{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LBAVFP3MXT5CGLF6W3NBP4R56B","short_pith_number":"pith:LBAVFP3M","schema_version":"1.0","canonical_sha256":"584152bf6cbcfa232cbeb6da17f23df07f5a5c54a79b944a2d9e9caf0b81b6f7","source":{"kind":"arxiv","id":"1404.0205","version":1},"attestation_state":"computed","paper":{"title":"One antimatter --- two possible thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A.Y. Klimenko, U. Maas","submitted_at":"2014-04-01T11:44:06Z","abstract_excerpt":"Conventional thermodynamics, which is formulated for our world populated by radiation and matter, can be extended to describe physical properties of antimatter in two mutually exclusive ways: CP-invariant or CPT-invariant. Here we refer to invariance of physical laws under charge (C), parity (P) and time reversal (T) transformations. While in quantum field theory CPT invariance is a theorem confirmed by experiments, the symmetry principles applied to macroscopic phenomena or to the whole of the Universe represent only hypotheses. Since both versions of thermodynamics are different only in thei"},"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":"1404.0205","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-04-01T11:44:06Z","cross_cats_sorted":[],"title_canon_sha256":"cd8b09a7d74e46fc8cf17c276b591ae1f3953f3132bf83b35c6fe8fd88409f41","abstract_canon_sha256":"2e41a6e021690e84c76a83eab92cd5deac62760ba76dc486cc274a677853fb1c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:04.870921Z","signature_b64":"V9mYKzHAicYaZ2Y4e/TwWJjHPIyMu05s87/z+VaKpIvLRNdMqwMehUnVkQ4Vm2OxblS5AG+nItSb5dOp/WN0CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"584152bf6cbcfa232cbeb6da17f23df07f5a5c54a79b944a2d9e9caf0b81b6f7","last_reissued_at":"2026-05-18T02:55:04.870278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:04.870278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One antimatter --- two possible thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A.Y. Klimenko, U. Maas","submitted_at":"2014-04-01T11:44:06Z","abstract_excerpt":"Conventional thermodynamics, which is formulated for our world populated by radiation and matter, can be extended to describe physical properties of antimatter in two mutually exclusive ways: CP-invariant or CPT-invariant. Here we refer to invariance of physical laws under charge (C), parity (P) and time reversal (T) transformations. While in quantum field theory CPT invariance is a theorem confirmed by experiments, the symmetry principles applied to macroscopic phenomena or to the whole of the Universe represent only hypotheses. Since both versions of thermodynamics are different only in thei"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.0205","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":"1404.0205","created_at":"2026-05-18T02:55:04.870385+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.0205v1","created_at":"2026-05-18T02:55:04.870385+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.0205","created_at":"2026-05-18T02:55:04.870385+00:00"},{"alias_kind":"pith_short_12","alias_value":"LBAVFP3MXT5C","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_16","alias_value":"LBAVFP3MXT5CGLF6","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_8","alias_value":"LBAVFP3M","created_at":"2026-05-18T12:28:35.611951+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.13922","citing_title":"Decoherence, Perturbations and Symmetry in Lindblad Dynamics -- Implications for Diffractive Dissociation","ref_index":55,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B","json":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B.json","graph_json":"https://pith.science/api/pith-number/LBAVFP3MXT5CGLF6W3NBP4R56B/graph.json","events_json":"https://pith.science/api/pith-number/LBAVFP3MXT5CGLF6W3NBP4R56B/events.json","paper":"https://pith.science/paper/LBAVFP3M"},"agent_actions":{"view_html":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B","download_json":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B.json","view_paper":"https://pith.science/paper/LBAVFP3M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.0205&json=true","fetch_graph":"https://pith.science/api/pith-number/LBAVFP3MXT5CGLF6W3NBP4R56B/graph.json","fetch_events":"https://pith.science/api/pith-number/LBAVFP3MXT5CGLF6W3NBP4R56B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B/action/storage_attestation","attest_author":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B/action/author_attestation","sign_citation":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B/action/citation_signature","submit_replication":"https://pith.science/pith/LBAVFP3MXT5CGLF6W3NBP4R56B/action/replication_record"}},"created_at":"2026-05-18T02:55:04.870385+00:00","updated_at":"2026-05-18T02:55:04.870385+00:00"}