{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:XVM2PUJJ335MEZVALB46F2GKQL","short_pith_number":"pith:XVM2PUJJ","canonical_record":{"source":{"id":"2306.01351","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-02T08:24:15Z","cross_cats_sorted":[],"title_canon_sha256":"65c492dd16dc5a07261cd6908468f43d55434a64b70873f07a71061e010e96e2","abstract_canon_sha256":"7d730d0134e6cb4e2bd8764096e29ee8b90b51419f4812fc69fcbc4f6916417a"},"schema_version":"1.0"},"canonical_sha256":"bd59a7d129defac266a05879e2e8ca82dbcd77bcf3f77bd2e079cd02a1e67ec1","source":{"kind":"arxiv","id":"2306.01351","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.01351","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"arxiv_version","alias_value":"2306.01351v1","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.01351","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_12","alias_value":"XVM2PUJJ335M","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_16","alias_value":"XVM2PUJJ335MEZVA","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_8","alias_value":"XVM2PUJJ","created_at":"2026-07-05T06:16:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:XVM2PUJJ335MEZVALB46F2GKQL","target":"record","payload":{"canonical_record":{"source":{"id":"2306.01351","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-02T08:24:15Z","cross_cats_sorted":[],"title_canon_sha256":"65c492dd16dc5a07261cd6908468f43d55434a64b70873f07a71061e010e96e2","abstract_canon_sha256":"7d730d0134e6cb4e2bd8764096e29ee8b90b51419f4812fc69fcbc4f6916417a"},"schema_version":"1.0"},"canonical_sha256":"bd59a7d129defac266a05879e2e8ca82dbcd77bcf3f77bd2e079cd02a1e67ec1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:16:52.921903Z","signature_b64":"jCyhb+WWx2JzahYxTdNyg31/32gsk6V296qtnQtxHq1JrvB4K/yRjmf1oMPECqx3U6jP6LNovExkX3VUxfdmDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd59a7d129defac266a05879e2e8ca82dbcd77bcf3f77bd2e079cd02a1e67ec1","last_reissued_at":"2026-07-05T06:16:52.921575Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:16:52.921575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2306.01351","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":"2026-07-05T06:16:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0S4XWJ9QIOeeZfZr6omD+JJ+Z7WcboPBl0oml7IO11PiejcTAraq9Am5ElKV8CHF2nny2b8HsfaHYHb3zT1+AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T08:36:26.210704Z"},"content_sha256":"ceeec5f94a6fca5f0104ab4e2a3b417153b59230d2576218964b3c45c71b1b7b","schema_version":"1.0","event_id":"sha256:ceeec5f94a6fca5f0104ab4e2a3b417153b59230d2576218964b3c45c71b1b7b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:XVM2PUJJ335MEZVALB46F2GKQL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Properties of Hot Nuclear Matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Alessandro Lovato, Lucas Tonetto, Omar Benhar","submitted_at":"2023-06-02T08:24:15Z","abstract_excerpt":"A fully quantitative description of equilibrium and dynamical properties of hot nuclear matter will be needed for the interpretation of the available and forthcoming astrophysical data, providing information on the post merger phase of a neutron star coalescence. We discuss the results of a recently developed theoretical model,based on a phenomenological nuclear Hamiltonian including two- and three-nucleon potentials, to study the temperature dependence of average and single-particle properties of nuclear matter relevant to astrophysical applications. The potential of the proposed approach for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.01351","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2306.01351/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T06:16:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YcLacX8fO05/B+8SsIvTlQZNRggVkrYCEtn+UVuxQfkT5SwpyCuA6Q578adPguWX3pwcQcWBNzwNxswc9WKBBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T08:36:26.211439Z"},"content_sha256":"caef3b06fb41821b43d083bd1bebc45d2d629ab1f6d59e347a142df0527ce9bf","schema_version":"1.0","event_id":"sha256:caef3b06fb41821b43d083bd1bebc45d2d629ab1f6d59e347a142df0527ce9bf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XVM2PUJJ335MEZVALB46F2GKQL/bundle.json","state_url":"https://pith.science/pith/XVM2PUJJ335MEZVALB46F2GKQL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XVM2PUJJ335MEZVALB46F2GKQL/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":"2026-08-11T08:36:26Z","links":{"resolver":"https://pith.science/pith/XVM2PUJJ335MEZVALB46F2GKQL","bundle":"https://pith.science/pith/XVM2PUJJ335MEZVALB46F2GKQL/bundle.json","state":"https://pith.science/pith/XVM2PUJJ335MEZVALB46F2GKQL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XVM2PUJJ335MEZVALB46F2GKQL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:XVM2PUJJ335MEZVALB46F2GKQL","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":"7d730d0134e6cb4e2bd8764096e29ee8b90b51419f4812fc69fcbc4f6916417a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-02T08:24:15Z","title_canon_sha256":"65c492dd16dc5a07261cd6908468f43d55434a64b70873f07a71061e010e96e2"},"schema_version":"1.0","source":{"id":"2306.01351","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2306.01351","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"arxiv_version","alias_value":"2306.01351v1","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.01351","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_12","alias_value":"XVM2PUJJ335M","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_16","alias_value":"XVM2PUJJ335MEZVA","created_at":"2026-07-05T06:16:52Z"},{"alias_kind":"pith_short_8","alias_value":"XVM2PUJJ","created_at":"2026-07-05T06:16:52Z"}],"graph_snapshots":[{"event_id":"sha256:caef3b06fb41821b43d083bd1bebc45d2d629ab1f6d59e347a142df0527ce9bf","target":"graph","created_at":"2026-07-05T06:16:52Z","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/2306.01351/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A fully quantitative description of equilibrium and dynamical properties of hot nuclear matter will be needed for the interpretation of the available and forthcoming astrophysical data, providing information on the post merger phase of a neutron star coalescence. We discuss the results of a recently developed theoretical model,based on a phenomenological nuclear Hamiltonian including two- and three-nucleon potentials, to study the temperature dependence of average and single-particle properties of nuclear matter relevant to astrophysical applications. The potential of the proposed approach for","authors_text":"Alessandro Lovato, Lucas Tonetto, Omar Benhar","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-02T08:24:15Z","title":"Properties of Hot Nuclear Matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.01351","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:ceeec5f94a6fca5f0104ab4e2a3b417153b59230d2576218964b3c45c71b1b7b","target":"record","created_at":"2026-07-05T06:16:52Z","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":"7d730d0134e6cb4e2bd8764096e29ee8b90b51419f4812fc69fcbc4f6916417a","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-02T08:24:15Z","title_canon_sha256":"65c492dd16dc5a07261cd6908468f43d55434a64b70873f07a71061e010e96e2"},"schema_version":"1.0","source":{"id":"2306.01351","kind":"arxiv","version":1}},"canonical_sha256":"bd59a7d129defac266a05879e2e8ca82dbcd77bcf3f77bd2e079cd02a1e67ec1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bd59a7d129defac266a05879e2e8ca82dbcd77bcf3f77bd2e079cd02a1e67ec1","first_computed_at":"2026-07-05T06:16:52.921575Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:16:52.921575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jCyhb+WWx2JzahYxTdNyg31/32gsk6V296qtnQtxHq1JrvB4K/yRjmf1oMPECqx3U6jP6LNovExkX3VUxfdmDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:16:52.921903Z","signed_message":"canonical_sha256_bytes"},"source_id":"2306.01351","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ceeec5f94a6fca5f0104ab4e2a3b417153b59230d2576218964b3c45c71b1b7b","sha256:caef3b06fb41821b43d083bd1bebc45d2d629ab1f6d59e347a142df0527ce9bf"],"state_sha256":"e25980fb3f95f68e02d65bc168e48dca9b031a76e371a91f70a38c9e5d5584fd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dL2y3pAm+G0emBzkHGmxWfv6EFvIxwxgK+8zhgZjIXSEEBK97VH5QXJADgzi86GOnM2H9nr9DgH4SiWcI8IOAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T08:36:26.217498Z","bundle_sha256":"d800273e58f9f823bba057b0d03c6793435745e4c7cfb3152bade095dc141f2c"}}