{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:ALVIBLQTR5KXJZ7GMCJCU26NVD","short_pith_number":"pith:ALVIBLQT","canonical_record":{"source":{"id":"2312.12426","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-12-19T18:56:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"4bf5613fffcaeac4d0d957b9b05f7576050c36488f24678270fa27f7626e5c8b","abstract_canon_sha256":"458e29a4eebfc13ac310261653fa8404dabc2a53fc19d83c89fba8a12931fa81"},"schema_version":"1.0"},"canonical_sha256":"02ea80ae138f5574e7e660922a6bcda8dd262211d22397265713e845556b55d6","source":{"kind":"arxiv","id":"2312.12426","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2312.12426","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"2312.12426v1","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.12426","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"ALVIBLQTR5KX","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"ALVIBLQTR5KXJZ7G","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"ALVIBLQT","created_at":"2026-07-05T07:26:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:ALVIBLQTR5KXJZ7GMCJCU26NVD","target":"record","payload":{"canonical_record":{"source":{"id":"2312.12426","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-12-19T18:56:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"4bf5613fffcaeac4d0d957b9b05f7576050c36488f24678270fa27f7626e5c8b","abstract_canon_sha256":"458e29a4eebfc13ac310261653fa8404dabc2a53fc19d83c89fba8a12931fa81"},"schema_version":"1.0"},"canonical_sha256":"02ea80ae138f5574e7e660922a6bcda8dd262211d22397265713e845556b55d6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:26:03.500046Z","signature_b64":"6UvEmMFWwh+1cZZIQL0S8XpPGj00rIqqiWI5dRRg3+Kj4j5qiVjmoDGMM7KWjkuuxJ5w9xGLW9SoZMFNjxqDDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"02ea80ae138f5574e7e660922a6bcda8dd262211d22397265713e845556b55d6","last_reissued_at":"2026-07-05T07:26:03.499560Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:26:03.499560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2312.12426","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":"2026-07-05T07:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gxrnj865VhSu/7f/6mq/5mlNA8/vtSHtsdGxm//kTfdU/qDLKvno0l+Q0HC9KGpll7dbGv+8Pwtz8qasHWXbDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T19:54:24.235646Z"},"content_sha256":"d0dbd99349d215e997583b20c8fff2759f085826aa514ac2ee59adb783d530c3","schema_version":"1.0","event_id":"sha256:d0dbd99349d215e997583b20c8fff2759f085826aa514ac2ee59adb783d530c3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:ALVIBLQTR5KXJZ7GMCJCU26NVD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"ROSE: A reduced-order scattering emulator for optical models","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"physics.comp-ph","authors_text":"Daniel Odell, Edgard Bonilla, Filomena M. Nunes, Kyle Beyer, Kyle Godbey, Manuel Catacora-Rios, Moses Y.-H. Chan, Pablo Giuliani, Richard J. Furnstahl","submitted_at":"2023-12-19T18:56:00Z","abstract_excerpt":"A new generation of phenomenological optical potentials requires robust calibration and uncertainty quantification, motivating the use of Bayesian statistical methods. These Bayesian methods usually require calculating observables for thousands or even millions of parameter sets, making fast and accurate emulators highly desirable or even essential. Emulating scattering across different energies or with interactions such as optical potentials is challenging because of the non-affine parameter dependence, meaning the parameters do not all factorize from individual operators. Here we introduce a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.12426","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/2312.12426/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":"2026-07-05T07:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ROLPRUGmx5McSAKNj4BNg8LTGuZOWuI9IHMW9Js3htAA4XtC0gcAEnxqwCfvMzQLzk3eVdT1ag7i3pUQZ0r2CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T19:54:24.236011Z"},"content_sha256":"3fe7c62ce4f3bb777f482b83f9697306c76d06f8dceb0ef2b934d851a683ef7a","schema_version":"1.0","event_id":"sha256:3fe7c62ce4f3bb777f482b83f9697306c76d06f8dceb0ef2b934d851a683ef7a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/bundle.json","state_url":"https://pith.science/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/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":"2026-07-06T19:54:24Z","links":{"resolver":"https://pith.science/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD","bundle":"https://pith.science/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/bundle.json","state":"https://pith.science/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ALVIBLQTR5KXJZ7GMCJCU26NVD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:ALVIBLQTR5KXJZ7GMCJCU26NVD","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":"458e29a4eebfc13ac310261653fa8404dabc2a53fc19d83c89fba8a12931fa81","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-12-19T18:56:00Z","title_canon_sha256":"4bf5613fffcaeac4d0d957b9b05f7576050c36488f24678270fa27f7626e5c8b"},"schema_version":"1.0","source":{"id":"2312.12426","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2312.12426","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"2312.12426v1","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.12426","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"ALVIBLQTR5KX","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"ALVIBLQTR5KXJZ7G","created_at":"2026-07-05T07:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"ALVIBLQT","created_at":"2026-07-05T07:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:3fe7c62ce4f3bb777f482b83f9697306c76d06f8dceb0ef2b934d851a683ef7a","target":"graph","created_at":"2026-07-05T07:26:03Z","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/2312.12426/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A new generation of phenomenological optical potentials requires robust calibration and uncertainty quantification, motivating the use of Bayesian statistical methods. These Bayesian methods usually require calculating observables for thousands or even millions of parameter sets, making fast and accurate emulators highly desirable or even essential. Emulating scattering across different energies or with interactions such as optical potentials is challenging because of the non-affine parameter dependence, meaning the parameters do not all factorize from individual operators. Here we introduce a","authors_text":"Daniel Odell, Edgard Bonilla, Filomena M. Nunes, Kyle Beyer, Kyle Godbey, Manuel Catacora-Rios, Moses Y.-H. Chan, Pablo Giuliani, Richard J. Furnstahl","cross_cats":["nucl-th"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-12-19T18:56:00Z","title":"ROSE: A reduced-order scattering emulator for optical models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.12426","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:d0dbd99349d215e997583b20c8fff2759f085826aa514ac2ee59adb783d530c3","target":"record","created_at":"2026-07-05T07:26:03Z","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":"458e29a4eebfc13ac310261653fa8404dabc2a53fc19d83c89fba8a12931fa81","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2023-12-19T18:56:00Z","title_canon_sha256":"4bf5613fffcaeac4d0d957b9b05f7576050c36488f24678270fa27f7626e5c8b"},"schema_version":"1.0","source":{"id":"2312.12426","kind":"arxiv","version":1}},"canonical_sha256":"02ea80ae138f5574e7e660922a6bcda8dd262211d22397265713e845556b55d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"02ea80ae138f5574e7e660922a6bcda8dd262211d22397265713e845556b55d6","first_computed_at":"2026-07-05T07:26:03.499560Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:26:03.499560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6UvEmMFWwh+1cZZIQL0S8XpPGj00rIqqiWI5dRRg3+Kj4j5qiVjmoDGMM7KWjkuuxJ5w9xGLW9SoZMFNjxqDDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:26:03.500046Z","signed_message":"canonical_sha256_bytes"},"source_id":"2312.12426","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d0dbd99349d215e997583b20c8fff2759f085826aa514ac2ee59adb783d530c3","sha256:3fe7c62ce4f3bb777f482b83f9697306c76d06f8dceb0ef2b934d851a683ef7a"],"state_sha256":"a3aef4d370237aaa5f2d5fb818cbcf75ca05a43be545c035c7c7f18800de76f9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fgoU15E3VZtSIgxR4dBngOoE4fO48rDMx9179w8bA7UOtZon2m/IsRE8gRY0N65B0KVKBlfvnoy6+cjmW9STAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T19:54:24.237984Z","bundle_sha256":"0b7c64f0324527738e71fea1fbd2dc35e72cc248173cb7d36a5c0ff851536ca8"}}