{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:MNY5OPJXZHCAARCRXQHCVYSGTY","short_pith_number":"pith:MNY5OPJX","canonical_record":{"source":{"id":"1407.0657","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-07-02T17:29:52Z","cross_cats_sorted":["hep-ph","nucl-ex","physics.data-an"],"title_canon_sha256":"84207afc07bf07f8665c25ef05afb6bb1cfa8f3bd297bf176856dca49621d950","abstract_canon_sha256":"a1ac0a8ea1dfa25e9c75931483ad473787db751cf1b9235a37a4a915bcd4ba08"},"schema_version":"1.0"},"canonical_sha256":"6371d73d37c9c4004451bc0e2ae2469e14319d583edf8c868bb8be290ff40c87","source":{"kind":"arxiv","id":"1407.0657","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.0657","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"arxiv_version","alias_value":"1407.0657v2","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.0657","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"pith_short_12","alias_value":"MNY5OPJXZHCA","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MNY5OPJXZHCAARCR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MNY5OPJX","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:MNY5OPJXZHCAARCRXQHCVYSGTY","target":"record","payload":{"canonical_record":{"source":{"id":"1407.0657","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-07-02T17:29:52Z","cross_cats_sorted":["hep-ph","nucl-ex","physics.data-an"],"title_canon_sha256":"84207afc07bf07f8665c25ef05afb6bb1cfa8f3bd297bf176856dca49621d950","abstract_canon_sha256":"a1ac0a8ea1dfa25e9c75931483ad473787db751cf1b9235a37a4a915bcd4ba08"},"schema_version":"1.0"},"canonical_sha256":"6371d73d37c9c4004451bc0e2ae2469e14319d583edf8c868bb8be290ff40c87","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:15:00.540777Z","signature_b64":"iipCdfYUzcX5146mPqAbgIM15ld6/n8V9PD+yQcQCtpjlVr4CSRUWYIg7G10Z97+Va1Llmcxtl3NiCXzzBsbCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6371d73d37c9c4004451bc0e2ae2469e14319d583edf8c868bb8be290ff40c87","last_reissued_at":"2026-05-18T01:15:00.540228Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:15:00.540228Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.0657","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":"2026-05-18T01:15:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BNnFQsm0r0ncwbnZqQjoUPWvSTCP7pEIpK56gxIfeMQxL8PkEb7973aevac93Yjv5bxlkJuGrRu4QVrDE3EtBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:06:38.555501Z"},"content_sha256":"003ace9928005622ed8230c425d1c265d7065c5adfd488e5adbc8c16fce61c6b","schema_version":"1.0","event_id":"sha256:003ace9928005622ed8230c425d1c265d7065c5adfd488e5adbc8c16fce61c6b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:MNY5OPJXZHCAARCRXQHCVYSGTY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A recipe for EFT uncertainty quantification in nuclear physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex","physics.data-an"],"primary_cat":"nucl-th","authors_text":"D.R. Phillips, R.J. Furnstahl, S. Wesolowski","submitted_at":"2014-07-02T17:29:52Z","abstract_excerpt":"The application of effective field theory (EFT) methods to nuclear systems provides the opportunity to rigorously estimate the uncertainties originating in the nuclear Hamiltonian. Yet this is just one source of uncertainty in the observables predicted by calculations based on nuclear EFTs. We discuss the goals of uncertainty quantification in such calculations and outline a recipe to obtain statistically meaningful error bars for their predictions. We argue that the different sources of theory error can be accounted for within a Bayesian framework, as we illustrate using a toy model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.0657","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":"2026-05-18T01:15:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F2uWwU6zpFwoDDUETmvZWfr3hQYKlx7IJLILaMduekZ+3y63A9oV1Ka2GxIC1DxWFGR23Vxdwb3Gm1eE8cANDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:06:38.555856Z"},"content_sha256":"0f5803e6ba0bb9af116f6932036771878fde46805ebd52cc8799b96b1f06514e","schema_version":"1.0","event_id":"sha256:0f5803e6ba0bb9af116f6932036771878fde46805ebd52cc8799b96b1f06514e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/bundle.json","state_url":"https://pith.science/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/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":"2026-05-28T05:06:38Z","links":{"resolver":"https://pith.science/pith/MNY5OPJXZHCAARCRXQHCVYSGTY","bundle":"https://pith.science/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/bundle.json","state":"https://pith.science/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MNY5OPJXZHCAARCRXQHCVYSGTY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:MNY5OPJXZHCAARCRXQHCVYSGTY","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":"a1ac0a8ea1dfa25e9c75931483ad473787db751cf1b9235a37a4a915bcd4ba08","cross_cats_sorted":["hep-ph","nucl-ex","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-07-02T17:29:52Z","title_canon_sha256":"84207afc07bf07f8665c25ef05afb6bb1cfa8f3bd297bf176856dca49621d950"},"schema_version":"1.0","source":{"id":"1407.0657","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.0657","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"arxiv_version","alias_value":"1407.0657v2","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.0657","created_at":"2026-05-18T01:15:00Z"},{"alias_kind":"pith_short_12","alias_value":"MNY5OPJXZHCA","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"MNY5OPJXZHCAARCR","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"MNY5OPJX","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:0f5803e6ba0bb9af116f6932036771878fde46805ebd52cc8799b96b1f06514e","target":"graph","created_at":"2026-05-18T01:15:00Z","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 application of effective field theory (EFT) methods to nuclear systems provides the opportunity to rigorously estimate the uncertainties originating in the nuclear Hamiltonian. Yet this is just one source of uncertainty in the observables predicted by calculations based on nuclear EFTs. We discuss the goals of uncertainty quantification in such calculations and outline a recipe to obtain statistically meaningful error bars for their predictions. We argue that the different sources of theory error can be accounted for within a Bayesian framework, as we illustrate using a toy model.","authors_text":"D.R. Phillips, R.J. Furnstahl, S. Wesolowski","cross_cats":["hep-ph","nucl-ex","physics.data-an"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-07-02T17:29:52Z","title":"A recipe for EFT uncertainty quantification in nuclear physics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.0657","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":"sha256:003ace9928005622ed8230c425d1c265d7065c5adfd488e5adbc8c16fce61c6b","target":"record","created_at":"2026-05-18T01:15:00Z","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":"a1ac0a8ea1dfa25e9c75931483ad473787db751cf1b9235a37a4a915bcd4ba08","cross_cats_sorted":["hep-ph","nucl-ex","physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-07-02T17:29:52Z","title_canon_sha256":"84207afc07bf07f8665c25ef05afb6bb1cfa8f3bd297bf176856dca49621d950"},"schema_version":"1.0","source":{"id":"1407.0657","kind":"arxiv","version":2}},"canonical_sha256":"6371d73d37c9c4004451bc0e2ae2469e14319d583edf8c868bb8be290ff40c87","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6371d73d37c9c4004451bc0e2ae2469e14319d583edf8c868bb8be290ff40c87","first_computed_at":"2026-05-18T01:15:00.540228Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:15:00.540228Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iipCdfYUzcX5146mPqAbgIM15ld6/n8V9PD+yQcQCtpjlVr4CSRUWYIg7G10Z97+Va1Llmcxtl3NiCXzzBsbCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:15:00.540777Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.0657","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:003ace9928005622ed8230c425d1c265d7065c5adfd488e5adbc8c16fce61c6b","sha256:0f5803e6ba0bb9af116f6932036771878fde46805ebd52cc8799b96b1f06514e"],"state_sha256":"f0c9d389d2d77d6f904ed5002885090212c0206863d85f2c4e3cd599cc8430b4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"70kn5nwXS1pDzB80f780KLHuDxxiGNQAzH81+PiffNQNRzActnOrPzIvj5/SaSUEW9sw83JbsNjzL5i1bo7kDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T05:06:38.557758Z","bundle_sha256":"7a7c063ef2520e84af4e50d963ac47c65144d2cf8a52056aff24ee5b088333ac"}}