{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:7ILSQIJSXF3QEIAGATVIH2YQ6V","short_pith_number":"pith:7ILSQIJS","schema_version":"1.0","canonical_sha256":"fa17282132b97702200604ea83eb10f579fe5f80fce7e5f316166d45365aa058","source":{"kind":"arxiv","id":"2502.10798","version":1},"attestation_state":"computed","paper":{"title":"Triply heavy tetraquark states with different flavors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hui-Min Yang, Shi-Lin Zhu, Wei-Lin Wu, Yao Ma","submitted_at":"2025-02-15T13:40:09Z","abstract_excerpt":"We investigate the $S$-wave triply heavy tetraquark systems, including the $QQ^{(\\prime)}\\bar Q^{(\\prime)}\\bar q$ and $QQ^{(\\prime)}\\bar Q^{(\\prime)}\\bar s$ configurations ($Q^{(\\prime)} = c, b$, $q = u, d$) with spin-parity $J^P = 0^+$, $1^+$, and $2^+$, within the framework of the constituent quark model. We construct the wave functions for these systems, incorporating complete color-spin wave functions and spatial wave functions with three different Jacobi coordinate configurations. We use complex scaling and Gaussian expansion method to solve the complex-scaled four-body Schr\\\"{o}dinger eq"},"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":"2502.10798","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-15T13:40:09Z","cross_cats_sorted":[],"title_canon_sha256":"d86be20f48403239186b6daefd19148671b570d893b8be7dab5398ffd20e31fd","abstract_canon_sha256":"4e97168f6258c6643796b83b25cefa60d5e0647534552b1ffa9425ed3e9adb5f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:14:58.287298Z","signature_b64":"fQrw4LPRg1sIzEIZutetbomh8r7H2fPF4aVLSAAGxyOG7G5ItWnCAgbOPMUtmMg0F9UQX2cmZzS9rPUIzDPSBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa17282132b97702200604ea83eb10f579fe5f80fce7e5f316166d45365aa058","last_reissued_at":"2026-07-05T10:14:58.286832Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:14:58.286832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Triply heavy tetraquark states with different flavors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hui-Min Yang, Shi-Lin Zhu, Wei-Lin Wu, Yao Ma","submitted_at":"2025-02-15T13:40:09Z","abstract_excerpt":"We investigate the $S$-wave triply heavy tetraquark systems, including the $QQ^{(\\prime)}\\bar Q^{(\\prime)}\\bar q$ and $QQ^{(\\prime)}\\bar Q^{(\\prime)}\\bar s$ configurations ($Q^{(\\prime)} = c, b$, $q = u, d$) with spin-parity $J^P = 0^+$, $1^+$, and $2^+$, within the framework of the constituent quark model. We construct the wave functions for these systems, incorporating complete color-spin wave functions and spatial wave functions with three different Jacobi coordinate configurations. We use complex scaling and Gaussian expansion method to solve the complex-scaled four-body Schr\\\"{o}dinger eq"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.10798","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/2502.10798/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":"2502.10798","created_at":"2026-07-05T10:14:58.286887+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.10798v1","created_at":"2026-07-05T10:14:58.286887+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.10798","created_at":"2026-07-05T10:14:58.286887+00:00"},{"alias_kind":"pith_short_12","alias_value":"7ILSQIJSXF3Q","created_at":"2026-07-05T10:14:58.286887+00:00"},{"alias_kind":"pith_short_16","alias_value":"7ILSQIJSXF3QEIAG","created_at":"2026-07-05T10:14:58.286887+00:00"},{"alias_kind":"pith_short_8","alias_value":"7ILSQIJS","created_at":"2026-07-05T10:14:58.286887+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.05793","citing_title":"Compactness, mass spectra, and strong stability of singly heavy tetraquarks","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V","json":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V.json","graph_json":"https://pith.science/api/pith-number/7ILSQIJSXF3QEIAGATVIH2YQ6V/graph.json","events_json":"https://pith.science/api/pith-number/7ILSQIJSXF3QEIAGATVIH2YQ6V/events.json","paper":"https://pith.science/paper/7ILSQIJS"},"agent_actions":{"view_html":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V","download_json":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V.json","view_paper":"https://pith.science/paper/7ILSQIJS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.10798&json=true","fetch_graph":"https://pith.science/api/pith-number/7ILSQIJSXF3QEIAGATVIH2YQ6V/graph.json","fetch_events":"https://pith.science/api/pith-number/7ILSQIJSXF3QEIAGATVIH2YQ6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V/action/storage_attestation","attest_author":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V/action/author_attestation","sign_citation":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V/action/citation_signature","submit_replication":"https://pith.science/pith/7ILSQIJSXF3QEIAGATVIH2YQ6V/action/replication_record"}},"created_at":"2026-07-05T10:14:58.286887+00:00","updated_at":"2026-07-05T10:14:58.286887+00:00"}