{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:LNN5V72GFVNSTLAOBTIDCC2XWX","short_pith_number":"pith:LNN5V72G","canonical_record":{"source":{"id":"1207.5737","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-07-24T16:16:50Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f46b605c202c325f63912bce5c4c1979a27be3fc30e8ce2fe4d2093fd279d816","abstract_canon_sha256":"c632b537a9b79db4ed46d30da6475377f4f1b574b512c3ea4da2a8d8377a80ca"},"schema_version":"1.0"},"canonical_sha256":"5b5bdaff462d5b29ac0e0cd0310b57b5cbf2fb43b673ebd98b1b37c9216ab964","source":{"kind":"arxiv","id":"1207.5737","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5737","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5737v1","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5737","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"pith_short_12","alias_value":"LNN5V72GFVNS","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"LNN5V72GFVNSTLAO","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"LNN5V72G","created_at":"2026-05-18T12:27:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:LNN5V72GFVNSTLAOBTIDCC2XWX","target":"record","payload":{"canonical_record":{"source":{"id":"1207.5737","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-07-24T16:16:50Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f46b605c202c325f63912bce5c4c1979a27be3fc30e8ce2fe4d2093fd279d816","abstract_canon_sha256":"c632b537a9b79db4ed46d30da6475377f4f1b574b512c3ea4da2a8d8377a80ca"},"schema_version":"1.0"},"canonical_sha256":"5b5bdaff462d5b29ac0e0cd0310b57b5cbf2fb43b673ebd98b1b37c9216ab964","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:08.377970Z","signature_b64":"PAY/Zf7dYJHkIacmBaoj/n3B+fcm+JdRprcqabmaAa8nsnxeLaLN6tkbfdPhAV+96bqy5dVW+D4dfpV5xIDLDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b5bdaff462d5b29ac0e0cd0310b57b5cbf2fb43b673ebd98b1b37c9216ab964","last_reissued_at":"2026-05-18T01:56:08.377380Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:08.377380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.5737","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":"2026-05-18T01:56:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kCoZBZap5afOGheooLPwNS3ORihpVeprQ9w8Qgs3VO92zQ45ic9mzs4HaeTBh8ottHIPRedDhyB0zQTNVuIJBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T04:35:59.811692Z"},"content_sha256":"54a6497106c19636321bf0ed65755e2977afcad7b51ef6fa3989ccb153b3664a","schema_version":"1.0","event_id":"sha256:54a6497106c19636321bf0ed65755e2977afcad7b51ef6fa3989ccb153b3664a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:LNN5V72GFVNSTLAOBTIDCC2XWX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Specific shear viscosity in hot rotating systems of paired fermions","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"N. Dinh Dang, N. Quang Hung","submitted_at":"2012-07-24T16:16:50Z","abstract_excerpt":"The specific shear viscosity $\\bar\\eta$ of a classically rotating system of nucleons that interact via a monopole pairing interaction is calculated including the effects of thermal fluctuations and coupling to pair vibrations within the selfconsistent quasiparticle random-phase approximation. It is found that $\\bar\\eta$ increases with angular momentum $M$ at a given temperature $T$. In medium and heavy systems, $\\bar\\eta$ decreases with increasing $T$ at $T\\geq$ 2 MeV and this feature is not affected much by angular momentum. But in lighter systems (with the mass number $A\\leq$ 20), $\\bar\\eta$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5737","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":"2026-05-18T01:56:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9AdkpI+V5vDq40FkxwmeAwg/UrLxe73JHToL4i9TDGEPltF/mKeAcxViBaYz2+OJYnus7c6v4kNiskqrjWdNDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T04:35:59.812052Z"},"content_sha256":"c2368cc27bcec46f561a8b77d64038b088de62f84e8ba0a1b297dedf2211f9d2","schema_version":"1.0","event_id":"sha256:c2368cc27bcec46f561a8b77d64038b088de62f84e8ba0a1b297dedf2211f9d2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/bundle.json","state_url":"https://pith.science/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/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":"2026-06-23T04:35:59Z","links":{"resolver":"https://pith.science/pith/LNN5V72GFVNSTLAOBTIDCC2XWX","bundle":"https://pith.science/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/bundle.json","state":"https://pith.science/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LNN5V72GFVNSTLAOBTIDCC2XWX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:LNN5V72GFVNSTLAOBTIDCC2XWX","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":"c632b537a9b79db4ed46d30da6475377f4f1b574b512c3ea4da2a8d8377a80ca","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-07-24T16:16:50Z","title_canon_sha256":"f46b605c202c325f63912bce5c4c1979a27be3fc30e8ce2fe4d2093fd279d816"},"schema_version":"1.0","source":{"id":"1207.5737","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5737","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5737v1","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5737","created_at":"2026-05-18T01:56:08Z"},{"alias_kind":"pith_short_12","alias_value":"LNN5V72GFVNS","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"LNN5V72GFVNSTLAO","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"LNN5V72G","created_at":"2026-05-18T12:27:14Z"}],"graph_snapshots":[{"event_id":"sha256:c2368cc27bcec46f561a8b77d64038b088de62f84e8ba0a1b297dedf2211f9d2","target":"graph","created_at":"2026-05-18T01:56:08Z","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":"The specific shear viscosity $\\bar\\eta$ of a classically rotating system of nucleons that interact via a monopole pairing interaction is calculated including the effects of thermal fluctuations and coupling to pair vibrations within the selfconsistent quasiparticle random-phase approximation. It is found that $\\bar\\eta$ increases with angular momentum $M$ at a given temperature $T$. In medium and heavy systems, $\\bar\\eta$ decreases with increasing $T$ at $T\\geq$ 2 MeV and this feature is not affected much by angular momentum. But in lighter systems (with the mass number $A\\leq$ 20), $\\bar\\eta$","authors_text":"N. Dinh Dang, N. Quang Hung","cross_cats":["nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-07-24T16:16:50Z","title":"Specific shear viscosity in hot rotating systems of paired fermions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5737","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":"sha256:54a6497106c19636321bf0ed65755e2977afcad7b51ef6fa3989ccb153b3664a","target":"record","created_at":"2026-05-18T01:56:08Z","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":"c632b537a9b79db4ed46d30da6475377f4f1b574b512c3ea4da2a8d8377a80ca","cross_cats_sorted":["nucl-ex"],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-07-24T16:16:50Z","title_canon_sha256":"f46b605c202c325f63912bce5c4c1979a27be3fc30e8ce2fe4d2093fd279d816"},"schema_version":"1.0","source":{"id":"1207.5737","kind":"arxiv","version":1}},"canonical_sha256":"5b5bdaff462d5b29ac0e0cd0310b57b5cbf2fb43b673ebd98b1b37c9216ab964","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5b5bdaff462d5b29ac0e0cd0310b57b5cbf2fb43b673ebd98b1b37c9216ab964","first_computed_at":"2026-05-18T01:56:08.377380Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:56:08.377380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PAY/Zf7dYJHkIacmBaoj/n3B+fcm+JdRprcqabmaAa8nsnxeLaLN6tkbfdPhAV+96bqy5dVW+D4dfpV5xIDLDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:56:08.377970Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.5737","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:54a6497106c19636321bf0ed65755e2977afcad7b51ef6fa3989ccb153b3664a","sha256:c2368cc27bcec46f561a8b77d64038b088de62f84e8ba0a1b297dedf2211f9d2"],"state_sha256":"2a87596825165f108eb707eb6e2560e22c5add2f2eec23563cae72676b00d81e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ejo9ZEAT0gHzxXiEJiggeo6Cm24pqohrVqMhq1Nkog4VRJZtGFCwPQmmu/a8OnQyKNSXqtG/Z5CPC4fEXj12Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-23T04:35:59.814029Z","bundle_sha256":"19f4bf2e1cd4571f0e077cf17e5c5a0e6808344da6cd180a03deb5f3832601bc"}}