{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:7CO3L3YKRWP47HALDFCNU5Y5PX","short_pith_number":"pith:7CO3L3YK","canonical_record":{"source":{"id":"1603.01805","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-06T09:04:31Z","cross_cats_sorted":[],"title_canon_sha256":"c815ca5252c32ed104997c31498efd1d78cd9387f0adb2ddbcb554e59360f63a","abstract_canon_sha256":"2c8da5b7e1f5266353e9398d3d27f8d2ce22f36ec9ef2230805aed5da8ea1680"},"schema_version":"1.0"},"canonical_sha256":"f89db5ef0a8d9fcf9c0b1944da771d7dcd15d36fc04b957ccc4eb6d1d41a325c","source":{"kind":"arxiv","id":"1603.01805","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.01805","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"arxiv_version","alias_value":"1603.01805v1","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01805","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"pith_short_12","alias_value":"7CO3L3YKRWP4","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7CO3L3YKRWP47HAL","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7CO3L3YK","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:7CO3L3YKRWP47HALDFCNU5Y5PX","target":"record","payload":{"canonical_record":{"source":{"id":"1603.01805","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-06T09:04:31Z","cross_cats_sorted":[],"title_canon_sha256":"c815ca5252c32ed104997c31498efd1d78cd9387f0adb2ddbcb554e59360f63a","abstract_canon_sha256":"2c8da5b7e1f5266353e9398d3d27f8d2ce22f36ec9ef2230805aed5da8ea1680"},"schema_version":"1.0"},"canonical_sha256":"f89db5ef0a8d9fcf9c0b1944da771d7dcd15d36fc04b957ccc4eb6d1d41a325c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:12.120568Z","signature_b64":"HXAPVEJLpKPbr5atqcmNOTb5iroCfPBihfA2ZW9MOkyntn+HV5svkRlCqoORWY0Cs6UlrkotpAQzrOT0wuCwBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f89db5ef0a8d9fcf9c0b1944da771d7dcd15d36fc04b957ccc4eb6d1d41a325c","last_reissued_at":"2026-05-18T01:12:12.119986Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:12.119986Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1603.01805","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":"2026-05-18T01:12:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oZyXLMNS1Qyz4benBv5/VZ7wYs1jKXFWrSotu4XPWAR7IVntmmpJzIQlEp9Fey/AA2BuILTrcgwGdOKyQ6j5Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T07:19:04.477190Z"},"content_sha256":"425fc118fcede2b80d35004859802e32cfb79c4d8536d2f3c811fa735e6af772","schema_version":"1.0","event_id":"sha256:425fc118fcede2b80d35004859802e32cfb79c4d8536d2f3c811fa735e6af772"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:7CO3L3YKRWP47HALDFCNU5Y5PX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Consistency between the monopole strength of the Hoyle state determined by structural calculation and that extracted from reaction observables","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Kazuyuki Ogata, Kosho Minomo","submitted_at":"2016-03-06T09:04:31Z","abstract_excerpt":"We analyze the $\\alpha$-$^{12}$C inelastic scattering to the $0^+_2$ state of $^{12}$C, the Hoyle state, in a fully microscopic framework. With no free adjustable parameter, the inelastic cross sections at forward angles are well reproduced by the microscopic reaction calculation using the transition density of $^{12}$C obtained by the resonating group method and the nucleon-nucleon $g$ matrix interaction developed by the Melbourne group. It is thus shown that the monopole transition strength obtained by the structural calculation is consistent with that extracted from the reaction observable,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01805","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":""},"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":"2026-05-18T01:12:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WPnE1EtHRAGeN2q3Y5w5JsGAr29ziEnzQp7VdyuW5OHu/RmNhbmGpth2xIsgc1RWC5VTwXaKl+OSspmIYXKGCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T07:19:04.477558Z"},"content_sha256":"e7a5555ed5f6100977a215fe75c41e754d5649f0c2c2c3ac3460151ce766d5d4","schema_version":"1.0","event_id":"sha256:e7a5555ed5f6100977a215fe75c41e754d5649f0c2c2c3ac3460151ce766d5d4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/bundle.json","state_url":"https://pith.science/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/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":"2026-06-05T07:19:04Z","links":{"resolver":"https://pith.science/pith/7CO3L3YKRWP47HALDFCNU5Y5PX","bundle":"https://pith.science/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/bundle.json","state":"https://pith.science/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7CO3L3YKRWP47HALDFCNU5Y5PX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:7CO3L3YKRWP47HALDFCNU5Y5PX","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":"2c8da5b7e1f5266353e9398d3d27f8d2ce22f36ec9ef2230805aed5da8ea1680","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-06T09:04:31Z","title_canon_sha256":"c815ca5252c32ed104997c31498efd1d78cd9387f0adb2ddbcb554e59360f63a"},"schema_version":"1.0","source":{"id":"1603.01805","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.01805","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"arxiv_version","alias_value":"1603.01805v1","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01805","created_at":"2026-05-18T01:12:12Z"},{"alias_kind":"pith_short_12","alias_value":"7CO3L3YKRWP4","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"7CO3L3YKRWP47HAL","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"7CO3L3YK","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:e7a5555ed5f6100977a215fe75c41e754d5649f0c2c2c3ac3460151ce766d5d4","target":"graph","created_at":"2026-05-18T01:12:12Z","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":"We analyze the $\\alpha$-$^{12}$C inelastic scattering to the $0^+_2$ state of $^{12}$C, the Hoyle state, in a fully microscopic framework. With no free adjustable parameter, the inelastic cross sections at forward angles are well reproduced by the microscopic reaction calculation using the transition density of $^{12}$C obtained by the resonating group method and the nucleon-nucleon $g$ matrix interaction developed by the Melbourne group. It is thus shown that the monopole transition strength obtained by the structural calculation is consistent with that extracted from the reaction observable,","authors_text":"Kazuyuki Ogata, Kosho Minomo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-06T09:04:31Z","title":"Consistency between the monopole strength of the Hoyle state determined by structural calculation and that extracted from reaction observables"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01805","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":"sha256:425fc118fcede2b80d35004859802e32cfb79c4d8536d2f3c811fa735e6af772","target":"record","created_at":"2026-05-18T01:12:12Z","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":"2c8da5b7e1f5266353e9398d3d27f8d2ce22f36ec9ef2230805aed5da8ea1680","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-06T09:04:31Z","title_canon_sha256":"c815ca5252c32ed104997c31498efd1d78cd9387f0adb2ddbcb554e59360f63a"},"schema_version":"1.0","source":{"id":"1603.01805","kind":"arxiv","version":1}},"canonical_sha256":"f89db5ef0a8d9fcf9c0b1944da771d7dcd15d36fc04b957ccc4eb6d1d41a325c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f89db5ef0a8d9fcf9c0b1944da771d7dcd15d36fc04b957ccc4eb6d1d41a325c","first_computed_at":"2026-05-18T01:12:12.119986Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:12.119986Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HXAPVEJLpKPbr5atqcmNOTb5iroCfPBihfA2ZW9MOkyntn+HV5svkRlCqoORWY0Cs6UlrkotpAQzrOT0wuCwBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:12.120568Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.01805","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:425fc118fcede2b80d35004859802e32cfb79c4d8536d2f3c811fa735e6af772","sha256:e7a5555ed5f6100977a215fe75c41e754d5649f0c2c2c3ac3460151ce766d5d4"],"state_sha256":"6432511ef3fe26cedb765b6694d9eea572c70b64bf396cb2268f8dd77472421b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ifwat3qc7yOsKnaFO9giDgxnQX1xA082AHTmz4ILlYZImZRAfREJ2wOJc36OACnt01Y2khNhCMIAAuy6hKrLCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T07:19:04.479533Z","bundle_sha256":"382571f81f474464def4cb287392b664d1646c237ac732ab66cf2dd5811de30d"}}