{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:2P6KG7DLEL3LUUU4SMGB2R5RUL","short_pith_number":"pith:2P6KG7DL","schema_version":"1.0","canonical_sha256":"d3fca37c6b22f6ba529c930c1d47b1a2ccd2bcafbf8bac769553f4f22c2159ac","source":{"kind":"arxiv","id":"1807.06795","version":2},"attestation_state":"computed","paper":{"title":"Radiative transitions of doubly charmed baryons in lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"G. Erkol, H. Bahtiyar, K. U. Can, M. Oka, T. T. Takahashi","submitted_at":"2018-07-18T07:00:51Z","abstract_excerpt":"We evaluate the spin-$3/2 \\to$ spin-$1/2$ electromagnetic transitions of the doubly charmed baryons on 2+1 flavor, $32^3 \\times 64$ PACS-CS lattices with a pion mass of $156(9)$ MeV/c$^2$. A relativistic heavy quark action is employed to minimize the associated systematic errors on charm-quark observables. We extract the magnetic dipole, $M1$, and the electric quadrupole, $E2$, transition form factors. In order to make a reliable estimate of the $M1$ form factor, we carry out an analysis by including the effect of excited-state contributions. We find that the $M1$ transition is dominant and li"},"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":"1807.06795","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-07-18T07:00:51Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e546a3e567eb0c551a0f0832b2233c6fe9f4ef8afb86f837ef361590d418937a","abstract_canon_sha256":"724e0597f100952c3f7ec8cd1970fde18020f27ca84b1a75261459a5cf06b1d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:04.447772Z","signature_b64":"kNtiYGq5xA4vz6CCoJyf9JXV4y+XlpWP9/FLTxHuT9/8q1L3qkJyp+HnHaCX1WvEyMuzHCQ7Qcm/DjzTMuoECg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3fca37c6b22f6ba529c930c1d47b1a2ccd2bcafbf8bac769553f4f22c2159ac","last_reissued_at":"2026-05-17T23:58:04.447312Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:04.447312Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative transitions of doubly charmed baryons in lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"G. Erkol, H. Bahtiyar, K. U. Can, M. Oka, T. T. Takahashi","submitted_at":"2018-07-18T07:00:51Z","abstract_excerpt":"We evaluate the spin-$3/2 \\to$ spin-$1/2$ electromagnetic transitions of the doubly charmed baryons on 2+1 flavor, $32^3 \\times 64$ PACS-CS lattices with a pion mass of $156(9)$ MeV/c$^2$. A relativistic heavy quark action is employed to minimize the associated systematic errors on charm-quark observables. We extract the magnetic dipole, $M1$, and the electric quadrupole, $E2$, transition form factors. In order to make a reliable estimate of the $M1$ form factor, we carry out an analysis by including the effect of excited-state contributions. We find that the $M1$ transition is dominant and li"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.06795","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":"1807.06795","created_at":"2026-05-17T23:58:04.447379+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.06795v2","created_at":"2026-05-17T23:58:04.447379+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.06795","created_at":"2026-05-17T23:58:04.447379+00:00"},{"alias_kind":"pith_short_12","alias_value":"2P6KG7DLEL3L","created_at":"2026-05-18T12:32:02.567920+00:00"},{"alias_kind":"pith_short_16","alias_value":"2P6KG7DLEL3LUUU4","created_at":"2026-05-18T12:32:02.567920+00:00"},{"alias_kind":"pith_short_8","alias_value":"2P6KG7DL","created_at":"2026-05-18T12:32:02.567920+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2601.07015","citing_title":"Light cone QCD sum rules study of the rare radiative $\\Xi^{*}_{bb}\\to\\Xi_b\\gamma$ decay","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2602.05502","citing_title":"Electromagnetic polarizabilities of the triplet hadrons in heavy hadron chiral perturbation theory","ref_index":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL","json":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL.json","graph_json":"https://pith.science/api/pith-number/2P6KG7DLEL3LUUU4SMGB2R5RUL/graph.json","events_json":"https://pith.science/api/pith-number/2P6KG7DLEL3LUUU4SMGB2R5RUL/events.json","paper":"https://pith.science/paper/2P6KG7DL"},"agent_actions":{"view_html":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL","download_json":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL.json","view_paper":"https://pith.science/paper/2P6KG7DL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.06795&json=true","fetch_graph":"https://pith.science/api/pith-number/2P6KG7DLEL3LUUU4SMGB2R5RUL/graph.json","fetch_events":"https://pith.science/api/pith-number/2P6KG7DLEL3LUUU4SMGB2R5RUL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL/action/storage_attestation","attest_author":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL/action/author_attestation","sign_citation":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL/action/citation_signature","submit_replication":"https://pith.science/pith/2P6KG7DLEL3LUUU4SMGB2R5RUL/action/replication_record"}},"created_at":"2026-05-17T23:58:04.447379+00:00","updated_at":"2026-05-17T23:58:04.447379+00:00"}