{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:DDP5GZFLDWQ2VMO4ELDCLJDXRG","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":"e0f3b0680d41205dfe5b149265e8afc37c5bc34e415e362ea8f1ca82da7cc5ab","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2023-07-24T13:07:20Z","title_canon_sha256":"7ef25fdbe2e5d186ad95c1b15ad18b228551b14c308913791f73c665a71c6cad"},"schema_version":"1.0","source":{"id":"2307.12764","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.12764","created_at":"2026-07-05T06:33:58Z"},{"alias_kind":"arxiv_version","alias_value":"2307.12764v1","created_at":"2026-07-05T06:33:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.12764","created_at":"2026-07-05T06:33:58Z"},{"alias_kind":"pith_short_12","alias_value":"DDP5GZFLDWQ2","created_at":"2026-07-05T06:33:58Z"},{"alias_kind":"pith_short_16","alias_value":"DDP5GZFLDWQ2VMO4","created_at":"2026-07-05T06:33:58Z"},{"alias_kind":"pith_short_8","alias_value":"DDP5GZFL","created_at":"2026-07-05T06:33:58Z"}],"graph_snapshots":[{"event_id":"sha256:8f7ae8a3051feedf34250ad223ef0e4577736fb0c4920867ea2be2fd9de1af44","target":"graph","created_at":"2026-07-05T06:33:58Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2307.12764/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show how residual stresses emerge in a visco-elastic material as a signature of its past flow history, through an interplay between flow-modified microscopic relaxation and macroscopic features of the flow. Long-lasting temporal-history dependence of the microscopic dynamics and nonlinear rheology are incorporated through the mode-coupling theory of the glass transition (MCT). The theory's integral constitutive equation (ICE) is coupled to continuum mechanics in a finite-element method (FEM) scheme that tracks the flow history through the Finger tensor. The method is suitable for a calculat","authors_text":"Sebastian Steinh\\\"auser, Stefan Turek, Thomas Voigtmann, Timm Treskatis","cross_cats":["physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2023-07-24T13:07:20Z","title":"Residual stresses couple microscopic and macroscopic scales"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.12764","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:b86eb024589e22d348de579201cb816579622dfbdaec62de590513041e812b18","target":"record","created_at":"2026-07-05T06:33:58Z","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":"e0f3b0680d41205dfe5b149265e8afc37c5bc34e415e362ea8f1ca82da7cc5ab","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2023-07-24T13:07:20Z","title_canon_sha256":"7ef25fdbe2e5d186ad95c1b15ad18b228551b14c308913791f73c665a71c6cad"},"schema_version":"1.0","source":{"id":"2307.12764","kind":"arxiv","version":1}},"canonical_sha256":"18dfd364ab1da1aab1dc22c625a4778980a7e6cdb4f1bd601e11cd0586786d16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18dfd364ab1da1aab1dc22c625a4778980a7e6cdb4f1bd601e11cd0586786d16","first_computed_at":"2026-07-05T06:33:58.307061Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:33:58.307061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SpE1ZkcG4AAgnvCWR4PxTFYLX/AtUtZhCW6gLCFKZPCOoZEr97iEaKnv+YH/gj3gDv1Ckz2TVcwuf8PyuFpiDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:33:58.307484Z","signed_message":"canonical_sha256_bytes"},"source_id":"2307.12764","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b86eb024589e22d348de579201cb816579622dfbdaec62de590513041e812b18","sha256:8f7ae8a3051feedf34250ad223ef0e4577736fb0c4920867ea2be2fd9de1af44"],"state_sha256":"53b5661fa9fc66f655bb57611fd6b27091a681359c984e7edc0638be4c7ddabc"}