{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:444BUXZMDWWXLDAOET5QGROGY3","short_pith_number":"pith:444BUXZM","schema_version":"1.0","canonical_sha256":"e7381a5f2c1dad758c0e24fb0345c6c6c9453425824bc984cdfb9e92f60208dd","source":{"kind":"arxiv","id":"1510.00454","version":1},"attestation_state":"computed","paper":{"title":"Massive Yang-Mills for Vector and Axial-Vector Spectral Functions at Finite Temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Paul M. Hohler, Ralf Rapp","submitted_at":"2015-10-02T00:16:41Z","abstract_excerpt":"The hadronic mechanism which leads to chiral symmetry restoration is explored in the context of the rho-pi-a_1 system using Massive Yang-Mills, a hadronic effective theory which governs their microscopic interactions. In this approach, vector and axial-vector mesons are implemented as gauge bosons of a local chiral gauge group. We have previously shown that this model can describe the experimentally measured vector and axial-vector spectral functions in vacuum. Here, we carry the analysis to finite temperatures by evaluating medium effects in a pion gas and calculating thermal spectral functio"},"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":"1510.00454","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-10-02T00:16:41Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"9f24d0016535031db47b5fb78aae195539e4a5b40d3b085dfe27e9de1faedb31","abstract_canon_sha256":"3409a1e37d4b94a668c44af2265972376c15ffdf1836622a5afaf39a1c9b006e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:48.324058Z","signature_b64":"9ZMAs4nsRUOycVnfGafeOxrz70r48LyLtiuQaM9KZcYfySn8/p5S22j4vCb0kfxk7c29bbMSrHvV41FIKh4lBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7381a5f2c1dad758c0e24fb0345c6c6c9453425824bc984cdfb9e92f60208dd","last_reissued_at":"2026-05-18T01:16:48.323452Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:48.323452Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Massive Yang-Mills for Vector and Axial-Vector Spectral Functions at Finite Temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Paul M. Hohler, Ralf Rapp","submitted_at":"2015-10-02T00:16:41Z","abstract_excerpt":"The hadronic mechanism which leads to chiral symmetry restoration is explored in the context of the rho-pi-a_1 system using Massive Yang-Mills, a hadronic effective theory which governs their microscopic interactions. In this approach, vector and axial-vector mesons are implemented as gauge bosons of a local chiral gauge group. We have previously shown that this model can describe the experimentally measured vector and axial-vector spectral functions in vacuum. Here, we carry the analysis to finite temperatures by evaluating medium effects in a pion gas and calculating thermal spectral functio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.00454","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":""},"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":"1510.00454","created_at":"2026-05-18T01:16:48.323534+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.00454v1","created_at":"2026-05-18T01:16:48.323534+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.00454","created_at":"2026-05-18T01:16:48.323534+00:00"},{"alias_kind":"pith_short_12","alias_value":"444BUXZMDWWX","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"444BUXZMDWWXLDAO","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"444BUXZM","created_at":"2026-05-18T12:29:02.477457+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/444BUXZMDWWXLDAOET5QGROGY3","json":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3.json","graph_json":"https://pith.science/api/pith-number/444BUXZMDWWXLDAOET5QGROGY3/graph.json","events_json":"https://pith.science/api/pith-number/444BUXZMDWWXLDAOET5QGROGY3/events.json","paper":"https://pith.science/paper/444BUXZM"},"agent_actions":{"view_html":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3","download_json":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3.json","view_paper":"https://pith.science/paper/444BUXZM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.00454&json=true","fetch_graph":"https://pith.science/api/pith-number/444BUXZMDWWXLDAOET5QGROGY3/graph.json","fetch_events":"https://pith.science/api/pith-number/444BUXZMDWWXLDAOET5QGROGY3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3/action/storage_attestation","attest_author":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3/action/author_attestation","sign_citation":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3/action/citation_signature","submit_replication":"https://pith.science/pith/444BUXZMDWWXLDAOET5QGROGY3/action/replication_record"}},"created_at":"2026-05-18T01:16:48.323534+00:00","updated_at":"2026-05-18T01:16:48.323534+00:00"}