{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:QXBBCWBE24K5RIBBN7WDUSOLBZ","short_pith_number":"pith:QXBBCWBE","canonical_record":{"source":{"id":"physics/0605236","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.data-an","submitted_at":"2006-05-26T19:45:50Z","cross_cats_sorted":[],"title_canon_sha256":"dec6c7bdae4db191e20bd299e458de78d4951840a6e635fede11e3b2a05132ad","abstract_canon_sha256":"5f4b2989e5fa429620fd25d6a0037ad5dd8ad2c2d6de0a62f1a7b4e6207cf0ec"},"schema_version":"1.0"},"canonical_sha256":"85c2115824d715d8a0216fec3a49cb0e533ebd27f3d2f71190069d2cea4db1ab","source":{"kind":"arxiv","id":"physics/0605236","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0605236","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0605236v1","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0605236","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_12","alias_value":"QXBBCWBE24K5","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_16","alias_value":"QXBBCWBE24K5RIBB","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_8","alias_value":"QXBBCWBE","created_at":"2026-07-04T14:55:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:QXBBCWBE24K5RIBBN7WDUSOLBZ","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0605236","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.data-an","submitted_at":"2006-05-26T19:45:50Z","cross_cats_sorted":[],"title_canon_sha256":"dec6c7bdae4db191e20bd299e458de78d4951840a6e635fede11e3b2a05132ad","abstract_canon_sha256":"5f4b2989e5fa429620fd25d6a0037ad5dd8ad2c2d6de0a62f1a7b4e6207cf0ec"},"schema_version":"1.0"},"canonical_sha256":"85c2115824d715d8a0216fec3a49cb0e533ebd27f3d2f71190069d2cea4db1ab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:55:10.878944Z","signature_b64":"8DSyNHulbpHpSdSxZlcV4KemcoOz/owyFI7kjbrpuyCjueB+4/YVMd9aiUG3t9tDCQL6AyDFNca79MHtlEixDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"85c2115824d715d8a0216fec3a49cb0e533ebd27f3d2f71190069d2cea4db1ab","last_reissued_at":"2026-07-04T14:55:10.878599Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:55:10.878599Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0605236","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":"2026-07-04T14:55:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SzxNXna9S5jHRKj3MVDz7otMv+WILgv2KfMKj+2v01ZicBUy1sloV9vbRj2x1UhEh3oNl4qQHi4dU4PaL5v3Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T12:03:44.698733Z"},"content_sha256":"1aa5078a229759e6c912e78db3881def6d4acf8cc8cfa162777fd031447a94f4","schema_version":"1.0","event_id":"sha256:1aa5078a229759e6c912e78db3881def6d4acf8cc8cfa162777fd031447a94f4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:QXBBCWBE24K5RIBBN7WDUSOLBZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A more exact solution for incorporating multiplicative systematic uncertainties in branching ratio limits","license":"","headline":"","cross_cats":[],"primary_cat":"physics.data-an","authors_text":"K. Stenson","submitted_at":"2006-05-26T19:45:50Z","abstract_excerpt":"A method to include multiplicative systematic uncertainties into branching ratio limits was proposed by M. Convery. That solution used approximations which are not necessarily valid. This note provides a solution without approximations and compares the results."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0605236","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/physics/0605236/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":"2026-07-04T14:55:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2f5G2xph+8aZPvSdz9IXeKtNOiazmbGnO+p1y6o7pGyXnZAwyQG5zNuNACtTAfAx9RvnEH9r7p+Fbs/hzO4ECQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T12:03:44.699229Z"},"content_sha256":"d7e45fffbba520cec34ffda2524da5b7efbaccce46922cba224589f0b4ecc738","schema_version":"1.0","event_id":"sha256:d7e45fffbba520cec34ffda2524da5b7efbaccce46922cba224589f0b4ecc738"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/bundle.json","state_url":"https://pith.science/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/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":"2026-08-05T12:03:44Z","links":{"resolver":"https://pith.science/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ","bundle":"https://pith.science/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/bundle.json","state":"https://pith.science/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QXBBCWBE24K5RIBBN7WDUSOLBZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:QXBBCWBE24K5RIBBN7WDUSOLBZ","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":"5f4b2989e5fa429620fd25d6a0037ad5dd8ad2c2d6de0a62f1a7b4e6207cf0ec","cross_cats_sorted":[],"license":"","primary_cat":"physics.data-an","submitted_at":"2006-05-26T19:45:50Z","title_canon_sha256":"dec6c7bdae4db191e20bd299e458de78d4951840a6e635fede11e3b2a05132ad"},"schema_version":"1.0","source":{"id":"physics/0605236","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0605236","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0605236v1","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0605236","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_12","alias_value":"QXBBCWBE24K5","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_16","alias_value":"QXBBCWBE24K5RIBB","created_at":"2026-07-04T14:55:10Z"},{"alias_kind":"pith_short_8","alias_value":"QXBBCWBE","created_at":"2026-07-04T14:55:10Z"}],"graph_snapshots":[{"event_id":"sha256:d7e45fffbba520cec34ffda2524da5b7efbaccce46922cba224589f0b4ecc738","target":"graph","created_at":"2026-07-04T14:55:10Z","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/physics/0605236/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A method to include multiplicative systematic uncertainties into branching ratio limits was proposed by M. Convery. That solution used approximations which are not necessarily valid. This note provides a solution without approximations and compares the results.","authors_text":"K. Stenson","cross_cats":[],"headline":"","license":"","primary_cat":"physics.data-an","submitted_at":"2006-05-26T19:45:50Z","title":"A more exact solution for incorporating multiplicative systematic uncertainties in branching ratio limits"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0605236","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":"sha256:1aa5078a229759e6c912e78db3881def6d4acf8cc8cfa162777fd031447a94f4","target":"record","created_at":"2026-07-04T14:55:10Z","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":"5f4b2989e5fa429620fd25d6a0037ad5dd8ad2c2d6de0a62f1a7b4e6207cf0ec","cross_cats_sorted":[],"license":"","primary_cat":"physics.data-an","submitted_at":"2006-05-26T19:45:50Z","title_canon_sha256":"dec6c7bdae4db191e20bd299e458de78d4951840a6e635fede11e3b2a05132ad"},"schema_version":"1.0","source":{"id":"physics/0605236","kind":"arxiv","version":1}},"canonical_sha256":"85c2115824d715d8a0216fec3a49cb0e533ebd27f3d2f71190069d2cea4db1ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"85c2115824d715d8a0216fec3a49cb0e533ebd27f3d2f71190069d2cea4db1ab","first_computed_at":"2026-07-04T14:55:10.878599Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:55:10.878599Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8DSyNHulbpHpSdSxZlcV4KemcoOz/owyFI7kjbrpuyCjueB+4/YVMd9aiUG3t9tDCQL6AyDFNca79MHtlEixDA==","signature_status":"signed_v1","signed_at":"2026-07-04T14:55:10.878944Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0605236","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1aa5078a229759e6c912e78db3881def6d4acf8cc8cfa162777fd031447a94f4","sha256:d7e45fffbba520cec34ffda2524da5b7efbaccce46922cba224589f0b4ecc738"],"state_sha256":"44eba125463883043edc3ce965f5a37d971934d3712efaa474875c70e8adc313"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LMRzsrVhGWBTr/lf2vwJzYW1gDgIekOoAcT8c4+ye1ZtQOTZZr9H70JA0eP3w5MawKUT8+VgB/PZmsYkYKoXBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T12:03:44.703131Z","bundle_sha256":"a5dd6aa021fd2055410117e71c9f15edba0f8b4b98ca436276490e067f8d215b"}}