{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:K65IJTJC2DU3R3H6724QHLRFFR","short_pith_number":"pith:K65IJTJC","schema_version":"1.0","canonical_sha256":"57ba84cd22d0e9b8ecfefeb903ae252c648c11c6c82ae0f1285f9230b689e6d4","source":{"kind":"arxiv","id":"2412.14342","version":1},"attestation_state":"computed","paper":{"title":"Simulation of thermal conduction by asymmetric dark matter in realistic stars and planets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","astro-ph.SR"],"primary_cat":"hep-ph","authors_text":"Aaron C. Vincent, Hannah Banks, Rashaad Reid, Stephanie Beram","submitted_at":"2024-12-18T21:27:13Z","abstract_excerpt":"Dark matter captured in stars can act as an additional heat transport mechanism, modifying fusion rates and asteroseismoloigcal observables. Calculations of heat transport rates rely on approximate solutions to the Boltzmann equation, which have never been verified in realistic stars. Here, we simulate heat transport in the Sun, the Earth, and a brown dwarf model, using realistic radial temperature, density, composition and gravitational potential profiles. We show that the formalism developed in arXiv:2111.06895 remains accurate across all celestial objects considered, across a wide range of "},"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":"2412.14342","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-12-18T21:27:13Z","cross_cats_sorted":["astro-ph.CO","astro-ph.SR"],"title_canon_sha256":"17435d292eeef72e06536e2830548805b12cc4a5432c1b25275823cfdf219fd1","abstract_canon_sha256":"e2f004bc9e1bc5620f7124195d7d3d897cb6ce9bc15099d2b4427c14e54edb3f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:51:45.927796Z","signature_b64":"NpNCMXjoAzob0FwON8cAkwUuwI31IbQG+xkMYOWpLkq+4qa7QerWAhFVg0ogSQ/O2rtIZO3jdQ9uZ0rB2ieiDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57ba84cd22d0e9b8ecfefeb903ae252c648c11c6c82ae0f1285f9230b689e6d4","last_reissued_at":"2026-07-05T09:51:45.927298Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:51:45.927298Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulation of thermal conduction by asymmetric dark matter in realistic stars and planets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","astro-ph.SR"],"primary_cat":"hep-ph","authors_text":"Aaron C. Vincent, Hannah Banks, Rashaad Reid, Stephanie Beram","submitted_at":"2024-12-18T21:27:13Z","abstract_excerpt":"Dark matter captured in stars can act as an additional heat transport mechanism, modifying fusion rates and asteroseismoloigcal observables. Calculations of heat transport rates rely on approximate solutions to the Boltzmann equation, which have never been verified in realistic stars. Here, we simulate heat transport in the Sun, the Earth, and a brown dwarf model, using realistic radial temperature, density, composition and gravitational potential profiles. We show that the formalism developed in arXiv:2111.06895 remains accurate across all celestial objects considered, across a wide range of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.14342","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/2412.14342/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":"2412.14342","created_at":"2026-07-05T09:51:45.927366+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.14342v1","created_at":"2026-07-05T09:51:45.927366+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.14342","created_at":"2026-07-05T09:51:45.927366+00:00"},{"alias_kind":"pith_short_12","alias_value":"K65IJTJC2DU3","created_at":"2026-07-05T09:51:45.927366+00:00"},{"alias_kind":"pith_short_16","alias_value":"K65IJTJC2DU3R3H6","created_at":"2026-07-05T09:51:45.927366+00:00"},{"alias_kind":"pith_short_8","alias_value":"K65IJTJC","created_at":"2026-07-05T09:51:45.927366+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.09998","citing_title":"Constraints and Projections for Millicharged Dark Matter in the Sun with Water Cherenkov Neutrino Detectors","ref_index":98,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR","json":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR.json","graph_json":"https://pith.science/api/pith-number/K65IJTJC2DU3R3H6724QHLRFFR/graph.json","events_json":"https://pith.science/api/pith-number/K65IJTJC2DU3R3H6724QHLRFFR/events.json","paper":"https://pith.science/paper/K65IJTJC"},"agent_actions":{"view_html":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR","download_json":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR.json","view_paper":"https://pith.science/paper/K65IJTJC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.14342&json=true","fetch_graph":"https://pith.science/api/pith-number/K65IJTJC2DU3R3H6724QHLRFFR/graph.json","fetch_events":"https://pith.science/api/pith-number/K65IJTJC2DU3R3H6724QHLRFFR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR/action/storage_attestation","attest_author":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR/action/author_attestation","sign_citation":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR/action/citation_signature","submit_replication":"https://pith.science/pith/K65IJTJC2DU3R3H6724QHLRFFR/action/replication_record"}},"created_at":"2026-07-05T09:51:45.927366+00:00","updated_at":"2026-07-05T09:51:45.927366+00:00"}