{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LVM2PQX5JIAEVKIFZDSSQDGZ44","short_pith_number":"pith:LVM2PQX5","canonical_record":{"source":{"id":"1402.4121","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-15T14:16:05Z","cross_cats_sorted":[],"title_canon_sha256":"c1979550514db893209d531919a26727678f3e96acb7425d71bbbc85989544d2","abstract_canon_sha256":"0b921d991a072ea6b89555c1bb3c016cd9f3b461b813b0f5658b067bffbea006"},"schema_version":"1.0"},"canonical_sha256":"5d59a7c2fd4a004aa905c8e5280cd9e71690f5b85f94d9ce9b8dfe3779e57259","source":{"kind":"arxiv","id":"1402.4121","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.4121","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"arxiv_version","alias_value":"1402.4121v1","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4121","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"pith_short_12","alias_value":"LVM2PQX5JIAE","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LVM2PQX5JIAEVKIF","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LVM2PQX5","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LVM2PQX5JIAEVKIFZDSSQDGZ44","target":"record","payload":{"canonical_record":{"source":{"id":"1402.4121","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-15T14:16:05Z","cross_cats_sorted":[],"title_canon_sha256":"c1979550514db893209d531919a26727678f3e96acb7425d71bbbc85989544d2","abstract_canon_sha256":"0b921d991a072ea6b89555c1bb3c016cd9f3b461b813b0f5658b067bffbea006"},"schema_version":"1.0"},"canonical_sha256":"5d59a7c2fd4a004aa905c8e5280cd9e71690f5b85f94d9ce9b8dfe3779e57259","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:38.197330Z","signature_b64":"wrcIxkEAqIsO0VoY1IuXzEHYT4/q1eZf7Zyl7Mi6/9H06LWQds/zaDRSvfE5d5GEosAatfVgNQCrBfIfcxgMBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d59a7c2fd4a004aa905c8e5280cd9e71690f5b85f94d9ce9b8dfe3779e57259","last_reissued_at":"2026-05-18T02:39:38.196882Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:38.196882Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.4121","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":"2026-05-18T02:39:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FEcAzWKaM0mDRfA5AlwdzWrjujO5ujOBtSTgzfMxYD8H0NdZ+zrZ9IaD41s43L7W/bnKn+H0rPETKYBJsvguDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T16:40:24.531392Z"},"content_sha256":"c10d095d3cb66adf52e77f84d2a81dfa70dcee5caab98c17203d3c017cb84776","schema_version":"1.0","event_id":"sha256:c10d095d3cb66adf52e77f84d2a81dfa70dcee5caab98c17203d3c017cb84776"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LVM2PQX5JIAEVKIFZDSSQDGZ44","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bifurcations in dissipative fermionic dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"M. Colonna, M. Di Prima, P. Napolitani","submitted_at":"2014-02-15T14:16:05Z","abstract_excerpt":"The Boltzmann-Langevin One-Body model (BLOB), is a novel one-body transport approach, based on the solution of the Boltzmann-Langevin equation in three dimensions; it is used to handle large-amplitude phase-space fluctuations and has a broad applicability for dissipative fermionic dynamics. We study the occurrence of bifurcations in the dynamical trajectories describing heavy-ion collisions at Fermi energies.\n  The model, applied to dilute systems formed in such collisions, reveals to be closer to the observation than previous attempts to include a Langevin term in Boltzmann theories. The onse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4121","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":"2026-05-18T02:39:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zg4ZtJ9W46n3bsnuuF8HyM6znFosonCb2iHpsZP1/YaULJQG0J0QVoYYpbKmzU8CCdj+kbYGLPRrL2ouhYdVBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T16:40:24.532018Z"},"content_sha256":"ca5d1b4afce36b3e9b722abf2eed1db52d4928b823be9c43a2289a9cca584848","schema_version":"1.0","event_id":"sha256:ca5d1b4afce36b3e9b722abf2eed1db52d4928b823be9c43a2289a9cca584848"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/bundle.json","state_url":"https://pith.science/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/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":"2026-06-07T16:40:24Z","links":{"resolver":"https://pith.science/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44","bundle":"https://pith.science/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/bundle.json","state":"https://pith.science/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LVM2PQX5JIAEVKIFZDSSQDGZ44/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LVM2PQX5JIAEVKIFZDSSQDGZ44","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":"0b921d991a072ea6b89555c1bb3c016cd9f3b461b813b0f5658b067bffbea006","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-15T14:16:05Z","title_canon_sha256":"c1979550514db893209d531919a26727678f3e96acb7425d71bbbc85989544d2"},"schema_version":"1.0","source":{"id":"1402.4121","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.4121","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"arxiv_version","alias_value":"1402.4121v1","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4121","created_at":"2026-05-18T02:39:38Z"},{"alias_kind":"pith_short_12","alias_value":"LVM2PQX5JIAE","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LVM2PQX5JIAEVKIF","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LVM2PQX5","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:ca5d1b4afce36b3e9b722abf2eed1db52d4928b823be9c43a2289a9cca584848","target":"graph","created_at":"2026-05-18T02:39:38Z","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 Boltzmann-Langevin One-Body model (BLOB), is a novel one-body transport approach, based on the solution of the Boltzmann-Langevin equation in three dimensions; it is used to handle large-amplitude phase-space fluctuations and has a broad applicability for dissipative fermionic dynamics. We study the occurrence of bifurcations in the dynamical trajectories describing heavy-ion collisions at Fermi energies.\n  The model, applied to dilute systems formed in such collisions, reveals to be closer to the observation than previous attempts to include a Langevin term in Boltzmann theories. The onse","authors_text":"M. Colonna, M. Di Prima, P. Napolitani","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-15T14:16:05Z","title":"Bifurcations in dissipative fermionic dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4121","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:c10d095d3cb66adf52e77f84d2a81dfa70dcee5caab98c17203d3c017cb84776","target":"record","created_at":"2026-05-18T02:39:38Z","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":"0b921d991a072ea6b89555c1bb3c016cd9f3b461b813b0f5658b067bffbea006","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-15T14:16:05Z","title_canon_sha256":"c1979550514db893209d531919a26727678f3e96acb7425d71bbbc85989544d2"},"schema_version":"1.0","source":{"id":"1402.4121","kind":"arxiv","version":1}},"canonical_sha256":"5d59a7c2fd4a004aa905c8e5280cd9e71690f5b85f94d9ce9b8dfe3779e57259","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5d59a7c2fd4a004aa905c8e5280cd9e71690f5b85f94d9ce9b8dfe3779e57259","first_computed_at":"2026-05-18T02:39:38.196882Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:38.196882Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wrcIxkEAqIsO0VoY1IuXzEHYT4/q1eZf7Zyl7Mi6/9H06LWQds/zaDRSvfE5d5GEosAatfVgNQCrBfIfcxgMBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:38.197330Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.4121","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c10d095d3cb66adf52e77f84d2a81dfa70dcee5caab98c17203d3c017cb84776","sha256:ca5d1b4afce36b3e9b722abf2eed1db52d4928b823be9c43a2289a9cca584848"],"state_sha256":"271644dabd0602b59eee70df1a987e26b9f3e311092b956b92febfb751780a7e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AkVl2RFQM+wsC0iuPUmPPLyNdY4UyXP6ONVZMuawmNogKrI36GxOABCUsAiwWrLa4hqxrYbGxi2FHkrmsFCfDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T16:40:24.535983Z","bundle_sha256":"145168fbda107496bb2c68637b7500c91919073f115c0a5618dd27baf2291866"}}