{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:T555JCFU4Q6EKEFTEQHABWSQI7","short_pith_number":"pith:T555JCFU","schema_version":"1.0","canonical_sha256":"9f7bd488b4e43c4510b3240e00da5047e3523bc0634dd1fec43f19d082a56f86","source":{"kind":"arxiv","id":"2011.04980","version":4},"attestation_state":"computed","paper":{"title":"Molecular states from $D^{(*)}\\bar{D}^{(*)}/B^{(*)}\\bar{B}^{(*)}$ and $D^{(*)}D^{(*)}/\\bar{B}^{(*)}\\bar{B}^{(*)}$ interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Han-Yu Jiang, Jun He, Zuo-Ming Ding","submitted_at":"2020-11-10T08:58:27Z","abstract_excerpt":"In this work, we preform a systematic investigation about hidden heavy and doubly heavy molecular states from the $D^{(*)}\\bar{D}^{(*)}/B^{(*)}\\bar{B}^{(*)}$ and $D^{(*)}D^{(*)}/\\bar{B}^{(*)}\\bar{B}^{(*)}$ interactions in the quasipotential Bethe-Salpeter equation (qBSE) approach. With the help of Lagrangians with heavy quark and chiral symmetries, interaction potentials are constructed within the one-boson-exchange model in which we include the $\\pi$, $\\eta$, $\\rho$, $\\omega$ and $\\sigma$ exchanges, as well as $J/\\psi$ or $\\Upsilon$ exchange. Possible bound states from the interactions consid"},"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":"2011.04980","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-11-10T08:58:27Z","cross_cats_sorted":[],"title_canon_sha256":"8aef5befc34e16969111666cfcfce1f5c5576cb6c5f80d5854fbc8d02cfdeed6","abstract_canon_sha256":"3a202343cd2724be7065018a2bbe81801a8ac3ce0838006224f569ff0c9d3073"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:25:29.352572Z","signature_b64":"Y+hWk6pDOtngMgtVOtkSvAo0WG6FEV7l6dnPkYvOjg07uoo35Pp9tcaQaPccV/abO+0Rn6wrUpYhgvyIbm+mBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9f7bd488b4e43c4510b3240e00da5047e3523bc0634dd1fec43f19d082a56f86","last_reissued_at":"2026-07-05T03:25:29.352175Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:25:29.352175Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Molecular states from $D^{(*)}\\bar{D}^{(*)}/B^{(*)}\\bar{B}^{(*)}$ and $D^{(*)}D^{(*)}/\\bar{B}^{(*)}\\bar{B}^{(*)}$ interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Han-Yu Jiang, Jun He, Zuo-Ming Ding","submitted_at":"2020-11-10T08:58:27Z","abstract_excerpt":"In this work, we preform a systematic investigation about hidden heavy and doubly heavy molecular states from the $D^{(*)}\\bar{D}^{(*)}/B^{(*)}\\bar{B}^{(*)}$ and $D^{(*)}D^{(*)}/\\bar{B}^{(*)}\\bar{B}^{(*)}$ interactions in the quasipotential Bethe-Salpeter equation (qBSE) approach. With the help of Lagrangians with heavy quark and chiral symmetries, interaction potentials are constructed within the one-boson-exchange model in which we include the $\\pi$, $\\eta$, $\\rho$, $\\omega$ and $\\sigma$ exchanges, as well as $J/\\psi$ or $\\Upsilon$ exchange. Possible bound states from the interactions consid"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.04980","kind":"arxiv","version":4},"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/2011.04980/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":"2011.04980","created_at":"2026-07-05T03:25:29.352231+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.04980v4","created_at":"2026-07-05T03:25:29.352231+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.04980","created_at":"2026-07-05T03:25:29.352231+00:00"},{"alias_kind":"pith_short_12","alias_value":"T555JCFU4Q6E","created_at":"2026-07-05T03:25:29.352231+00:00"},{"alias_kind":"pith_short_16","alias_value":"T555JCFU4Q6EKEFT","created_at":"2026-07-05T03:25:29.352231+00:00"},{"alias_kind":"pith_short_8","alias_value":"T555JCFU","created_at":"2026-07-05T03:25:29.352231+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.01921","citing_title":"Hunting for $B\\bar B$ molecular state $X_{b0}$ via radiative transition of $\\Upsilon(10753)$","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7","json":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7.json","graph_json":"https://pith.science/api/pith-number/T555JCFU4Q6EKEFTEQHABWSQI7/graph.json","events_json":"https://pith.science/api/pith-number/T555JCFU4Q6EKEFTEQHABWSQI7/events.json","paper":"https://pith.science/paper/T555JCFU"},"agent_actions":{"view_html":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7","download_json":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7.json","view_paper":"https://pith.science/paper/T555JCFU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.04980&json=true","fetch_graph":"https://pith.science/api/pith-number/T555JCFU4Q6EKEFTEQHABWSQI7/graph.json","fetch_events":"https://pith.science/api/pith-number/T555JCFU4Q6EKEFTEQHABWSQI7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7/action/storage_attestation","attest_author":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7/action/author_attestation","sign_citation":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7/action/citation_signature","submit_replication":"https://pith.science/pith/T555JCFU4Q6EKEFTEQHABWSQI7/action/replication_record"}},"created_at":"2026-07-05T03:25:29.352231+00:00","updated_at":"2026-07-05T03:25:29.352231+00:00"}