{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:JVVEKVL4TPGM4JYR2QS72KYQIH","short_pith_number":"pith:JVVEKVL4","schema_version":"1.0","canonical_sha256":"4d6a45557c9bccce2711d425fd2b1041eaffae049c91f5d51655f137e3b6b3fd","source":{"kind":"arxiv","id":"2305.09436","version":1},"attestation_state":"computed","paper":{"title":"Searching for the open flavor tetraquark $T^{++}_{c\\bar{s}0}(2900)$ in the process $B^+\\to K^+ D^+ D^-$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, En Wang, Man-Yu Duan","submitted_at":"2023-05-16T13:48:44Z","abstract_excerpt":"Inspired by recent observations of $T_{c\\bar{s}0}(2900)^0$ in the $D_s^+ \\pi^-$ invariant mass distribution of $B^0 \\to \\bar{D}^0 D_s^+ \\pi^-$ decay and $T_{c\\bar{s}0}(2900)^{++}$ in the $D_s^+ \\pi^+$ invariant mass distribution of $B^+ \\to D^- D_s^+ \\pi^+$ decay, we investigate the $T_{c\\bar{s}0}(2900)^{++}$ contribution to the $B^+ \\to K^+ D^+ D^-$ decay in a molecular scenario, where we consider $T_{c\\bar{s}0}(2900)r^{++}$ as a $D^{\\ast +} K^{\\ast+}$ molecular state. Our estimations indicate that the fit fraction of $T_{c\\bar{s}0}(2900)^{++}$ in the $B^+ \\to K^+ D^+ D^-$ is about $12.5\\%$, "},"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":"2305.09436","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-05-16T13:48:44Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"b62c0918516a839343075e6e1060e7797284efd1f9b1a576b462daabe70c2bb3","abstract_canon_sha256":"9aa5d40850320c856ad841948886beb6f1a88d2b42c1a4273461f979a955b225"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:10:47.925380Z","signature_b64":"jDoCKZjeNUP368Cx9WZ/u7ls9Fv/4RDgQoFppptdeSgljzewF8+JXzQQBtjLpP8LPlAjKuMNBn2iPN4qqVerAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d6a45557c9bccce2711d425fd2b1041eaffae049c91f5d51655f137e3b6b3fd","last_reissued_at":"2026-07-05T06:10:47.925026Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:10:47.925026Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Searching for the open flavor tetraquark $T^{++}_{c\\bar{s}0}(2900)$ in the process $B^+\\to K^+ D^+ D^-$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, En Wang, Man-Yu Duan","submitted_at":"2023-05-16T13:48:44Z","abstract_excerpt":"Inspired by recent observations of $T_{c\\bar{s}0}(2900)^0$ in the $D_s^+ \\pi^-$ invariant mass distribution of $B^0 \\to \\bar{D}^0 D_s^+ \\pi^-$ decay and $T_{c\\bar{s}0}(2900)^{++}$ in the $D_s^+ \\pi^+$ invariant mass distribution of $B^+ \\to D^- D_s^+ \\pi^+$ decay, we investigate the $T_{c\\bar{s}0}(2900)^{++}$ contribution to the $B^+ \\to K^+ D^+ D^-$ decay in a molecular scenario, where we consider $T_{c\\bar{s}0}(2900)r^{++}$ as a $D^{\\ast +} K^{\\ast+}$ molecular state. Our estimations indicate that the fit fraction of $T_{c\\bar{s}0}(2900)^{++}$ in the $B^+ \\to K^+ D^+ D^-$ is about $12.5\\%$, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.09436","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/2305.09436/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":"2305.09436","created_at":"2026-07-05T06:10:47.925081+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.09436v1","created_at":"2026-07-05T06:10:47.925081+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.09436","created_at":"2026-07-05T06:10:47.925081+00:00"},{"alias_kind":"pith_short_12","alias_value":"JVVEKVL4TPGM","created_at":"2026-07-05T06:10:47.925081+00:00"},{"alias_kind":"pith_short_16","alias_value":"JVVEKVL4TPGM4JYR","created_at":"2026-07-05T06:10:47.925081+00:00"},{"alias_kind":"pith_short_8","alias_value":"JVVEKVL4","created_at":"2026-07-05T06:10:47.925081+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.05799","citing_title":"$T^a_{c\\bar{s}0}(2900)$, $T_{cs0}^*(2870)^0$, and other singly-heavy tetraquark states","ref_index":60,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19553","citing_title":"Exotic $T^*_{csJ}$ and $T^*_{c\\bar{s}J}$ states and coupled-channel scattering at the $SU(3)$ flavour symmetric point from lattice QCD","ref_index":3,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH","json":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH.json","graph_json":"https://pith.science/api/pith-number/JVVEKVL4TPGM4JYR2QS72KYQIH/graph.json","events_json":"https://pith.science/api/pith-number/JVVEKVL4TPGM4JYR2QS72KYQIH/events.json","paper":"https://pith.science/paper/JVVEKVL4"},"agent_actions":{"view_html":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH","download_json":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH.json","view_paper":"https://pith.science/paper/JVVEKVL4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.09436&json=true","fetch_graph":"https://pith.science/api/pith-number/JVVEKVL4TPGM4JYR2QS72KYQIH/graph.json","fetch_events":"https://pith.science/api/pith-number/JVVEKVL4TPGM4JYR2QS72KYQIH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH/action/storage_attestation","attest_author":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH/action/author_attestation","sign_citation":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH/action/citation_signature","submit_replication":"https://pith.science/pith/JVVEKVL4TPGM4JYR2QS72KYQIH/action/replication_record"}},"created_at":"2026-07-05T06:10:47.925081+00:00","updated_at":"2026-07-05T06:10:47.925081+00:00"}