{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:EYECFPF2TEUL7VQ6ZPSPQR2VOB","short_pith_number":"pith:EYECFPF2","canonical_record":{"source":{"id":"1611.04768","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T10:07:54Z","cross_cats_sorted":["hep-ex","physics.data-an"],"title_canon_sha256":"f71ed7a83006a36f81f5f7e8aa8841e1fedb79ea3df56ce895650c9ac08101aa","abstract_canon_sha256":"584b4a4dbc7f410c065365b7e5c6316d157859c6070ffe7b7eee12d3b16ca7ea"},"schema_version":"1.0"},"canonical_sha256":"260822bcba9928bfd61ecbe4f84755707c00ed1b4349cbdac692f85792c8a958","source":{"kind":"arxiv","id":"1611.04768","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.04768","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"arxiv_version","alias_value":"1611.04768v2","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04768","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"pith_short_12","alias_value":"EYECFPF2TEUL","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"EYECFPF2TEUL7VQ6","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"EYECFPF2","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:EYECFPF2TEUL7VQ6ZPSPQR2VOB","target":"record","payload":{"canonical_record":{"source":{"id":"1611.04768","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T10:07:54Z","cross_cats_sorted":["hep-ex","physics.data-an"],"title_canon_sha256":"f71ed7a83006a36f81f5f7e8aa8841e1fedb79ea3df56ce895650c9ac08101aa","abstract_canon_sha256":"584b4a4dbc7f410c065365b7e5c6316d157859c6070ffe7b7eee12d3b16ca7ea"},"schema_version":"1.0"},"canonical_sha256":"260822bcba9928bfd61ecbe4f84755707c00ed1b4349cbdac692f85792c8a958","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:45.433751Z","signature_b64":"2a7xyndIUv5EQP9sxoLx0wEH2t52cUnC1ufyw/Un/To5v8gxXxrFBToET/oQbfOJF1VHC7nJ1d4Z+B8NDhyXBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"260822bcba9928bfd61ecbe4f84755707c00ed1b4349cbdac692f85792c8a958","last_reissued_at":"2026-05-18T00:45:45.433123Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:45.433123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.04768","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:45:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WKfXn292M5tvloR0j7UMc1JW7Nr9JfRgEPrBwEJbGLt7mKRZylw8LVaj1WpNBsdiVypZ6O1h5UvQr7QkQdBZCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T18:09:10.722893Z"},"content_sha256":"4cd650d8e833eb11cf4155bca681148af7467e5c2e907255b2a7187bb22df416","schema_version":"1.0","event_id":"sha256:4cd650d8e833eb11cf4155bca681148af7467e5c2e907255b2a7187bb22df416"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:EYECFPF2TEUL7VQ6ZPSPQR2VOB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modelling theoretical uncertainties in phenomenological analyses for particle physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","physics.data-an"],"primary_cat":"hep-ph","authors_text":"J\\'er\\^ome Charles, Luiz Vale Silva, S\\'ebastien Descotes-Genon, Valentin Niess","submitted_at":"2016-11-15T10:07:54Z","abstract_excerpt":"The determination of the fundamental parameters of the Standard Model (and its extensions) is often limited by the presence of statistical and theoretical uncertainties. We present several models for the latter uncertainties (random, nuisance, external) in the frequentist framework, and we derive the corresponding $p$-values. In the case of the nuisance approach where theoretical uncertainties are modeled as biases, we highlight the important, but arbitrary, issue of the range of variation chosen for the bias parameters. We introduce the concept of adaptive $p$-value, which is obtained by adju"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.04768","kind":"arxiv","version":2},"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":"2026-05-18T00:45:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OnzVfxBaQsO7eFkktMYrfXbx63r4geSGbjr17GPKYpRRNDl5M2hB4OacdW2VFZSEGfM2KdN3lWDu5sr6mV88Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T18:09:10.723232Z"},"content_sha256":"23ccd7a6bf941ae8d6ad082000c9d66e1f4db3ba6b21b847325a4659ef7fa9d2","schema_version":"1.0","event_id":"sha256:23ccd7a6bf941ae8d6ad082000c9d66e1f4db3ba6b21b847325a4659ef7fa9d2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/bundle.json","state_url":"https://pith.science/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/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":"2026-06-27T18:09:10Z","links":{"resolver":"https://pith.science/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB","bundle":"https://pith.science/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/bundle.json","state":"https://pith.science/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EYECFPF2TEUL7VQ6ZPSPQR2VOB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:EYECFPF2TEUL7VQ6ZPSPQR2VOB","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":"584b4a4dbc7f410c065365b7e5c6316d157859c6070ffe7b7eee12d3b16ca7ea","cross_cats_sorted":["hep-ex","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T10:07:54Z","title_canon_sha256":"f71ed7a83006a36f81f5f7e8aa8841e1fedb79ea3df56ce895650c9ac08101aa"},"schema_version":"1.0","source":{"id":"1611.04768","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.04768","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"arxiv_version","alias_value":"1611.04768v2","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04768","created_at":"2026-05-18T00:45:45Z"},{"alias_kind":"pith_short_12","alias_value":"EYECFPF2TEUL","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"EYECFPF2TEUL7VQ6","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"EYECFPF2","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:23ccd7a6bf941ae8d6ad082000c9d66e1f4db3ba6b21b847325a4659ef7fa9d2","target":"graph","created_at":"2026-05-18T00:45:45Z","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 determination of the fundamental parameters of the Standard Model (and its extensions) is often limited by the presence of statistical and theoretical uncertainties. We present several models for the latter uncertainties (random, nuisance, external) in the frequentist framework, and we derive the corresponding $p$-values. In the case of the nuisance approach where theoretical uncertainties are modeled as biases, we highlight the important, but arbitrary, issue of the range of variation chosen for the bias parameters. We introduce the concept of adaptive $p$-value, which is obtained by adju","authors_text":"J\\'er\\^ome Charles, Luiz Vale Silva, S\\'ebastien Descotes-Genon, Valentin Niess","cross_cats":["hep-ex","physics.data-an"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T10:07:54Z","title":"Modelling theoretical uncertainties in phenomenological analyses for particle physics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.04768","kind":"arxiv","version":2},"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":"sha256:4cd650d8e833eb11cf4155bca681148af7467e5c2e907255b2a7187bb22df416","target":"record","created_at":"2026-05-18T00:45:45Z","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":"584b4a4dbc7f410c065365b7e5c6316d157859c6070ffe7b7eee12d3b16ca7ea","cross_cats_sorted":["hep-ex","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T10:07:54Z","title_canon_sha256":"f71ed7a83006a36f81f5f7e8aa8841e1fedb79ea3df56ce895650c9ac08101aa"},"schema_version":"1.0","source":{"id":"1611.04768","kind":"arxiv","version":2}},"canonical_sha256":"260822bcba9928bfd61ecbe4f84755707c00ed1b4349cbdac692f85792c8a958","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"260822bcba9928bfd61ecbe4f84755707c00ed1b4349cbdac692f85792c8a958","first_computed_at":"2026-05-18T00:45:45.433123Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:45:45.433123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2a7xyndIUv5EQP9sxoLx0wEH2t52cUnC1ufyw/Un/To5v8gxXxrFBToET/oQbfOJF1VHC7nJ1d4Z+B8NDhyXBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:45:45.433751Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.04768","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4cd650d8e833eb11cf4155bca681148af7467e5c2e907255b2a7187bb22df416","sha256:23ccd7a6bf941ae8d6ad082000c9d66e1f4db3ba6b21b847325a4659ef7fa9d2"],"state_sha256":"c7745d18699a7b7e99d442db5c5afcfdda7d6900614976c6c66618fd20ac2699"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d0+OWiFzyoHCVxAFVgYI9XtvZZSviMPft8O0yw8AhP+63qZQ/DRxsSYtfm9aOM4obUkROE8kXCpAZSIHpspBAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T18:09:10.725080Z","bundle_sha256":"4f7b753d82eea06f1b01ede572dd7b4fa42ae8fcc416bdd0eae20ec79ee56a65"}}