{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:E7ON3FICW6OYBYE2TELR6GVMVN","short_pith_number":"pith:E7ON3FIC","schema_version":"1.0","canonical_sha256":"27dcdd9502b79d80e09a99171f1aacab6492da3246c1ff7248673fbf7502a966","source":{"kind":"arxiv","id":"1707.00979","version":2},"attestation_state":"computed","paper":{"title":"Magnetized strange quark matter in $f(R,T)$ gravity with bilinear and special form of time varying deceleration parameter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Binaya K. Bishi, Parbati Sahoo, P.K. Sahoo, Sezgin Ayg\\\"un","submitted_at":"2017-07-01T07:02:56Z","abstract_excerpt":"In this paper, we have studied homogeneous and anisotropic, locally rotationally symmetric (LRS) Bianchi type-I universe model with magnetized strange quark matter (MSQM) distribution and cosmological constant $\\Lambda$ in $f(R,T)$ gravity. The exact solutions of the field equations are obtained under bilinear and special form of time varying deceleration parameter (DP). Firstly we have considered two specific form of bilinear DP with a single parameter of the form: $q=\\frac{\\alpha(1-t)}{1+t}$ and $q=-\\frac{\\alpha t}{1+t}$, which leads to a function with constant or linear nature with respect "},"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":"1707.00979","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-07-01T07:02:56Z","cross_cats_sorted":[],"title_canon_sha256":"f45bb1942a5375a30464591790e74714db32bd2777c49bd58cc4d2acde1ea619","abstract_canon_sha256":"47a6c3fab9f455ef8929640bfbfd10d54ff30037c5e8268e8e7996ed0eab32a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:19.186342Z","signature_b64":"HrJLsf8y73MLX6KdYbZ8Ie7DlgNR0gEcpzQW6rDuc0Fgwb6WTBGc4rFF0vR9cqWe845C/L51s7fdMU86lnhgAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27dcdd9502b79d80e09a99171f1aacab6492da3246c1ff7248673fbf7502a966","last_reissued_at":"2026-05-18T00:31:19.185588Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:19.185588Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetized strange quark matter in $f(R,T)$ gravity with bilinear and special form of time varying deceleration parameter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Binaya K. Bishi, Parbati Sahoo, P.K. Sahoo, Sezgin Ayg\\\"un","submitted_at":"2017-07-01T07:02:56Z","abstract_excerpt":"In this paper, we have studied homogeneous and anisotropic, locally rotationally symmetric (LRS) Bianchi type-I universe model with magnetized strange quark matter (MSQM) distribution and cosmological constant $\\Lambda$ in $f(R,T)$ gravity. The exact solutions of the field equations are obtained under bilinear and special form of time varying deceleration parameter (DP). Firstly we have considered two specific form of bilinear DP with a single parameter of the form: $q=\\frac{\\alpha(1-t)}{1+t}$ and $q=-\\frac{\\alpha t}{1+t}$, which leads to a function with constant or linear nature with respect "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.00979","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1707.00979","created_at":"2026-05-18T00:31:19.185724+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.00979v2","created_at":"2026-05-18T00:31:19.185724+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.00979","created_at":"2026-05-18T00:31:19.185724+00:00"},{"alias_kind":"pith_short_12","alias_value":"E7ON3FICW6OY","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"E7ON3FICW6OYBYE2","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"E7ON3FIC","created_at":"2026-05-18T12:31:12.930513+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/E7ON3FICW6OYBYE2TELR6GVMVN","json":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN.json","graph_json":"https://pith.science/api/pith-number/E7ON3FICW6OYBYE2TELR6GVMVN/graph.json","events_json":"https://pith.science/api/pith-number/E7ON3FICW6OYBYE2TELR6GVMVN/events.json","paper":"https://pith.science/paper/E7ON3FIC"},"agent_actions":{"view_html":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN","download_json":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN.json","view_paper":"https://pith.science/paper/E7ON3FIC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.00979&json=true","fetch_graph":"https://pith.science/api/pith-number/E7ON3FICW6OYBYE2TELR6GVMVN/graph.json","fetch_events":"https://pith.science/api/pith-number/E7ON3FICW6OYBYE2TELR6GVMVN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN/action/storage_attestation","attest_author":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN/action/author_attestation","sign_citation":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN/action/citation_signature","submit_replication":"https://pith.science/pith/E7ON3FICW6OYBYE2TELR6GVMVN/action/replication_record"}},"created_at":"2026-05-18T00:31:19.185724+00:00","updated_at":"2026-05-18T00:31:19.185724+00:00"}