{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:CIWN5QCIDIDIK2TQSSFF7RTJHQ","short_pith_number":"pith:CIWN5QCI","schema_version":"1.0","canonical_sha256":"122cdec0481a06856a70948a5fc6693c23a4adf8ea8ff2261825951d4c722330","source":{"kind":"arxiv","id":"1806.04864","version":1},"attestation_state":"computed","paper":{"title":"Transition magnetic moments of $J^P=\\frac{3}{2}^+$ decuplet to $J^P=\\frac{1}{2}^+$ octet baryons in the chiral constituent quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Harleen Dahiya","submitted_at":"2018-06-13T06:44:04Z","abstract_excerpt":"In light of the developments of the chiral constituent quark model ($\\chi$CQM) in studying low energy hadronic matrix elements of the ground-state baryons, we have extended this model to investigate their transition properties. The magnetic moments of transitions from the $J^P=\\frac{3}{2}^+$ decuplet to $J^P=\\frac{1}{2}^+$ octet baryons have been calculated with explicit valence quark spin, sea quark spin and sea quark orbital angular momentum contributions. Since the experimental data is available for only a few transitions, we have compared our results with the results of other available mod"},"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":"1806.04864","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-13T06:44:04Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"817aef679a0e31de3c1b2ea2d46901b38e6a203b7edea22d03c803fd28019ca1","abstract_canon_sha256":"8f8cdd1f0b4f3a375f0652b836b3a7314258200cb9f216b3e3f5573ced9ddad4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:55.991445Z","signature_b64":"i7Tmg0O0fSVIbWVgrptJjFwPim0Um1tiIWw4wH5UL3nUXYnbAOBmunxPG8LHvIYsguRbR1PKH1VA/+CPpu5/Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"122cdec0481a06856a70948a5fc6693c23a4adf8ea8ff2261825951d4c722330","last_reissued_at":"2026-05-18T00:04:55.990718Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:55.990718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transition magnetic moments of $J^P=\\frac{3}{2}^+$ decuplet to $J^P=\\frac{1}{2}^+$ octet baryons in the chiral constituent quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Harleen Dahiya","submitted_at":"2018-06-13T06:44:04Z","abstract_excerpt":"In light of the developments of the chiral constituent quark model ($\\chi$CQM) in studying low energy hadronic matrix elements of the ground-state baryons, we have extended this model to investigate their transition properties. The magnetic moments of transitions from the $J^P=\\frac{3}{2}^+$ decuplet to $J^P=\\frac{1}{2}^+$ octet baryons have been calculated with explicit valence quark spin, sea quark spin and sea quark orbital angular momentum contributions. Since the experimental data is available for only a few transitions, we have compared our results with the results of other available mod"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.04864","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":"1806.04864","created_at":"2026-05-18T00:04:55.990829+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.04864v1","created_at":"2026-05-18T00:04:55.990829+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.04864","created_at":"2026-05-18T00:04:55.990829+00:00"},{"alias_kind":"pith_short_12","alias_value":"CIWN5QCIDIDI","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_16","alias_value":"CIWN5QCIDIDIK2TQ","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_8","alias_value":"CIWN5QCI","created_at":"2026-05-18T12:32:16.446611+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/CIWN5QCIDIDIK2TQSSFF7RTJHQ","json":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ.json","graph_json":"https://pith.science/api/pith-number/CIWN5QCIDIDIK2TQSSFF7RTJHQ/graph.json","events_json":"https://pith.science/api/pith-number/CIWN5QCIDIDIK2TQSSFF7RTJHQ/events.json","paper":"https://pith.science/paper/CIWN5QCI"},"agent_actions":{"view_html":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ","download_json":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ.json","view_paper":"https://pith.science/paper/CIWN5QCI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.04864&json=true","fetch_graph":"https://pith.science/api/pith-number/CIWN5QCIDIDIK2TQSSFF7RTJHQ/graph.json","fetch_events":"https://pith.science/api/pith-number/CIWN5QCIDIDIK2TQSSFF7RTJHQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ/action/storage_attestation","attest_author":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ/action/author_attestation","sign_citation":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ/action/citation_signature","submit_replication":"https://pith.science/pith/CIWN5QCIDIDIK2TQSSFF7RTJHQ/action/replication_record"}},"created_at":"2026-05-18T00:04:55.990829+00:00","updated_at":"2026-05-18T00:04:55.990829+00:00"}