{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:SLERHPVUNP3S4YWBSKK5E32HPS","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":"8297870e4fe23193a8a8ca9705dd6e9135b9343c263fb1d1f0b18924c7d0365e","cross_cats_sorted":["cond-mat.stat-mech","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-07-20T17:32:21Z","title_canon_sha256":"53d0cae9eac7b1f11dafb16026c4b3f947b32e29f26396d2edfa7abb65f906dc"},"schema_version":"1.0","source":{"id":"1907.08846","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1907.08846","created_at":"2026-07-05T01:25:22Z"},{"alias_kind":"arxiv_version","alias_value":"1907.08846v2","created_at":"2026-07-05T01:25:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.08846","created_at":"2026-07-05T01:25:22Z"},{"alias_kind":"pith_short_12","alias_value":"SLERHPVUNP3S","created_at":"2026-07-05T01:25:22Z"},{"alias_kind":"pith_short_16","alias_value":"SLERHPVUNP3S4YWB","created_at":"2026-07-05T01:25:22Z"},{"alias_kind":"pith_short_8","alias_value":"SLERHPVU","created_at":"2026-07-05T01:25:22Z"}],"graph_snapshots":[{"event_id":"sha256:0a46193f4e333bb3868d8b2f55f1fa80a70e6c4cfc9c406bd10f8414ec4907bb","target":"graph","created_at":"2026-07-05T01:25:22Z","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/1907.08846/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Dense emulsions, colloidal gels, microgels, and foams all display a solid-like behavior at rest characterized by a yield stress, above which the material flows like a liquid. Such a fluidization transition often consists of long-lasting transient flows that involve shear-banded velocity profiles. The characteristic time for full fluidization, $\\tau_\\text{f}$, has been reported to decay as a power-law of the shear rate $\\dot \\gamma$ and of the shear stress $\\sigma$ with respective exponents $\\alpha$ and $\\beta$. Strikingly, the ratio of these exponents was empirically observed to coincide with ","authors_text":"Catherine Barentin, Federico Toschi, Mauro Sbragaglia, Roberto Benzi, S\\'ebastien Manneville, Thibaut Divoux","cross_cats":["cond-mat.stat-mech","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-07-20T17:32:21Z","title":"Unified theoretical and experimental view on transient shear banding"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.08846","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":"sha256:56de98aa4c7da9bb11c5766f46bf40ddee13c9f292f4ff8c83c5f888c04cdd7c","target":"record","created_at":"2026-07-05T01:25:22Z","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":"8297870e4fe23193a8a8ca9705dd6e9135b9343c263fb1d1f0b18924c7d0365e","cross_cats_sorted":["cond-mat.stat-mech","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-07-20T17:32:21Z","title_canon_sha256":"53d0cae9eac7b1f11dafb16026c4b3f947b32e29f26396d2edfa7abb65f906dc"},"schema_version":"1.0","source":{"id":"1907.08846","kind":"arxiv","version":2}},"canonical_sha256":"92c913beb46bf72e62c19295d26f477cbf0492e45c6b39c5425107326775c647","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"92c913beb46bf72e62c19295d26f477cbf0492e45c6b39c5425107326775c647","first_computed_at":"2026-07-05T01:25:22.073303Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:25:22.073303Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IqjymG/dNhIvlVxJc4iKoGyaXTW8lC4Gtc74u8C5Oai0o/1VWEpX1+1r8cZvs1Mb5DAOcO7vqB4GeAdQ8srVAg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:25:22.073710Z","signed_message":"canonical_sha256_bytes"},"source_id":"1907.08846","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:56de98aa4c7da9bb11c5766f46bf40ddee13c9f292f4ff8c83c5f888c04cdd7c","sha256:0a46193f4e333bb3868d8b2f55f1fa80a70e6c4cfc9c406bd10f8414ec4907bb"],"state_sha256":"03b97ea38f08e64746516ad486d73c98c765297f0e44092c6700c87ebe7af8b5"}