{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:X4B3CYYF2D4MNJPXFDHHQKUATF","short_pith_number":"pith:X4B3CYYF","schema_version":"1.0","canonical_sha256":"bf03b16305d0f8c6a5f728ce782a809970fe0de2f89aebc9da1bfd29ba239367","source":{"kind":"arxiv","id":"1812.02908","version":1},"attestation_state":"computed","paper":{"title":"Description of the critical point symmetry in 124Te by IBM-2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Chengfu Mu, Dali Zhang","submitted_at":"2018-12-07T05:07:29Z","abstract_excerpt":"Based on the neutron and proton degrees of freedom, the low-lying energy levels, the $E2$, $M1$ and $E0$ transition strengths of nucleus $^{124}$Te have been calculated by the neutron-proton interacting boson model. The calculated results are quite consistent with the experimental data. By comparing the key observables of states at the critical point of $\\textrm{U}_{\\pi \\nu}(5)$--$\\textrm{O}_{\\pi \\nu}(6)$ transition with experimental data and calculated results, we show that the $^{124}$Te is a possible nucleus at the critical point of the second order phase transition from vibration to unstab"},"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":"1812.02908","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-12-07T05:07:29Z","cross_cats_sorted":[],"title_canon_sha256":"585cb50609231a4c15ac9ca2ad96d4bd51d0c0993d5ccff2683e62dab2627894","abstract_canon_sha256":"898516b6cddd026c3a44c438b2415792905917cb107e2d32b11e11c1aacb3591"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:09.340052Z","signature_b64":"ydJvqDBGNFEgpJsiDZuc4VhveMy3om4CPK9vyiqrzoZFUyuAx7nSTImlTswYWol8NdSje5Ir8c1CSoFsKJkbAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf03b16305d0f8c6a5f728ce782a809970fe0de2f89aebc9da1bfd29ba239367","last_reissued_at":"2026-05-17T23:50:09.339572Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:09.339572Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Description of the critical point symmetry in 124Te by IBM-2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Chengfu Mu, Dali Zhang","submitted_at":"2018-12-07T05:07:29Z","abstract_excerpt":"Based on the neutron and proton degrees of freedom, the low-lying energy levels, the $E2$, $M1$ and $E0$ transition strengths of nucleus $^{124}$Te have been calculated by the neutron-proton interacting boson model. The calculated results are quite consistent with the experimental data. By comparing the key observables of states at the critical point of $\\textrm{U}_{\\pi \\nu}(5)$--$\\textrm{O}_{\\pi \\nu}(6)$ transition with experimental data and calculated results, we show that the $^{124}$Te is a possible nucleus at the critical point of the second order phase transition from vibration to unstab"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.02908","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":"1812.02908","created_at":"2026-05-17T23:50:09.339653+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.02908v1","created_at":"2026-05-17T23:50:09.339653+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.02908","created_at":"2026-05-17T23:50:09.339653+00:00"},{"alias_kind":"pith_short_12","alias_value":"X4B3CYYF2D4M","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"X4B3CYYF2D4MNJPX","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"X4B3CYYF","created_at":"2026-05-18T12:33:01.666342+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/X4B3CYYF2D4MNJPXFDHHQKUATF","json":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF.json","graph_json":"https://pith.science/api/pith-number/X4B3CYYF2D4MNJPXFDHHQKUATF/graph.json","events_json":"https://pith.science/api/pith-number/X4B3CYYF2D4MNJPXFDHHQKUATF/events.json","paper":"https://pith.science/paper/X4B3CYYF"},"agent_actions":{"view_html":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF","download_json":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF.json","view_paper":"https://pith.science/paper/X4B3CYYF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.02908&json=true","fetch_graph":"https://pith.science/api/pith-number/X4B3CYYF2D4MNJPXFDHHQKUATF/graph.json","fetch_events":"https://pith.science/api/pith-number/X4B3CYYF2D4MNJPXFDHHQKUATF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF/action/storage_attestation","attest_author":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF/action/author_attestation","sign_citation":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF/action/citation_signature","submit_replication":"https://pith.science/pith/X4B3CYYF2D4MNJPXFDHHQKUATF/action/replication_record"}},"created_at":"2026-05-17T23:50:09.339653+00:00","updated_at":"2026-05-17T23:50:09.339653+00:00"}