{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:4526JVQFSHYD25UX52V23RKOQ2","short_pith_number":"pith:4526JVQF","schema_version":"1.0","canonical_sha256":"e775e4d60591f03d7697eeabadc54e868dc379cb2f0899f8515a1d048f7c62e5","source":{"kind":"arxiv","id":"2211.01846","version":2},"attestation_state":"computed","paper":{"title":"Theoretical investigation of the molecular nature of $D_{s0}^*(2317)$ and $D_{s1}(2460)$ and the possibility of observing the $D\\bar{D}K$ bound state $K_{c\\bar{c}}(4180)$ in inclusive $e^+e^-\\to c\\bar{c}$ collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Tian-Chen Wu","submitted_at":"2022-11-03T14:33:16Z","abstract_excerpt":"Searching for exotic multiquark states and elucidating their nature remains a central topic in understanding quantum chromodynamics--the underlying theory of the strong interaction. Two of the most studied such states are the charm-strange states $D_{s0}^*(2317)$ and $D_{s1}(2460)$. In this letter, we show for the first time that their prompt production yields in inclusive $e^+e^-\\to c\\bar{c}$ collisions near $\\sqrt{s}=10.6$ GeV measured by the BABAR Collaboration, $Y(D_{s0}^*(2317))$ and $Y(D_{s1}(2460))$, in particular the ratio $R=Y(D_{s0}^*(2317))/Y(D_{s1}(2460))$, can be well explained in"},"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":"2211.01846","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-11-03T14:33:16Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"c8ae6690aed5a8be1b958d41a29663d351ccf7e2d4763c656e61a0380022d1fc","abstract_canon_sha256":"8bd28153a1c0099f4872a11b52b386e9645c1b1cf57d78c19e5da392aa3767fd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:34:21.025507Z","signature_b64":"9FryO/vNXiHa1GuOK7wbLvQkn6w0Hg7Wxokm7d2ABef24jycYU3UUopP7abebmlt3EykTQWCd7vkoaQatI4yAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e775e4d60591f03d7697eeabadc54e868dc379cb2f0899f8515a1d048f7c62e5","last_reissued_at":"2026-07-05T06:34:21.025165Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:34:21.025165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theoretical investigation of the molecular nature of $D_{s0}^*(2317)$ and $D_{s1}(2460)$ and the possibility of observing the $D\\bar{D}K$ bound state $K_{c\\bar{c}}(4180)$ in inclusive $e^+e^-\\to c\\bar{c}$ collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Tian-Chen Wu","submitted_at":"2022-11-03T14:33:16Z","abstract_excerpt":"Searching for exotic multiquark states and elucidating their nature remains a central topic in understanding quantum chromodynamics--the underlying theory of the strong interaction. Two of the most studied such states are the charm-strange states $D_{s0}^*(2317)$ and $D_{s1}(2460)$. In this letter, we show for the first time that their prompt production yields in inclusive $e^+e^-\\to c\\bar{c}$ collisions near $\\sqrt{s}=10.6$ GeV measured by the BABAR Collaboration, $Y(D_{s0}^*(2317))$ and $Y(D_{s1}(2460))$, in particular the ratio $R=Y(D_{s0}^*(2317))/Y(D_{s1}(2460))$, can be well explained in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.01846","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/2211.01846/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":"2211.01846","created_at":"2026-07-05T06:34:21.025217+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.01846v2","created_at":"2026-07-05T06:34:21.025217+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.01846","created_at":"2026-07-05T06:34:21.025217+00:00"},{"alias_kind":"pith_short_12","alias_value":"4526JVQFSHYD","created_at":"2026-07-05T06:34:21.025217+00:00"},{"alias_kind":"pith_short_16","alias_value":"4526JVQFSHYD25UX","created_at":"2026-07-05T06:34:21.025217+00:00"},{"alias_kind":"pith_short_8","alias_value":"4526JVQF","created_at":"2026-07-05T06:34:21.025217+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.11358","citing_title":"Implication of the existence of $J^{PC}=0^{--}$ $\\bar{D}_sDK$ bound state on nature of $D_{s0}^*(2317)$ and new configuration of exotic state","ref_index":41,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2","json":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2.json","graph_json":"https://pith.science/api/pith-number/4526JVQFSHYD25UX52V23RKOQ2/graph.json","events_json":"https://pith.science/api/pith-number/4526JVQFSHYD25UX52V23RKOQ2/events.json","paper":"https://pith.science/paper/4526JVQF"},"agent_actions":{"view_html":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2","download_json":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2.json","view_paper":"https://pith.science/paper/4526JVQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.01846&json=true","fetch_graph":"https://pith.science/api/pith-number/4526JVQFSHYD25UX52V23RKOQ2/graph.json","fetch_events":"https://pith.science/api/pith-number/4526JVQFSHYD25UX52V23RKOQ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2/action/storage_attestation","attest_author":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2/action/author_attestation","sign_citation":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2/action/citation_signature","submit_replication":"https://pith.science/pith/4526JVQFSHYD25UX52V23RKOQ2/action/replication_record"}},"created_at":"2026-07-05T06:34:21.025217+00:00","updated_at":"2026-07-05T06:34:21.025217+00:00"}