{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:ZAYTSI2ZQONCJJML375DCM2VEL","short_pith_number":"pith:ZAYTSI2Z","canonical_record":{"source":{"id":"hep-ph/9510406","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-10-25T16:02:31Z","cross_cats_sorted":[],"title_canon_sha256":"21be76e29b39d9f67479dd4171e6904e8dbb735d63178f17e49f5ff5a7ca31db","abstract_canon_sha256":"c7771c039b64e1153b3046755dee1df28b0f090ea8ffcb180ecbd672d47d76d6"},"schema_version":"1.0"},"canonical_sha256":"c831392359839a24a58bdffa31335522f698a5dd18c5b856a6b7d91082087a4b","source":{"kind":"arxiv","id":"hep-ph/9510406","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9510406","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9510406v1","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9510406","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_12","alias_value":"ZAYTSI2ZQONC","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_16","alias_value":"ZAYTSI2ZQONCJJML","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_8","alias_value":"ZAYTSI2Z","created_at":"2026-07-04T14:29:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:ZAYTSI2ZQONCJJML375DCM2VEL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9510406","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-10-25T16:02:31Z","cross_cats_sorted":[],"title_canon_sha256":"21be76e29b39d9f67479dd4171e6904e8dbb735d63178f17e49f5ff5a7ca31db","abstract_canon_sha256":"c7771c039b64e1153b3046755dee1df28b0f090ea8ffcb180ecbd672d47d76d6"},"schema_version":"1.0"},"canonical_sha256":"c831392359839a24a58bdffa31335522f698a5dd18c5b856a6b7d91082087a4b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:29:49.958412Z","signature_b64":"J8EskTO1DYCpbLzmX+JoQUoFWTwqVzs9sCJcLeW4Rp5LtE4KVtijvYKN0Z+7LlXwsRsPIVooOdXgYjG/K99OCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c831392359839a24a58bdffa31335522f698a5dd18c5b856a6b7d91082087a4b","last_reissued_at":"2026-07-04T14:29:49.958049Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:29:49.958049Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9510406","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":"2026-07-04T14:29:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"N4j2BTodFlHfP6jmVUNH8GraeVx4Q6Q6yx/8FNoGSsZVuaGIDFGs8MlEkgHKUR4jMb4m9b2ow9TStCiF4+kgBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T17:38:46.864950Z"},"content_sha256":"574f027aba90499660e9205e2dd1f63638546a0ac92e50779c12dc718aed805f","schema_version":"1.0","event_id":"sha256:574f027aba90499660e9205e2dd1f63638546a0ac92e50779c12dc718aed805f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:ZAYTSI2ZQONCJJML375DCM2VEL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hadronic Decays of Excited Heavy Quarkonia","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Res Urech, Thomas Mannel","submitted_at":"1995-10-25T16:02:31Z","abstract_excerpt":"We construct an effective Lagrangian for the hadronic decays of a heavy excited $s$-wave-spin-one quarkonium into its ground state. We show that reasonable fits to the measured invariant mass spectra in the $J/\\psi$ and $\\Upsilon$ systems can be obtained working in the chiral limit. The mass dependence of the various terms in the Lagrangian is discussed on the basis of a quark model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9510406","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/hep-ph/9510406/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":"2026-07-04T14:29:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ROOqxtoiCfE8O4j+YKEiZvPOAjwjKJMh/CgNo9Fe3b6Zb/uK2wozvvgAdgLZoxAV2ogWinlfQWxuYVWLmoK3BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T17:38:46.865455Z"},"content_sha256":"fa78f75a4c3cad040dea365eb7ffa3a6d29ead1332af91c9d6d628a42a41f8aa","schema_version":"1.0","event_id":"sha256:fa78f75a4c3cad040dea365eb7ffa3a6d29ead1332af91c9d6d628a42a41f8aa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZAYTSI2ZQONCJJML375DCM2VEL/bundle.json","state_url":"https://pith.science/pith/ZAYTSI2ZQONCJJML375DCM2VEL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZAYTSI2ZQONCJJML375DCM2VEL/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":"2026-08-03T17:38:46Z","links":{"resolver":"https://pith.science/pith/ZAYTSI2ZQONCJJML375DCM2VEL","bundle":"https://pith.science/pith/ZAYTSI2ZQONCJJML375DCM2VEL/bundle.json","state":"https://pith.science/pith/ZAYTSI2ZQONCJJML375DCM2VEL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZAYTSI2ZQONCJJML375DCM2VEL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:ZAYTSI2ZQONCJJML375DCM2VEL","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":"c7771c039b64e1153b3046755dee1df28b0f090ea8ffcb180ecbd672d47d76d6","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-10-25T16:02:31Z","title_canon_sha256":"21be76e29b39d9f67479dd4171e6904e8dbb735d63178f17e49f5ff5a7ca31db"},"schema_version":"1.0","source":{"id":"hep-ph/9510406","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9510406","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9510406v1","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9510406","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_12","alias_value":"ZAYTSI2ZQONC","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_16","alias_value":"ZAYTSI2ZQONCJJML","created_at":"2026-07-04T14:29:49Z"},{"alias_kind":"pith_short_8","alias_value":"ZAYTSI2Z","created_at":"2026-07-04T14:29:49Z"}],"graph_snapshots":[{"event_id":"sha256:fa78f75a4c3cad040dea365eb7ffa3a6d29ead1332af91c9d6d628a42a41f8aa","target":"graph","created_at":"2026-07-04T14:29:49Z","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/hep-ph/9510406/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We construct an effective Lagrangian for the hadronic decays of a heavy excited $s$-wave-spin-one quarkonium into its ground state. We show that reasonable fits to the measured invariant mass spectra in the $J/\\psi$ and $\\Upsilon$ systems can be obtained working in the chiral limit. The mass dependence of the various terms in the Lagrangian is discussed on the basis of a quark model.","authors_text":"Res Urech, Thomas Mannel","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-10-25T16:02:31Z","title":"Hadronic Decays of Excited Heavy Quarkonia"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9510406","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":"sha256:574f027aba90499660e9205e2dd1f63638546a0ac92e50779c12dc718aed805f","target":"record","created_at":"2026-07-04T14:29:49Z","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":"c7771c039b64e1153b3046755dee1df28b0f090ea8ffcb180ecbd672d47d76d6","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1995-10-25T16:02:31Z","title_canon_sha256":"21be76e29b39d9f67479dd4171e6904e8dbb735d63178f17e49f5ff5a7ca31db"},"schema_version":"1.0","source":{"id":"hep-ph/9510406","kind":"arxiv","version":1}},"canonical_sha256":"c831392359839a24a58bdffa31335522f698a5dd18c5b856a6b7d91082087a4b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c831392359839a24a58bdffa31335522f698a5dd18c5b856a6b7d91082087a4b","first_computed_at":"2026-07-04T14:29:49.958049Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:29:49.958049Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"J8EskTO1DYCpbLzmX+JoQUoFWTwqVzs9sCJcLeW4Rp5LtE4KVtijvYKN0Z+7LlXwsRsPIVooOdXgYjG/K99OCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T14:29:49.958412Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9510406","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:574f027aba90499660e9205e2dd1f63638546a0ac92e50779c12dc718aed805f","sha256:fa78f75a4c3cad040dea365eb7ffa3a6d29ead1332af91c9d6d628a42a41f8aa"],"state_sha256":"ec1f7063c5f954484f3535adf12add223fe17cd4e9903e0c4e9e46d76b676951"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ukM6GGhlC7o//93GExel+ceTYvLAoDH27jV8kRpSK2VKr+OqUzeePDFHxcJBCIIYijt5+1SCYRuOioVMdJGeAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T17:38:46.869114Z","bundle_sha256":"ef3fbb913fb5b0bda092586f5488a0ea20335f16a662d8a11c0aeeb3ad1f5186"}}