{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:3K7M3AYSLPCO7IE6SRWR7P5YDS","short_pith_number":"pith:3K7M3AYS","schema_version":"1.0","canonical_sha256":"dabecd83125bc4efa09e946d1fbfb81cbb46c3c9f52c9780414f3bb72a70d467","source":{"kind":"arxiv","id":"1410.0137","version":1},"attestation_state":"computed","paper":{"title":"$\\bar D^*D^*_0$ and $\\bar B^*B^*_0 (1^--)$ molecules at N2LO from QSSR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Rabemananjara, F.Fanomezana, S.Narison","submitted_at":"2014-10-01T07:56:48Z","abstract_excerpt":"We estimate the $\\bar D^*D^*_0$ and $\\bar B^*B^*_0(1^--)$ molecules masses and couplings using QCD spectral sum rules (QSSR)known perturbatively to N2LO of PT series and including the contributions of non-perturabtive condensates up to the dimension-eight. Our results improve earlier LO results obtained from QSSR in the current literature. We obtain $M_{D^*D^*_0} = 5244(228)$ MeV which is heavier than the experimental candidates Y(4260); Y(4360); Y(4660) suggesting that they cannot be pure molecule states. We predict $M_{B^*B^*_0}= 11920(159)$ MeV to be tested in B-factory experiments."},"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":"1410.0137","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-10-01T07:56:48Z","cross_cats_sorted":[],"title_canon_sha256":"679be5e84ec785a4c1095655438c2f013b1ea0e9fa38e869370be16e3f162f7a","abstract_canon_sha256":"13ba30bf9611ca0f4313b74039c8180d1ad367b74a608f286284d78539a59357"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:17.917351Z","signature_b64":"wlYp+GWSyuH5RYUZe33wURPNfVwI+P9DuRSZfT1sCsJN9eVG7mlBo+fnqzhNqGgJq6I/36w6LFsWfanbT8pjAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dabecd83125bc4efa09e946d1fbfb81cbb46c3c9f52c9780414f3bb72a70d467","last_reissued_at":"2026-05-18T02:41:17.916856Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:17.916856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\bar D^*D^*_0$ and $\\bar B^*B^*_0 (1^--)$ molecules at N2LO from QSSR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Rabemananjara, F.Fanomezana, S.Narison","submitted_at":"2014-10-01T07:56:48Z","abstract_excerpt":"We estimate the $\\bar D^*D^*_0$ and $\\bar B^*B^*_0(1^--)$ molecules masses and couplings using QCD spectral sum rules (QSSR)known perturbatively to N2LO of PT series and including the contributions of non-perturabtive condensates up to the dimension-eight. Our results improve earlier LO results obtained from QSSR in the current literature. We obtain $M_{D^*D^*_0} = 5244(228)$ MeV which is heavier than the experimental candidates Y(4260); Y(4360); Y(4660) suggesting that they cannot be pure molecule states. We predict $M_{B^*B^*_0}= 11920(159)$ MeV to be tested in B-factory experiments."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0137","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":"1410.0137","created_at":"2026-05-18T02:41:17.916934+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.0137v1","created_at":"2026-05-18T02:41:17.916934+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0137","created_at":"2026-05-18T02:41:17.916934+00:00"},{"alias_kind":"pith_short_12","alias_value":"3K7M3AYSLPCO","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"3K7M3AYSLPCO7IE6","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"3K7M3AYS","created_at":"2026-05-18T12:28:11.866339+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/3K7M3AYSLPCO7IE6SRWR7P5YDS","json":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS.json","graph_json":"https://pith.science/api/pith-number/3K7M3AYSLPCO7IE6SRWR7P5YDS/graph.json","events_json":"https://pith.science/api/pith-number/3K7M3AYSLPCO7IE6SRWR7P5YDS/events.json","paper":"https://pith.science/paper/3K7M3AYS"},"agent_actions":{"view_html":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS","download_json":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS.json","view_paper":"https://pith.science/paper/3K7M3AYS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.0137&json=true","fetch_graph":"https://pith.science/api/pith-number/3K7M3AYSLPCO7IE6SRWR7P5YDS/graph.json","fetch_events":"https://pith.science/api/pith-number/3K7M3AYSLPCO7IE6SRWR7P5YDS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS/action/storage_attestation","attest_author":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS/action/author_attestation","sign_citation":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS/action/citation_signature","submit_replication":"https://pith.science/pith/3K7M3AYSLPCO7IE6SRWR7P5YDS/action/replication_record"}},"created_at":"2026-05-18T02:41:17.916934+00:00","updated_at":"2026-05-18T02:41:17.916934+00:00"}