hao-Ran Guo, Quan Hernández-Aguayo, César Bose, Sownak Hernquist, Lars Yu, Luo Kang, Xi |
Author_xml | – sequence: 1 givenname: Wei surname: Wang fullname: Wang, Wei email: pwang@shao.ac.cn – sequence: 2 givenname: Peng surname: Wang fullname: Wang, Peng email: pwang@shao.ac.cn – sequence: 3 givenname: Hong surname: Guo fullname: Guo, Hong email: guohong@shao.ac.cn – sequence: 4 givenname: Xi surname: Kang fullname: Kang, Xi – sequence: 5 givenname: Noam I surname: Libeskind fullname: Libeskind, Noam I – sequence: 6 givenname: Daniela orcidid: 0000-0002-8808-803X surname: Galárraga-Espinosa fullname: Galárraga-Espinosa, Daniela – sequence: 7 givenname: Volker surname: Springel fullname: Springel, Volker – sequence: 8 givenname: Rahul orcidid: 0000-0001-6092-2187 surname: Kannan fullname: Kannan, Rahul – sequence: 9 givenname: Lars surname: Hernquist fullname: Hernquist, Lars – sequence: 10 givenname: Rüdiger orcidid: 0000-0003-3308-2420 surname: Pakmor fullname: Pakmor, Rüdiger – sequence: 11 givenname: Hao-Ran surname: Yu fullname: Yu, Hao-Ran – sequence: 12 givenname: Sownak orcidid: 0000-0002-0974-5266 surname: Bose fullname: Bose, Sownak – sequence: 13 givenname: Quan surname: Guo fullname: Guo, Quan email: guohong@shao.ac.cn – sequence: 14 givenname: Luo orcidid: 0000-0003-2341-9755 surname: Yu fullname: Yu, Luo – sequence: 15 givenname: César orcidid: 0000-0001-9921-8832 surname: Hernández-Aguayo fullname: Hernández-Aguayo, César |
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For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by... For decades, the boundary of cosmic filaments has been a subject of debate. In this work, we determine the physically motivated radii of filaments by... |
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SubjectTerms | Clusters Density distribution Filaments Mass transport |
Title | The boundary of cosmic filaments |
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