{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:3UMEATSXKBSIHXQJEUE7LOIBPU","short_pith_number":"pith:3UMEATSX","canonical_record":{"source":{"id":"1306.1307","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-06-06T06:39:14Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"0d7360c74ef354293c628dad0f9a9449ec6cc632225ad60069f7d0fa0314ba8e","abstract_canon_sha256":"5ea4849c6a930038c79377d0d562eb732860ccf49b0d14493aea65a79f208300"},"schema_version":"1.0"},"canonical_sha256":"dd18404e57506483de092509f5b9017d0e6a4e759dad4dc9347d224ec3fee863","source":{"kind":"arxiv","id":"1306.1307","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.1307","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"arxiv_version","alias_value":"1306.1307v1","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.1307","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"pith_short_12","alias_value":"3UMEATSXKBSI","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3UMEATSXKBSIHXQJ","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3UMEATSX","created_at":"2026-05-18T12:27:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:3UMEATSXKBSIHXQJEUE7LOIBPU","target":"record","payload":{"canonical_record":{"source":{"id":"1306.1307","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-06-06T06:39:14Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"0d7360c74ef354293c628dad0f9a9449ec6cc632225ad60069f7d0fa0314ba8e","abstract_canon_sha256":"5ea4849c6a930038c79377d0d562eb732860ccf49b0d14493aea65a79f208300"},"schema_version":"1.0"},"canonical_sha256":"dd18404e57506483de092509f5b9017d0e6a4e759dad4dc9347d224ec3fee863","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:20:58.096533Z","signature_b64":"O6z1z8qiKgSntC3WaP+OpTiRsHgHMMLcVUGTdFIRzMoq0eThAIEYFMzu6CfXESm4rcWWiCinDIH8HoY47munCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd18404e57506483de092509f5b9017d0e6a4e759dad4dc9347d224ec3fee863","last_reissued_at":"2026-05-18T03:20:58.095939Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:20:58.095939Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.1307","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":"2026-05-18T03:20:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Td1Pojm4m66yNnd6u7CUmVrRUVtU8RiIFvrT+qAR7ZmFT4DKJcUts+ZUBEx3v6buPBV7kGIV1dcEtSIRQmwHAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T16:23:28.860225Z"},"content_sha256":"4c52b6f66d83c1881dd3d168afde50b4a230cba51c7695244b0a60ea4440c4c5","schema_version":"1.0","event_id":"sha256:4c52b6f66d83c1881dd3d168afde50b4a230cba51c7695244b0a60ea4440c4c5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:3UMEATSXKBSIHXQJEUE7LOIBPU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Extension of Classical Nucleation Theory for Uniformly Sheared Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.stat-mech","authors_text":"Anatolii V. Mokshin, Bulat N. Galimzyanov, Jean-Louis Barrat","submitted_at":"2013-06-06T06:39:14Z","abstract_excerpt":"Nucleation is an out-of-equilibrium process, which can be strongly affected by the presence of external fields. In this letter, we report a simple extension of classical nucleation theory to systems submitted to an homogeneous shear flow. The theory involves accounting for the anisotropy of the critical nucleus formation, and introduces a shear rate dependent effective temperature. This extended theory is used to analyze the results of extensive molecular dynamics simulations, which explore a broad range of shear rates and undercoolings. At fixed temperature, a maximum in the nucleation rate i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.1307","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":"2026-05-18T03:20:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"73mS0uCxXx3tCWXMM9gsikrLp4DgETnXmCa4/tjYT3ymMRM+qsLF0qBKzofG8zGYiQRxqeXpCbRApJc0iMQeAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T16:23:28.860594Z"},"content_sha256":"8ba70b44cd6667b07e37afa029f248f03461ff3cc67097911a9f97ebf931ab9d","schema_version":"1.0","event_id":"sha256:8ba70b44cd6667b07e37afa029f248f03461ff3cc67097911a9f97ebf931ab9d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/bundle.json","state_url":"https://pith.science/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/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":"2026-05-29T16:23:28Z","links":{"resolver":"https://pith.science/pith/3UMEATSXKBSIHXQJEUE7LOIBPU","bundle":"https://pith.science/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/bundle.json","state":"https://pith.science/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3UMEATSXKBSIHXQJEUE7LOIBPU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:3UMEATSXKBSIHXQJEUE7LOIBPU","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":"5ea4849c6a930038c79377d0d562eb732860ccf49b0d14493aea65a79f208300","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-06-06T06:39:14Z","title_canon_sha256":"0d7360c74ef354293c628dad0f9a9449ec6cc632225ad60069f7d0fa0314ba8e"},"schema_version":"1.0","source":{"id":"1306.1307","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.1307","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"arxiv_version","alias_value":"1306.1307v1","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.1307","created_at":"2026-05-18T03:20:58Z"},{"alias_kind":"pith_short_12","alias_value":"3UMEATSXKBSI","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_16","alias_value":"3UMEATSXKBSIHXQJ","created_at":"2026-05-18T12:27:32Z"},{"alias_kind":"pith_short_8","alias_value":"3UMEATSX","created_at":"2026-05-18T12:27:32Z"}],"graph_snapshots":[{"event_id":"sha256:8ba70b44cd6667b07e37afa029f248f03461ff3cc67097911a9f97ebf931ab9d","target":"graph","created_at":"2026-05-18T03:20:58Z","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":"Nucleation is an out-of-equilibrium process, which can be strongly affected by the presence of external fields. In this letter, we report a simple extension of classical nucleation theory to systems submitted to an homogeneous shear flow. The theory involves accounting for the anisotropy of the critical nucleus formation, and introduces a shear rate dependent effective temperature. This extended theory is used to analyze the results of extensive molecular dynamics simulations, which explore a broad range of shear rates and undercoolings. At fixed temperature, a maximum in the nucleation rate i","authors_text":"Anatolii V. Mokshin, Bulat N. Galimzyanov, Jean-Louis Barrat","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-06-06T06:39:14Z","title":"Extension of Classical Nucleation Theory for Uniformly Sheared Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.1307","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":"sha256:4c52b6f66d83c1881dd3d168afde50b4a230cba51c7695244b0a60ea4440c4c5","target":"record","created_at":"2026-05-18T03:20:58Z","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":"5ea4849c6a930038c79377d0d562eb732860ccf49b0d14493aea65a79f208300","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-06-06T06:39:14Z","title_canon_sha256":"0d7360c74ef354293c628dad0f9a9449ec6cc632225ad60069f7d0fa0314ba8e"},"schema_version":"1.0","source":{"id":"1306.1307","kind":"arxiv","version":1}},"canonical_sha256":"dd18404e57506483de092509f5b9017d0e6a4e759dad4dc9347d224ec3fee863","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dd18404e57506483de092509f5b9017d0e6a4e759dad4dc9347d224ec3fee863","first_computed_at":"2026-05-18T03:20:58.095939Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:20:58.095939Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O6z1z8qiKgSntC3WaP+OpTiRsHgHMMLcVUGTdFIRzMoq0eThAIEYFMzu6CfXESm4rcWWiCinDIH8HoY47munCA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:20:58.096533Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.1307","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4c52b6f66d83c1881dd3d168afde50b4a230cba51c7695244b0a60ea4440c4c5","sha256:8ba70b44cd6667b07e37afa029f248f03461ff3cc67097911a9f97ebf931ab9d"],"state_sha256":"c3f7057cc1bf031e32684eeea4bf6fe55c5510c2e396cd592ac98a0e9bda5fa0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"46Wh9dzDZ2NywF0LNBKgehNVMJpCxkJZ55rTkjrZy8OUzMu7VO5w6X0bjvU+vZfZuF1T+XRjs1tFmtmmHKEXCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T16:23:28.863771Z","bundle_sha256":"f0a2507308bce97aebd76ccf40c746227ee56f6fb6af9a2443053040b071ccbf"}}