{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:T2LX2ZSLGIETCCUG2KCR3TZ7EJ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"281297e7cce2413f4207ec8ea95fdfaacd6f16cfc2d49acbd453587f538636de","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2021-05-15T23:28:12Z","title_canon_sha256":"c071e48e829e0fb217c7fc582c39cfcbe6809edababff752015834c0e6f19c95"},"schema_version":"1.0","source":{"id":"2105.07313","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2105.07313","created_at":"2026-07-05T03:43:02Z"},{"alias_kind":"arxiv_version","alias_value":"2105.07313v4","created_at":"2026-07-05T03:43:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2105.07313","created_at":"2026-07-05T03:43:02Z"},{"alias_kind":"pith_short_12","alias_value":"T2LX2ZSLGIET","created_at":"2026-07-05T03:43:02Z"},{"alias_kind":"pith_short_16","alias_value":"T2LX2ZSLGIETCCUG","created_at":"2026-07-05T03:43:02Z"},{"alias_kind":"pith_short_8","alias_value":"T2LX2ZSL","created_at":"2026-07-05T03:43:02Z"}],"graph_snapshots":[{"event_id":"sha256:b2547c50dedbb1e2384e5c18d139fe7daba30d148b301cd2b40d657270d8f161","target":"graph","created_at":"2026-07-05T03:43:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2105.07313/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The relativistic transformation rule for temperature is a subject under debate for more than 110 years. Several incompatible proposals exist in the literature, but a final resolution is still missing. In this work, we reconsider the problem of relativistic transformation rules for a number of thermodynamic parameters, including temperature, chemical potential, pressure, entropy and enthalpy densities for a relativistic perfect fluid using relativistic kinetic theory. The analysis is carried out in a fully relativistic covariant manner, and the explicit transformation rules for the above quanti","authors_text":"Liu Zhao, Shaofan Liu, Xin Hao","cross_cats":["cond-mat.stat-mech","hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2021-05-15T23:28:12Z","title":"Relativistic transformation of thermodynamic parameters and refined Saha equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2105.07313","kind":"arxiv","version":4},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2a2f7ce54c1ab5c42d426f7e4a59d53ca278a1b0a41c85bedd10ea78575fdc85","target":"record","created_at":"2026-07-05T03:43:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"281297e7cce2413f4207ec8ea95fdfaacd6f16cfc2d49acbd453587f538636de","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2021-05-15T23:28:12Z","title_canon_sha256":"c071e48e829e0fb217c7fc582c39cfcbe6809edababff752015834c0e6f19c95"},"schema_version":"1.0","source":{"id":"2105.07313","kind":"arxiv","version":4}},"canonical_sha256":"9e977d664b3209310a86d2851dcf3f227709b64ba609757092472b2dabbca893","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e977d664b3209310a86d2851dcf3f227709b64ba609757092472b2dabbca893","first_computed_at":"2026-07-05T03:43:02.301385Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:43:02.301385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"r/3hEoun5LBRQvKzPfGqpfQWhR5T44tfdc7s1T8Oqvd0Yv/ORi1WyWoxdnQXEjjXLTFNUG0hGkDNuezNu+nyCA==","signature_status":"signed_v1","signed_at":"2026-07-05T03:43:02.301952Z","signed_message":"canonical_sha256_bytes"},"source_id":"2105.07313","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2a2f7ce54c1ab5c42d426f7e4a59d53ca278a1b0a41c85bedd10ea78575fdc85","sha256:b2547c50dedbb1e2384e5c18d139fe7daba30d148b301cd2b40d657270d8f161"],"state_sha256":"cecc4e4fed200307dcfd56d13af079b8bc2e3f78119c6bac24da8eb038b12bbb"}