{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:CC3O5RRND6ZFENYLU4B3SV7J36","short_pith_number":"pith:CC3O5RRN","schema_version":"1.0","canonical_sha256":"10b6eec62d1fb252370ba703b957e9df88f351130bc22d4f2d5a6dc374fa7787","source":{"kind":"arxiv","id":"2501.03147","version":2},"attestation_state":"computed","paper":{"title":"Predictions for Bottomonium from a Relativistic Screened Potential Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bhaghyesh, Chaitanya Anil Bokade","submitted_at":"2025-01-06T17:14:03Z","abstract_excerpt":"In this work, a comprehensive analysis of the mass spectra and decay properties of bottomonium states using a relativistic screened potential model is carried out. The mass spectrum, decay constants, $E1$ transitions, $M1$ transitions, and annihilation decay widths are evaluated. The interpretation of $\\Upsilon(10355)$, $\\Upsilon(10580)$,$\\Upsilon(10860)$, and $\\Upsilon(11020)$ as $S-D$ mixed bottomonium states are analysed. The $\\Upsilon(10355)$ state is considered to be $3S-2D$, $\\Upsilon(10580)$ state is considered to be $4S-3D$ mixed state, the $\\Upsilon(10753)$ is obtained as purely $\\Ups"},"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":"2501.03147","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-06T17:14:03Z","cross_cats_sorted":[],"title_canon_sha256":"299f160428befa94945dee18f189aaac283a666886ef9d23e3f21189b67b2ab4","abstract_canon_sha256":"2156ef48728ca490e7bd58e9c953d92bab7572aabca813f6e3ee57e089ce4cbe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:43:30.385976Z","signature_b64":"PGtek45A6jzF7nuHkxofNnM5X83VpH6jWu75C/qdT/pkJityktojhWwQ9kWRMg4ID4iaIODdCisZBE5dYaikDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10b6eec62d1fb252370ba703b957e9df88f351130bc22d4f2d5a6dc374fa7787","last_reissued_at":"2026-07-05T11:43:30.385514Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:43:30.385514Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Predictions for Bottomonium from a Relativistic Screened Potential Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bhaghyesh, Chaitanya Anil Bokade","submitted_at":"2025-01-06T17:14:03Z","abstract_excerpt":"In this work, a comprehensive analysis of the mass spectra and decay properties of bottomonium states using a relativistic screened potential model is carried out. The mass spectrum, decay constants, $E1$ transitions, $M1$ transitions, and annihilation decay widths are evaluated. The interpretation of $\\Upsilon(10355)$, $\\Upsilon(10580)$,$\\Upsilon(10860)$, and $\\Upsilon(11020)$ as $S-D$ mixed bottomonium states are analysed. The $\\Upsilon(10355)$ state is considered to be $3S-2D$, $\\Upsilon(10580)$ state is considered to be $4S-3D$ mixed state, the $\\Upsilon(10753)$ is obtained as purely $\\Ups"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.03147","kind":"arxiv","version":2},"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/2501.03147/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":"2501.03147","created_at":"2026-07-05T11:43:30.385574+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.03147v2","created_at":"2026-07-05T11:43:30.385574+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.03147","created_at":"2026-07-05T11:43:30.385574+00:00"},{"alias_kind":"pith_short_12","alias_value":"CC3O5RRND6ZF","created_at":"2026-07-05T11:43:30.385574+00:00"},{"alias_kind":"pith_short_16","alias_value":"CC3O5RRND6ZFENYL","created_at":"2026-07-05T11:43:30.385574+00:00"},{"alias_kind":"pith_short_8","alias_value":"CC3O5RRN","created_at":"2026-07-05T11:43:30.385574+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/CC3O5RRND6ZFENYLU4B3SV7J36","json":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36.json","graph_json":"https://pith.science/api/pith-number/CC3O5RRND6ZFENYLU4B3SV7J36/graph.json","events_json":"https://pith.science/api/pith-number/CC3O5RRND6ZFENYLU4B3SV7J36/events.json","paper":"https://pith.science/paper/CC3O5RRN"},"agent_actions":{"view_html":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36","download_json":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36.json","view_paper":"https://pith.science/paper/CC3O5RRN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.03147&json=true","fetch_graph":"https://pith.science/api/pith-number/CC3O5RRND6ZFENYLU4B3SV7J36/graph.json","fetch_events":"https://pith.science/api/pith-number/CC3O5RRND6ZFENYLU4B3SV7J36/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36/action/storage_attestation","attest_author":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36/action/author_attestation","sign_citation":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36/action/citation_signature","submit_replication":"https://pith.science/pith/CC3O5RRND6ZFENYLU4B3SV7J36/action/replication_record"}},"created_at":"2026-07-05T11:43:30.385574+00:00","updated_at":"2026-07-05T11:43:30.385574+00:00"}