{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:ZM74SHOBD6YFADRHVJYKOCPJOR","short_pith_number":"pith:ZM74SHOB","canonical_record":{"source":{"id":"hep-ph/9706223","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-06-03T09:52:39Z","cross_cats_sorted":[],"title_canon_sha256":"7030866914966c40a58c3cf240bba17b29272670c6b74b0ffbf0041b43289571","abstract_canon_sha256":"25257420fa5296faa2f0c80b2b28d57c576d9b549169843f23417b20ba61565a"},"schema_version":"1.0"},"canonical_sha256":"cb3fc91dc11fb0500e27aa70a709e97473c37a4a159664af9934b7251a4c8065","source":{"kind":"arxiv","id":"hep-ph/9706223","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9706223","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9706223v1","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9706223","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_12","alias_value":"ZM74SHOBD6YF","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"ZM74SHOBD6YFADRH","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"ZM74SHOB","created_at":"2026-07-04T15:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:ZM74SHOBD6YFADRHVJYKOCPJOR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9706223","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-06-03T09:52:39Z","cross_cats_sorted":[],"title_canon_sha256":"7030866914966c40a58c3cf240bba17b29272670c6b74b0ffbf0041b43289571","abstract_canon_sha256":"25257420fa5296faa2f0c80b2b28d57c576d9b549169843f23417b20ba61565a"},"schema_version":"1.0"},"canonical_sha256":"cb3fc91dc11fb0500e27aa70a709e97473c37a4a159664af9934b7251a4c8065","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:27:23.189002Z","signature_b64":"6wY8vNXL4uQ4gUJ2mQ38/WakVaNVVVUEBWu5WYwLM3Yb/5hn2BTLfnoMxvFbCqNxcphYbeJIkAT6hyANCmiqBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb3fc91dc11fb0500e27aa70a709e97473c37a4a159664af9934b7251a4c8065","last_reissued_at":"2026-07-04T15:27:23.188603Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:27:23.188603Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9706223","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":"2026-07-04T15:27:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"caijAN6RUeyPlHQvt7jFz9SPjYtz7aghkfdcjpR6n4JRsjy6WwXICSkw88u8+aYP/f2HdeELUj4mUnlbWqypAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T13:13:41.036636Z"},"content_sha256":"dbe9e9f365165b7d6a23d16905aee99f01a6fb6ee39c22cd57113e5d30b3028d","schema_version":"1.0","event_id":"sha256:dbe9e9f365165b7d6a23d16905aee99f01a6fb6ee39c22cd57113e5d30b3028d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:ZM74SHOBD6YFADRHVJYKOCPJOR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonleptonic two-body charmed meson decays in an effective model for their semileptonic decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Bajc, S. Fajfer R. J. Oakes, S. Prelov\\v{s}ek","submitted_at":"1997-06-03T09:52:39Z","abstract_excerpt":"We analyze $D \\to P V$, $D \\to PP$ and $D \\to VV$ decays within a model developed to describe the semileptonic decays $D \\to V l \\nu_l$ and $D\\to P l \\nu_l$. This model combines the heavy quark effective Lagrangian and chiral perturbation theory. We determine amplitudes for decays in which the direct weak annihilation of the initial $D$ meson is absent or negligible, and in which the final state interactions are small. This analysis reduces the arbitrariness in the choice of model parameters. The calculated decay widths are in good agreement with the experimental results."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9706223","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/9706223/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":"2026-07-04T15:27:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zReoVLok466mgs8605N9SnR8zLqL2XOLfL44PK0DLpBGzvTwhKr0n9ZI3Cv7lNgsYBniZwa8VAohzmv1lOsaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T13:13:41.037755Z"},"content_sha256":"0aa7b093f60b7f362ed99b02f01954ad77bdfc7e0b85c146d2d58fef9306e8b7","schema_version":"1.0","event_id":"sha256:0aa7b093f60b7f362ed99b02f01954ad77bdfc7e0b85c146d2d58fef9306e8b7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/bundle.json","state_url":"https://pith.science/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/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":"2026-08-04T13:13:41Z","links":{"resolver":"https://pith.science/pith/ZM74SHOBD6YFADRHVJYKOCPJOR","bundle":"https://pith.science/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/bundle.json","state":"https://pith.science/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZM74SHOBD6YFADRHVJYKOCPJOR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:ZM74SHOBD6YFADRHVJYKOCPJOR","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":"25257420fa5296faa2f0c80b2b28d57c576d9b549169843f23417b20ba61565a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1997-06-03T09:52:39Z","title_canon_sha256":"7030866914966c40a58c3cf240bba17b29272670c6b74b0ffbf0041b43289571"},"schema_version":"1.0","source":{"id":"hep-ph/9706223","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9706223","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9706223v1","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9706223","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_12","alias_value":"ZM74SHOBD6YF","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"ZM74SHOBD6YFADRH","created_at":"2026-07-04T15:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"ZM74SHOB","created_at":"2026-07-04T15:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:0aa7b093f60b7f362ed99b02f01954ad77bdfc7e0b85c146d2d58fef9306e8b7","target":"graph","created_at":"2026-07-04T15:27:23Z","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/9706223/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We analyze $D \\to P V$, $D \\to PP$ and $D \\to VV$ decays within a model developed to describe the semileptonic decays $D \\to V l \\nu_l$ and $D\\to P l \\nu_l$. This model combines the heavy quark effective Lagrangian and chiral perturbation theory. We determine amplitudes for decays in which the direct weak annihilation of the initial $D$ meson is absent or negligible, and in which the final state interactions are small. This analysis reduces the arbitrariness in the choice of model parameters. The calculated decay widths are in good agreement with the experimental results.","authors_text":"B. Bajc, S. Fajfer R. J. Oakes, S. Prelov\\v{s}ek","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1997-06-03T09:52:39Z","title":"Nonleptonic two-body charmed meson decays in an effective model for their semileptonic decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9706223","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:dbe9e9f365165b7d6a23d16905aee99f01a6fb6ee39c22cd57113e5d30b3028d","target":"record","created_at":"2026-07-04T15:27:23Z","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":"25257420fa5296faa2f0c80b2b28d57c576d9b549169843f23417b20ba61565a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1997-06-03T09:52:39Z","title_canon_sha256":"7030866914966c40a58c3cf240bba17b29272670c6b74b0ffbf0041b43289571"},"schema_version":"1.0","source":{"id":"hep-ph/9706223","kind":"arxiv","version":1}},"canonical_sha256":"cb3fc91dc11fb0500e27aa70a709e97473c37a4a159664af9934b7251a4c8065","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cb3fc91dc11fb0500e27aa70a709e97473c37a4a159664af9934b7251a4c8065","first_computed_at":"2026-07-04T15:27:23.188603Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:27:23.188603Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6wY8vNXL4uQ4gUJ2mQ38/WakVaNVVVUEBWu5WYwLM3Yb/5hn2BTLfnoMxvFbCqNxcphYbeJIkAT6hyANCmiqBQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:27:23.189002Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9706223","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dbe9e9f365165b7d6a23d16905aee99f01a6fb6ee39c22cd57113e5d30b3028d","sha256:0aa7b093f60b7f362ed99b02f01954ad77bdfc7e0b85c146d2d58fef9306e8b7"],"state_sha256":"5a2acdcb8fafc4f6a52f926419ea53fafdc1b192fd6b7d3bc96e4b34bd29ea62"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DNPKg9gCerzi/bcNV7vn6h7g6Mvs15QPtr264nCVazQholEDNgo3441eZxSIIUS4WYo5TpMotnwfPpOuLtI6CQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T13:13:41.044162Z","bundle_sha256":"f8d452860a24983d8ba48ef45c61edc84170c593f720a109d4fc0d89ae25834a"}}