{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:5JQD5Z5SFNNB444TNC7LQWBQJK","short_pith_number":"pith:5JQD5Z5S","schema_version":"1.0","canonical_sha256":"ea603ee7b22b5a1e739368beb858304a971f326dd582c7d9dda8f5dea56a5ce8","source":{"kind":"arxiv","id":"2209.03414","version":2},"attestation_state":"computed","paper":{"title":"Dynamical systems analysis in $f(T,\\phi)$ gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"B. Mishra, Jackson Levi Said, L.K. Duchaniya, S.A. Kadam","submitted_at":"2022-09-03T04:47:42Z","abstract_excerpt":"Teleparallel based cosmological models provide a description of gravity in which torsion is the mediator of gravitation. Several extensions have been made within the so-called Teleparallel equivalent of general relativity which is equivalent to general relativity at the level of the equations of motion where attempts are made to study the extensions of this form of gravity and to describe more general functions of the torsion scalar $T$. One of these extensions is $f(T,\\phi)$ gravity; $T$ and $\\phi$ respectively denote the torsion scalar and scalar field. In this work, the dynamical system ana"},"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":"2209.03414","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2022-09-03T04:47:42Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b580ecb96640c9fb571267224bb71e6f80830a710fb2771cea62d117cdebd4c4","abstract_canon_sha256":"59417098ec3e53a45dad64e2d079e93dc200325af5d8a8a6a94733d136ba3b30"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:33:17.633134Z","signature_b64":"fLmOjNQJelCyDfOZfDZ7CiItGjlMCh4/CA6RIYxc7hr2qsSZbIJ1mlOfdRJJiUsTCS9CgWh2Bnhm+9bigEM7Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea603ee7b22b5a1e739368beb858304a971f326dd582c7d9dda8f5dea56a5ce8","last_reissued_at":"2026-07-05T05:33:17.632654Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:33:17.632654Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical systems analysis in $f(T,\\phi)$ gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"B. Mishra, Jackson Levi Said, L.K. Duchaniya, S.A. Kadam","submitted_at":"2022-09-03T04:47:42Z","abstract_excerpt":"Teleparallel based cosmological models provide a description of gravity in which torsion is the mediator of gravitation. Several extensions have been made within the so-called Teleparallel equivalent of general relativity which is equivalent to general relativity at the level of the equations of motion where attempts are made to study the extensions of this form of gravity and to describe more general functions of the torsion scalar $T$. One of these extensions is $f(T,\\phi)$ gravity; $T$ and $\\phi$ respectively denote the torsion scalar and scalar field. In this work, the dynamical system ana"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.03414","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.03414/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":"2209.03414","created_at":"2026-07-05T05:33:17.632712+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.03414v2","created_at":"2026-07-05T05:33:17.632712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.03414","created_at":"2026-07-05T05:33:17.632712+00:00"},{"alias_kind":"pith_short_12","alias_value":"5JQD5Z5SFNNB","created_at":"2026-07-05T05:33:17.632712+00:00"},{"alias_kind":"pith_short_16","alias_value":"5JQD5Z5SFNNB444T","created_at":"2026-07-05T05:33:17.632712+00:00"},{"alias_kind":"pith_short_8","alias_value":"5JQD5Z5S","created_at":"2026-07-05T05:33:17.632712+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.11923","citing_title":"Late Time Phenomena in $f(T,\\mathcal{T})$ Gravity Framework: Role of $H_0$ Priors","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK","json":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK.json","graph_json":"https://pith.science/api/pith-number/5JQD5Z5SFNNB444TNC7LQWBQJK/graph.json","events_json":"https://pith.science/api/pith-number/5JQD5Z5SFNNB444TNC7LQWBQJK/events.json","paper":"https://pith.science/paper/5JQD5Z5S"},"agent_actions":{"view_html":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK","download_json":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK.json","view_paper":"https://pith.science/paper/5JQD5Z5S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.03414&json=true","fetch_graph":"https://pith.science/api/pith-number/5JQD5Z5SFNNB444TNC7LQWBQJK/graph.json","fetch_events":"https://pith.science/api/pith-number/5JQD5Z5SFNNB444TNC7LQWBQJK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK/action/storage_attestation","attest_author":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK/action/author_attestation","sign_citation":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK/action/citation_signature","submit_replication":"https://pith.science/pith/5JQD5Z5SFNNB444TNC7LQWBQJK/action/replication_record"}},"created_at":"2026-07-05T05:33:17.632712+00:00","updated_at":"2026-07-05T05:33:17.632712+00:00"}