{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:UCE736DUNS5WFXA7JQG4SSCKOZ","short_pith_number":"pith:UCE736DU","schema_version":"1.0","canonical_sha256":"a089fdf8746cbb62dc1f4c0dc9484a7653c7f4c2854f8f0982a7cd7b08905197","source":{"kind":"arxiv","id":"1707.00236","version":2},"attestation_state":"computed","paper":{"title":"Structure of krypton isotopes within the interacting boson model derived from the Gogny energy density functional","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"H. Abusara, K. Nomura, L. M. Robledo, R. Rodr\\'iguez-Guzm\\'an, Y. M. Humadi","submitted_at":"2017-07-02T05:03:55Z","abstract_excerpt":"The evolution and coexistence of the nuclear shapes as well as the corresponding low-lying collective states and electromagnetic transition rates are investigated along the Krypton isotopic chain within the framework of the interacting boson model (IBM). The IBM Hamiltonian is determined through mean-field calculations based on the several parametrizations of the Gogny energy density functional and the relativistic mean-field Lagrangian. The mean-field energy surfaces, as functions of the axial $\\beta$ and triaxial $\\gamma$ quadrupole deformations, are mapped onto the expectation value of the "},"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":"1707.00236","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-07-02T05:03:55Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"5175a24f1a2a91c63933734d8a29f465647aad7e4b72943adb0dba6afd3b6ace","abstract_canon_sha256":"2a3aad51e2ea23c61e22d47ebb0b98b88bf0123285428bf4a0fa41ec0d292953"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:19.668420Z","signature_b64":"KkT4WOdlrK/lyC2U//rgA9NW3Bee0fmlQXAJwXaEJduoSb3P/bLGi0ZjOchRKGY5vp+jd5gfvIdZLjIVsy6PBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a089fdf8746cbb62dc1f4c0dc9484a7653c7f4c2854f8f0982a7cd7b08905197","last_reissued_at":"2026-05-18T00:35:19.667956Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:19.667956Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Structure of krypton isotopes within the interacting boson model derived from the Gogny energy density functional","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"H. Abusara, K. Nomura, L. M. Robledo, R. Rodr\\'iguez-Guzm\\'an, Y. M. Humadi","submitted_at":"2017-07-02T05:03:55Z","abstract_excerpt":"The evolution and coexistence of the nuclear shapes as well as the corresponding low-lying collective states and electromagnetic transition rates are investigated along the Krypton isotopic chain within the framework of the interacting boson model (IBM). The IBM Hamiltonian is determined through mean-field calculations based on the several parametrizations of the Gogny energy density functional and the relativistic mean-field Lagrangian. The mean-field energy surfaces, as functions of the axial $\\beta$ and triaxial $\\gamma$ quadrupole deformations, are mapped onto the expectation value of the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.00236","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":"1707.00236","created_at":"2026-05-18T00:35:19.668019+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.00236v2","created_at":"2026-05-18T00:35:19.668019+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.00236","created_at":"2026-05-18T00:35:19.668019+00:00"},{"alias_kind":"pith_short_12","alias_value":"UCE736DUNS5W","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"UCE736DUNS5WFXA7","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"UCE736DU","created_at":"2026-05-18T12:31:46.661854+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/UCE736DUNS5WFXA7JQG4SSCKOZ","json":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ.json","graph_json":"https://pith.science/api/pith-number/UCE736DUNS5WFXA7JQG4SSCKOZ/graph.json","events_json":"https://pith.science/api/pith-number/UCE736DUNS5WFXA7JQG4SSCKOZ/events.json","paper":"https://pith.science/paper/UCE736DU"},"agent_actions":{"view_html":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ","download_json":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ.json","view_paper":"https://pith.science/paper/UCE736DU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.00236&json=true","fetch_graph":"https://pith.science/api/pith-number/UCE736DUNS5WFXA7JQG4SSCKOZ/graph.json","fetch_events":"https://pith.science/api/pith-number/UCE736DUNS5WFXA7JQG4SSCKOZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ/action/storage_attestation","attest_author":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ/action/author_attestation","sign_citation":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ/action/citation_signature","submit_replication":"https://pith.science/pith/UCE736DUNS5WFXA7JQG4SSCKOZ/action/replication_record"}},"created_at":"2026-05-18T00:35:19.668019+00:00","updated_at":"2026-05-18T00:35:19.668019+00:00"}