{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:P6DYWV4MQHV5R5G7PJNCOFZR34","short_pith_number":"pith:P6DYWV4M","schema_version":"1.0","canonical_sha256":"7f878b578c81ebd8f4df7a5a271731df07809d5bf692769cb0cace01c7e8a963","source":{"kind":"arxiv","id":"1411.6195","version":1},"attestation_state":"computed","paper":{"title":"Semiclassical shell-structure moment of inertia within the phase-space approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. G. Magner, D. V. Gorpinchenko, J. Bartel, J. P. Blocki","submitted_at":"2014-11-23T06:00:18Z","abstract_excerpt":"The moment of inertia for nuclear collective rotations was derived within the semiclassical approach based on the cranking model and the Strutinsky shell-correction method by using the non-perturbative periodic-orbit theory in the phase space variables. This moment of inertia for adiabatic (statistical-equilibrium) rotations can be approximated by the generalized rigid-body moment of inertia accounting for the shell corrections of the particle density. A semiclassical phase-space trace formula allows to express quite accurately the shell components of the moment of inertia in terms of the free"},"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":"1411.6195","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-11-23T06:00:18Z","cross_cats_sorted":[],"title_canon_sha256":"8f0ae818eafe9dca06a218f53c453fe8c12f7888002f994033f9d97b8ff5cf51","abstract_canon_sha256":"559f3874aab27f3d7a877aeab7f239f645ce0b674474b1ac6f900ffac9d1646a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:00.528440Z","signature_b64":"7uHrODz8OqgAcGf6qtZUg4+rnZh7SyjosQLI7HDAxB3M5fT1Egkq74zCFlffV/2YzWe+3t6IpHSdcQVLGD5lAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f878b578c81ebd8f4df7a5a271731df07809d5bf692769cb0cace01c7e8a963","last_reissued_at":"2026-05-18T02:33:00.528102Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:00.528102Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Semiclassical shell-structure moment of inertia within the phase-space approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. G. Magner, D. V. Gorpinchenko, J. Bartel, J. P. Blocki","submitted_at":"2014-11-23T06:00:18Z","abstract_excerpt":"The moment of inertia for nuclear collective rotations was derived within the semiclassical approach based on the cranking model and the Strutinsky shell-correction method by using the non-perturbative periodic-orbit theory in the phase space variables. This moment of inertia for adiabatic (statistical-equilibrium) rotations can be approximated by the generalized rigid-body moment of inertia accounting for the shell corrections of the particle density. A semiclassical phase-space trace formula allows to express quite accurately the shell components of the moment of inertia in terms of the free"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.6195","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":"1411.6195","created_at":"2026-05-18T02:33:00.528156+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.6195v1","created_at":"2026-05-18T02:33:00.528156+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.6195","created_at":"2026-05-18T02:33:00.528156+00:00"},{"alias_kind":"pith_short_12","alias_value":"P6DYWV4MQHV5","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"P6DYWV4MQHV5R5G7","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"P6DYWV4M","created_at":"2026-05-18T12:28:43.426989+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34","json":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34.json","graph_json":"https://pith.science/api/pith-number/P6DYWV4MQHV5R5G7PJNCOFZR34/graph.json","events_json":"https://pith.science/api/pith-number/P6DYWV4MQHV5R5G7PJNCOFZR34/events.json","paper":"https://pith.science/paper/P6DYWV4M"},"agent_actions":{"view_html":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34","download_json":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34.json","view_paper":"https://pith.science/paper/P6DYWV4M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.6195&json=true","fetch_graph":"https://pith.science/api/pith-number/P6DYWV4MQHV5R5G7PJNCOFZR34/graph.json","fetch_events":"https://pith.science/api/pith-number/P6DYWV4MQHV5R5G7PJNCOFZR34/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34/action/storage_attestation","attest_author":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34/action/author_attestation","sign_citation":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34/action/citation_signature","submit_replication":"https://pith.science/pith/P6DYWV4MQHV5R5G7PJNCOFZR34/action/replication_record"}},"created_at":"2026-05-18T02:33:00.528156+00:00","updated_at":"2026-05-18T02:33:00.528156+00:00"}