{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LLZ5EAFJT5SQO6BR6OIRD5325A","short_pith_number":"pith:LLZ5EAFJ","schema_version":"1.0","canonical_sha256":"5af3d200a99f65077831f39111f77ae80f1ec772976050e5742a96fe47498a77","source":{"kind":"arxiv","id":"1403.4032","version":2},"attestation_state":"computed","paper":{"title":"Production of charm-strange hadronic molecules at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Feng-Kun Guo, Ulf-G. Mei{\\ss}ner, Wei Wang, Zhi Yang","submitted_at":"2014-03-17T09:15:42Z","abstract_excerpt":"We explore the inclusive hadroproduction of the D_{s0}^*(2317), D_{s1}(2460) and D_{sJ}(2860) states at the Large Hadron Collider under the assumption that these hadrons are S-wave meson-meson molecules. In addition, the D_{s2}(2910), a predicted bound state of the D_2(2460)K system, is also discussed. We first derive a factorisation formula for the production rates based on effective field theory. Then we make use of two MC event generators, Herwig and Pythia, to simulate the production of pairs of charmed mesons and kaons. Using effective field theory to handle the final state interaction am"},"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":"1403.4032","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-17T09:15:42Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"7b93946f87b7ecdd1e7f1c603aa93b03e5c828083c674d3558058433f409b745","abstract_canon_sha256":"16daa43297da68d9f7e408c0814a2ccacb2b9b492492e1826dd25bd41fa39138"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:49:55.576663Z","signature_b64":"ocKGUh1TiR6E3Kz/BFSQiDcXtbzVPJhbyegFtfpy6jCq/2JR1aX9KJNK9rS/4QNoYqmNGneJa+P1BX3sYDm0CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5af3d200a99f65077831f39111f77ae80f1ec772976050e5742a96fe47498a77","last_reissued_at":"2026-05-18T02:49:55.575934Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:49:55.575934Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of charm-strange hadronic molecules at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Feng-Kun Guo, Ulf-G. Mei{\\ss}ner, Wei Wang, Zhi Yang","submitted_at":"2014-03-17T09:15:42Z","abstract_excerpt":"We explore the inclusive hadroproduction of the D_{s0}^*(2317), D_{s1}(2460) and D_{sJ}(2860) states at the Large Hadron Collider under the assumption that these hadrons are S-wave meson-meson molecules. In addition, the D_{s2}(2910), a predicted bound state of the D_2(2460)K system, is also discussed. We first derive a factorisation formula for the production rates based on effective field theory. Then we make use of two MC event generators, Herwig and Pythia, to simulate the production of pairs of charmed mesons and kaons. Using effective field theory to handle the final state interaction am"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4032","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":""},"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":"1403.4032","created_at":"2026-05-18T02:49:55.576069+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.4032v2","created_at":"2026-05-18T02:49:55.576069+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4032","created_at":"2026-05-18T02:49:55.576069+00:00"},{"alias_kind":"pith_short_12","alias_value":"LLZ5EAFJT5SQ","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"LLZ5EAFJT5SQO6BR","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"LLZ5EAFJ","created_at":"2026-05-18T12:28:38.356838+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.19641","citing_title":"Determining the width of $D_{s0}^{*}(2317)$ by using $T_{c\\bar{s}0}^{a}(2327)$ in a molecular frame","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A","json":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A.json","graph_json":"https://pith.science/api/pith-number/LLZ5EAFJT5SQO6BR6OIRD5325A/graph.json","events_json":"https://pith.science/api/pith-number/LLZ5EAFJT5SQO6BR6OIRD5325A/events.json","paper":"https://pith.science/paper/LLZ5EAFJ"},"agent_actions":{"view_html":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A","download_json":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A.json","view_paper":"https://pith.science/paper/LLZ5EAFJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.4032&json=true","fetch_graph":"https://pith.science/api/pith-number/LLZ5EAFJT5SQO6BR6OIRD5325A/graph.json","fetch_events":"https://pith.science/api/pith-number/LLZ5EAFJT5SQO6BR6OIRD5325A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A/action/storage_attestation","attest_author":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A/action/author_attestation","sign_citation":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A/action/citation_signature","submit_replication":"https://pith.science/pith/LLZ5EAFJT5SQO6BR6OIRD5325A/action/replication_record"}},"created_at":"2026-05-18T02:49:55.576069+00:00","updated_at":"2026-05-18T02:49:55.576069+00:00"}