{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:OXPLFQYCQFMW6TO3SCRD3XFWTY","short_pith_number":"pith:OXPLFQYC","canonical_record":{"source":{"id":"2307.11481","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-21T10:32:23Z","cross_cats_sorted":[],"title_canon_sha256":"6d67ccd12f8992be31c2a6d59df7cdda738e1fa24316975808aa02b2cef707f4","abstract_canon_sha256":"f5624451caec84bef6bd789f628f63ab36e369db21102093c0a8febf60285319"},"schema_version":"1.0"},"canonical_sha256":"75deb2c30281596f4ddb90a23ddcb69e14693b922ea86d61b438b196878ab370","source":{"kind":"arxiv","id":"2307.11481","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.11481","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"arxiv_version","alias_value":"2307.11481v1","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.11481","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_12","alias_value":"OXPLFQYCQFMW","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_16","alias_value":"OXPLFQYCQFMW6TO3","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_8","alias_value":"OXPLFQYC","created_at":"2026-07-05T06:33:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:OXPLFQYCQFMW6TO3SCRD3XFWTY","target":"record","payload":{"canonical_record":{"source":{"id":"2307.11481","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-21T10:32:23Z","cross_cats_sorted":[],"title_canon_sha256":"6d67ccd12f8992be31c2a6d59df7cdda738e1fa24316975808aa02b2cef707f4","abstract_canon_sha256":"f5624451caec84bef6bd789f628f63ab36e369db21102093c0a8febf60285319"},"schema_version":"1.0"},"canonical_sha256":"75deb2c30281596f4ddb90a23ddcb69e14693b922ea86d61b438b196878ab370","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:33:27.996919Z","signature_b64":"Rc4IqRKJye8SOWCgMuy1z0YpTBdU5gHuI2zlhS6MHDvKeShuS52g4NjElek040Cdqir9fGlX4/4h7eoDiZbpAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75deb2c30281596f4ddb90a23ddcb69e14693b922ea86d61b438b196878ab370","last_reissued_at":"2026-07-05T06:33:27.996493Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:33:27.996493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2307.11481","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:33:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qetbMTiNwOcbe4h8qH4hv9zjBTA9fsuWK4vdGGP+W859WnZQAqpdEeYK32zDfzyzfahKZfWpfbJ5hM2TcrBMAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-24T23:48:17.794346Z"},"content_sha256":"2b894774369f32b534afec73092cec53052114603800ff867f89e81564c21676","schema_version":"1.0","event_id":"sha256:2b894774369f32b534afec73092cec53052114603800ff867f89e81564c21676"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:OXPLFQYCQFMW6TO3SCRD3XFWTY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quarkonium spectroscopy of the linear plus modified Yukawa potential","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajay Kumar Rai, Kaushal R Purohit, Pooja Jakhad","submitted_at":"2023-07-21T10:32:23Z","abstract_excerpt":"In this article, the linear plus modified Yukawa potential (LIMYP) is used as the quark antiquark interaction potential for the approximate analytical bound state solution of the Klein Gordon equation in three-dimensional space. The energy eigenvalues and associated wavefunction are obtained by solving the Klein Gordon equation analytically using the Nikiforov Uvarov (NU) method. The mass spectra of heavy mesons such as charmonium $(c\\bar{c})$, bottomonium $(b\\bar{b})$, and $b\\bar{c}$ for various quantum states are obtained using the energy spectra expression. In comparison to experimental dat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.11481","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/2307.11481/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:33:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5DzpcwupFu+1ti1mGXLINdBrFVDwAeTEEArdura68Ibax83ryifdL7OZgonpl127gMH9fmiNNyjb6/4RMbFbAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-24T23:48:17.794728Z"},"content_sha256":"f9c28bc749620bb3ac87637e1f0fb0601ba101afaceabc9c1e1f69f90b6cd037","schema_version":"1.0","event_id":"sha256:f9c28bc749620bb3ac87637e1f0fb0601ba101afaceabc9c1e1f69f90b6cd037"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/bundle.json","state_url":"https://pith.science/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-24T23:48:17Z","links":{"resolver":"https://pith.science/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY","bundle":"https://pith.science/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/bundle.json","state":"https://pith.science/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OXPLFQYCQFMW6TO3SCRD3XFWTY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:OXPLFQYCQFMW6TO3SCRD3XFWTY","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"f5624451caec84bef6bd789f628f63ab36e369db21102093c0a8febf60285319","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-21T10:32:23Z","title_canon_sha256":"6d67ccd12f8992be31c2a6d59df7cdda738e1fa24316975808aa02b2cef707f4"},"schema_version":"1.0","source":{"id":"2307.11481","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.11481","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"arxiv_version","alias_value":"2307.11481v1","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.11481","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_12","alias_value":"OXPLFQYCQFMW","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_16","alias_value":"OXPLFQYCQFMW6TO3","created_at":"2026-07-05T06:33:27Z"},{"alias_kind":"pith_short_8","alias_value":"OXPLFQYC","created_at":"2026-07-05T06:33:27Z"}],"graph_snapshots":[{"event_id":"sha256:f9c28bc749620bb3ac87637e1f0fb0601ba101afaceabc9c1e1f69f90b6cd037","target":"graph","created_at":"2026-07-05T06:33:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2307.11481/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this article, the linear plus modified Yukawa potential (LIMYP) is used as the quark antiquark interaction potential for the approximate analytical bound state solution of the Klein Gordon equation in three-dimensional space. The energy eigenvalues and associated wavefunction are obtained by solving the Klein Gordon equation analytically using the Nikiforov Uvarov (NU) method. The mass spectra of heavy mesons such as charmonium $(c\\bar{c})$, bottomonium $(b\\bar{b})$, and $b\\bar{c}$ for various quantum states are obtained using the energy spectra expression. In comparison to experimental dat","authors_text":"Ajay Kumar Rai, Kaushal R Purohit, Pooja Jakhad","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-21T10:32:23Z","title":"Quarkonium spectroscopy of the linear plus modified Yukawa potential"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.11481","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2b894774369f32b534afec73092cec53052114603800ff867f89e81564c21676","target":"record","created_at":"2026-07-05T06:33:27Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"f5624451caec84bef6bd789f628f63ab36e369db21102093c0a8febf60285319","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-21T10:32:23Z","title_canon_sha256":"6d67ccd12f8992be31c2a6d59df7cdda738e1fa24316975808aa02b2cef707f4"},"schema_version":"1.0","source":{"id":"2307.11481","kind":"arxiv","version":1}},"canonical_sha256":"75deb2c30281596f4ddb90a23ddcb69e14693b922ea86d61b438b196878ab370","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"75deb2c30281596f4ddb90a23ddcb69e14693b922ea86d61b438b196878ab370","first_computed_at":"2026-07-05T06:33:27.996493Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:33:27.996493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Rc4IqRKJye8SOWCgMuy1z0YpTBdU5gHuI2zlhS6MHDvKeShuS52g4NjElek040Cdqir9fGlX4/4h7eoDiZbpAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:33:27.996919Z","signed_message":"canonical_sha256_bytes"},"source_id":"2307.11481","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2b894774369f32b534afec73092cec53052114603800ff867f89e81564c21676","sha256:f9c28bc749620bb3ac87637e1f0fb0601ba101afaceabc9c1e1f69f90b6cd037"],"state_sha256":"2af6617266b499024b60b71fb40656a86aeb2b2ba37f6a082d2a5751ca54b735"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e+6+NsnIHZA+MXURXkbUXJ+DGiMA1Zk2eeuCZ+wxjWe0Yp0vS97tQamzG20cSweNUlKyM9rIbT6xokNjQfGrAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-24T23:48:17.797205Z","bundle_sha256":"54313898133d6a0374814b4cc48f8fcbfd8c5daf197de3c67b386aa19ee67746"}}