Formation and Abundance of Late Forming Primordial Black Holes as Dark Matter
We propose a novel mechanism where Primordial Black Hole (PBH) dark matter is formed much later in the history of the universe between the epoch of Big Bang Nucleosynthesis (BBN) and Cosmic Microwave Background (CMB) photon decoupling. In our setup, one does not need to modify the scale-invariant in...
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description | We propose a novel mechanism where Primordial Black Hole (PBH) dark matter is formed much later in the history of the universe between the epoch of Big Bang Nucleosynthesis (BBN) and Cosmic Microwave Background (CMB) photon decoupling. In our setup, one does not need to modify the scale-invariant inflationary power spectra; instead, a late phase transition in strongly interacting fermion-scalar fluid (which naturally occurs around red-shift \( 10^6 \leq \, z_{\scriptscriptstyle T} \, \leq 10^8\) ) creates an instability in the density perturbation as sound speed turns imaginary. As a result, the dark matter perturbation grows exponentially in sub-Compton scales. This follows the immediate formation of early dense dark matter halo, which finally evolves into PBH due to cooling through scalar radiation. We calculate the variance of the density perturbations and PBH fractional abundances \(f(M)\) by using a non-monochromatic mass function. We find the peak of our PBH mass function lies between \(10^{-16} - 10^{-14}\) solar mass for \( z_{\scriptscriptstyle T} \simeq 10^6\), and thus it can be the entire dark matter of the universe. In PBH formation, one would expect a temporary phase where an attractive scalar balances the Fermi pressure. We numerically confirm that such a state indeed exists, and we find the radius and density profile of the temporary static structure of the dark matter halo, which finally evolves to PBH due to cooling through scalar radiation. |
doi_str_mv | 10.48550/arxiv.2204.09628 |
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In our setup, one does not need to modify the scale-invariant inflationary power spectra; instead, a late phase transition in strongly interacting fermion-scalar fluid (which naturally occurs around red-shift \( 10^6 \leq \, z_{\scriptscriptstyle T} \, \leq 10^8\) ) creates an instability in the density perturbation as sound speed turns imaginary. As a result, the dark matter perturbation grows exponentially in sub-Compton scales. This follows the immediate formation of early dense dark matter halo, which finally evolves into PBH due to cooling through scalar radiation. We calculate the variance of the density perturbations and PBH fractional abundances \(f(M)\) by using a non-monochromatic mass function. We find the peak of our PBH mass function lies between \(10^{-16} - 10^{-14}\) solar mass for \( z_{\scriptscriptstyle T} \simeq 10^6\), and thus it can be the entire dark matter of the universe. In PBH formation, one would expect a temporary phase where an attractive scalar balances the Fermi pressure. We numerically confirm that such a state indeed exists, and we find the radius and density profile of the temporary static structure of the dark matter halo, which finally evolves to PBH due to cooling through scalar radiation.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2204.09628</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Abundance ; Big bang cosmology ; Big Bang theory ; Black holes ; Cooling ; Cosmic microwave background ; Dark matter ; Decoupling ; Density ; Doppler effect ; Fermions ; Microbalances ; Nuclear fusion ; Nuclei (nuclear physics) ; Perturbation ; Phase transitions ; Physics - Cosmology and Nongalactic Astrophysics ; Physics - General Relativity and Quantum Cosmology ; Physics - High Energy Physics - Phenomenology ; Physics - High Energy Physics - Theory ; Power spectra ; Radiation ; Red shift ; Universe</subject><ispartof>arXiv.org, 2022-06</ispartof><rights>2022. 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In our setup, one does not need to modify the scale-invariant inflationary power spectra; instead, a late phase transition in strongly interacting fermion-scalar fluid (which naturally occurs around red-shift \( 10^6 \leq \, z_{\scriptscriptstyle T} \, \leq 10^8\) ) creates an instability in the density perturbation as sound speed turns imaginary. As a result, the dark matter perturbation grows exponentially in sub-Compton scales. This follows the immediate formation of early dense dark matter halo, which finally evolves into PBH due to cooling through scalar radiation. We calculate the variance of the density perturbations and PBH fractional abundances \(f(M)\) by using a non-monochromatic mass function. We find the peak of our PBH mass function lies between \(10^{-16} - 10^{-14}\) solar mass for \( z_{\scriptscriptstyle T} \simeq 10^6\), and thus it can be the entire dark matter of the universe. In PBH formation, one would expect a temporary phase where an attractive scalar balances the Fermi pressure. We numerically confirm that such a state indeed exists, and we find the radius and density profile of the temporary static structure of the dark matter halo, which finally evolves to PBH due to cooling through scalar radiation.</description><subject>Abundance</subject><subject>Big bang cosmology</subject><subject>Big Bang theory</subject><subject>Black holes</subject><subject>Cooling</subject><subject>Cosmic microwave background</subject><subject>Dark matter</subject><subject>Decoupling</subject><subject>Density</subject><subject>Doppler effect</subject><subject>Fermions</subject><subject>Microbalances</subject><subject>Nuclear fusion</subject><subject>Nuclei (nuclear physics)</subject><subject>Perturbation</subject><subject>Phase transitions</subject><subject>Physics - Cosmology and Nongalactic Astrophysics</subject><subject>Physics - General Relativity and Quantum Cosmology</subject><subject>Physics - High Energy Physics - Phenomenology</subject><subject>Physics - High Energy Physics - Theory</subject><subject>Power spectra</subject><subject>Radiation</subject><subject>Red shift</subject><subject>Universe</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj8FOwzAQRC0kJKrSD-CEJc4p9jqOk2MplCKlgkPv0TrroLRpXJwEwd-TtpzmMKPRe4zdSTGPU63FI4af-nsOIOK5yBJIr9gElJJRGgPcsFnX7YQQkBjQWk3YZuXDAfvatxxb4gs7tIRt6biveI6946e-bj_5R6gPPlCNDX9qsNzztW9cx7Hjzxj2fIN978Itu66w6dzsP6dsu3rZLtdR_v76tlzkEWqQkckUqTihyjhpMTVgLZZJrMpMO2tIxAosKZLpyGml0KW0YKgilyZkiFBN2f3l9uxaHEc0DL_Fybk4O4-Lh8viGPzX4Lq-2PkhtCNTAYlWApSUUv0BdqtY8A</recordid><startdate>20220609</startdate><enddate>20220609</enddate><creator>Chakraborty, Amlan</creator><creator>Chanda, Prolay K</creator><creator>Kanhaiya Lal Pandey</creator><creator>Das, Subinoy</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20220609</creationdate><title>Formation and Abundance of Late Forming Primordial Black Holes as Dark Matter</title><author>Chakraborty, Amlan ; 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In our setup, one does not need to modify the scale-invariant inflationary power spectra; instead, a late phase transition in strongly interacting fermion-scalar fluid (which naturally occurs around red-shift \( 10^6 \leq \, z_{\scriptscriptstyle T} \, \leq 10^8\) ) creates an instability in the density perturbation as sound speed turns imaginary. As a result, the dark matter perturbation grows exponentially in sub-Compton scales. This follows the immediate formation of early dense dark matter halo, which finally evolves into PBH due to cooling through scalar radiation. We calculate the variance of the density perturbations and PBH fractional abundances \(f(M)\) by using a non-monochromatic mass function. We find the peak of our PBH mass function lies between \(10^{-16} - 10^{-14}\) solar mass for \( z_{\scriptscriptstyle T} \simeq 10^6\), and thus it can be the entire dark matter of the universe. In PBH formation, one would expect a temporary phase where an attractive scalar balances the Fermi pressure. We numerically confirm that such a state indeed exists, and we find the radius and density profile of the temporary static structure of the dark matter halo, which finally evolves to PBH due to cooling through scalar radiation.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2204.09628</doi><oa>free_for_read</oa></addata></record> |
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subjects | Abundance Big bang cosmology Big Bang theory Black holes Cooling Cosmic microwave background Dark matter Decoupling Density Doppler effect Fermions Microbalances Nuclear fusion Nuclei (nuclear physics) Perturbation Phase transitions Physics - Cosmology and Nongalactic Astrophysics Physics - General Relativity and Quantum Cosmology Physics - High Energy Physics - Phenomenology Physics - High Energy Physics - Theory Power spectra Radiation Red shift Universe |
title | Formation and Abundance of Late Forming Primordial Black Holes as Dark Matter |
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