{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:GK6XCSXADPM5L6CS7EOYRE7GJ6","short_pith_number":"pith:GK6XCSXA","schema_version":"1.0","canonical_sha256":"32bd714ae01bd9d5f852f91d8893e64fbdaf4ccf25dd194e9de137d2d3a0a8de","source":{"kind":"arxiv","id":"2201.03355","version":1},"attestation_state":"computed","paper":{"title":"Exploring delaying and heating effects on the 21-cm signature of fuzzy dark matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.CO","authors_text":"Debanjan Sarkar, Ely D. Kovetz, Jordan Flitter","submitted_at":"2022-01-10T14:16:29Z","abstract_excerpt":"In the fuzzy dark matter (FDM) model, dark matter is composed of ultra-light particles with a de Broglie wavelength of $\\sim$kpc, above which it behaves like cold dark matter (CDM). Due to this, FDM suppresses the growth of structure on small scales, which delays the onset of the cosmic dawn (CD) and the subsequent epoch of reionization (EoR). This leaves potential signatures in the sky averaged 21-cm signal (global), as well as in the 21-cm fluctuations, which can be sought for with ongoing and future 21-cm global and intensity mapping experiments. To do so reliably, it is crucial to include "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2201.03355","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.CO","submitted_at":"2022-01-10T14:16:29Z","cross_cats_sorted":[],"title_canon_sha256":"0679110ad4481be753e9331352cc42e10b0bc8883984d27f10ebc0245beb55f0","abstract_canon_sha256":"dc66ac4bca1cc617fa20896b29d99b7d0df478e32461ddfe3432a0f49afd21d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:27:50.959111Z","signature_b64":"Dgmcj476Oc/N2psXzE7x1es9o9Nv+XHI9WEH6tU3CBwNBqT3RU103UPJKM0c/v8CtI2Y99HgSVCtOAvYZzM1CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32bd714ae01bd9d5f852f91d8893e64fbdaf4ccf25dd194e9de137d2d3a0a8de","last_reissued_at":"2026-07-05T04:27:50.958626Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:27:50.958626Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring delaying and heating effects on the 21-cm signature of fuzzy dark matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.CO","authors_text":"Debanjan Sarkar, Ely D. Kovetz, Jordan Flitter","submitted_at":"2022-01-10T14:16:29Z","abstract_excerpt":"In the fuzzy dark matter (FDM) model, dark matter is composed of ultra-light particles with a de Broglie wavelength of $\\sim$kpc, above which it behaves like cold dark matter (CDM). Due to this, FDM suppresses the growth of structure on small scales, which delays the onset of the cosmic dawn (CD) and the subsequent epoch of reionization (EoR). This leaves potential signatures in the sky averaged 21-cm signal (global), as well as in the 21-cm fluctuations, which can be sought for with ongoing and future 21-cm global and intensity mapping experiments. To do so reliably, it is crucial to include "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2201.03355","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2201.03355/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2201.03355","created_at":"2026-07-05T04:27:50.958681+00:00"},{"alias_kind":"arxiv_version","alias_value":"2201.03355v1","created_at":"2026-07-05T04:27:50.958681+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2201.03355","created_at":"2026-07-05T04:27:50.958681+00:00"},{"alias_kind":"pith_short_12","alias_value":"GK6XCSXADPM5","created_at":"2026-07-05T04:27:50.958681+00:00"},{"alias_kind":"pith_short_16","alias_value":"GK6XCSXADPM5L6CS","created_at":"2026-07-05T04:27:50.958681+00:00"},{"alias_kind":"pith_short_8","alias_value":"GK6XCSXA","created_at":"2026-07-05T04:27:50.958681+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.18884","citing_title":"Primordial black holes and the velocity acoustic oscillations features in 21 cm signals from the cosmic Dark Ages","ref_index":32,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6","json":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6.json","graph_json":"https://pith.science/api/pith-number/GK6XCSXADPM5L6CS7EOYRE7GJ6/graph.json","events_json":"https://pith.science/api/pith-number/GK6XCSXADPM5L6CS7EOYRE7GJ6/events.json","paper":"https://pith.science/paper/GK6XCSXA"},"agent_actions":{"view_html":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6","download_json":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6.json","view_paper":"https://pith.science/paper/GK6XCSXA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2201.03355&json=true","fetch_graph":"https://pith.science/api/pith-number/GK6XCSXADPM5L6CS7EOYRE7GJ6/graph.json","fetch_events":"https://pith.science/api/pith-number/GK6XCSXADPM5L6CS7EOYRE7GJ6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6/action/storage_attestation","attest_author":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6/action/author_attestation","sign_citation":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6/action/citation_signature","submit_replication":"https://pith.science/pith/GK6XCSXADPM5L6CS7EOYRE7GJ6/action/replication_record"}},"created_at":"2026-07-05T04:27:50.958681+00:00","updated_at":"2026-07-05T04:27:50.958681+00:00"}