{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:QMHNZTJTFPU4UD352XXN6DH7US","short_pith_number":"pith:QMHNZTJT","schema_version":"1.0","canonical_sha256":"830edccd332be9ca0f7dd5eedf0cffa4863ba5ccd9da5a510f6b5cb81fa248e2","source":{"kind":"arxiv","id":"1208.2682","version":3},"attestation_state":"computed","paper":{"title":"Systematics of quadrupole moments and energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"L. Zamick, S. J. Q. Robinson, S. Yeager, Xiaofei Yu, Y. Y. Sharon","submitted_at":"2012-08-13T19:51:27Z","abstract_excerpt":"We define the \"quadrupole ratio\" r_{Q}=\\dfrac{Q_{0}(S)}{Q_{0}(B)} where Q_{0}(S) is the intrinsic quadrupole moment obtained from the static quadrupole moment of the 2_{1}^{+} state of an even-even nucleus and Q_{0}(B) the intrinsic quadrupole moment obtained from B(E2)_{0\\rightarrow2} . In both cases we assume a simple rotational formula connecting the rotating frame to the laboratory frame. The quantity r_{Q} would be one if the rotational model were perfect and the energy ratio E(4)/E(2) would be 10/3. In the simple vibrational model, r_{Q} would be zero and E(4)/E(2) would be two. There ar"},"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":"1208.2682","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-08-13T19:51:27Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"b85af007de79a80bd38d112cd7f21ea93f90229a5e9ac67e45200355093d36ab","abstract_canon_sha256":"1d90853209a927edde636f302a612c5dc442f0e7b6b9956e8f39bbc569f1d857"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:23.908036Z","signature_b64":"KXxKiSdcz32HpBO1IyYYSHn6BH2VF+eKpiatU9GeeZRHqzWDHkw6XY2yxC77zFYXCJkXzUJSRH3ZWnEu2q88CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"830edccd332be9ca0f7dd5eedf0cffa4863ba5ccd9da5a510f6b5cb81fa248e2","last_reissued_at":"2026-05-18T00:50:23.907296Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:23.907296Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Systematics of quadrupole moments and energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"L. Zamick, S. J. Q. Robinson, S. Yeager, Xiaofei Yu, Y. Y. Sharon","submitted_at":"2012-08-13T19:51:27Z","abstract_excerpt":"We define the \"quadrupole ratio\" r_{Q}=\\dfrac{Q_{0}(S)}{Q_{0}(B)} where Q_{0}(S) is the intrinsic quadrupole moment obtained from the static quadrupole moment of the 2_{1}^{+} state of an even-even nucleus and Q_{0}(B) the intrinsic quadrupole moment obtained from B(E2)_{0\\rightarrow2} . In both cases we assume a simple rotational formula connecting the rotating frame to the laboratory frame. The quantity r_{Q} would be one if the rotational model were perfect and the energy ratio E(4)/E(2) would be 10/3. In the simple vibrational model, r_{Q} would be zero and E(4)/E(2) would be two. There ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.2682","kind":"arxiv","version":3},"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":"1208.2682","created_at":"2026-05-18T00:50:23.907423+00:00"},{"alias_kind":"arxiv_version","alias_value":"1208.2682v3","created_at":"2026-05-18T00:50:23.907423+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.2682","created_at":"2026-05-18T00:50:23.907423+00:00"},{"alias_kind":"pith_short_12","alias_value":"QMHNZTJTFPU4","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_16","alias_value":"QMHNZTJTFPU4UD35","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_8","alias_value":"QMHNZTJT","created_at":"2026-05-18T12:27:18.751474+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/QMHNZTJTFPU4UD352XXN6DH7US","json":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US.json","graph_json":"https://pith.science/api/pith-number/QMHNZTJTFPU4UD352XXN6DH7US/graph.json","events_json":"https://pith.science/api/pith-number/QMHNZTJTFPU4UD352XXN6DH7US/events.json","paper":"https://pith.science/paper/QMHNZTJT"},"agent_actions":{"view_html":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US","download_json":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US.json","view_paper":"https://pith.science/paper/QMHNZTJT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1208.2682&json=true","fetch_graph":"https://pith.science/api/pith-number/QMHNZTJTFPU4UD352XXN6DH7US/graph.json","fetch_events":"https://pith.science/api/pith-number/QMHNZTJTFPU4UD352XXN6DH7US/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US/action/storage_attestation","attest_author":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US/action/author_attestation","sign_citation":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US/action/citation_signature","submit_replication":"https://pith.science/pith/QMHNZTJTFPU4UD352XXN6DH7US/action/replication_record"}},"created_at":"2026-05-18T00:50:23.907423+00:00","updated_at":"2026-05-18T00:50:23.907423+00:00"}