{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:47UEPN6EMUJW7RV6UIMDMCAGNX","short_pith_number":"pith:47UEPN6E","schema_version":"1.0","canonical_sha256":"e7e847b7c465136fc6bea2183608066de07280f9326718fb8c767749d1b4a4e0","source":{"kind":"arxiv","id":"2404.15186","version":1},"attestation_state":"computed","paper":{"title":"Diabatic Dynamical Diquark Bound States: Mass Corrections and Widths","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Richard F. Lebed, Steven R. Martinez","submitted_at":"2024-04-23T16:27:44Z","abstract_excerpt":"Using the diabatic formalism, which generalizes the adiabatic approximation in the Born-Oppenheimer formalism, we apply well-known Hamiltonian methods to calculate the effect of open di-meson thresholds that lie well below the mass of elementary $c\\bar c q\\bar q^\\prime$, $c\\bar c s\\bar s$, and $c \\bar c q \\bar s$ tetraquark bound states. We compute the resulting mass shifts for these states, as well as their decay widths to the corresponding meson pairs. Each mass eigenstate, originally produced using a bound-state approximation under the diabatic formalism, consists of an admixture of a compa"},"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":"2404.15186","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-04-23T16:27:44Z","cross_cats_sorted":[],"title_canon_sha256":"339aee3fbfb6f5038244c7af913cb842582f2adce4a9e86f252c552650d9d183","abstract_canon_sha256":"33b377ad6b42f092e2f6070461de428c0b4a7b2dd01da11fd201fbc75052b158"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:11:16.564763Z","signature_b64":"LKEd66Mw3bo7YaKjBRr0LOwDWvloKTDnpSuo+WrsdyiX4rUqR68bYkP7ttCHw8hMuhfEPRFJaxc/f6PndUDYBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7e847b7c465136fc6bea2183608066de07280f9326718fb8c767749d1b4a4e0","last_reissued_at":"2026-07-05T08:11:16.564256Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:11:16.564256Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Diabatic Dynamical Diquark Bound States: Mass Corrections and Widths","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Richard F. Lebed, Steven R. Martinez","submitted_at":"2024-04-23T16:27:44Z","abstract_excerpt":"Using the diabatic formalism, which generalizes the adiabatic approximation in the Born-Oppenheimer formalism, we apply well-known Hamiltonian methods to calculate the effect of open di-meson thresholds that lie well below the mass of elementary $c\\bar c q\\bar q^\\prime$, $c\\bar c s\\bar s$, and $c \\bar c q \\bar s$ tetraquark bound states. We compute the resulting mass shifts for these states, as well as their decay widths to the corresponding meson pairs. Each mass eigenstate, originally produced using a bound-state approximation under the diabatic formalism, consists of an admixture of a compa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.15186","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2404.15186/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":"2404.15186","created_at":"2026-07-05T08:11:16.564312+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.15186v1","created_at":"2026-07-05T08:11:16.564312+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.15186","created_at":"2026-07-05T08:11:16.564312+00:00"},{"alias_kind":"pith_short_12","alias_value":"47UEPN6EMUJW","created_at":"2026-07-05T08:11:16.564312+00:00"},{"alias_kind":"pith_short_16","alias_value":"47UEPN6EMUJW7RV6","created_at":"2026-07-05T08:11:16.564312+00:00"},{"alias_kind":"pith_short_8","alias_value":"47UEPN6E","created_at":"2026-07-05T08:11:16.564312+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.15704","citing_title":"Hidden-Strangeness Tetraquarks in the Dynamical Diquark Model","ref_index":72,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX","json":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX.json","graph_json":"https://pith.science/api/pith-number/47UEPN6EMUJW7RV6UIMDMCAGNX/graph.json","events_json":"https://pith.science/api/pith-number/47UEPN6EMUJW7RV6UIMDMCAGNX/events.json","paper":"https://pith.science/paper/47UEPN6E"},"agent_actions":{"view_html":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX","download_json":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX.json","view_paper":"https://pith.science/paper/47UEPN6E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.15186&json=true","fetch_graph":"https://pith.science/api/pith-number/47UEPN6EMUJW7RV6UIMDMCAGNX/graph.json","fetch_events":"https://pith.science/api/pith-number/47UEPN6EMUJW7RV6UIMDMCAGNX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX/action/storage_attestation","attest_author":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX/action/author_attestation","sign_citation":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX/action/citation_signature","submit_replication":"https://pith.science/pith/47UEPN6EMUJW7RV6UIMDMCAGNX/action/replication_record"}},"created_at":"2026-07-05T08:11:16.564312+00:00","updated_at":"2026-07-05T08:11:16.564312+00:00"}