Stochastic gravitational wave background from the collisions of dark matter halos

被引:0
|
作者
Yan, Qiming [1 ,2 ,3 ,4 ,5 ]
Ren, Xin [1 ,2 ]
Zhao, Yaqi [1 ,2 ]
Saridakis, Emmanuel N. [1 ,2 ,6 ,7 ]
机构
[1] Univ Sci & Technol China, Sch Phys Sci, Deep Space Explorat Lab, Hefei 230026, Anhui, Peoples R China
[2] Univ Sci & Technol China, Sch Astron & Space Sci, Dept Astron, CAS Key Lab Res Galaxies & Cosmol, Hefei 230026, Anhui, Peoples R China
[3] Univ Chinese Acad Sci, Sch Astron & Space Sci, Beijing 100049, Peoples R China
[4] Peking Univ, Kavli Inst Astron & Astrophys, Beijing 100871, Peoples R China
[5] Peking Univ, Sch Phys, Beijing 100871, Peoples R China
[6] Natl Observ Athens, Athens 11852, Greece
[7] Univ Catolica Norte, Dept Matemat, Avda Angamos 0610,1280 Casilla, Antofagasta, Chile
来源
EUROPEAN PHYSICAL JOURNAL C | 2024年 / 84卷 / 01期
关键词
BLACK-HOLES; CONSTRAINTS; GENERATION; EVOLUTION;
D O I
10.1140/epjc/s10052-024-12397-2
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We investigate the effect of the dark matter (DM) halos collisions, namely collisions of galaxies and galaxy clusters, through gravitational bremsstrahlung, on the stochastic gravitational wave background. We first calculate the gravitational wave signal of a single collision event, assuming point masses and linear perturbation theory. Then we proceed to the calculation of the energy spectrum of the collective effect of all dark matter collisions in the Universe. Concerning the DM halo collision rate, we show that it is given by the product of the number density of DM halos, which is calculated by the extended Press-Schechter (EPS) theory, with the collision rate of a single DM halo, which is given by simulation results, with a function of the linear growth rate of matter density through cosmological evolution. Hence, integrating over all mass and distance ranges, we finally extract the spectrum of the stochastic gravitational wave background created by DM halos collisions. As we show, the resulting contribution to the stochastic gravitational wave background is of the order of h(c) approximate to 10(-29) in the band of f approximate to 10(-15)Hz. However, in very low frequency band, it is larger. With current observational sensitivity it cannot be detected.
引用
收藏
页数:11
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