{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:FVSCCIVPSDF3Y5UQLWLAKCZSHS","short_pith_number":"pith:FVSCCIVP","schema_version":"1.0","canonical_sha256":"2d642122af90cbbc76905d96050b323cbe6f0c3e815d4de8e8a41666df512174","source":{"kind":"arxiv","id":"1110.3136","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamic potentials from shifted boundary conditions: the scalar-field theory case","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Harvey B. Meyer, Leonardo Giusti","submitted_at":"2011-10-14T07:59:07Z","abstract_excerpt":"In a thermal field theory, the cumulants of the momentum distribution can be extracted from the dependence of the Euclidean path integral on a shift in the fields built into the temporal boundary condition. When combined with the Ward identities associated with the invariance of the theory under the Poincare' group, thermodynamic potentials such as the entropy or the pressure can be directly inferred from the response of the system to the shift. Crucially the argument holds, up to harmless finite-size and discretization effects, even if translational and rotational invariance are broken to a d"},"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":"1110.3136","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2011-10-14T07:59:07Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"84ec3504f9826033ade7d2ac4f800c48116143ec546d188c37b4313ce6d16107","abstract_canon_sha256":"a285827453249e929742c4843fb8db033347473b876439418bcf13f56919f664"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:12.440811Z","signature_b64":"tl7ez0sITUJzoUh4TuXUf0wt4CWqThDzTXZx/iR0uAbdfCdi8IXQCk6HQlPkMQ/WUzlwlDg613sxbVTuapVfCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d642122af90cbbc76905d96050b323cbe6f0c3e815d4de8e8a41666df512174","last_reissued_at":"2026-05-18T02:00:12.440251Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:12.440251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamic potentials from shifted boundary conditions: the scalar-field theory case","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Harvey B. Meyer, Leonardo Giusti","submitted_at":"2011-10-14T07:59:07Z","abstract_excerpt":"In a thermal field theory, the cumulants of the momentum distribution can be extracted from the dependence of the Euclidean path integral on a shift in the fields built into the temporal boundary condition. When combined with the Ward identities associated with the invariance of the theory under the Poincare' group, thermodynamic potentials such as the entropy or the pressure can be directly inferred from the response of the system to the shift. Crucially the argument holds, up to harmless finite-size and discretization effects, even if translational and rotational invariance are broken to a d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.3136","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":"1110.3136","created_at":"2026-05-18T02:00:12.440327+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.3136v1","created_at":"2026-05-18T02:00:12.440327+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.3136","created_at":"2026-05-18T02:00:12.440327+00:00"},{"alias_kind":"pith_short_12","alias_value":"FVSCCIVPSDF3","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_16","alias_value":"FVSCCIVPSDF3Y5UQ","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_8","alias_value":"FVSCCIVP","created_at":"2026-05-18T12:26:28.662955+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/FVSCCIVPSDF3Y5UQLWLAKCZSHS","json":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS.json","graph_json":"https://pith.science/api/pith-number/FVSCCIVPSDF3Y5UQLWLAKCZSHS/graph.json","events_json":"https://pith.science/api/pith-number/FVSCCIVPSDF3Y5UQLWLAKCZSHS/events.json","paper":"https://pith.science/paper/FVSCCIVP"},"agent_actions":{"view_html":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS","download_json":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS.json","view_paper":"https://pith.science/paper/FVSCCIVP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.3136&json=true","fetch_graph":"https://pith.science/api/pith-number/FVSCCIVPSDF3Y5UQLWLAKCZSHS/graph.json","fetch_events":"https://pith.science/api/pith-number/FVSCCIVPSDF3Y5UQLWLAKCZSHS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS/action/storage_attestation","attest_author":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS/action/author_attestation","sign_citation":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS/action/citation_signature","submit_replication":"https://pith.science/pith/FVSCCIVPSDF3Y5UQLWLAKCZSHS/action/replication_record"}},"created_at":"2026-05-18T02:00:12.440327+00:00","updated_at":"2026-05-18T02:00:12.440327+00:00"}