{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5EPRH32NDGZJBQPZRXPDT2ZAUW","short_pith_number":"pith:5EPRH32N","schema_version":"1.0","canonical_sha256":"e91f13ef4d19b290c1f98dde39eb20a5b134829977eceb03815afebfdc0543fa","source":{"kind":"arxiv","id":"1205.0165","version":2},"attestation_state":"computed","paper":{"title":"Description of Even-Even Xe isotopes in the transitional region of IBM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Sabri, M. A. Jafarizadeh, N. Fouladi","submitted_at":"2012-05-01T14:19:35Z","abstract_excerpt":"Properties of Xe isotopes isotopes are studied in the U(5)<->O(6) transitional region of Interacting Boson Model (IBM-1). The energy levels and B(E2)transition rates are calculated via the affine SU(1,1)Lie Algebra. The agreement with the most recent experimental is acceptable. The evaluated Hamiltonian control parameters suggest a spherical to (/gamma)-soft shape transition and propose the Xe(A=130)nucleus as the best candidate for the E(5)symmetry."},"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":"1205.0165","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-05-01T14:19:35Z","cross_cats_sorted":[],"title_canon_sha256":"1cb252bd4243ddf835a164dc912edeea1dacb1c3444e68b07b15cf594a65eab0","abstract_canon_sha256":"7ca134054c2488619ae67d3e8a1570451d718824da422ef66e707b8ea7aca842"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:27.617213Z","signature_b64":"rJc5ct8hHjPzV4W/3eXqDuZR/oNpnvAWbrRGHuwhIZczpLpPGb8op9LFh+AoY8Z52UmAuG2qvg7ksmaqReznCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e91f13ef4d19b290c1f98dde39eb20a5b134829977eceb03815afebfdc0543fa","last_reissued_at":"2026-05-18T03:29:27.616425Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:27.616425Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Description of Even-Even Xe isotopes in the transitional region of IBM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Sabri, M. A. Jafarizadeh, N. Fouladi","submitted_at":"2012-05-01T14:19:35Z","abstract_excerpt":"Properties of Xe isotopes isotopes are studied in the U(5)<->O(6) transitional region of Interacting Boson Model (IBM-1). The energy levels and B(E2)transition rates are calculated via the affine SU(1,1)Lie Algebra. The agreement with the most recent experimental is acceptable. The evaluated Hamiltonian control parameters suggest a spherical to (/gamma)-soft shape transition and propose the Xe(A=130)nucleus as the best candidate for the E(5)symmetry."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.0165","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":"1205.0165","created_at":"2026-05-18T03:29:27.616552+00:00"},{"alias_kind":"arxiv_version","alias_value":"1205.0165v2","created_at":"2026-05-18T03:29:27.616552+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.0165","created_at":"2026-05-18T03:29:27.616552+00:00"},{"alias_kind":"pith_short_12","alias_value":"5EPRH32NDGZJ","created_at":"2026-05-18T12:26:53.410803+00:00"},{"alias_kind":"pith_short_16","alias_value":"5EPRH32NDGZJBQPZ","created_at":"2026-05-18T12:26:53.410803+00:00"},{"alias_kind":"pith_short_8","alias_value":"5EPRH32N","created_at":"2026-05-18T12:26:53.410803+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/5EPRH32NDGZJBQPZRXPDT2ZAUW","json":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW.json","graph_json":"https://pith.science/api/pith-number/5EPRH32NDGZJBQPZRXPDT2ZAUW/graph.json","events_json":"https://pith.science/api/pith-number/5EPRH32NDGZJBQPZRXPDT2ZAUW/events.json","paper":"https://pith.science/paper/5EPRH32N"},"agent_actions":{"view_html":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW","download_json":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW.json","view_paper":"https://pith.science/paper/5EPRH32N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1205.0165&json=true","fetch_graph":"https://pith.science/api/pith-number/5EPRH32NDGZJBQPZRXPDT2ZAUW/graph.json","fetch_events":"https://pith.science/api/pith-number/5EPRH32NDGZJBQPZRXPDT2ZAUW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW/action/storage_attestation","attest_author":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW/action/author_attestation","sign_citation":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW/action/citation_signature","submit_replication":"https://pith.science/pith/5EPRH32NDGZJBQPZRXPDT2ZAUW/action/replication_record"}},"created_at":"2026-05-18T03:29:27.616552+00:00","updated_at":"2026-05-18T03:29:27.616552+00:00"}