{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:B5BMQSPVHGN7FXTRYV4XLU6BSP","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":"8e81c53ba9b94731d427f464d2811ed4144a955f81e58d8aea619f0024e874e4","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2019-09-12T14:20:21Z","title_canon_sha256":"5e8b706435c435298fec2b0c7fc46a14da130f1410a937c9abc4261b27ece26e"},"schema_version":"1.0","source":{"id":"1909.05706","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.05706","created_at":"2026-07-05T01:39:24Z"},{"alias_kind":"arxiv_version","alias_value":"1909.05706v1","created_at":"2026-07-05T01:39:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.05706","created_at":"2026-07-05T01:39:24Z"},{"alias_kind":"pith_short_12","alias_value":"B5BMQSPVHGN7","created_at":"2026-07-05T01:39:24Z"},{"alias_kind":"pith_short_16","alias_value":"B5BMQSPVHGN7FXTR","created_at":"2026-07-05T01:39:24Z"},{"alias_kind":"pith_short_8","alias_value":"B5BMQSPV","created_at":"2026-07-05T01:39:24Z"}],"graph_snapshots":[{"event_id":"sha256:ea0cd0ac5415c7f0953a02074a11894e1faf78a8fcf661e1946c26ec726a17f2","target":"graph","created_at":"2026-07-05T01:39:24Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1909.05706/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Plastic deformation of most crystalline materials is due to the motion of lattice dislocations. Therefore, the simulation of the interaction and dynamics of these defects has become state-of-the-art method to study work hardening, size effects, creep and many other mechanical properties of metallic specimens. Lot of efforts have been made to make the simulations realistic by including specific dislocation mechanisms and the effect of free surfaces. However, less attention has been devoted to the numerical scheme that is used to solve the equations of motion.\n  In this paper we propose a scheme","authors_text":"G\\'abor P\\'eterffy, P\\'eter Dus\\'an Isp\\'anovity","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2019-09-12T14:20:21Z","title":"An efficient implicit method for discrete dislocation dynamics simulations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.05706","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:d8547b6c8167fbe53cf4056a3c07cbf29caba62b91e8467b38c4a00adc7b3172","target":"record","created_at":"2026-07-05T01:39:24Z","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":"8e81c53ba9b94731d427f464d2811ed4144a955f81e58d8aea619f0024e874e4","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2019-09-12T14:20:21Z","title_canon_sha256":"5e8b706435c435298fec2b0c7fc46a14da130f1410a937c9abc4261b27ece26e"},"schema_version":"1.0","source":{"id":"1909.05706","kind":"arxiv","version":1}},"canonical_sha256":"0f42c849f5399bf2de71c57975d3c193fda6bbd290e9026ab18727dbe4cd8f92","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0f42c849f5399bf2de71c57975d3c193fda6bbd290e9026ab18727dbe4cd8f92","first_computed_at":"2026-07-05T01:39:24.750037Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:39:24.750037Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JrWo8EXc6rmrdDpJhW26+A6Ha0EOf/JGWUHMD3xA1xlIeWK9kq1G7Ox2twCKKhwGEnnTh9x4uRXodYl0hfqaCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T01:39:24.750441Z","signed_message":"canonical_sha256_bytes"},"source_id":"1909.05706","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d8547b6c8167fbe53cf4056a3c07cbf29caba62b91e8467b38c4a00adc7b3172","sha256:ea0cd0ac5415c7f0953a02074a11894e1faf78a8fcf661e1946c26ec726a17f2"],"state_sha256":"39783b99c25cb71d034df4238b32d032a1879de34fbba26411f3eb4e67bd3b9b"}