{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:OCVWPGVBZAIHAIS3VCJBTZLECR","short_pith_number":"pith:OCVWPGVB","schema_version":"1.0","canonical_sha256":"70ab679aa1c81070225ba89219e564146fbfbc13a23d0afeee6472845cf8f34b","source":{"kind":"arxiv","id":"1505.07760","version":2},"attestation_state":"computed","paper":{"title":"Quantum corrections to the stress-energy tensor in thermodynamic equilibrium with acceleration","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"gr-qc","authors_text":"E. Grossi (University of Florence, F. Becattini, Italy)","submitted_at":"2015-05-28T17:14:22Z","abstract_excerpt":"We show that the stress-energy tensor has additional terms with respect to the ideal form in states of global thermodynamic equilibrium in flat spacetime with non-vanishing acceleration and vorticity. These corrections are of quantum origin and their leading terms are second order in the gradients of the thermodynamic fields. Their relevant coefficients can be expressed in terms of correlators of the stress-energy tensor operator and the generators of the Lorentz group. With respect to previous assessments, we find that there are more second order coefficients and that all thermodynamic functi"},"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":"1505.07760","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-05-28T17:14:22Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"e4ddc159cc68da4b70a7b7bea98506185191986dcd908db8a830a42d2388d63e","abstract_canon_sha256":"95a378bc3711540f3b86bc15c585023691aaef7ee107cff541d5a5bcee18d7dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:16.545849Z","signature_b64":"aeq+41zitYqwbjUr1sA9hM9Eh58EK6a3eoB7z5Q05k9B6FGj7gAf0fgIo42CT2ohtE1yNDOSttZJgn5OeMaWCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"70ab679aa1c81070225ba89219e564146fbfbc13a23d0afeee6472845cf8f34b","last_reissued_at":"2026-05-18T01:34:16.545064Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:16.545064Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum corrections to the stress-energy tensor in thermodynamic equilibrium with acceleration","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"gr-qc","authors_text":"E. Grossi (University of Florence, F. Becattini, Italy)","submitted_at":"2015-05-28T17:14:22Z","abstract_excerpt":"We show that the stress-energy tensor has additional terms with respect to the ideal form in states of global thermodynamic equilibrium in flat spacetime with non-vanishing acceleration and vorticity. These corrections are of quantum origin and their leading terms are second order in the gradients of the thermodynamic fields. Their relevant coefficients can be expressed in terms of correlators of the stress-energy tensor operator and the generators of the Lorentz group. With respect to previous assessments, we find that there are more second order coefficients and that all thermodynamic functi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.07760","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":"1505.07760","created_at":"2026-05-18T01:34:16.545195+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.07760v2","created_at":"2026-05-18T01:34:16.545195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.07760","created_at":"2026-05-18T01:34:16.545195+00:00"},{"alias_kind":"pith_short_12","alias_value":"OCVWPGVBZAIH","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_16","alias_value":"OCVWPGVBZAIHAIS3","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_8","alias_value":"OCVWPGVB","created_at":"2026-05-18T12:29:34.919912+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2503.17291","citing_title":"Linear sigma model with quarks and Polyakov loop in rotation: phase diagrams, Tolman-Ehrenfest law and mechanical properties","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"2602.20970","citing_title":"Spatial confinement-deconfinement transition in accelerated gluodynamics within lattice simulation","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR","json":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR.json","graph_json":"https://pith.science/api/pith-number/OCVWPGVBZAIHAIS3VCJBTZLECR/graph.json","events_json":"https://pith.science/api/pith-number/OCVWPGVBZAIHAIS3VCJBTZLECR/events.json","paper":"https://pith.science/paper/OCVWPGVB"},"agent_actions":{"view_html":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR","download_json":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR.json","view_paper":"https://pith.science/paper/OCVWPGVB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.07760&json=true","fetch_graph":"https://pith.science/api/pith-number/OCVWPGVBZAIHAIS3VCJBTZLECR/graph.json","fetch_events":"https://pith.science/api/pith-number/OCVWPGVBZAIHAIS3VCJBTZLECR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR/action/storage_attestation","attest_author":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR/action/author_attestation","sign_citation":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR/action/citation_signature","submit_replication":"https://pith.science/pith/OCVWPGVBZAIHAIS3VCJBTZLECR/action/replication_record"}},"created_at":"2026-05-18T01:34:16.545195+00:00","updated_at":"2026-05-18T01:34:16.545195+00:00"}