{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:7GXXZFVNTHFGBV2IOFF72IHFZC","short_pith_number":"pith:7GXXZFVN","canonical_record":{"source":{"id":"1507.07874","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-28T17:54:39Z","cross_cats_sorted":[],"title_canon_sha256":"538694961f72ff274d53d442b7de56a4fd68903caf1d1aaec0978e7b9d17cc06","abstract_canon_sha256":"7a7c81ded6de862e73154ef757b3d443a149a4819e42fd00600bca74c3aa0054"},"schema_version":"1.0"},"canonical_sha256":"f9af7c96ad99ca60d748714bfd20e5c88fa7b798bced8c2d990ce7c561ff1167","source":{"kind":"arxiv","id":"1507.07874","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.07874","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"arxiv_version","alias_value":"1507.07874v1","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.07874","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"pith_short_12","alias_value":"7GXXZFVNTHFG","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"7GXXZFVNTHFGBV2I","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"7GXXZFVN","created_at":"2026-05-18T12:29:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:7GXXZFVNTHFGBV2IOFF72IHFZC","target":"record","payload":{"canonical_record":{"source":{"id":"1507.07874","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-28T17:54:39Z","cross_cats_sorted":[],"title_canon_sha256":"538694961f72ff274d53d442b7de56a4fd68903caf1d1aaec0978e7b9d17cc06","abstract_canon_sha256":"7a7c81ded6de862e73154ef757b3d443a149a4819e42fd00600bca74c3aa0054"},"schema_version":"1.0"},"canonical_sha256":"f9af7c96ad99ca60d748714bfd20e5c88fa7b798bced8c2d990ce7c561ff1167","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:36:11.695142Z","signature_b64":"AhS1UKcnfV0y9voe7qFSjsT8TLqkMfUYTrsJERSejyLD84tqTqA4oMjVAias8eMv651C+2dW8upZZULGtf22DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9af7c96ad99ca60d748714bfd20e5c88fa7b798bced8c2d990ce7c561ff1167","last_reissued_at":"2026-05-18T01:36:11.694408Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:36:11.694408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1507.07874","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:36:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/Jk/C615d7nu511k83RwwuCC2Ne10CFGjBaOAWFTOUpwDWM5Q7KXgZS9xCXNYhxh8iEf1p4pjr7oRnJ7boB2DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:16:53.459945Z"},"content_sha256":"a7690e54773f5b37b6dbdae931667f65e093b3aa53b5b9dab6ec5d4a246226ed","schema_version":"1.0","event_id":"sha256:a7690e54773f5b37b6dbdae931667f65e093b3aa53b5b9dab6ec5d4a246226ed"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:7GXXZFVNTHFGBV2IOFF72IHFZC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Degenerate limit thermodynamics beyond leading order for models of dense matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Brian Muccioli, Constantinos Constantinou, James M. Lattimer, Madappa Prakash","submitted_at":"2015-07-28T17:54:39Z","abstract_excerpt":"Analytical formulas for next-to-leading order temperature corrections to the thermal state variables of interacting nucleons in bulk matter are derived in the degenerate limit. The formalism developed is applicable to a wide class of non-relativistic and relativistic models of hot and dense matter currently used in nuclear physics and astrophysics (supernovae, proto-neutron stars and neutron star mergers) as well as in condensed matter physics. We consider the general case of arbitrary dimensionality of momentum space and an arbitrary degree of relativity (for relativistic mean-field theoretic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.07874","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:36:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gf5q5QJlfk3fJXvXtFBWYHhO3Gosu2uVJGSqBbdBot+xJpQuWZIYt/DfEbyAZasMaiedvjjSXQSMDyVGPZ/4Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:16:53.460286Z"},"content_sha256":"4fd6da5a3f06222b51b57c2b56cbe3d01cb7711c8ba5ce5e088a642ad9a0093d","schema_version":"1.0","event_id":"sha256:4fd6da5a3f06222b51b57c2b56cbe3d01cb7711c8ba5ce5e088a642ad9a0093d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/bundle.json","state_url":"https://pith.science/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T21:16:53Z","links":{"resolver":"https://pith.science/pith/7GXXZFVNTHFGBV2IOFF72IHFZC","bundle":"https://pith.science/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/bundle.json","state":"https://pith.science/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7GXXZFVNTHFGBV2IOFF72IHFZC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:7GXXZFVNTHFGBV2IOFF72IHFZC","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":"7a7c81ded6de862e73154ef757b3d443a149a4819e42fd00600bca74c3aa0054","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-28T17:54:39Z","title_canon_sha256":"538694961f72ff274d53d442b7de56a4fd68903caf1d1aaec0978e7b9d17cc06"},"schema_version":"1.0","source":{"id":"1507.07874","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.07874","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"arxiv_version","alias_value":"1507.07874v1","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.07874","created_at":"2026-05-18T01:36:11Z"},{"alias_kind":"pith_short_12","alias_value":"7GXXZFVNTHFG","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"7GXXZFVNTHFGBV2I","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"7GXXZFVN","created_at":"2026-05-18T12:29:10Z"}],"graph_snapshots":[{"event_id":"sha256:4fd6da5a3f06222b51b57c2b56cbe3d01cb7711c8ba5ce5e088a642ad9a0093d","target":"graph","created_at":"2026-05-18T01:36:11Z","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"},"paper":{"abstract_excerpt":"Analytical formulas for next-to-leading order temperature corrections to the thermal state variables of interacting nucleons in bulk matter are derived in the degenerate limit. The formalism developed is applicable to a wide class of non-relativistic and relativistic models of hot and dense matter currently used in nuclear physics and astrophysics (supernovae, proto-neutron stars and neutron star mergers) as well as in condensed matter physics. We consider the general case of arbitrary dimensionality of momentum space and an arbitrary degree of relativity (for relativistic mean-field theoretic","authors_text":"Brian Muccioli, Constantinos Constantinou, James M. Lattimer, Madappa Prakash","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-28T17:54:39Z","title":"Degenerate limit thermodynamics beyond leading order for models of dense matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.07874","kind":"arxiv","version":1},"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:a7690e54773f5b37b6dbdae931667f65e093b3aa53b5b9dab6ec5d4a246226ed","target":"record","created_at":"2026-05-18T01:36:11Z","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":"7a7c81ded6de862e73154ef757b3d443a149a4819e42fd00600bca74c3aa0054","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-07-28T17:54:39Z","title_canon_sha256":"538694961f72ff274d53d442b7de56a4fd68903caf1d1aaec0978e7b9d17cc06"},"schema_version":"1.0","source":{"id":"1507.07874","kind":"arxiv","version":1}},"canonical_sha256":"f9af7c96ad99ca60d748714bfd20e5c88fa7b798bced8c2d990ce7c561ff1167","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f9af7c96ad99ca60d748714bfd20e5c88fa7b798bced8c2d990ce7c561ff1167","first_computed_at":"2026-05-18T01:36:11.694408Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:36:11.694408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AhS1UKcnfV0y9voe7qFSjsT8TLqkMfUYTrsJERSejyLD84tqTqA4oMjVAias8eMv651C+2dW8upZZULGtf22DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:36:11.695142Z","signed_message":"canonical_sha256_bytes"},"source_id":"1507.07874","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a7690e54773f5b37b6dbdae931667f65e093b3aa53b5b9dab6ec5d4a246226ed","sha256:4fd6da5a3f06222b51b57c2b56cbe3d01cb7711c8ba5ce5e088a642ad9a0093d"],"state_sha256":"9ff67dbf77c37227dc416578f9ffd70b70a197dbea1781c82b56834c3ee89986"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZFpl3VCcUDX1tlSL+ztzcR54O5edq0ZA1VGVvR5gjPBCgN8lj2BiZ+fxcRUUmvkE6g0ZVyoOJpQ0XQ2tmYEiAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T21:16:53.462100Z","bundle_sha256":"92879f846aaeabf1af3fedc9d88a89de120fdbb72c60c9d754e01c57d74ca1e0"}}