{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:553QFJGOETQWSACQYQSQMMDICK","short_pith_number":"pith:553QFJGO","schema_version":"1.0","canonical_sha256":"ef7702a4ce24e1690050c42506306812ac3326987bc7c347be0271be3a889d6b","source":{"kind":"arxiv","id":"1401.7105","version":1},"attestation_state":"computed","paper":{"title":"Size measurement of dynamically generated hadronic resonances with finite volume effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"nucl-th","authors_text":"Kyoto), Takayasu Sekihara (KEK, Tetsuo Hyodo (Kyoto U., Tsukuba), Yukawa Inst.","submitted_at":"2014-01-28T07:35:55Z","abstract_excerpt":"The structures of the hyperon resonance $\\Lambda (1405)$ and the scalar mesons $\\sigma$, $f_{0}(980)$, and $a_{0}(980)$ are investigated based on the coupled-channels chiral dynamics with finite volume effect. The finite volume effect is utilized to extract the coupling constant, compositeness, and mean squared distance between two constituents of a Feshbach resonance state as well as a stable bound state. In this framework, the real-valued size of the resonance can be defined from the downward shift of the resonance pole according to the decreasing finite box size $L$ on a given closed channe"},"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":"1401.7105","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-01-28T07:35:55Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"1d6722585c11f03a547c96e711afad1e859e6efad05cf46907fd5d3ccc9343f8","abstract_canon_sha256":"ae44287df6e32be3575085beeb2eb9de3eb3e4ae0ed5ede6243929343d1c8635"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:50.849122Z","signature_b64":"GMgipjj+sughFuq9MVPYg8Rnhm1MrHseoooWenPHOOdI7K66tvYD2YdVlC3BQ9vFnoxg7GWONDsvrdizVwcqAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef7702a4ce24e1690050c42506306812ac3326987bc7c347be0271be3a889d6b","last_reissued_at":"2026-05-18T03:00:50.848504Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:50.848504Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Size measurement of dynamically generated hadronic resonances with finite volume effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"nucl-th","authors_text":"Kyoto), Takayasu Sekihara (KEK, Tetsuo Hyodo (Kyoto U., Tsukuba), Yukawa Inst.","submitted_at":"2014-01-28T07:35:55Z","abstract_excerpt":"The structures of the hyperon resonance $\\Lambda (1405)$ and the scalar mesons $\\sigma$, $f_{0}(980)$, and $a_{0}(980)$ are investigated based on the coupled-channels chiral dynamics with finite volume effect. The finite volume effect is utilized to extract the coupling constant, compositeness, and mean squared distance between two constituents of a Feshbach resonance state as well as a stable bound state. In this framework, the real-valued size of the resonance can be defined from the downward shift of the resonance pole according to the decreasing finite box size $L$ on a given closed channe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.7105","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":"1401.7105","created_at":"2026-05-18T03:00:50.848580+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.7105v1","created_at":"2026-05-18T03:00:50.848580+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.7105","created_at":"2026-05-18T03:00:50.848580+00:00"},{"alias_kind":"pith_short_12","alias_value":"553QFJGOETQW","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_16","alias_value":"553QFJGOETQWSACQ","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_8","alias_value":"553QFJGO","created_at":"2026-05-18T12:28:14.216126+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/553QFJGOETQWSACQYQSQMMDICK","json":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK.json","graph_json":"https://pith.science/api/pith-number/553QFJGOETQWSACQYQSQMMDICK/graph.json","events_json":"https://pith.science/api/pith-number/553QFJGOETQWSACQYQSQMMDICK/events.json","paper":"https://pith.science/paper/553QFJGO"},"agent_actions":{"view_html":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK","download_json":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK.json","view_paper":"https://pith.science/paper/553QFJGO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.7105&json=true","fetch_graph":"https://pith.science/api/pith-number/553QFJGOETQWSACQYQSQMMDICK/graph.json","fetch_events":"https://pith.science/api/pith-number/553QFJGOETQWSACQYQSQMMDICK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK/action/storage_attestation","attest_author":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK/action/author_attestation","sign_citation":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK/action/citation_signature","submit_replication":"https://pith.science/pith/553QFJGOETQWSACQYQSQMMDICK/action/replication_record"}},"created_at":"2026-05-18T03:00:50.848580+00:00","updated_at":"2026-05-18T03:00:50.848580+00:00"}