The model-independent theoretical upper bound on the thermal dark matter (DM) mass can be derived from the maximum inelastic DM cross section featuring the whole observed DM abundance. We deploy partial-wave unitarity of the scattering matrix to derive the maximal thermally averaged cross section for general number-changing processes (with ), which may involve standard model particles or occur solely within the dark sector. The usual upper limit on the DM mass for -wave annihilation is around 130 TeV (1 GeV) for (3) and only applies in the case of a freeze-out occurring in the standard cosmological scenario. We consider the effects of two nonstandard cosmological evolutions, characterized by low-temperature reheating: (i) a kinationlike scenario and (ii) an early matter-dominated scenario. In the first case, early freeze-out strengthens the unitarity bound to a few TeVs for weakly interacting massive particles (WIMPs); while in the second case, the WIMP DM can be as heavy as due to a large entropy dilution.
{ "_oai": { "updated": "2024-02-24T00:30:27Z", "id": "oai:repo.scoap3.org:83612", "sets": [ "PRD" ] }, "authors": [ { "raw_name": "Nicol\u00e1s Bernal", "affiliations": [ { "country": "United Arab Emirates", "value": "New York University Abu Dhabi, P.O. Box 129188, Saadiyat Island, Abu Dhabi, United Arab Emirates" } ], "surname": "Bernal", "given_names": "Nicol\u00e1s", "full_name": "Bernal, Nicol\u00e1s" }, { "raw_name": "Partha Konar", "affiliations": [ { "country": "India", "value": "Physical Research Laboratory, Ahmedabad 380009, Gujarat, India" } ], "surname": "Konar", "given_names": "Partha", "full_name": "Konar, Partha" }, { "raw_name": "Sudipta Show", "affiliations": [ { "country": "India", "value": "Physical Research Laboratory, Ahmedabad 380009, Gujarat, India" } ], "surname": "Show", "given_names": "Sudipta", "full_name": "Show, Sudipta" } ], "titles": [ { "source": "APS", "title": "Unitarity bound on dark matter in low-temperature reheating scenarios" } ], "dois": [ { "value": "10.1103/PhysRevD.109.035018" } ], "publication_info": [ { "journal_volume": "109", "journal_title": "Physical Review D", "material": "article", "journal_issue": "3", "year": 2024 } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2024-02-24T00:30:22.000380", "source": "APS", "method": "APS", "submission_number": "d80f401ed2ab11eea49c8e4864f4776e" }, "page_nr": [ 16 ], "license": [ { "url": "https://creativecommons.org/licenses/by/4.0/", "license": "CC-BY-4.0" } ], "copyright": [ { "statement": "Published by the American Physical Society", "year": "2024" } ], "control_number": "83612", "record_creation_date": "2024-02-23T16:30:07.387256", "_files": [ { "checksum": "md5:86dc14acacf3081b4878ea78b55cc916", "filetype": "pdf", "bucket": "5e75ef68-ee2a-4c0b-a2fc-98016b77ffb6", "version_id": "e61e700c-2bf4-4717-9b4a-ae201fd349ad", "key": "10.1103/PhysRevD.109.035018.pdf", "size": 1449441 }, { "checksum": "md5:e53fc695192fe77c351a5349e513201f", "filetype": "xml", "bucket": "5e75ef68-ee2a-4c0b-a2fc-98016b77ffb6", "version_id": "109c9dbb-0acd-414e-aee1-7f7dc9a7d6bb", "key": "10.1103/PhysRevD.109.035018.xml", "size": 278307 } ], "collections": [ { "primary": "HEP" }, { "primary": "Citeable" }, { "primary": "Published" } ], "arxiv_eprints": [ { "categories": [ "hep-ph" ], "value": "2311.01587" } ], "abstracts": [ { "source": "APS", "value": "The model-independent theoretical upper bound on the thermal dark matter (DM) mass can be derived from the maximum inelastic DM cross section featuring the whole observed DM abundance. We deploy partial-wave unitarity of the scattering matrix to derive the maximal thermally averaged cross section for general number-changing processes <math><mi>r</mi><mo>\u2192</mo><mn>2</mn></math> (with <math><mi>r</mi><mo>\u2265</mo><mn>2</mn></math>), which may involve standard model particles or occur solely within the dark sector. The usual upper limit on the DM mass for <math><mi>s</mi></math>-wave annihilation is around 130 TeV (1 GeV) for <math><mi>r</mi><mo>=</mo><mn>2</mn></math> (3) and only applies in the case of a freeze-out occurring in the standard cosmological scenario. We consider the effects of two nonstandard cosmological evolutions, characterized by low-temperature reheating: (i) a kinationlike scenario and (ii) an early matter-dominated scenario. In the first case, early freeze-out strengthens the unitarity bound to a few TeVs for weakly interacting massive particles (WIMPs); while in the second case, the WIMP DM can be as heavy as <math><mo>\u223c</mo><msup><mn>10</mn><mn>10</mn></msup><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math> due to a large entropy dilution." } ], "imprints": [ { "date": "2024-02-23", "publisher": "APS" } ] }