{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:RLKEH3FPXBEOXMRFGZWP6YONBO","short_pith_number":"pith:RLKEH3FP","schema_version":"1.0","canonical_sha256":"8ad443ecafb848ebb225366cff61cd0b86406c10e50b51809021aec967e263f1","source":{"kind":"arxiv","id":"1804.10228","version":2},"attestation_state":"computed","paper":{"title":"Finite-temperature relativistic nuclear field theory: an application to the dipole response","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Elena Litvinova, Herlik Wibowo","submitted_at":"2018-04-26T18:25:52Z","abstract_excerpt":"Nuclear response theory beyond the one-loop approximation is formulated for the case of finite temperature. For this purpose, the time blocking approximation to the time-dependent part of the in-medium nucleon-nucleon interaction amplitude is adopted for the thermal (imaginary-time) Green's function formalism. We found that introducing a soft blocking, instead of a sharp blocking at zero temperature, brings the Bethe-Salpeter equation to a single frequency variable equation also at finite temperatures. The method is implemented self-consistently in the framework of Quantum Hadrodynamics and de"},"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":"1804.10228","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-26T18:25:52Z","cross_cats_sorted":[],"title_canon_sha256":"58c8a6372bc9846bead87b86616deb3955f5db8c63e9349497315cd5eb9beeef","abstract_canon_sha256":"694c128cfa5748b1adccf802edea61249726c2be4a74e3e283321163a3962ad6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:59.988242Z","signature_b64":"kk6HtWzOhlnMpdkHep/8gFwm/sSp7FJOH2rEbM05e3+lDpoZxMdqUZ3gkYtcsniXhtENNS/do+MXwSOTRHhsCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ad443ecafb848ebb225366cff61cd0b86406c10e50b51809021aec967e263f1","last_reissued_at":"2026-05-18T00:06:59.987653Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:59.987653Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-temperature relativistic nuclear field theory: an application to the dipole response","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Elena Litvinova, Herlik Wibowo","submitted_at":"2018-04-26T18:25:52Z","abstract_excerpt":"Nuclear response theory beyond the one-loop approximation is formulated for the case of finite temperature. For this purpose, the time blocking approximation to the time-dependent part of the in-medium nucleon-nucleon interaction amplitude is adopted for the thermal (imaginary-time) Green's function formalism. We found that introducing a soft blocking, instead of a sharp blocking at zero temperature, brings the Bethe-Salpeter equation to a single frequency variable equation also at finite temperatures. The method is implemented self-consistently in the framework of Quantum Hadrodynamics and de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.10228","kind":"arxiv","version":2},"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":"1804.10228","created_at":"2026-05-18T00:06:59.987743+00:00"},{"alias_kind":"arxiv_version","alias_value":"1804.10228v2","created_at":"2026-05-18T00:06:59.987743+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.10228","created_at":"2026-05-18T00:06:59.987743+00:00"},{"alias_kind":"pith_short_12","alias_value":"RLKEH3FPXBEO","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_16","alias_value":"RLKEH3FPXBEOXMRF","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_8","alias_value":"RLKEH3FP","created_at":"2026-05-18T12:32:50.500415+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/RLKEH3FPXBEOXMRFGZWP6YONBO","json":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO.json","graph_json":"https://pith.science/api/pith-number/RLKEH3FPXBEOXMRFGZWP6YONBO/graph.json","events_json":"https://pith.science/api/pith-number/RLKEH3FPXBEOXMRFGZWP6YONBO/events.json","paper":"https://pith.science/paper/RLKEH3FP"},"agent_actions":{"view_html":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO","download_json":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO.json","view_paper":"https://pith.science/paper/RLKEH3FP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1804.10228&json=true","fetch_graph":"https://pith.science/api/pith-number/RLKEH3FPXBEOXMRFGZWP6YONBO/graph.json","fetch_events":"https://pith.science/api/pith-number/RLKEH3FPXBEOXMRFGZWP6YONBO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO/action/storage_attestation","attest_author":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO/action/author_attestation","sign_citation":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO/action/citation_signature","submit_replication":"https://pith.science/pith/RLKEH3FPXBEOXMRFGZWP6YONBO/action/replication_record"}},"created_at":"2026-05-18T00:06:59.987743+00:00","updated_at":"2026-05-18T00:06:59.987743+00:00"}