{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:3WDZUMFW7HF4Y6OT7U5GAHYAEN","short_pith_number":"pith:3WDZUMFW","schema_version":"1.0","canonical_sha256":"dd879a30b6f9cbcc79d3fd3a601f002352203f73b992b6b764f51dfa1627f6e0","source":{"kind":"arxiv","id":"2401.04917","version":1},"attestation_state":"computed","paper":{"title":"Charged Anisotropic Spherical Collapse in $f(\\mathcal{R},\\mathcal{T},\\mathcal{Q})$ Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Sharif, Tayyab Naseer","submitted_at":"2024-01-10T04:01:45Z","abstract_excerpt":"This paper discusses the gravitational collapse of dynamical self-gravitating fluid distribution in $f(\\mathcal{R},\\mathcal{T},\\mathcal{Q})$ gravity, where $\\mathcal{Q}=\\mathcal{R}_{\\varphi\\vartheta}\\mathcal{T}^{\\varphi\\vartheta}$. In this regard, we assume a charged anisotropic spherical geometry involving dissipation flux and adopt standard model of the form $\\mathcal{R}+\\Phi\\sqrt{\\mathcal{T}}+\\Psi\\mathcal{Q}$, where $\\Phi$ and $\\Psi$ symbolize real-valued coupling parameters. The Misner-Sharp as well as M\\\"{u}ler-Israel Stewart mechanisms are employed to formulate the corresponding dynamica"},"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":"2401.04917","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2024-01-10T04:01:45Z","cross_cats_sorted":[],"title_canon_sha256":"3ed50bce3d1b4b8dff97185c5c72671127b07bb5aa7f509e2542c08b172f7e13","abstract_canon_sha256":"65b9c2ed7037b13a8205f8e8cab16a7b83897d01610570ce4c83df5a72440d12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:32:00.450538Z","signature_b64":"e3V+BC/Mf12zA4X7SdAzaQ7tSDhHo8BkE73RehZSZ5/5VAr+ZVFCiG9zMBu6E7wHb0vYbSGdUDWwVw8pQ5o9BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd879a30b6f9cbcc79d3fd3a601f002352203f73b992b6b764f51dfa1627f6e0","last_reissued_at":"2026-07-05T07:32:00.450066Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:32:00.450066Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charged Anisotropic Spherical Collapse in $f(\\mathcal{R},\\mathcal{T},\\mathcal{Q})$ Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Sharif, Tayyab Naseer","submitted_at":"2024-01-10T04:01:45Z","abstract_excerpt":"This paper discusses the gravitational collapse of dynamical self-gravitating fluid distribution in $f(\\mathcal{R},\\mathcal{T},\\mathcal{Q})$ gravity, where $\\mathcal{Q}=\\mathcal{R}_{\\varphi\\vartheta}\\mathcal{T}^{\\varphi\\vartheta}$. In this regard, we assume a charged anisotropic spherical geometry involving dissipation flux and adopt standard model of the form $\\mathcal{R}+\\Phi\\sqrt{\\mathcal{T}}+\\Psi\\mathcal{Q}$, where $\\Phi$ and $\\Psi$ symbolize real-valued coupling parameters. The Misner-Sharp as well as M\\\"{u}ler-Israel Stewart mechanisms are employed to formulate the corresponding dynamica"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.04917","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/2401.04917/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":"2401.04917","created_at":"2026-07-05T07:32:00.450127+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.04917v1","created_at":"2026-07-05T07:32:00.450127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.04917","created_at":"2026-07-05T07:32:00.450127+00:00"},{"alias_kind":"pith_short_12","alias_value":"3WDZUMFW7HF4","created_at":"2026-07-05T07:32:00.450127+00:00"},{"alias_kind":"pith_short_16","alias_value":"3WDZUMFW7HF4Y6OT","created_at":"2026-07-05T07:32:00.450127+00:00"},{"alias_kind":"pith_short_8","alias_value":"3WDZUMFW","created_at":"2026-07-05T07:32:00.450127+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/3WDZUMFW7HF4Y6OT7U5GAHYAEN","json":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN.json","graph_json":"https://pith.science/api/pith-number/3WDZUMFW7HF4Y6OT7U5GAHYAEN/graph.json","events_json":"https://pith.science/api/pith-number/3WDZUMFW7HF4Y6OT7U5GAHYAEN/events.json","paper":"https://pith.science/paper/3WDZUMFW"},"agent_actions":{"view_html":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN","download_json":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN.json","view_paper":"https://pith.science/paper/3WDZUMFW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.04917&json=true","fetch_graph":"https://pith.science/api/pith-number/3WDZUMFW7HF4Y6OT7U5GAHYAEN/graph.json","fetch_events":"https://pith.science/api/pith-number/3WDZUMFW7HF4Y6OT7U5GAHYAEN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN/action/storage_attestation","attest_author":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN/action/author_attestation","sign_citation":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN/action/citation_signature","submit_replication":"https://pith.science/pith/3WDZUMFW7HF4Y6OT7U5GAHYAEN/action/replication_record"}},"created_at":"2026-07-05T07:32:00.450127+00:00","updated_at":"2026-07-05T07:32:00.450127+00:00"}