{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:LJFIMU23WYBQV5XIYIT4EXSCLE","short_pith_number":"pith:LJFIMU23","schema_version":"1.0","canonical_sha256":"5a4a86535bb6030af6e8c227c25e42590b3f1abb9adb81e44354d3faabd0e112","source":{"kind":"arxiv","id":"1806.05366","version":1},"attestation_state":"computed","paper":{"title":"Masses and Strong Decay properties of Radially Excited Bottom states B(2S)and B(2P) with their Strange Partners Bs(2S) and Bs(2P)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Upadhyay, Pallavi Gupta","submitted_at":"2018-06-14T05:15:44Z","abstract_excerpt":"In this paper, we analyzed the experimentally available radially excited charm mesons to predict the similar spectra for the n=2 bottom mesons. In the heavy quark effective theory, we explore the flavor independent parameters to calculate the masses for the experimentally unknown n=2 bottom mesons B(2S), B(2P), Bs(2S) and Bs(2P). We have also analyzed these bottom masses by applying the QCD and 1/mQ corrections to the lagrangian leading to the modification of flavor symmetry parameters as. Further strong decay widths are determined using these calculated masses to check the sensitivity of thes"},"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":"1806.05366","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-14T05:15:44Z","cross_cats_sorted":[],"title_canon_sha256":"d87d10d82e9c8688e1a011432e76b2ecb1b329aaf2c26b3711d4a9e5f66c049d","abstract_canon_sha256":"e18efffd902070ce5e061df607c02822e0d76991712987c2cfc0c076b413ed41"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:05.266571Z","signature_b64":"e372zoKS9QeA93NFWDy/2xjIhekW0j/wEA+Q0Q2/S3koU7pznkVWr7+OC3BKSvDq6jI6PjPjO+QpE5ZdpPlcBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a4a86535bb6030af6e8c227c25e42590b3f1abb9adb81e44354d3faabd0e112","last_reissued_at":"2026-05-18T00:03:05.266165Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:05.266165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Masses and Strong Decay properties of Radially Excited Bottom states B(2S)and B(2P) with their Strange Partners Bs(2S) and Bs(2P)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Upadhyay, Pallavi Gupta","submitted_at":"2018-06-14T05:15:44Z","abstract_excerpt":"In this paper, we analyzed the experimentally available radially excited charm mesons to predict the similar spectra for the n=2 bottom mesons. In the heavy quark effective theory, we explore the flavor independent parameters to calculate the masses for the experimentally unknown n=2 bottom mesons B(2S), B(2P), Bs(2S) and Bs(2P). We have also analyzed these bottom masses by applying the QCD and 1/mQ corrections to the lagrangian leading to the modification of flavor symmetry parameters as. Further strong decay widths are determined using these calculated masses to check the sensitivity of thes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.05366","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":"1806.05366","created_at":"2026-05-18T00:03:05.266231+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.05366v1","created_at":"2026-05-18T00:03:05.266231+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.05366","created_at":"2026-05-18T00:03:05.266231+00:00"},{"alias_kind":"pith_short_12","alias_value":"LJFIMU23WYBQ","created_at":"2026-05-18T12:32:37.024351+00:00"},{"alias_kind":"pith_short_16","alias_value":"LJFIMU23WYBQV5XI","created_at":"2026-05-18T12:32:37.024351+00:00"},{"alias_kind":"pith_short_8","alias_value":"LJFIMU23","created_at":"2026-05-18T12:32:37.024351+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/LJFIMU23WYBQV5XIYIT4EXSCLE","json":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE.json","graph_json":"https://pith.science/api/pith-number/LJFIMU23WYBQV5XIYIT4EXSCLE/graph.json","events_json":"https://pith.science/api/pith-number/LJFIMU23WYBQV5XIYIT4EXSCLE/events.json","paper":"https://pith.science/paper/LJFIMU23"},"agent_actions":{"view_html":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE","download_json":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE.json","view_paper":"https://pith.science/paper/LJFIMU23","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.05366&json=true","fetch_graph":"https://pith.science/api/pith-number/LJFIMU23WYBQV5XIYIT4EXSCLE/graph.json","fetch_events":"https://pith.science/api/pith-number/LJFIMU23WYBQV5XIYIT4EXSCLE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE/action/storage_attestation","attest_author":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE/action/author_attestation","sign_citation":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE/action/citation_signature","submit_replication":"https://pith.science/pith/LJFIMU23WYBQV5XIYIT4EXSCLE/action/replication_record"}},"created_at":"2026-05-18T00:03:05.266231+00:00","updated_at":"2026-05-18T00:03:05.266231+00:00"}