{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:253Y5GDGGHVPXSHHBV24V3AHD3","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":"a36d33d482ba6550ade8c280c1938f6b2b3b990d16f5d160659ad11bc52e9199","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mes-hall","physics.app-ph","physics.atm-clus"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-11-14T08:10:19Z","title_canon_sha256":"99a9a5d219d341f074ad898ab22bf984a57bf90f39ff00f487bc94b59d856149"},"schema_version":"1.0","source":{"id":"1711.04989","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.04989","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"arxiv_version","alias_value":"1711.04989v1","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.04989","created_at":"2026-05-18T00:23:29Z"},{"alias_kind":"pith_short_12","alias_value":"253Y5GDGGHVP","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"253Y5GDGGHVPXSHH","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"253Y5GDG","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:c023427755f40624d6e07a1f1d0f8f41473bcff31d2d165657afd675cf762b53","target":"graph","created_at":"2026-05-18T00:23:29Z","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 we study morphological characteristics of the critically-sized crystalline nuclei at initial stage of the shear-induced crystallization of a model single-component amorphous (glassy) system. These characteristics are estimated quantitatively through statistical treatment of the non-equilibrium molecular dynamics simulation results for the system under steady shear at various (fixed) values of the shear rate $\\dot\\gamma$ and at different temperatures. It is found that the sheared glassy system is crystallized through nucleation mechanism. From analysis of a time-dependent trajector","authors_text":"Anatolii V. Mokshin, Bulat N. Galimzyanov","cross_cats":["cond-mat.dis-nn","cond-mat.mes-hall","physics.app-ph","physics.atm-clus"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-11-14T08:10:19Z","title":"Morphology of Critically-Sized Crystalline Nuclei at Shear-Induced Crystal Nucleation in Amorphous Solid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.04989","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":"sha256:3710ba6bc873c71f34a5aa3d3e1ca48473915deed8ea60122ed1e79f0eef6b5d","target":"record","created_at":"2026-05-18T00:23:29Z","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":"a36d33d482ba6550ade8c280c1938f6b2b3b990d16f5d160659ad11bc52e9199","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.mes-hall","physics.app-ph","physics.atm-clus"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-11-14T08:10:19Z","title_canon_sha256":"99a9a5d219d341f074ad898ab22bf984a57bf90f39ff00f487bc94b59d856149"},"schema_version":"1.0","source":{"id":"1711.04989","kind":"arxiv","version":1}},"canonical_sha256":"d7778e986631eafbc8e70d75caec071ed8047444c1d2c8d0193f6c7807e7dace","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d7778e986631eafbc8e70d75caec071ed8047444c1d2c8d0193f6c7807e7dace","first_computed_at":"2026-05-18T00:23:29.445123Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:29.445123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qniF8GE9WZ+DNl5GAKOssc6dnFSW5UP7N49bAegeSu4KkXWOGLu13RRht8CwedrmAYDrLtPkEGX5lkwt0g+XAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:29.445643Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.04989","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3710ba6bc873c71f34a5aa3d3e1ca48473915deed8ea60122ed1e79f0eef6b5d","sha256:c023427755f40624d6e07a1f1d0f8f41473bcff31d2d165657afd675cf762b53"],"state_sha256":"68392cdaa72dfef015137d3ea4b2cf0dcaeb849e1d8da427b93ee48592d6c894"}