{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:MPEQMPRB2NXOJ4L6PJX2PDKF2M","short_pith_number":"pith:MPEQMPRB","schema_version":"1.0","canonical_sha256":"63c9063e21d36ee4f17e7a6fa78d45d30b9bbcd2e73160cd937dc8ab1af6c534","source":{"kind":"arxiv","id":"2012.05096","version":1},"attestation_state":"computed","paper":{"title":"Is $X(7200)$ the heavy anti-quark diquark symmetry partner of $ X(3872)$?","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Ming-Zhu Liu","submitted_at":"2020-12-09T15:05:49Z","abstract_excerpt":"The $D^{(\\ast)}\\Xi_{cc}^{(\\ast)}$ system and $\\bar{\\Xi}_{cc}^{(\\ast)}\\Xi_{cc}^{(\\ast)}$ system can be related to the $D^{(\\ast)}\\bar{D}^{(\\ast)}$ system via heavy anti-quark di-quark symmetry (HADS). In this work, we employ a contact-range effective field theory to systematically investigate the likely existence of molecules in these systems in terms of the hypothesis that X(3872) is a $1^{++}$~$D\\bar{D}^{\\ast}$ bound state in the isospin symmetry limit, with some of the unknown low energy constants estimated using the light-meson saturation approximation. In the meson-meson system, a $J^{PC}="},"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":"2012.05096","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2020-12-09T15:05:49Z","cross_cats_sorted":[],"title_canon_sha256":"3676ba7ff25f8a51b3317ad9be882410df2dbc61f4ea332bfb32e62563a01cc1","abstract_canon_sha256":"133e0de57a53afb3221a06e0bbf3a63d72e55e1fd4c29141100a3fbcb7a0702b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:23:21.958483Z","signature_b64":"cAPTcr+yFxHNHlb1OeUR5Zxi7LVTlkO/jmqPsyF6pnKWWjlP6+8G23r0VT+84qIcnki3YmxurtScbvjHHfHvCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"63c9063e21d36ee4f17e7a6fa78d45d30b9bbcd2e73160cd937dc8ab1af6c534","last_reissued_at":"2026-07-05T02:23:21.958010Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:23:21.958010Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Is $X(7200)$ the heavy anti-quark diquark symmetry partner of $ X(3872)$?","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Ming-Zhu Liu","submitted_at":"2020-12-09T15:05:49Z","abstract_excerpt":"The $D^{(\\ast)}\\Xi_{cc}^{(\\ast)}$ system and $\\bar{\\Xi}_{cc}^{(\\ast)}\\Xi_{cc}^{(\\ast)}$ system can be related to the $D^{(\\ast)}\\bar{D}^{(\\ast)}$ system via heavy anti-quark di-quark symmetry (HADS). In this work, we employ a contact-range effective field theory to systematically investigate the likely existence of molecules in these systems in terms of the hypothesis that X(3872) is a $1^{++}$~$D\\bar{D}^{\\ast}$ bound state in the isospin symmetry limit, with some of the unknown low energy constants estimated using the light-meson saturation approximation. In the meson-meson system, a $J^{PC}="},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.05096","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/2012.05096/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":"2012.05096","created_at":"2026-07-05T02:23:21.958067+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.05096v1","created_at":"2026-07-05T02:23:21.958067+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.05096","created_at":"2026-07-05T02:23:21.958067+00:00"},{"alias_kind":"pith_short_12","alias_value":"MPEQMPRB2NXO","created_at":"2026-07-05T02:23:21.958067+00:00"},{"alias_kind":"pith_short_16","alias_value":"MPEQMPRB2NXOJ4L6","created_at":"2026-07-05T02:23:21.958067+00:00"},{"alias_kind":"pith_short_8","alias_value":"MPEQMPRB","created_at":"2026-07-05T02:23:21.958067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.11433","citing_title":"A novel configuration of gluonic tetraquark state","ref_index":74,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M","json":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M.json","graph_json":"https://pith.science/api/pith-number/MPEQMPRB2NXOJ4L6PJX2PDKF2M/graph.json","events_json":"https://pith.science/api/pith-number/MPEQMPRB2NXOJ4L6PJX2PDKF2M/events.json","paper":"https://pith.science/paper/MPEQMPRB"},"agent_actions":{"view_html":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M","download_json":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M.json","view_paper":"https://pith.science/paper/MPEQMPRB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.05096&json=true","fetch_graph":"https://pith.science/api/pith-number/MPEQMPRB2NXOJ4L6PJX2PDKF2M/graph.json","fetch_events":"https://pith.science/api/pith-number/MPEQMPRB2NXOJ4L6PJX2PDKF2M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M/action/storage_attestation","attest_author":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M/action/author_attestation","sign_citation":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M/action/citation_signature","submit_replication":"https://pith.science/pith/MPEQMPRB2NXOJ4L6PJX2PDKF2M/action/replication_record"}},"created_at":"2026-07-05T02:23:21.958067+00:00","updated_at":"2026-07-05T02:23:21.958067+00:00"}