Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9784
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dc.contributor.authorSalazar, Edgar M.en_US
dc.contributor.authorRozo, Eduardoen_US
dc.contributor.authorGarcia, Rafaelen_US
dc.contributor.authorKokron, Nickolasen_US
dc.contributor.authorADHIKARI, SUSMITAen_US
dc.contributor.authorDiemer, Benedikten_US
dc.contributor.authorOsinga, Calvinen_US
dc.date.accessioned2025-05-01T03:56:08Z-
dc.date.available2025-05-01T03:56:08Z-
dc.date.issued2025-02en_US
dc.identifier.citationPhysical Review D, 111, 043527.en_US
dc.identifier.issn2470-0010en_US
dc.identifier.issn2470-0029en_US
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.111.043527en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/9784-
dc.description.abstractAccurate modeling of the one-to-two halo transition has long been difficult to achieve. We demonstrate that physically motivated halo definitions that respect the bimodal phase-space distribution of dark matter particles near halos resolves this difficulty. Specifically, the two phase-space components are overlapping and correspond to (1) particles orbiting the halo and (2) particles infalling into the halo for the first time. Motivated by this decomposition, García et al. [Mon. Not. R. Astron. Soc. 521, 2464 (2023)] advocated for defining halos as the collection of particles orbiting their self-generated potential. This definition identifies the traditional one-halo term of the halo-mass correlation function with the distribution of orbiting particles around a halo, while the two-halo term governs the distribution of infalling particles. We use dark matter simulations to demonstrate that the distribution of orbiting particles is finite and can be characterized by a single physical scale 𝑟h, which we refer to as the halo radius. The two-halo term is described using a simple yet accurate empirical model based on the Zel’dovich correlation function. We further demonstrate that the halo radius imprints itself on the distribution of infalling particles at small scales. Our final model for the halo-mass correlation function is accurate at the ≈2% level for 𝑟∈[0.1,50]  ℎ−1 Mpc. The Fourier transform of our best-fit model describes the halo-mass power spectrum with comparable accuracy for 𝑘∈[0.06,6.0]  ℎ Mpc−1.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectDark matteren_US
dc.subject2025-APR-WEEK1en_US
dc.subjectTOC-APR-2025en_US
dc.subject2025en_US
dc.titleDynamics-based halo model for large scale structureen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Den_US
dc.publication.originofpublisherForeignen_US
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