{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MMTYTFFXUCESNHVDXN64PBLA3V","short_pith_number":"pith:MMTYTFFX","schema_version":"1.0","canonical_sha256":"63278994b7a089269ea3bb7dc78560dd6a7f3adb25965beb6b2d9f657ac09a19","source":{"kind":"arxiv","id":"2304.02482","version":1},"attestation_state":"computed","paper":{"title":"Baryogenesis in $f(R,L_m)$ gravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Lakhan V. Jaybhaye, P.K. Sahoo, Snehasish Bhattacharjee","submitted_at":"2023-04-04T12:50:08Z","abstract_excerpt":"This paper aims to recreate the gravitational baryogenesis epoch in the framework of the $f(R,L_m)$ theory of gravity, where $R$ and $L_m$ are the curvature scalar and the matter Langragian, respectively. In particular, we examine the model, $f(R,L_m) = \\frac{R}{2} + L_m ^{\\alpha} + \\zeta$, under the supposition that the universe is saturated with dark energy and perfect fluid, with a non-zero baryon to entropy ratio during a radiation dominance era. We confine the model with the gravitational baryogenesis scenario, emphasizing the appropriate values of model parameters compatible with the bar"},"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":"2304.02482","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2023-04-04T12:50:08Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"52f82c65f021420b1cc8dc927dd5794a4c3bac82c4d5a3cdb174519983fef9c5","abstract_canon_sha256":"716fd56b4b89b4f04d7b207531c43c3992cda1b043678556fdb15bbcc8e0902f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:58:26.038230Z","signature_b64":"kV4XGnKV8BUGP539J9Tpz0OwO7hXV826NXEnayyUbJ5k3pNLSTAnDaAWz7Rcy/MJ+nX4VkCCQFVL+HFZp4tiAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"63278994b7a089269ea3bb7dc78560dd6a7f3adb25965beb6b2d9f657ac09a19","last_reissued_at":"2026-07-05T05:58:26.037633Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:58:26.037633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryogenesis in $f(R,L_m)$ gravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Lakhan V. Jaybhaye, P.K. Sahoo, Snehasish Bhattacharjee","submitted_at":"2023-04-04T12:50:08Z","abstract_excerpt":"This paper aims to recreate the gravitational baryogenesis epoch in the framework of the $f(R,L_m)$ theory of gravity, where $R$ and $L_m$ are the curvature scalar and the matter Langragian, respectively. In particular, we examine the model, $f(R,L_m) = \\frac{R}{2} + L_m ^{\\alpha} + \\zeta$, under the supposition that the universe is saturated with dark energy and perfect fluid, with a non-zero baryon to entropy ratio during a radiation dominance era. We confine the model with the gravitational baryogenesis scenario, emphasizing the appropriate values of model parameters compatible with the bar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2304.02482","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/2304.02482/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":"2304.02482","created_at":"2026-07-05T05:58:26.037695+00:00"},{"alias_kind":"arxiv_version","alias_value":"2304.02482v1","created_at":"2026-07-05T05:58:26.037695+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.02482","created_at":"2026-07-05T05:58:26.037695+00:00"},{"alias_kind":"pith_short_12","alias_value":"MMTYTFFXUCES","created_at":"2026-07-05T05:58:26.037695+00:00"},{"alias_kind":"pith_short_16","alias_value":"MMTYTFFXUCESNHVD","created_at":"2026-07-05T05:58:26.037695+00:00"},{"alias_kind":"pith_short_8","alias_value":"MMTYTFFX","created_at":"2026-07-05T05:58:26.037695+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V","json":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V.json","graph_json":"https://pith.science/api/pith-number/MMTYTFFXUCESNHVDXN64PBLA3V/graph.json","events_json":"https://pith.science/api/pith-number/MMTYTFFXUCESNHVDXN64PBLA3V/events.json","paper":"https://pith.science/paper/MMTYTFFX"},"agent_actions":{"view_html":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V","download_json":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V.json","view_paper":"https://pith.science/paper/MMTYTFFX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2304.02482&json=true","fetch_graph":"https://pith.science/api/pith-number/MMTYTFFXUCESNHVDXN64PBLA3V/graph.json","fetch_events":"https://pith.science/api/pith-number/MMTYTFFXUCESNHVDXN64PBLA3V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V/action/storage_attestation","attest_author":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V/action/author_attestation","sign_citation":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V/action/citation_signature","submit_replication":"https://pith.science/pith/MMTYTFFXUCESNHVDXN64PBLA3V/action/replication_record"}},"created_at":"2026-07-05T05:58:26.037695+00:00","updated_at":"2026-07-05T05:58:26.037695+00:00"}