{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:AWQQUZN67QJBTGODLVLOH3PQBG","short_pith_number":"pith:AWQQUZN6","canonical_record":{"source":{"id":"1402.3487","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-02-14T15:06:08Z","cross_cats_sorted":[],"title_canon_sha256":"5dec7928cb20b9073bbab996473888ae963adc2366732ba438d6472ded4c36eb","abstract_canon_sha256":"0182637593090e270cf38ba53d6cc6c0dc05bc0dfdb3b4f9199ef4f1f7387a07"},"schema_version":"1.0"},"canonical_sha256":"05a10a65befc121999c35d56e3edf009a76bd479c007829d4f01ec1af40386b6","source":{"kind":"arxiv","id":"1402.3487","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.3487","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1402.3487v3","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.3487","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"AWQQUZN67QJB","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"AWQQUZN67QJBTGOD","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"AWQQUZN6","created_at":"2026-05-18T12:28:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:AWQQUZN67QJBTGODLVLOH3PQBG","target":"record","payload":{"canonical_record":{"source":{"id":"1402.3487","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-02-14T15:06:08Z","cross_cats_sorted":[],"title_canon_sha256":"5dec7928cb20b9073bbab996473888ae963adc2366732ba438d6472ded4c36eb","abstract_canon_sha256":"0182637593090e270cf38ba53d6cc6c0dc05bc0dfdb3b4f9199ef4f1f7387a07"},"schema_version":"1.0"},"canonical_sha256":"05a10a65befc121999c35d56e3edf009a76bd479c007829d4f01ec1af40386b6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:16.522681Z","signature_b64":"3nE3fEH/bb9885MTLx6x+vZbXi+KZp67PcUYpXIzPAR/kAUrpjVJsug9HXO7j1Gvaqrlr6cRi7CICxiFAJxfDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"05a10a65befc121999c35d56e3edf009a76bd479c007829d4f01ec1af40386b6","last_reissued_at":"2026-05-18T02:39:16.522260Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:16.522260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.3487","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/jdBxgBplSuCKPf652hH0n4/JVzg9iQrEHyHdOEje7pKpfrQEg38+yEm4F+6hHdi7aMpI/ZJkiwVDH0pqucdCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T13:07:44.429897Z"},"content_sha256":"880615303665b9392cc06c30d4e3194d0e12d4e24980ffd9f10d761aa123d4de","schema_version":"1.0","event_id":"sha256:880615303665b9392cc06c30d4e3194d0e12d4e24980ffd9f10d761aa123d4de"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:AWQQUZN67QJBTGODLVLOH3PQBG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamically self-consistent non-stochastic micromagnetic model for the ferromagnetic state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Arne Vansteenkiste, Bartel Van Waeyenberge, Mykola Dvornik","submitted_at":"2014-02-14T15:06:08Z","abstract_excerpt":"In this work, a self-consistent thermodynamic approach to micromagnetism is presented. The magnetic degrees of freedom are modeled using the Landau-Lifshitz-Baryakhtar theory, that separates the different contributions to the magnetic damping, and thereby allows them to be coupled to the electron and phonon systems in a self-consistent way. We show that this model can quantitatively reproduce ultrafast magnetization dynamics in Nickel."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.3487","kind":"arxiv","version":3},"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":"2026-05-18T02:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IrMxBo8wFQSLCXJ5RxRUlKCMsRZ6iUnTmfJ3r292D/yD/lJqRDoLAqDh019fnSGHHZHJf3qUrm2CkQNW9TFSCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T13:07:44.430227Z"},"content_sha256":"501d773c634fe38739d585e5975ebdded4c5296d54f0c89448ed2bac513d6e78","schema_version":"1.0","event_id":"sha256:501d773c634fe38739d585e5975ebdded4c5296d54f0c89448ed2bac513d6e78"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AWQQUZN67QJBTGODLVLOH3PQBG/bundle.json","state_url":"https://pith.science/pith/AWQQUZN67QJBTGODLVLOH3PQBG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AWQQUZN67QJBTGODLVLOH3PQBG/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":"2026-06-21T13:07:44Z","links":{"resolver":"https://pith.science/pith/AWQQUZN67QJBTGODLVLOH3PQBG","bundle":"https://pith.science/pith/AWQQUZN67QJBTGODLVLOH3PQBG/bundle.json","state":"https://pith.science/pith/AWQQUZN67QJBTGODLVLOH3PQBG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AWQQUZN67QJBTGODLVLOH3PQBG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:AWQQUZN67QJBTGODLVLOH3PQBG","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":"0182637593090e270cf38ba53d6cc6c0dc05bc0dfdb3b4f9199ef4f1f7387a07","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-02-14T15:06:08Z","title_canon_sha256":"5dec7928cb20b9073bbab996473888ae963adc2366732ba438d6472ded4c36eb"},"schema_version":"1.0","source":{"id":"1402.3487","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.3487","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1402.3487v3","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.3487","created_at":"2026-05-18T02:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"AWQQUZN67QJB","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"AWQQUZN67QJBTGOD","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"AWQQUZN6","created_at":"2026-05-18T12:28:19Z"}],"graph_snapshots":[{"event_id":"sha256:501d773c634fe38739d585e5975ebdded4c5296d54f0c89448ed2bac513d6e78","target":"graph","created_at":"2026-05-18T02:39:16Z","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":"In this work, a self-consistent thermodynamic approach to micromagnetism is presented. The magnetic degrees of freedom are modeled using the Landau-Lifshitz-Baryakhtar theory, that separates the different contributions to the magnetic damping, and thereby allows them to be coupled to the electron and phonon systems in a self-consistent way. We show that this model can quantitatively reproduce ultrafast magnetization dynamics in Nickel.","authors_text":"Arne Vansteenkiste, Bartel Van Waeyenberge, Mykola Dvornik","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-02-14T15:06:08Z","title":"Thermodynamically self-consistent non-stochastic micromagnetic model for the ferromagnetic state"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.3487","kind":"arxiv","version":3},"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":"sha256:880615303665b9392cc06c30d4e3194d0e12d4e24980ffd9f10d761aa123d4de","target":"record","created_at":"2026-05-18T02:39:16Z","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":"0182637593090e270cf38ba53d6cc6c0dc05bc0dfdb3b4f9199ef4f1f7387a07","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-02-14T15:06:08Z","title_canon_sha256":"5dec7928cb20b9073bbab996473888ae963adc2366732ba438d6472ded4c36eb"},"schema_version":"1.0","source":{"id":"1402.3487","kind":"arxiv","version":3}},"canonical_sha256":"05a10a65befc121999c35d56e3edf009a76bd479c007829d4f01ec1af40386b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"05a10a65befc121999c35d56e3edf009a76bd479c007829d4f01ec1af40386b6","first_computed_at":"2026-05-18T02:39:16.522260Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:39:16.522260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3nE3fEH/bb9885MTLx6x+vZbXi+KZp67PcUYpXIzPAR/kAUrpjVJsug9HXO7j1Gvaqrlr6cRi7CICxiFAJxfDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:39:16.522681Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.3487","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:880615303665b9392cc06c30d4e3194d0e12d4e24980ffd9f10d761aa123d4de","sha256:501d773c634fe38739d585e5975ebdded4c5296d54f0c89448ed2bac513d6e78"],"state_sha256":"f01e13cb6cf2ae21da6630ec3e3cc0e1ce8a1eeae55ac1565dfdc81931d0229d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ErXIPIDV1oZzdfKrnk9bVJh3kc1uGF10XC/yK5+1tvFuGMtxR15N2VFAsT+FXRzsb7h9thNtY+SERPKQMVM+Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-21T13:07:44.432351Z","bundle_sha256":"9c660cf07c88209dc6d81575af67158320a32cf13b7539f6fa5e8ce29fd8ed93"}}