{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:IOETOEYRGNUGSLQVIH3NYLNPSR","short_pith_number":"pith:IOETOEYR","schema_version":"1.0","canonical_sha256":"43893713113368692e1541f6dc2daf946ac66e1e376f8c2551a2331faa0aab2b","source":{"kind":"arxiv","id":"2608.07131","version":1},"attestation_state":"computed","paper":{"title":"Microscopic description of the fission process including intrinsic excitations. Part II: 240Pu excited and asymmetric fission paths within the Schrodinger Collective","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Lacroix, D. Regnier, L.M. Robledo, N. Dubray, N. Pillet, P. Carpentier, R.N. Bernard, W. Younes","submitted_at":"2026-08-07T11:46:22Z","abstract_excerpt":"This second article of the trilogy presents the implementation of a third protocol, referred to as Continuous Deflation, designed to construct continuous and regular excited paths within the Schrodinger Collective-Intrinsic Model (SCIM), with applications to nuclear fission. We show that the use of standard 2QP excitations, even when combined with particle-number projection, prevents a consistent application of the SCIM framework. Motivated by the central role of pair breaking in low-energy fission, we explore how to construct intrinsic excited states that incorporate this mechanism while sati"},"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":"2608.07131","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"nucl-th","submitted_at":"2026-08-07T11:46:22Z","cross_cats_sorted":[],"title_canon_sha256":"d612faad04f129234f46382e3e8a71829bd7f79fbdaf240f4e723fe7db098453","abstract_canon_sha256":"a9f51962280df6be38e6047f587814fd765b505ce41f3613bf25536ea9297a46"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-10T01:13:23.593086Z","signature_b64":"oL5mDTU/+ZLHVy3HoGsTmI0JjVZeNMcaGJFVM1wnBO6QPvC84DoDmsEGUnMZKl0IKuQGUX5TBC/m9fNKgAU/Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"43893713113368692e1541f6dc2daf946ac66e1e376f8c2551a2331faa0aab2b","last_reissued_at":"2026-08-10T01:13:23.590448Z","signature_status":"signed_v1","first_computed_at":"2026-08-10T01:13:23.590448Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic description of the fission process including intrinsic excitations. Part II: 240Pu excited and asymmetric fission paths within the Schrodinger Collective","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Lacroix, D. Regnier, L.M. Robledo, N. Dubray, N. Pillet, P. Carpentier, R.N. Bernard, W. Younes","submitted_at":"2026-08-07T11:46:22Z","abstract_excerpt":"This second article of the trilogy presents the implementation of a third protocol, referred to as Continuous Deflation, designed to construct continuous and regular excited paths within the Schrodinger Collective-Intrinsic Model (SCIM), with applications to nuclear fission. We show that the use of standard 2QP excitations, even when combined with particle-number projection, prevents a consistent application of the SCIM framework. Motivated by the central role of pair breaking in low-energy fission, we explore how to construct intrinsic excited states that incorporate this mechanism while sati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.07131","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/2608.07131/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2608.07131","created_at":"2026-08-10T01:13:23.591637+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.07131v1","created_at":"2026-08-10T01:13:23.591637+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.07131","created_at":"2026-08-10T01:13:23.591637+00:00"},{"alias_kind":"pith_short_12","alias_value":"IOETOEYRGNUG","created_at":"2026-08-10T01:13:23.591637+00:00"},{"alias_kind":"pith_short_16","alias_value":"IOETOEYRGNUGSLQV","created_at":"2026-08-10T01:13:23.591637+00:00"},{"alias_kind":"pith_short_8","alias_value":"IOETOEYR","created_at":"2026-08-10T01:13:23.591637+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/IOETOEYRGNUGSLQVIH3NYLNPSR","json":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR.json","graph_json":"https://pith.science/api/pith-number/IOETOEYRGNUGSLQVIH3NYLNPSR/graph.json","events_json":"https://pith.science/api/pith-number/IOETOEYRGNUGSLQVIH3NYLNPSR/events.json","paper":"https://pith.science/paper/IOETOEYR"},"agent_actions":{"view_html":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR","download_json":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR.json","view_paper":"https://pith.science/paper/IOETOEYR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.07131&json=true","fetch_graph":"https://pith.science/api/pith-number/IOETOEYRGNUGSLQVIH3NYLNPSR/graph.json","fetch_events":"https://pith.science/api/pith-number/IOETOEYRGNUGSLQVIH3NYLNPSR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR/action/storage_attestation","attest_author":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR/action/author_attestation","sign_citation":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR/action/citation_signature","submit_replication":"https://pith.science/pith/IOETOEYRGNUGSLQVIH3NYLNPSR/action/replication_record"}},"created_at":"2026-08-10T01:13:23.591637+00:00","updated_at":"2026-08-10T01:13:23.591637+00:00"}