{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:T7HX4UFRBKC73S6QNVKTCAF5S4","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":"ed4112785360ac8c54074eb965bfd4d3a16dfea0c4743693db929ca31a7d69a4","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"q-bio.SC","submitted_at":"2026-06-29T13:15:19Z","title_canon_sha256":"45f7291fe941d49dd41f970e029ae761b0afbfd8c91c7f3bfa5e680b9b536580"},"schema_version":"1.0","source":{"id":"2606.30267","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.30267","created_at":"2026-06-30T02:17:56Z"},{"alias_kind":"arxiv_version","alias_value":"2606.30267v1","created_at":"2026-06-30T02:17:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.30267","created_at":"2026-06-30T02:17:56Z"},{"alias_kind":"pith_short_12","alias_value":"T7HX4UFRBKC7","created_at":"2026-06-30T02:17:56Z"},{"alias_kind":"pith_short_16","alias_value":"T7HX4UFRBKC73S6Q","created_at":"2026-06-30T02:17:56Z"},{"alias_kind":"pith_short_8","alias_value":"T7HX4UFR","created_at":"2026-06-30T02:17:56Z"}],"graph_snapshots":[{"event_id":"sha256:45d4d52737d7218e82f19eda3a4eb5b5820ea3af44f85fc33842b3db336c6a36","target":"graph","created_at":"2026-06-30T02:17:56Z","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/2606.30267/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Clathrin assemblies in cells can persist as flat plaques, abort after partial invagination, or close into clathrin-coated vesicles, but the determinants of these different fates remain unresolved. To investigate the stochastic and complex dynamics of clathrin assemblies, we have developed a kinetic Monte Carlo simulation framework that couples individual clathrin agents to an adaptive continuum membrane. In this hybrid discrete-continuum description, the effective coat bending rigidity and the preferred coat curvature emerge during growth, rather than being prescribed as material parameters. O","authors_text":"Germany), Johannes H. H. Dreckhoff, Leon Lettermann (Heidelberg University, Ulrich S. Schwarz","cross_cats":["cond-mat.soft","physics.bio-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"q-bio.SC","submitted_at":"2026-06-29T13:15:19Z","title":"Pathway variability, coat stiffening and mechanical adaptation during clathrin-mediated endocytosis"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.30267","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":"sha256:4426fc8edc96092009fe9e7fa603133f0dbf820338c543984d51c8808c74349e","target":"record","created_at":"2026-06-30T02:17:56Z","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":"ed4112785360ac8c54074eb965bfd4d3a16dfea0c4743693db929ca31a7d69a4","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"q-bio.SC","submitted_at":"2026-06-29T13:15:19Z","title_canon_sha256":"45f7291fe941d49dd41f970e029ae761b0afbfd8c91c7f3bfa5e680b9b536580"},"schema_version":"1.0","source":{"id":"2606.30267","kind":"arxiv","version":1}},"canonical_sha256":"9fcf7e50b10a85fdcbd06d553100bd9721da46597608cc375557acb6daefc18f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9fcf7e50b10a85fdcbd06d553100bd9721da46597608cc375557acb6daefc18f","first_computed_at":"2026-06-30T02:17:56.775480Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-30T02:17:56.775480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wtrgSHptULKw5ULqc+F5ekcb/fgTDUJ8qdGJ0nnvQBFdPpaSQLNKf2MwTjJ0fN0QrKjsy1YScxi1DSnW7Of2BA==","signature_status":"signed_v1","signed_at":"2026-06-30T02:17:56.776023Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.30267","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4426fc8edc96092009fe9e7fa603133f0dbf820338c543984d51c8808c74349e","sha256:45d4d52737d7218e82f19eda3a4eb5b5820ea3af44f85fc33842b3db336c6a36"],"state_sha256":"07caa4eb65684234e04ac28d7ead032d687c8a7015fabfc216cd3cba0a1d0711"}