{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:BLHBMSWM5TYMX6BQYHBOSHXIWG","short_pith_number":"pith:BLHBMSWM","schema_version":"1.0","canonical_sha256":"0ace164accecf0cbf830c1c2e91ee8b1b97ef74386fcdeb1c20fec6fa1bb8244","source":{"kind":"arxiv","id":"2011.14907","version":4},"attestation_state":"computed","paper":{"title":"Spin polarization dynamics in the Gubser-expanding background","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Gabriel Sophys, Radoslaw Ryblewski, Rajeev Singh","submitted_at":"2020-11-26T23:27:22Z","abstract_excerpt":"Evolution of spin polarization in the Gubser-expanding conformal perfect-fluid hydrodynamic background is studied. The analysis of the conformal transformation properties of the conservation laws is extended to the case of the angular momentum conservation. The explicit forms of equations of motion for spin components are derived and analysed, and some special solutions are found."},"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":"2011.14907","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2020-11-26T23:27:22Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"43516ee9f37da1d92d9d46a7a917424f7c06d9c0e5fec58dd23c423bae2cea89","abstract_canon_sha256":"c0abf4c8e4fcab5bc950b2ba78353fdc5a8612887ad87a35135ed8801bed335b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:37:32.295702Z","signature_b64":"ll91OIDfj4/Ui394b43jhw/lKhOgIFaalWAJJa2ZMzbG9zcxweoOQCnGW9oTGQ7D79KjUdTz9rRpqK3pydihCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ace164accecf0cbf830c1c2e91ee8b1b97ef74386fcdeb1c20fec6fa1bb8244","last_reissued_at":"2026-07-05T02:37:32.295293Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:37:32.295293Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin polarization dynamics in the Gubser-expanding background","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Gabriel Sophys, Radoslaw Ryblewski, Rajeev Singh","submitted_at":"2020-11-26T23:27:22Z","abstract_excerpt":"Evolution of spin polarization in the Gubser-expanding conformal perfect-fluid hydrodynamic background is studied. The analysis of the conformal transformation properties of the conservation laws is extended to the case of the angular momentum conservation. The explicit forms of equations of motion for spin components are derived and analysed, and some special solutions are found."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.14907","kind":"arxiv","version":4},"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/2011.14907/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":"2011.14907","created_at":"2026-07-05T02:37:32.295366+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.14907v4","created_at":"2026-07-05T02:37:32.295366+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.14907","created_at":"2026-07-05T02:37:32.295366+00:00"},{"alias_kind":"pith_short_12","alias_value":"BLHBMSWM5TYM","created_at":"2026-07-05T02:37:32.295366+00:00"},{"alias_kind":"pith_short_16","alias_value":"BLHBMSWM5TYMX6BQ","created_at":"2026-07-05T02:37:32.295366+00:00"},{"alias_kind":"pith_short_8","alias_value":"BLHBMSWM","created_at":"2026-07-05T02:37:32.295366+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.08219","citing_title":"Modeling $\\Lambda$ polarization in Au$+$Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV using relativistic spin hydrodynamics","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2601.15023","citing_title":"Carroll hydrodynamics with spin","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2605.12554","citing_title":"Spin dynamics and polarization in relativistic systems: recent developments","ref_index":45,"is_internal_anchor":false},{"citing_arxiv_id":"2605.08219","citing_title":"Modeling $\\Lambda$ polarization in Au$+$Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV using relativistic spin hydrodynamics","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01857","citing_title":"Boost-invariant and cylindrically symmetric perfect spin hydrodynamics","ref_index":84,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15926","citing_title":"Exact expectation values in a boost-invariant fluid of Dirac fermions with finite spin density","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG","json":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG.json","graph_json":"https://pith.science/api/pith-number/BLHBMSWM5TYMX6BQYHBOSHXIWG/graph.json","events_json":"https://pith.science/api/pith-number/BLHBMSWM5TYMX6BQYHBOSHXIWG/events.json","paper":"https://pith.science/paper/BLHBMSWM"},"agent_actions":{"view_html":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG","download_json":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG.json","view_paper":"https://pith.science/paper/BLHBMSWM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.14907&json=true","fetch_graph":"https://pith.science/api/pith-number/BLHBMSWM5TYMX6BQYHBOSHXIWG/graph.json","fetch_events":"https://pith.science/api/pith-number/BLHBMSWM5TYMX6BQYHBOSHXIWG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG/action/storage_attestation","attest_author":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG/action/author_attestation","sign_citation":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG/action/citation_signature","submit_replication":"https://pith.science/pith/BLHBMSWM5TYMX6BQYHBOSHXIWG/action/replication_record"}},"created_at":"2026-07-05T02:37:32.295366+00:00","updated_at":"2026-07-05T02:37:32.295366+00:00"}