{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:K3DKNA2IWP2R6S5SHAT7QG2MRG","short_pith_number":"pith:K3DKNA2I","canonical_record":{"source":{"id":"1702.05938","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-20T11:58:11Z","cross_cats_sorted":[],"title_canon_sha256":"e3f3b162d79cd3123540a4c0ca7620bdcc231062e6227194551d86e1a462d171","abstract_canon_sha256":"1170c4320fdb216392a6152e877cdfdfe3b329e8bcec0d9afa2dfe76d607b0a2"},"schema_version":"1.0"},"canonical_sha256":"56c6a68348b3f51f4bb23827f81b4c898aa4b5e96b2d695ecd52316219aca305","source":{"kind":"arxiv","id":"1702.05938","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.05938","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"arxiv_version","alias_value":"1702.05938v2","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.05938","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"pith_short_12","alias_value":"K3DKNA2IWP2R","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"K3DKNA2IWP2R6S5S","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"K3DKNA2I","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:K3DKNA2IWP2R6S5SHAT7QG2MRG","target":"record","payload":{"canonical_record":{"source":{"id":"1702.05938","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-20T11:58:11Z","cross_cats_sorted":[],"title_canon_sha256":"e3f3b162d79cd3123540a4c0ca7620bdcc231062e6227194551d86e1a462d171","abstract_canon_sha256":"1170c4320fdb216392a6152e877cdfdfe3b329e8bcec0d9afa2dfe76d607b0a2"},"schema_version":"1.0"},"canonical_sha256":"56c6a68348b3f51f4bb23827f81b4c898aa4b5e96b2d695ecd52316219aca305","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:23.507545Z","signature_b64":"6heo5ymg/t4kHcPkmhEJhaO+w1vRnBALianNGAkUgA5nnuJIuqUyNh9VSogqELNk/CwQiT+V+VrYUHPDeztgDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"56c6a68348b3f51f4bb23827f81b4c898aa4b5e96b2d695ecd52316219aca305","last_reissued_at":"2026-05-18T00:44:23.507129Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:23.507129Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.05938","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":"2026-05-18T00:44:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4FW9vZl7dS6LM4S3xYZk5fygGk/LDZhyapEowWT+C9RKb8RKLjnuCYIL7nbkRo5MLPQaArEYGQq7H4lPsqxECA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T18:21:28.249923Z"},"content_sha256":"6a737df7bb91949b25f12d9eff63b8393e4dff644fec3208bd13bdac45c70eaa","schema_version":"1.0","event_id":"sha256:6a737df7bb91949b25f12d9eff63b8393e4dff644fec3208bd13bdac45c70eaa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:K3DKNA2IWP2R6S5SHAT7QG2MRG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fission dynamics of $^{252}$Cf","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Dobrowolski, A. Zdeb, M. Warda","submitted_at":"2017-02-20T11:58:11Z","abstract_excerpt":"The time-dependent generator coordinate method with the gaussian overlap approximation (TDGCM+GOA) formalism is applied to describe the fission of $^{252}$Cf. We perform analysis of fission from the initial states laying in the energetic range from the ground state to the state located 4 MeV above the fission barrier. The fission fragment mass distributions, obtained for different parity, energy of levels and types of mixed states, are calculated and compared with experimental data. The impact of the total time of wave packet propagation on the final results is studied as well. The weak depend"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.05938","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":"2026-05-18T00:44:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1mRrayQmPf1RsFHwgrC6FVrkcsPoJ9P9JDS8oXmhtNb1Mm8vbKIWu+TS3iU+fP1tnPnSV4SWxfimlYyvD+ifDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T18:21:28.250578Z"},"content_sha256":"b18b03de87e8e6a6be82a121c6eafc1625cb40bde8b1e8fa846dddeefa87d8ce","schema_version":"1.0","event_id":"sha256:b18b03de87e8e6a6be82a121c6eafc1625cb40bde8b1e8fa846dddeefa87d8ce"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/bundle.json","state_url":"https://pith.science/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/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":"2026-05-31T18:21:28Z","links":{"resolver":"https://pith.science/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG","bundle":"https://pith.science/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/bundle.json","state":"https://pith.science/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/K3DKNA2IWP2R6S5SHAT7QG2MRG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:K3DKNA2IWP2R6S5SHAT7QG2MRG","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":"1170c4320fdb216392a6152e877cdfdfe3b329e8bcec0d9afa2dfe76d607b0a2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-20T11:58:11Z","title_canon_sha256":"e3f3b162d79cd3123540a4c0ca7620bdcc231062e6227194551d86e1a462d171"},"schema_version":"1.0","source":{"id":"1702.05938","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.05938","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"arxiv_version","alias_value":"1702.05938v2","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.05938","created_at":"2026-05-18T00:44:23Z"},{"alias_kind":"pith_short_12","alias_value":"K3DKNA2IWP2R","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"K3DKNA2IWP2R6S5S","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"K3DKNA2I","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:b18b03de87e8e6a6be82a121c6eafc1625cb40bde8b1e8fa846dddeefa87d8ce","target":"graph","created_at":"2026-05-18T00:44:23Z","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 time-dependent generator coordinate method with the gaussian overlap approximation (TDGCM+GOA) formalism is applied to describe the fission of $^{252}$Cf. We perform analysis of fission from the initial states laying in the energetic range from the ground state to the state located 4 MeV above the fission barrier. The fission fragment mass distributions, obtained for different parity, energy of levels and types of mixed states, are calculated and compared with experimental data. The impact of the total time of wave packet propagation on the final results is studied as well. The weak depend","authors_text":"A. Dobrowolski, A. Zdeb, M. Warda","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-20T11:58:11Z","title":"Fission dynamics of $^{252}$Cf"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.05938","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":"sha256:6a737df7bb91949b25f12d9eff63b8393e4dff644fec3208bd13bdac45c70eaa","target":"record","created_at":"2026-05-18T00:44:23Z","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":"1170c4320fdb216392a6152e877cdfdfe3b329e8bcec0d9afa2dfe76d607b0a2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-02-20T11:58:11Z","title_canon_sha256":"e3f3b162d79cd3123540a4c0ca7620bdcc231062e6227194551d86e1a462d171"},"schema_version":"1.0","source":{"id":"1702.05938","kind":"arxiv","version":2}},"canonical_sha256":"56c6a68348b3f51f4bb23827f81b4c898aa4b5e96b2d695ecd52316219aca305","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"56c6a68348b3f51f4bb23827f81b4c898aa4b5e96b2d695ecd52316219aca305","first_computed_at":"2026-05-18T00:44:23.507129Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:23.507129Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6heo5ymg/t4kHcPkmhEJhaO+w1vRnBALianNGAkUgA5nnuJIuqUyNh9VSogqELNk/CwQiT+V+VrYUHPDeztgDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:23.507545Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.05938","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6a737df7bb91949b25f12d9eff63b8393e4dff644fec3208bd13bdac45c70eaa","sha256:b18b03de87e8e6a6be82a121c6eafc1625cb40bde8b1e8fa846dddeefa87d8ce"],"state_sha256":"10f4fd98245269fb4bc3798416ffb574bb86bcc282b30710ee297d653456a3fa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7N31WIrPs3sDBZerRGPbBbX/yl5W6jj46vjtUl+bPp9PUJxuvDv/KuDqA7dikqQyoKlS3wZMD5BXcvl/Ul3DBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T18:21:28.254015Z","bundle_sha256":"7ad851bdb39835fe30f5772d3d5489f10a0d33a016b4f1f683920bd81427444e"}}