{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:FOVFPGTYGHGLQEFPMZGKAUROH5","short_pith_number":"pith:FOVFPGTY","canonical_record":{"source":{"id":"1211.7243","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-11-30T13:14:41Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"ced06f62528920232af53c794f3b52ee6e3b5efba4ff185c6649587d37a9e172","abstract_canon_sha256":"df2796c9551ddfdb0cc4db18500215577e319b6ddf49bd5eca8b6fda6eceedd0"},"schema_version":"1.0"},"canonical_sha256":"2baa579a7831ccb810af664ca0522e3f48d87ed1d38831c1c3c78ccb22e1c451","source":{"kind":"arxiv","id":"1211.7243","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.7243","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"arxiv_version","alias_value":"1211.7243v2","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.7243","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"pith_short_12","alias_value":"FOVFPGTYGHGL","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FOVFPGTYGHGLQEFP","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FOVFPGTY","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:FOVFPGTYGHGLQEFPMZGKAUROH5","target":"record","payload":{"canonical_record":{"source":{"id":"1211.7243","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-11-30T13:14:41Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"ced06f62528920232af53c794f3b52ee6e3b5efba4ff185c6649587d37a9e172","abstract_canon_sha256":"df2796c9551ddfdb0cc4db18500215577e319b6ddf49bd5eca8b6fda6eceedd0"},"schema_version":"1.0"},"canonical_sha256":"2baa579a7831ccb810af664ca0522e3f48d87ed1d38831c1c3c78ccb22e1c451","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:00:26.759627Z","signature_b64":"7/Ozrx8yNf/p0MV+wkZ3lJlcJ8xNTjwWWqi/Zdo+JLV87Es5zi9nRdIBoAGA5+lXu3FpV+ZUwAHcX5rIaO+qCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2baa579a7831ccb810af664ca0522e3f48d87ed1d38831c1c3c78ccb22e1c451","last_reissued_at":"2026-05-18T03:00:26.758978Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:00:26.758978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.7243","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":"2026-05-18T03:00:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0xcHVmbC02mCjEy5c1XeNkVpg7FTz5u3PB+IOAYQ70/wjJdpsKiuViL9DEjwl+0AfpHJyfeygF8Rj7z10lySCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:00:11.808738Z"},"content_sha256":"1695d7d0dea9f0e55c8792e2ab64dfab913f71f9166e9b0381b32b2df9b370e3","schema_version":"1.0","event_id":"sha256:1695d7d0dea9f0e55c8792e2ab64dfab913f71f9166e9b0381b32b2df9b370e3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:FOVFPGTYGHGLQEFPMZGKAUROH5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Shape evolution and the role of intruder configurations in Hg isotopes within the interacting boson model based on a Gogny energy density functional","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"K. Nomura, L. M. Robledo, R. Rodriguez-Guzman","submitted_at":"2012-11-30T13:14:41Z","abstract_excerpt":"The interacting boson model with configuration mixing, with parameters derived from the self-consistent mean-field calculation employing the microscopic Gogny energy density functional, is applied to the systematic analysis of the low-lying structure in Hg isotopes. Excitation energies, electromagnetic transition rates, deformation properties, and ground-state properties of the $^{172-204}$Hg nuclei are obtained by mapping the microscopic deformation energy surface onto the equivalent IBM Hamiltonian in the boson condensate. These results point to the overall systematic trend of the transition"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.7243","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":"2026-05-18T03:00:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9ZXVaisezkygd4MLQRN9iRhk+A6mWq4jruVlVOR+wDcSZykQL/nCrkTsuMuzT71ZRjPfbH6Zm0Oum3TPo5IEAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:00:11.809357Z"},"content_sha256":"ad70e1ab58e0198dd2b4d3b3de4ce4214bb042cb1fd8f1c7cbb93bcaf6a7a4b5","schema_version":"1.0","event_id":"sha256:ad70e1ab58e0198dd2b4d3b3de4ce4214bb042cb1fd8f1c7cbb93bcaf6a7a4b5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/bundle.json","state_url":"https://pith.science/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/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":"2026-05-26T11:00:11Z","links":{"resolver":"https://pith.science/pith/FOVFPGTYGHGLQEFPMZGKAUROH5","bundle":"https://pith.science/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/bundle.json","state":"https://pith.science/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FOVFPGTYGHGLQEFPMZGKAUROH5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:FOVFPGTYGHGLQEFPMZGKAUROH5","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":"df2796c9551ddfdb0cc4db18500215577e319b6ddf49bd5eca8b6fda6eceedd0","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-11-30T13:14:41Z","title_canon_sha256":"ced06f62528920232af53c794f3b52ee6e3b5efba4ff185c6649587d37a9e172"},"schema_version":"1.0","source":{"id":"1211.7243","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.7243","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"arxiv_version","alias_value":"1211.7243v2","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.7243","created_at":"2026-05-18T03:00:26Z"},{"alias_kind":"pith_short_12","alias_value":"FOVFPGTYGHGL","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FOVFPGTYGHGLQEFP","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FOVFPGTY","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:ad70e1ab58e0198dd2b4d3b3de4ce4214bb042cb1fd8f1c7cbb93bcaf6a7a4b5","target":"graph","created_at":"2026-05-18T03:00:26Z","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 interacting boson model with configuration mixing, with parameters derived from the self-consistent mean-field calculation employing the microscopic Gogny energy density functional, is applied to the systematic analysis of the low-lying structure in Hg isotopes. Excitation energies, electromagnetic transition rates, deformation properties, and ground-state properties of the $^{172-204}$Hg nuclei are obtained by mapping the microscopic deformation energy surface onto the equivalent IBM Hamiltonian in the boson condensate. These results point to the overall systematic trend of the transition","authors_text":"K. Nomura, L. M. Robledo, R. Rodriguez-Guzman","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-11-30T13:14:41Z","title":"Shape evolution and the role of intruder configurations in Hg isotopes within the interacting boson model based on a Gogny energy density functional"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.7243","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":"sha256:1695d7d0dea9f0e55c8792e2ab64dfab913f71f9166e9b0381b32b2df9b370e3","target":"record","created_at":"2026-05-18T03:00:26Z","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":"df2796c9551ddfdb0cc4db18500215577e319b6ddf49bd5eca8b6fda6eceedd0","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-11-30T13:14:41Z","title_canon_sha256":"ced06f62528920232af53c794f3b52ee6e3b5efba4ff185c6649587d37a9e172"},"schema_version":"1.0","source":{"id":"1211.7243","kind":"arxiv","version":2}},"canonical_sha256":"2baa579a7831ccb810af664ca0522e3f48d87ed1d38831c1c3c78ccb22e1c451","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2baa579a7831ccb810af664ca0522e3f48d87ed1d38831c1c3c78ccb22e1c451","first_computed_at":"2026-05-18T03:00:26.758978Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:00:26.758978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7/Ozrx8yNf/p0MV+wkZ3lJlcJ8xNTjwWWqi/Zdo+JLV87Es5zi9nRdIBoAGA5+lXu3FpV+ZUwAHcX5rIaO+qCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:00:26.759627Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.7243","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1695d7d0dea9f0e55c8792e2ab64dfab913f71f9166e9b0381b32b2df9b370e3","sha256:ad70e1ab58e0198dd2b4d3b3de4ce4214bb042cb1fd8f1c7cbb93bcaf6a7a4b5"],"state_sha256":"df9a258486223cd959992869eca27ac1e5b0c50e8968a309db9557734e5ce651"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TP9s+2/mMr8qSYfc+44cOS78crxdfQo+1SsQiLeCE4GqsOr7cc8WLNWsa1pvMtYish4fHysfpuffw4pewUnxAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T11:00:11.812670Z","bundle_sha256":"3258a58d727b70291039445057f7b8ba482375f714d0dcdb2c9116488d969131"}}