{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:TJXAKWT7RBQFYWTTAQPIZEKWH3","short_pith_number":"pith:TJXAKWT7","canonical_record":{"source":{"id":"1608.08406","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-30T11:34:01Z","cross_cats_sorted":[],"title_canon_sha256":"7c17dac6771dbc1401a6db6e83c9bed20b0f91e1dbe5a0581ade77c1332ae0e9","abstract_canon_sha256":"3e0243ce0cbaf4a1251fa30ed88cc3f7c4b0aa6f09ce610b20ed1e86a5074440"},"schema_version":"1.0"},"canonical_sha256":"9a6e055a7f88605c5a73041e8c91563ec60b26c1b0f4f35d64def9ca2dc551cf","source":{"kind":"arxiv","id":"1608.08406","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.08406","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.08406v1","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.08406","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"pith_short_12","alias_value":"TJXAKWT7RBQF","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"TJXAKWT7RBQFYWTT","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"TJXAKWT7","created_at":"2026-05-18T12:30:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:TJXAKWT7RBQFYWTTAQPIZEKWH3","target":"record","payload":{"canonical_record":{"source":{"id":"1608.08406","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-30T11:34:01Z","cross_cats_sorted":[],"title_canon_sha256":"7c17dac6771dbc1401a6db6e83c9bed20b0f91e1dbe5a0581ade77c1332ae0e9","abstract_canon_sha256":"3e0243ce0cbaf4a1251fa30ed88cc3f7c4b0aa6f09ce610b20ed1e86a5074440"},"schema_version":"1.0"},"canonical_sha256":"9a6e055a7f88605c5a73041e8c91563ec60b26c1b0f4f35d64def9ca2dc551cf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:19.563991Z","signature_b64":"PkVYgEzvRdPc+4yKryfhrWcqsTVqqb/MYfV2AgeTHglD5Ut9Z+3V+jARklr14ui/BlZSy8IopYYCig1UNlBxDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a6e055a7f88605c5a73041e8c91563ec60b26c1b0f4f35d64def9ca2dc551cf","last_reissued_at":"2026-05-18T01:07:19.563547Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:19.563547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.08406","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":"2026-05-18T01:07:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jB36/MVOL/1T7+S3kqRNvwRXAKmXM6NxYvAYR3TymfCP+QwGlX/1S26bhi3ZMEOdaSS4hGVXYJOfqJ5X8CtyBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T00:18:18.845608Z"},"content_sha256":"5764681f33bdafbf102a48fb5201425fcf3ca7e2421a93aab8cb51767b1b548a","schema_version":"1.0","event_id":"sha256:5764681f33bdafbf102a48fb5201425fcf3ca7e2421a93aab8cb51767b1b548a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:TJXAKWT7RBQFYWTTAQPIZEKWH3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Masses and decay widths of radially excited Bottom mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Upadhyay, Pallavi Gupta","submitted_at":"2016-08-30T11:34:01Z","abstract_excerpt":"Inspired from the experimental information coming from LHC [2,3] and Babar [4] for radially higher excited charmed mesons, we predict the masses and decays of the n=2 S-wave and P- wave bottom mesons using the effective lagrangian approach. Using heavy quark effective theory approach, non-perturbative parameters (?, ?1 and ?2) are fitted using the available experimental and theoretical informations on charm masses. Using heavy quark symmetry and the values of these fitted parameters, the masses of radially excited even and odd parity bottom mesons with and without strangness are predicted. The"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.08406","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":""},"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":"2026-05-18T01:07:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xt7AkTAox2S9hpvJLBIgWJxf75gFzFBS4Knmfm06PDCYv60Iyt5zFXJHwfuUUEu+EBf2xjHG7yZw5QwcZR+1Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T00:18:18.845981Z"},"content_sha256":"dd7ed7f7e1b628376a4378d3f7f730853c1fc491ae476c7c4aa3ea7922aeccea","schema_version":"1.0","event_id":"sha256:dd7ed7f7e1b628376a4378d3f7f730853c1fc491ae476c7c4aa3ea7922aeccea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/bundle.json","state_url":"https://pith.science/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/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":"2026-06-20T00:18:18Z","links":{"resolver":"https://pith.science/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3","bundle":"https://pith.science/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/bundle.json","state":"https://pith.science/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TJXAKWT7RBQFYWTTAQPIZEKWH3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:TJXAKWT7RBQFYWTTAQPIZEKWH3","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":"3e0243ce0cbaf4a1251fa30ed88cc3f7c4b0aa6f09ce610b20ed1e86a5074440","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-30T11:34:01Z","title_canon_sha256":"7c17dac6771dbc1401a6db6e83c9bed20b0f91e1dbe5a0581ade77c1332ae0e9"},"schema_version":"1.0","source":{"id":"1608.08406","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.08406","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"arxiv_version","alias_value":"1608.08406v1","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.08406","created_at":"2026-05-18T01:07:19Z"},{"alias_kind":"pith_short_12","alias_value":"TJXAKWT7RBQF","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"TJXAKWT7RBQFYWTT","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"TJXAKWT7","created_at":"2026-05-18T12:30:44Z"}],"graph_snapshots":[{"event_id":"sha256:dd7ed7f7e1b628376a4378d3f7f730853c1fc491ae476c7c4aa3ea7922aeccea","target":"graph","created_at":"2026-05-18T01:07:19Z","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"},"paper":{"abstract_excerpt":"Inspired from the experimental information coming from LHC [2,3] and Babar [4] for radially higher excited charmed mesons, we predict the masses and decays of the n=2 S-wave and P- wave bottom mesons using the effective lagrangian approach. Using heavy quark effective theory approach, non-perturbative parameters (?, ?1 and ?2) are fitted using the available experimental and theoretical informations on charm masses. Using heavy quark symmetry and the values of these fitted parameters, the masses of radially excited even and odd parity bottom mesons with and without strangness are predicted. The","authors_text":"A. Upadhyay, Pallavi Gupta","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-30T11:34:01Z","title":"Masses and decay widths of radially excited Bottom mesons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.08406","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":"sha256:5764681f33bdafbf102a48fb5201425fcf3ca7e2421a93aab8cb51767b1b548a","target":"record","created_at":"2026-05-18T01:07:19Z","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":"3e0243ce0cbaf4a1251fa30ed88cc3f7c4b0aa6f09ce610b20ed1e86a5074440","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-30T11:34:01Z","title_canon_sha256":"7c17dac6771dbc1401a6db6e83c9bed20b0f91e1dbe5a0581ade77c1332ae0e9"},"schema_version":"1.0","source":{"id":"1608.08406","kind":"arxiv","version":1}},"canonical_sha256":"9a6e055a7f88605c5a73041e8c91563ec60b26c1b0f4f35d64def9ca2dc551cf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9a6e055a7f88605c5a73041e8c91563ec60b26c1b0f4f35d64def9ca2dc551cf","first_computed_at":"2026-05-18T01:07:19.563547Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:07:19.563547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PkVYgEzvRdPc+4yKryfhrWcqsTVqqb/MYfV2AgeTHglD5Ut9Z+3V+jARklr14ui/BlZSy8IopYYCig1UNlBxDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:07:19.563991Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.08406","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5764681f33bdafbf102a48fb5201425fcf3ca7e2421a93aab8cb51767b1b548a","sha256:dd7ed7f7e1b628376a4378d3f7f730853c1fc491ae476c7c4aa3ea7922aeccea"],"state_sha256":"5dd613cb4c78480127c496a98009f5bb8fe4ac6c7ad242f53b1c532908b67d3b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lKwAlFlvo1tJkJxsK2ImiHTa12HLtiTlFzhkk7UBnPCXLRlp9+Mhh90PiLKTSU5DivjDjuv57PQCOLnvkCOjCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T00:18:18.848002Z","bundle_sha256":"04e38bc51ca0d6ea0744f24e02fb6696014f5674d9c18603515b2f7c6343a564"}}