{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:X7ZBN7OSH4KY2MQDS34H2OOMAL","short_pith_number":"pith:X7ZBN7OS","schema_version":"1.0","canonical_sha256":"bff216fdd23f158d320396f87d39cc02ef7ff2ca443cbc08efaf9663987b0949","source":{"kind":"arxiv","id":"2603.18610","version":2},"attestation_state":"computed","paper":{"title":"Signatures of the $\\Omega(2012)^{-}$ state in $\\Xi^*\\bar K$ Correlation Functions","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Albert Feijoo, Jia-Xin Lin, Miguel Albaladejo, Pablo Encarnaci\\'on","submitted_at":"2026-03-19T08:29:50Z","abstract_excerpt":"We investigate the $\\Omega(2012)$ resonance in the strangeness $S=-3$ sector within a coupled-channel chiral unitary approach and present the first quantitative predictions for femtoscopic correlation functions directly sensitive to its dynamics. The $\\Omega(2012)$ is dynamically generated as a quasi-bound $\\Xi^{\\ast}\\bar K$-$\\Omega\\eta$ molecular state, with its coupling to the $\\Xi\\bar{K}$ channel driven by $d$-wave transitions. Model parameters are constrained by the measured mass, width, and the Belle determination of the branching fraction $\\mathcal R^{\\Xi\\bar K\\pi}_{\\Xi\\bar K}$, yielding"},"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":"2603.18610","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T08:29:50Z","cross_cats_sorted":[],"title_canon_sha256":"eb120549df1804ebc4f5b8e39216f09bdec8e5a11aed16ed85455fd5df1fdc85","abstract_canon_sha256":"89cb25eb5ce39bf2ffd3ad36a84dc23738a2ca21bd06985057f15da942cf60a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-23T01:13:04.421918Z","signature_b64":"eQkUaYBKxE/Jj0T/x8JD4Y8BnRQNTRWYrp60FmV7my0JJaQmnbUJ7+Xk2PgPMAcc0ebdoRk+g4LQaoEKR4N+AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bff216fdd23f158d320396f87d39cc02ef7ff2ca443cbc08efaf9663987b0949","last_reissued_at":"2026-06-23T01:13:04.421281Z","signature_status":"signed_v1","first_computed_at":"2026-06-23T01:13:04.421281Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Signatures of the $\\Omega(2012)^{-}$ state in $\\Xi^*\\bar K$ Correlation Functions","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Albert Feijoo, Jia-Xin Lin, Miguel Albaladejo, Pablo Encarnaci\\'on","submitted_at":"2026-03-19T08:29:50Z","abstract_excerpt":"We investigate the $\\Omega(2012)$ resonance in the strangeness $S=-3$ sector within a coupled-channel chiral unitary approach and present the first quantitative predictions for femtoscopic correlation functions directly sensitive to its dynamics. The $\\Omega(2012)$ is dynamically generated as a quasi-bound $\\Xi^{\\ast}\\bar K$-$\\Omega\\eta$ molecular state, with its coupling to the $\\Xi\\bar{K}$ channel driven by $d$-wave transitions. Model parameters are constrained by the measured mass, width, and the Belle determination of the branching fraction $\\mathcal R^{\\Xi\\bar K\\pi}_{\\Xi\\bar K}$, yielding"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.18610","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/2603.18610/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":"2603.18610","created_at":"2026-06-23T01:13:04.421383+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.18610v2","created_at":"2026-06-23T01:13:04.421383+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.18610","created_at":"2026-06-23T01:13:04.421383+00:00"},{"alias_kind":"pith_short_12","alias_value":"X7ZBN7OSH4KY","created_at":"2026-06-23T01:13:04.421383+00:00"},{"alias_kind":"pith_short_16","alias_value":"X7ZBN7OSH4KY2MQD","created_at":"2026-06-23T01:13:04.421383+00:00"},{"alias_kind":"pith_short_8","alias_value":"X7ZBN7OS","created_at":"2026-06-23T01:13:04.421383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2604.25630","citing_title":"Probing the hadronic molecular nature of the $\\Omega(2012)$, $\\Omega(2380)$, and $\\Omega_c(3120)$ via femtoscopy correlation functions","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25630","citing_title":"Probing the hadronic molecular nature of the $\\Omega(2012)$, $\\Omega(2380)$, and $\\Omega_c(3120)$ via femtoscopy correlation functions","ref_index":70,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL","json":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL.json","graph_json":"https://pith.science/api/pith-number/X7ZBN7OSH4KY2MQDS34H2OOMAL/graph.json","events_json":"https://pith.science/api/pith-number/X7ZBN7OSH4KY2MQDS34H2OOMAL/events.json","paper":"https://pith.science/paper/X7ZBN7OS"},"agent_actions":{"view_html":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL","download_json":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL.json","view_paper":"https://pith.science/paper/X7ZBN7OS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.18610&json=true","fetch_graph":"https://pith.science/api/pith-number/X7ZBN7OSH4KY2MQDS34H2OOMAL/graph.json","fetch_events":"https://pith.science/api/pith-number/X7ZBN7OSH4KY2MQDS34H2OOMAL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL/action/storage_attestation","attest_author":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL/action/author_attestation","sign_citation":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL/action/citation_signature","submit_replication":"https://pith.science/pith/X7ZBN7OSH4KY2MQDS34H2OOMAL/action/replication_record"}},"created_at":"2026-06-23T01:13:04.421383+00:00","updated_at":"2026-06-23T01:13:04.421383+00:00"}