{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:UIVUV3NHU3J7CQQUUDU5XS3TTU","short_pith_number":"pith:UIVUV3NH","schema_version":"1.0","canonical_sha256":"a22b4aeda7a6d3f14214a0e9dbcb739d3af5549888f00f94d5b7c14927df6024","source":{"kind":"arxiv","id":"2202.12048","version":1},"attestation_state":"computed","paper":{"title":"Mass Spectra and Decay Properties of Singly Heavy Bottom-Strange Baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajay Kumar Rai, Amee Kakadiya, Zalak Shah","submitted_at":"2022-02-24T12:03:02Z","abstract_excerpt":"We enumerated ground and excited state masses of singly heavy bottom-strange baryons using the Hypercentral Constituent Quark Model (hCQM). The screening potential is used with color-Coulomb potential, as the confining potential. We determine the possible $J^P$ values to recently observed excited states like, $\\Xi_b(6100)$, $\\Xi_b(6227)$, $\\Xi_b(6327)$, $\\Xi_b(6333)$ and four $\\Omega_b(6316,6330,6340,6350)$ states. The Regge trajectories are plotted in $(J, M^2)$ plane to assign the $J^P$ values and quantum numbers to recently observed states. Using the calculated spectroscopic data, propertie"},"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":"2202.12048","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-24T12:03:02Z","cross_cats_sorted":[],"title_canon_sha256":"6813f41cdb39049ec2a819648278387e638ee5aab58e0c563895f52a4843d0da","abstract_canon_sha256":"50aa285372c5fe518317903412c5297a78180e51246c740d14c380f6e7c975d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:31:34.471923Z","signature_b64":"XnK28NXKGv8Q0HSdW+jDGKBEvquI3+Sn+jg9H8YEgvBAvS6+I5Ym8feLQdQVm8/f1Az+RVzGbE3NksAPhlVZAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a22b4aeda7a6d3f14214a0e9dbcb739d3af5549888f00f94d5b7c14927df6024","last_reissued_at":"2026-07-05T04:31:34.471403Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:31:34.471403Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mass Spectra and Decay Properties of Singly Heavy Bottom-Strange Baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajay Kumar Rai, Amee Kakadiya, Zalak Shah","submitted_at":"2022-02-24T12:03:02Z","abstract_excerpt":"We enumerated ground and excited state masses of singly heavy bottom-strange baryons using the Hypercentral Constituent Quark Model (hCQM). The screening potential is used with color-Coulomb potential, as the confining potential. We determine the possible $J^P$ values to recently observed excited states like, $\\Xi_b(6100)$, $\\Xi_b(6227)$, $\\Xi_b(6327)$, $\\Xi_b(6333)$ and four $\\Omega_b(6316,6330,6340,6350)$ states. The Regge trajectories are plotted in $(J, M^2)$ plane to assign the $J^P$ values and quantum numbers to recently observed states. Using the calculated spectroscopic data, propertie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.12048","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/2202.12048/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":"2202.12048","created_at":"2026-07-05T04:31:34.471467+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.12048v1","created_at":"2026-07-05T04:31:34.471467+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.12048","created_at":"2026-07-05T04:31:34.471467+00:00"},{"alias_kind":"pith_short_12","alias_value":"UIVUV3NHU3J7","created_at":"2026-07-05T04:31:34.471467+00:00"},{"alias_kind":"pith_short_16","alias_value":"UIVUV3NHU3J7CQQU","created_at":"2026-07-05T04:31:34.471467+00:00"},{"alias_kind":"pith_short_8","alias_value":"UIVUV3NH","created_at":"2026-07-05T04:31:34.471467+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.25925","citing_title":"Spin-dependent interactions and fine structure in the negative-parity singly heavy baryons","ref_index":16,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU","json":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU.json","graph_json":"https://pith.science/api/pith-number/UIVUV3NHU3J7CQQUUDU5XS3TTU/graph.json","events_json":"https://pith.science/api/pith-number/UIVUV3NHU3J7CQQUUDU5XS3TTU/events.json","paper":"https://pith.science/paper/UIVUV3NH"},"agent_actions":{"view_html":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU","download_json":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU.json","view_paper":"https://pith.science/paper/UIVUV3NH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.12048&json=true","fetch_graph":"https://pith.science/api/pith-number/UIVUV3NHU3J7CQQUUDU5XS3TTU/graph.json","fetch_events":"https://pith.science/api/pith-number/UIVUV3NHU3J7CQQUUDU5XS3TTU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU/action/storage_attestation","attest_author":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU/action/author_attestation","sign_citation":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU/action/citation_signature","submit_replication":"https://pith.science/pith/UIVUV3NHU3J7CQQUUDU5XS3TTU/action/replication_record"}},"created_at":"2026-07-05T04:31:34.471467+00:00","updated_at":"2026-07-05T04:31:34.471467+00:00"}