{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:POT5VZQGB4GOWMAXFXMFKQPSG4","short_pith_number":"pith:POT5VZQG","canonical_record":{"source":{"id":"1308.5662","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-26T19:42:14Z","cross_cats_sorted":["cond-mat.soft","cond-mat.stat-mech"],"title_canon_sha256":"4cde454190cd829aedc54c2d51747b778809f93af522aec4b40fae5d943b79ae","abstract_canon_sha256":"3787c7c90bb0aecf051918d96733973a0bbcdfc443ac441269212edc8d15f0ba"},"schema_version":"1.0"},"canonical_sha256":"7ba7dae6060f0ceb30172dd85541f2373c647ff404ae9dd467ccb39d57c46774","source":{"kind":"arxiv","id":"1308.5662","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.5662","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"arxiv_version","alias_value":"1308.5662v2","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.5662","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"pith_short_12","alias_value":"POT5VZQGB4GO","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"POT5VZQGB4GOWMAX","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"POT5VZQG","created_at":"2026-05-18T12:27:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:POT5VZQGB4GOWMAXFXMFKQPSG4","target":"record","payload":{"canonical_record":{"source":{"id":"1308.5662","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-26T19:42:14Z","cross_cats_sorted":["cond-mat.soft","cond-mat.stat-mech"],"title_canon_sha256":"4cde454190cd829aedc54c2d51747b778809f93af522aec4b40fae5d943b79ae","abstract_canon_sha256":"3787c7c90bb0aecf051918d96733973a0bbcdfc443ac441269212edc8d15f0ba"},"schema_version":"1.0"},"canonical_sha256":"7ba7dae6060f0ceb30172dd85541f2373c647ff404ae9dd467ccb39d57c46774","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:14:49.436065Z","signature_b64":"MrrHRJtfQvQ0gvz+7OIg8ol7KpKJLUCvmSbhZ1d/qZrxScO0qO6fXmbEilVrHf1Yn1aa6opVaAXX5vm6akcIAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ba7dae6060f0ceb30172dd85541f2373c647ff404ae9dd467ccb39d57c46774","last_reissued_at":"2026-05-18T03:14:49.435484Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:14:49.435484Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1308.5662","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":"2026-05-18T03:14:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WJqIyJVs4Wj6VZl8VBH5RrTWxuLkeuqEFVeUj26dUTlvi0yvpAmPnIzlOzylbaRkIrErhFDkJC2+QEXfyZwNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:48:11.396200Z"},"content_sha256":"3776334bded40bfcbe57c4fda2b29dc0277bc1d980ef08516b57aac784795d4a","schema_version":"1.0","event_id":"sha256:3776334bded40bfcbe57c4fda2b29dc0277bc1d980ef08516b57aac784795d4a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:POT5VZQGB4GOWMAXFXMFKQPSG4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Determination of the universality class of crystal plasticity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","cond-mat.stat-mech"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Georgios Tsekenis, Jonathan T. Uhl, Karin A. Dahmen, Nigel Goldenfeld","submitted_at":"2013-08-26T19:42:14Z","abstract_excerpt":"Although scaling phenomena have long been documented in crystalline plasticity, the universality class has been difficult to identify due to the rarity of avalanche events, which require large system sizes and long times in order to accurately measure scaling exponents and functions. Here we present comprehensive simulations of two-dimensional dislocation dynamics under shear, using finite-size scaling to extract scaling exponents and the avalanche profile scaling function from time-resolved measurements of slip-avalanches. Our results provide compelling evidence that both the static and dynam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.5662","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":"2026-05-18T03:14:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BB2TNuDAoGSxOi9LjiYvV33pl9PbJSNL9GMxb0T46YSHu+HBLDjAPd/i0Vu7sSRKkHtzoxgzz1+XeMDN5Z8kCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:48:11.396649Z"},"content_sha256":"7bb97b252509807d11a6abeac8c8aec025d150673cb2c6cea231b2f360a4b462","schema_version":"1.0","event_id":"sha256:7bb97b252509807d11a6abeac8c8aec025d150673cb2c6cea231b2f360a4b462"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/bundle.json","state_url":"https://pith.science/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/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":"2026-05-28T23:48:11Z","links":{"resolver":"https://pith.science/pith/POT5VZQGB4GOWMAXFXMFKQPSG4","bundle":"https://pith.science/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/bundle.json","state":"https://pith.science/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/POT5VZQGB4GOWMAXFXMFKQPSG4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:POT5VZQGB4GOWMAXFXMFKQPSG4","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":"3787c7c90bb0aecf051918d96733973a0bbcdfc443ac441269212edc8d15f0ba","cross_cats_sorted":["cond-mat.soft","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-26T19:42:14Z","title_canon_sha256":"4cde454190cd829aedc54c2d51747b778809f93af522aec4b40fae5d943b79ae"},"schema_version":"1.0","source":{"id":"1308.5662","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.5662","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"arxiv_version","alias_value":"1308.5662v2","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.5662","created_at":"2026-05-18T03:14:49Z"},{"alias_kind":"pith_short_12","alias_value":"POT5VZQGB4GO","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"POT5VZQGB4GOWMAX","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"POT5VZQG","created_at":"2026-05-18T12:27:54Z"}],"graph_snapshots":[{"event_id":"sha256:7bb97b252509807d11a6abeac8c8aec025d150673cb2c6cea231b2f360a4b462","target":"graph","created_at":"2026-05-18T03:14:49Z","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":"Although scaling phenomena have long been documented in crystalline plasticity, the universality class has been difficult to identify due to the rarity of avalanche events, which require large system sizes and long times in order to accurately measure scaling exponents and functions. Here we present comprehensive simulations of two-dimensional dislocation dynamics under shear, using finite-size scaling to extract scaling exponents and the avalanche profile scaling function from time-resolved measurements of slip-avalanches. Our results provide compelling evidence that both the static and dynam","authors_text":"Georgios Tsekenis, Jonathan T. Uhl, Karin A. Dahmen, Nigel Goldenfeld","cross_cats":["cond-mat.soft","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-26T19:42:14Z","title":"Determination of the universality class of crystal plasticity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.5662","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":"sha256:3776334bded40bfcbe57c4fda2b29dc0277bc1d980ef08516b57aac784795d4a","target":"record","created_at":"2026-05-18T03:14:49Z","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":"3787c7c90bb0aecf051918d96733973a0bbcdfc443ac441269212edc8d15f0ba","cross_cats_sorted":["cond-mat.soft","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-08-26T19:42:14Z","title_canon_sha256":"4cde454190cd829aedc54c2d51747b778809f93af522aec4b40fae5d943b79ae"},"schema_version":"1.0","source":{"id":"1308.5662","kind":"arxiv","version":2}},"canonical_sha256":"7ba7dae6060f0ceb30172dd85541f2373c647ff404ae9dd467ccb39d57c46774","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7ba7dae6060f0ceb30172dd85541f2373c647ff404ae9dd467ccb39d57c46774","first_computed_at":"2026-05-18T03:14:49.435484Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:14:49.435484Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MrrHRJtfQvQ0gvz+7OIg8ol7KpKJLUCvmSbhZ1d/qZrxScO0qO6fXmbEilVrHf1Yn1aa6opVaAXX5vm6akcIAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:14:49.436065Z","signed_message":"canonical_sha256_bytes"},"source_id":"1308.5662","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3776334bded40bfcbe57c4fda2b29dc0277bc1d980ef08516b57aac784795d4a","sha256:7bb97b252509807d11a6abeac8c8aec025d150673cb2c6cea231b2f360a4b462"],"state_sha256":"9af32af03e92f569a530d1c1097a247940a682d202ba8846585a8cdd21c21d90"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"12/q/PbxY8VTWr1CGaPk4s8k7CVZ5P/YIlGEmyaisTHafSqbvDIwa8pxd/JEPLOsyB/9ySbNZ6QCf8BZo4kfDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T23:48:11.399256Z","bundle_sha256":"87e08b491599b7616e7df7397450a2eb9d0bdbaa2bce5485c584cb59db96343e"}}