{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:OQ3RJ3RKVYBUL3EDMHPTPEWASZ","short_pith_number":"pith:OQ3RJ3RK","schema_version":"1.0","canonical_sha256":"743714ee2aae0345ec8361df3792c0966c30450fc78ae4ec04aa79c08b133404","source":{"kind":"arxiv","id":"1905.00713","version":2},"attestation_state":"computed","paper":{"title":"Electromagnetic properties of the $d^*(2380)$ hexaquark","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Pastore, D.P. Watts, M. Bashkanov","submitted_at":"2019-05-02T13:06:45Z","abstract_excerpt":"Experiments with intense photon and electron beams have the potential to provide access to nontrivial properties of the recently discovered $d^*(2380)$ hexaquark including its size, structure, magnetic moment, quadrupole and octupole deformations. In this paper we investigate the sensitivity of ongoing and planned experiments to various properties of the $d^*(2380)$, employing models based on both constituent quark and pion cloud frameworks. Our calculations indicate that for photoinduced reactions on the deuteron the $d^*(2380)$ is predominantly produced from the $D-wave$ component of the deu"},"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":"1905.00713","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-05-02T13:06:45Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"18828887b07a7c23ea8e4a3307c2b8d7f6c2385d8cf01bdd27a0e6bde34cb83e","abstract_canon_sha256":"7047555d7ecc04a5f17edf304c1ec4b03a8cb9c47cb58f0b37c0fe3aec125bcb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:50:39.829304Z","signature_b64":"a1AyU93PmmRSnK/1VnqyVoJgHOzdrecKgkzrvFDDyxgvFO7TKIAJ0iK3Ll4lcgbIi2OCLtdlKY0zPwqT0DLSDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"743714ee2aae0345ec8361df3792c0966c30450fc78ae4ec04aa79c08b133404","last_reissued_at":"2026-07-04T23:50:39.828867Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:50:39.828867Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic properties of the $d^*(2380)$ hexaquark","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Pastore, D.P. Watts, M. Bashkanov","submitted_at":"2019-05-02T13:06:45Z","abstract_excerpt":"Experiments with intense photon and electron beams have the potential to provide access to nontrivial properties of the recently discovered $d^*(2380)$ hexaquark including its size, structure, magnetic moment, quadrupole and octupole deformations. In this paper we investigate the sensitivity of ongoing and planned experiments to various properties of the $d^*(2380)$, employing models based on both constituent quark and pion cloud frameworks. Our calculations indicate that for photoinduced reactions on the deuteron the $d^*(2380)$ is predominantly produced from the $D-wave$ component of the deu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.00713","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1905.00713/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1905.00713","created_at":"2026-07-04T23:50:39.828947+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.00713v2","created_at":"2026-07-04T23:50:39.828947+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.00713","created_at":"2026-07-04T23:50:39.828947+00:00"},{"alias_kind":"pith_short_12","alias_value":"OQ3RJ3RKVYBU","created_at":"2026-07-04T23:50:39.828947+00:00"},{"alias_kind":"pith_short_16","alias_value":"OQ3RJ3RKVYBUL3ED","created_at":"2026-07-04T23:50:39.828947+00:00"},{"alias_kind":"pith_short_8","alias_value":"OQ3RJ3RK","created_at":"2026-07-04T23:50:39.828947+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.17549","citing_title":"Electromagnetic form factors and structure of the $T_{bb}$ tetraquark from lattice QCD","ref_index":85,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ","json":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ.json","graph_json":"https://pith.science/api/pith-number/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/graph.json","events_json":"https://pith.science/api/pith-number/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/events.json","paper":"https://pith.science/paper/OQ3RJ3RK"},"agent_actions":{"view_html":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ","download_json":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ.json","view_paper":"https://pith.science/paper/OQ3RJ3RK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.00713&json=true","fetch_graph":"https://pith.science/api/pith-number/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/graph.json","fetch_events":"https://pith.science/api/pith-number/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/action/storage_attestation","attest_author":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/action/author_attestation","sign_citation":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/action/citation_signature","submit_replication":"https://pith.science/pith/OQ3RJ3RKVYBUL3EDMHPTPEWASZ/action/replication_record"}},"created_at":"2026-07-04T23:50:39.828947+00:00","updated_at":"2026-07-04T23:50:39.828947+00:00"}