{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:2TH2JAJURDZX3U3SR2O3MOGVHZ","short_pith_number":"pith:2TH2JAJU","canonical_record":{"source":{"id":"1708.08465","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T18:00:08Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"ee394d83e630ccf84684cee7fd4711b3f103e039f06a992456e13512f57689e1","abstract_canon_sha256":"d6eaee02f6a427ba437d8d9ea8117a875c978b7784b2b5a7035fefa629b787b9"},"schema_version":"1.0"},"canonical_sha256":"d4cfa4813488f37dd3728e9db638d53e5186492e2d3fad1b9efd09b463a8b378","source":{"kind":"arxiv","id":"1708.08465","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.08465","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"arxiv_version","alias_value":"1708.08465v1","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08465","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"pith_short_12","alias_value":"2TH2JAJURDZX","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2TH2JAJURDZX3U3S","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2TH2JAJU","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:2TH2JAJURDZX3U3SR2O3MOGVHZ","target":"record","payload":{"canonical_record":{"source":{"id":"1708.08465","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T18:00:08Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"ee394d83e630ccf84684cee7fd4711b3f103e039f06a992456e13512f57689e1","abstract_canon_sha256":"d6eaee02f6a427ba437d8d9ea8117a875c978b7784b2b5a7035fefa629b787b9"},"schema_version":"1.0"},"canonical_sha256":"d4cfa4813488f37dd3728e9db638d53e5186492e2d3fad1b9efd09b463a8b378","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:33.191710Z","signature_b64":"I8vG8j4Y9PWddqab0muws+wyaQYOSUtQKQb8l3kmxgUdx6GckXucqoIavZCwS/JLXEtp36OdV3MLkYERjEZwCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4cfa4813488f37dd3728e9db638d53e5186492e2d3fad1b9efd09b463a8b378","last_reissued_at":"2026-05-17T23:59:33.191093Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:33.191093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.08465","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":"2026-05-17T23:59:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y3WppZ+sminvO0hFx1GcDKsEquORfSXe4Hm27iphj80/MF7Dbm0w94cUXC2CIofiozTGIw/NKW53USNH0CmMBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T11:47:25.921535Z"},"content_sha256":"de4bb82a1db66fef55600be68ccc015a3e97040b5099bfc5df2584293051a098","schema_version":"1.0","event_id":"sha256:de4bb82a1db66fef55600be68ccc015a3e97040b5099bfc5df2584293051a098"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:2TH2JAJURDZX3U3SR2O3MOGVHZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Determination of electric dipole transitions in heavy quarkonia using potential non-relativistic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Jorge Segovia, Sebastian Steinbei{\\ss}er","submitted_at":"2017-08-28T18:00:08Z","abstract_excerpt":"The electric dipole transitions $\\chi_{bJ}(1P)\\to \\gamma\\Upsilon(1S)$ with $J=0,1,2$ and $h_{b}(1P)\\to \\gamma\\eta_{b}(1S)$ are computed using the weak-coupling version of a low-energy effective field theory named potential non-relativistic QCD (pNRQCD). In order to improve convergence and thus give firm predictions for the studied reactions, the full static potential is incorporated into the leading order Hamiltonian; moreover, we must handle properly renormalon effects and re-summation of large logarithms. The precision we reach is $k_{\\gamma}^{3}/(mv)^{2} \\times \\mathcal{O}(v^{2})$, where $k"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08465","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":"2026-05-17T23:59:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aCrRxp2Eje9zk4CrTE/Rp26w9QYtqzRcLTQ+Vhf2M08u99SSgmvCUWYPgpOdOx8VROViAWIbQ1GgOpyK0LqaCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T11:47:25.921912Z"},"content_sha256":"693cb802e3fd68b17361d1eb42794d10a7ad8eba2df6614e63bda61698928d52","schema_version":"1.0","event_id":"sha256:693cb802e3fd68b17361d1eb42794d10a7ad8eba2df6614e63bda61698928d52"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/bundle.json","state_url":"https://pith.science/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/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":"2026-05-20T11:47:25Z","links":{"resolver":"https://pith.science/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ","bundle":"https://pith.science/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/bundle.json","state":"https://pith.science/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2TH2JAJURDZX3U3SR2O3MOGVHZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:2TH2JAJURDZX3U3SR2O3MOGVHZ","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":"d6eaee02f6a427ba437d8d9ea8117a875c978b7784b2b5a7035fefa629b787b9","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T18:00:08Z","title_canon_sha256":"ee394d83e630ccf84684cee7fd4711b3f103e039f06a992456e13512f57689e1"},"schema_version":"1.0","source":{"id":"1708.08465","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.08465","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"arxiv_version","alias_value":"1708.08465v1","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08465","created_at":"2026-05-17T23:59:33Z"},{"alias_kind":"pith_short_12","alias_value":"2TH2JAJURDZX","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2TH2JAJURDZX3U3S","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2TH2JAJU","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:693cb802e3fd68b17361d1eb42794d10a7ad8eba2df6614e63bda61698928d52","target":"graph","created_at":"2026-05-17T23:59:33Z","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":"The electric dipole transitions $\\chi_{bJ}(1P)\\to \\gamma\\Upsilon(1S)$ with $J=0,1,2$ and $h_{b}(1P)\\to \\gamma\\eta_{b}(1S)$ are computed using the weak-coupling version of a low-energy effective field theory named potential non-relativistic QCD (pNRQCD). In order to improve convergence and thus give firm predictions for the studied reactions, the full static potential is incorporated into the leading order Hamiltonian; moreover, we must handle properly renormalon effects and re-summation of large logarithms. The precision we reach is $k_{\\gamma}^{3}/(mv)^{2} \\times \\mathcal{O}(v^{2})$, where $k","authors_text":"Jorge Segovia, Sebastian Steinbei{\\ss}er","cross_cats":["hep-ex","hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T18:00:08Z","title":"Determination of electric dipole transitions in heavy quarkonia using potential non-relativistic QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08465","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:de4bb82a1db66fef55600be68ccc015a3e97040b5099bfc5df2584293051a098","target":"record","created_at":"2026-05-17T23:59:33Z","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":"d6eaee02f6a427ba437d8d9ea8117a875c978b7784b2b5a7035fefa629b787b9","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T18:00:08Z","title_canon_sha256":"ee394d83e630ccf84684cee7fd4711b3f103e039f06a992456e13512f57689e1"},"schema_version":"1.0","source":{"id":"1708.08465","kind":"arxiv","version":1}},"canonical_sha256":"d4cfa4813488f37dd3728e9db638d53e5186492e2d3fad1b9efd09b463a8b378","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d4cfa4813488f37dd3728e9db638d53e5186492e2d3fad1b9efd09b463a8b378","first_computed_at":"2026-05-17T23:59:33.191093Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:33.191093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"I8vG8j4Y9PWddqab0muws+wyaQYOSUtQKQb8l3kmxgUdx6GckXucqoIavZCwS/JLXEtp36OdV3MLkYERjEZwCg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:33.191710Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.08465","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:de4bb82a1db66fef55600be68ccc015a3e97040b5099bfc5df2584293051a098","sha256:693cb802e3fd68b17361d1eb42794d10a7ad8eba2df6614e63bda61698928d52"],"state_sha256":"f828bd75cec62c933300208c29fb474e3706bb434ac21fb4ff34549ffeb18910"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IIkDXQnoU7nXszLCALZz+x061y8IPHuyjg0hrmO+PSHkJrCxN50T+XrWG7lchcs0zn09tPSjFbHH7OfFG61NDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T11:47:25.923886Z","bundle_sha256":"1f3a22af2af68091119cbeb86fb1294249499370e78a4f7128d5fcbe1a25aec3"}}