{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:6XLIHU4EJL6VDTQBJS6SLTNOKO","short_pith_number":"pith:6XLIHU4E","schema_version":"1.0","canonical_sha256":"f5d683d3844afd51ce014cbd25cdae53a37342db41d77a75f1a5c597d467ec3e","source":{"kind":"arxiv","id":"1205.0938","version":2},"attestation_state":"computed","paper":{"title":"Any J-state solution of the DKP equation for a vector deformed Woods-Saxon potential","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Majid Hamzavi, Sameer M. Ikhdair","submitted_at":"2012-05-04T12:39:43Z","abstract_excerpt":"By using the Pekeris approximation, the Duffin-Kemmer-Petiau (DKP) equation is investigated for a vector deformed Woods-Saxon (dWS) potential. The parametric Nikiforov-Uvarov (NU) method is used in calculations. The approximate energy eigenvalue equation and the corresponding wave function spinor components are calculated for any total angular momentum J in closed form. The exact energy equation and wave function spinor components are also given for the J=0 case. We use a set of parameter values to obtain the numerical values for the energy states with various values of quantum levels (n,J) an"},"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":"1205.0938","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2012-05-04T12:39:43Z","cross_cats_sorted":[],"title_canon_sha256":"7826d2cef4144cc55c95f979aba37ace81364011b3f0f00fe7e77f7f67b0d950","abstract_canon_sha256":"285a62152575375e74268ead408f82a38d67e2d312b55cfa73443c4b04c4c63f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:04.465432Z","signature_b64":"6js7oQkNJM+yedNCzFX6sKfyusSIScEvcfPl6Ej7VP/znryOEuVO7DofkOANlkgmsl6ir5Oq9OVpsPQQO2bNBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5d683d3844afd51ce014cbd25cdae53a37342db41d77a75f1a5c597d467ec3e","last_reissued_at":"2026-05-18T03:44:04.464695Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:04.464695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Any J-state solution of the DKP equation for a vector deformed Woods-Saxon potential","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Majid Hamzavi, Sameer M. Ikhdair","submitted_at":"2012-05-04T12:39:43Z","abstract_excerpt":"By using the Pekeris approximation, the Duffin-Kemmer-Petiau (DKP) equation is investigated for a vector deformed Woods-Saxon (dWS) potential. The parametric Nikiforov-Uvarov (NU) method is used in calculations. The approximate energy eigenvalue equation and the corresponding wave function spinor components are calculated for any total angular momentum J in closed form. The exact energy equation and wave function spinor components are also given for the J=0 case. We use a set of parameter values to obtain the numerical values for the energy states with various values of quantum levels (n,J) an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.0938","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":""},"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":"1205.0938","created_at":"2026-05-18T03:44:04.464792+00:00"},{"alias_kind":"arxiv_version","alias_value":"1205.0938v2","created_at":"2026-05-18T03:44:04.464792+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.0938","created_at":"2026-05-18T03:44:04.464792+00:00"},{"alias_kind":"pith_short_12","alias_value":"6XLIHU4EJL6V","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"6XLIHU4EJL6VDTQB","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"6XLIHU4E","created_at":"2026-05-18T12:26:56.085431+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/6XLIHU4EJL6VDTQBJS6SLTNOKO","json":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO.json","graph_json":"https://pith.science/api/pith-number/6XLIHU4EJL6VDTQBJS6SLTNOKO/graph.json","events_json":"https://pith.science/api/pith-number/6XLIHU4EJL6VDTQBJS6SLTNOKO/events.json","paper":"https://pith.science/paper/6XLIHU4E"},"agent_actions":{"view_html":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO","download_json":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO.json","view_paper":"https://pith.science/paper/6XLIHU4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1205.0938&json=true","fetch_graph":"https://pith.science/api/pith-number/6XLIHU4EJL6VDTQBJS6SLTNOKO/graph.json","fetch_events":"https://pith.science/api/pith-number/6XLIHU4EJL6VDTQBJS6SLTNOKO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO/action/storage_attestation","attest_author":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO/action/author_attestation","sign_citation":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO/action/citation_signature","submit_replication":"https://pith.science/pith/6XLIHU4EJL6VDTQBJS6SLTNOKO/action/replication_record"}},"created_at":"2026-05-18T03:44:04.464792+00:00","updated_at":"2026-05-18T03:44:04.464792+00:00"}