{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:IYFPTV2JH2AK6M5FOGPVXMC4EY","short_pith_number":"pith:IYFPTV2J","schema_version":"1.0","canonical_sha256":"460af9d7493e80af33a5719f5bb05c262b6680e61b33ba8c42dc730dbb362fc6","source":{"kind":"arxiv","id":"1405.7583","version":1},"attestation_state":"computed","paper":{"title":"On $X(3872)$ production in high energy heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Martinez Torres, F. S. Navarra, K. P. Khemchandani, Luciano M. Abreu, M. Nielsen","submitted_at":"2014-05-29T15:08:11Z","abstract_excerpt":"We have determined the production cross sections of the $X(3872)$ state in the reactions $\\bar D D\\to\\pi X$, $\\bar D^* D\\to \\pi X$ and $\\bar D^* D^*\\to\\pi X$, information which is useful for studies of the $X(3872)$ meson abundance in heavy ion collisions. We construct a formalism considering $X$ as a molecular bound state of $\\bar D^0 D^{*0} - \\textrm{c.c}$, $D^- D^{*+} - \\textrm{c.c}$ and $D^-_s D^{*+}_s - \\textrm{c.c}$. To obtain the amplitudes related to these processes we have made use of effective field Lagrangians. The evaluation of the cross section of the processes involving $D^*$ mes"},"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":"1405.7583","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-29T15:08:11Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"417539331d88ea12cec9eea1923ddd1f4cbfcaaa689eec5a46d294323059d411","abstract_canon_sha256":"64b7d57674eadaac3c5321d976c09ec30b80a873a358d93b5f7dabe795c76c96"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:30:40.264542Z","signature_b64":"FD3vwSIXRrYBn3XL9KcVnpFZCTns8H16AcXRHrteY8JbVxhiSDAnBCBKNSTAxzX9ooYkDlmHtK2YTDxUPFIsBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"460af9d7493e80af33a5719f5bb05c262b6680e61b33ba8c42dc730dbb362fc6","last_reissued_at":"2026-05-18T02:30:40.264099Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:30:40.264099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On $X(3872)$ production in high energy heavy ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Martinez Torres, F. S. Navarra, K. P. Khemchandani, Luciano M. Abreu, M. Nielsen","submitted_at":"2014-05-29T15:08:11Z","abstract_excerpt":"We have determined the production cross sections of the $X(3872)$ state in the reactions $\\bar D D\\to\\pi X$, $\\bar D^* D\\to \\pi X$ and $\\bar D^* D^*\\to\\pi X$, information which is useful for studies of the $X(3872)$ meson abundance in heavy ion collisions. We construct a formalism considering $X$ as a molecular bound state of $\\bar D^0 D^{*0} - \\textrm{c.c}$, $D^- D^{*+} - \\textrm{c.c}$ and $D^-_s D^{*+}_s - \\textrm{c.c}$. To obtain the amplitudes related to these processes we have made use of effective field Lagrangians. The evaluation of the cross section of the processes involving $D^*$ mes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.7583","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":""},"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":"1405.7583","created_at":"2026-05-18T02:30:40.264163+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.7583v1","created_at":"2026-05-18T02:30:40.264163+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.7583","created_at":"2026-05-18T02:30:40.264163+00:00"},{"alias_kind":"pith_short_12","alias_value":"IYFPTV2JH2AK","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_16","alias_value":"IYFPTV2JH2AK6M5F","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_8","alias_value":"IYFPTV2J","created_at":"2026-05-18T12:28:33.132498+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY","json":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY.json","graph_json":"https://pith.science/api/pith-number/IYFPTV2JH2AK6M5FOGPVXMC4EY/graph.json","events_json":"https://pith.science/api/pith-number/IYFPTV2JH2AK6M5FOGPVXMC4EY/events.json","paper":"https://pith.science/paper/IYFPTV2J"},"agent_actions":{"view_html":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY","download_json":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY.json","view_paper":"https://pith.science/paper/IYFPTV2J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.7583&json=true","fetch_graph":"https://pith.science/api/pith-number/IYFPTV2JH2AK6M5FOGPVXMC4EY/graph.json","fetch_events":"https://pith.science/api/pith-number/IYFPTV2JH2AK6M5FOGPVXMC4EY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY/action/storage_attestation","attest_author":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY/action/author_attestation","sign_citation":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY/action/citation_signature","submit_replication":"https://pith.science/pith/IYFPTV2JH2AK6M5FOGPVXMC4EY/action/replication_record"}},"created_at":"2026-05-18T02:30:40.264163+00:00","updated_at":"2026-05-18T02:30:40.264163+00:00"}