{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:ITNXF6ZVIBTNCHC7EEL6DJK2J4","short_pith_number":"pith:ITNXF6ZV","schema_version":"1.0","canonical_sha256":"44db72fb354066d11c5f2117e1a55a4f36e1064f9821ea37661513cbbb56c746","source":{"kind":"arxiv","id":"2508.13903","version":1},"attestation_state":"computed","paper":{"title":"Role of Non-conserved Gravity Theory and Electric Charge in Constructing Complexity-free Stellar Models: A Novel Approach under Non-minimal Coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Tayyab Naseer","submitted_at":"2025-08-19T15:04:27Z","abstract_excerpt":"This study explores the application of complexity factor within the context of Rastall gravity, exploring its implications on a static spacetime admitting spherical symmetry associated with anisotropic fluids under an electromagnetic field. The field equations are derived for a static charged sphere that provides a foundational framework for analyzing gravitational effects in this non-conserved theory. The mass function is formulated by incorporating both fluid and geometric parameters, offering insights into how mass distribution affects spacetime curvature. Through orthogonal decomposition o"},"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":"2508.13903","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2025-08-19T15:04:27Z","cross_cats_sorted":[],"title_canon_sha256":"c3a4b50e4c440e945280405bbb20cd264082e3c63c0eefdeaec60f1d168c42a3","abstract_canon_sha256":"37ee4b4ba63a4c85c61c9a37f8659fceaadc2d1377b4d2f1d74221936ed44703"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:56:09.356982Z","signature_b64":"xGGSxhNEpaG0SsnSkwsxC5aXcgIKkwYjORVPUmKrD3iBR9uIWr9qDdc0NCxaIIoDkz6vrgKUdilYA3BAzNfUBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44db72fb354066d11c5f2117e1a55a4f36e1064f9821ea37661513cbbb56c746","last_reissued_at":"2026-07-05T11:56:09.356542Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:56:09.356542Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Role of Non-conserved Gravity Theory and Electric Charge in Constructing Complexity-free Stellar Models: A Novel Approach under Non-minimal Coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Tayyab Naseer","submitted_at":"2025-08-19T15:04:27Z","abstract_excerpt":"This study explores the application of complexity factor within the context of Rastall gravity, exploring its implications on a static spacetime admitting spherical symmetry associated with anisotropic fluids under an electromagnetic field. The field equations are derived for a static charged sphere that provides a foundational framework for analyzing gravitational effects in this non-conserved theory. The mass function is formulated by incorporating both fluid and geometric parameters, offering insights into how mass distribution affects spacetime curvature. Through orthogonal decomposition o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.13903","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/2508.13903/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":"2508.13903","created_at":"2026-07-05T11:56:09.356597+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.13903v1","created_at":"2026-07-05T11:56:09.356597+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.13903","created_at":"2026-07-05T11:56:09.356597+00:00"},{"alias_kind":"pith_short_12","alias_value":"ITNXF6ZVIBTN","created_at":"2026-07-05T11:56:09.356597+00:00"},{"alias_kind":"pith_short_16","alias_value":"ITNXF6ZVIBTNCHC7","created_at":"2026-07-05T11:56:09.356597+00:00"},{"alias_kind":"pith_short_8","alias_value":"ITNXF6ZV","created_at":"2026-07-05T11:56:09.356597+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/ITNXF6ZVIBTNCHC7EEL6DJK2J4","json":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4.json","graph_json":"https://pith.science/api/pith-number/ITNXF6ZVIBTNCHC7EEL6DJK2J4/graph.json","events_json":"https://pith.science/api/pith-number/ITNXF6ZVIBTNCHC7EEL6DJK2J4/events.json","paper":"https://pith.science/paper/ITNXF6ZV"},"agent_actions":{"view_html":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4","download_json":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4.json","view_paper":"https://pith.science/paper/ITNXF6ZV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.13903&json=true","fetch_graph":"https://pith.science/api/pith-number/ITNXF6ZVIBTNCHC7EEL6DJK2J4/graph.json","fetch_events":"https://pith.science/api/pith-number/ITNXF6ZVIBTNCHC7EEL6DJK2J4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4/action/storage_attestation","attest_author":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4/action/author_attestation","sign_citation":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4/action/citation_signature","submit_replication":"https://pith.science/pith/ITNXF6ZVIBTNCHC7EEL6DJK2J4/action/replication_record"}},"created_at":"2026-07-05T11:56:09.356597+00:00","updated_at":"2026-07-05T11:56:09.356597+00:00"}