{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:BFPNMCUZI2GE6OGVJS3MGNOOUM","short_pith_number":"pith:BFPNMCUZ","schema_version":"1.0","canonical_sha256":"095ed60a99468c4f38d54cb6c335cea327abedf90d5ccb5022583aa814c6203c","source":{"kind":"arxiv","id":"1908.07707","version":1},"attestation_state":"computed","paper":{"title":"Heavy quarkonia properties from a hard-wall confinement potential model with conformal symmetry perturbing effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ahmed Al-Jamel","submitted_at":"2019-08-21T04:33:49Z","abstract_excerpt":"Heavy $c\\bar c$ and $b\\bar b $ quarkonia are considered as systems confined within a hard-wall potential shaped after a linear combination of a cotangent-- with a square co-secant function. Wave functions and energy spectra are then obtained in closed forms in solving by the Nikiforov-Uvarov method the associated radial Schr\\\"{o}dinger equation in the presence of a centrifugal term. The interest in this potential is that in one parametrization it can account for a conformal symmetry of the strong interaction, and in another for its perturbation, a reason for which we here employ it to study st"},"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":"1908.07707","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-08-21T04:33:49Z","cross_cats_sorted":[],"title_canon_sha256":"8449f8960a475e622bac09fd48b517890f435caa94e50cd25e29c2bcf38e1fcc","abstract_canon_sha256":"51ac2bbcbf01604b6621eb03c216ce560b7202796a422e0ed727e251dff3abfe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:59:00.577044Z","signature_b64":"0TqO6HKA5ADS0t3xPz7M/FHNoRz4Ybf+3jZZ3fCtRmEJizEe75s/Q0bbKKlfj86bDG5kyY/RfUaEkkP+UJuTDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"095ed60a99468c4f38d54cb6c335cea327abedf90d5ccb5022583aa814c6203c","last_reissued_at":"2026-07-04T23:59:00.576628Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:59:00.576628Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy quarkonia properties from a hard-wall confinement potential model with conformal symmetry perturbing effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ahmed Al-Jamel","submitted_at":"2019-08-21T04:33:49Z","abstract_excerpt":"Heavy $c\\bar c$ and $b\\bar b $ quarkonia are considered as systems confined within a hard-wall potential shaped after a linear combination of a cotangent-- with a square co-secant function. Wave functions and energy spectra are then obtained in closed forms in solving by the Nikiforov-Uvarov method the associated radial Schr\\\"{o}dinger equation in the presence of a centrifugal term. The interest in this potential is that in one parametrization it can account for a conformal symmetry of the strong interaction, and in another for its perturbation, a reason for which we here employ it to study st"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.07707","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/1908.07707/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":"1908.07707","created_at":"2026-07-04T23:59:00.576687+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.07707v1","created_at":"2026-07-04T23:59:00.576687+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.07707","created_at":"2026-07-04T23:59:00.576687+00:00"},{"alias_kind":"pith_short_12","alias_value":"BFPNMCUZI2GE","created_at":"2026-07-04T23:59:00.576687+00:00"},{"alias_kind":"pith_short_16","alias_value":"BFPNMCUZI2GE6OGV","created_at":"2026-07-04T23:59:00.576687+00:00"},{"alias_kind":"pith_short_8","alias_value":"BFPNMCUZ","created_at":"2026-07-04T23:59:00.576687+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/BFPNMCUZI2GE6OGVJS3MGNOOUM","json":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM.json","graph_json":"https://pith.science/api/pith-number/BFPNMCUZI2GE6OGVJS3MGNOOUM/graph.json","events_json":"https://pith.science/api/pith-number/BFPNMCUZI2GE6OGVJS3MGNOOUM/events.json","paper":"https://pith.science/paper/BFPNMCUZ"},"agent_actions":{"view_html":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM","download_json":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM.json","view_paper":"https://pith.science/paper/BFPNMCUZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.07707&json=true","fetch_graph":"https://pith.science/api/pith-number/BFPNMCUZI2GE6OGVJS3MGNOOUM/graph.json","fetch_events":"https://pith.science/api/pith-number/BFPNMCUZI2GE6OGVJS3MGNOOUM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM/action/storage_attestation","attest_author":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM/action/author_attestation","sign_citation":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM/action/citation_signature","submit_replication":"https://pith.science/pith/BFPNMCUZI2GE6OGVJS3MGNOOUM/action/replication_record"}},"created_at":"2026-07-04T23:59:00.576687+00:00","updated_at":"2026-07-04T23:59:00.576687+00:00"}