{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:VKMLGLORQLPNOGHL3H6NE7MXXX","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":"b2c58460a544d5d6457bca4d13d2e7a9f50f483c2f74b7a306ac0dc8d1d81a90","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-07-27T16:38:44Z","title_canon_sha256":"80b52e1bc9adc077c061aaba235c78baf1d4556b306f90b8da78be5d9022d855"},"schema_version":"1.0","source":{"id":"2507.20350","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.20350","created_at":"2026-07-05T11:44:17Z"},{"alias_kind":"arxiv_version","alias_value":"2507.20350v1","created_at":"2026-07-05T11:44:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.20350","created_at":"2026-07-05T11:44:17Z"},{"alias_kind":"pith_short_12","alias_value":"VKMLGLORQLPN","created_at":"2026-07-05T11:44:17Z"},{"alias_kind":"pith_short_16","alias_value":"VKMLGLORQLPNOGHL","created_at":"2026-07-05T11:44:17Z"},{"alias_kind":"pith_short_8","alias_value":"VKMLGLOR","created_at":"2026-07-05T11:44:17Z"}],"graph_snapshots":[{"event_id":"sha256:d3fca35a844a918a6482dd57bf9f626f2a5841a80a856439245cde49ebfa8c2d","target":"graph","created_at":"2026-07-05T11:44:17Z","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/2507.20350/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We introduce and study a non-equilibrium stochastic model of two fluctuating interfaces which interact through short-range attractive interactions at their points of contact. Beginning from an entangled state, the system exhibits diverse dynamics -- ranging from fast transients with small lifetimes to ultraslow evolution through quasi-stationary states -- and reaches stuck, entangled, or detached steady states. Near the stuck-detached transition, two distinct dynamical modes of evolution co-occur. When the two surfaces evolve through similar dynamics (both Edwards-Wilkinson or both Kardar-Pari","authors_text":"Malay Bandyopadhyay, Mustansir Barma, Samvit Mahapatra","cross_cats":["cond-mat.soft","physics.bio-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-07-27T16:38:44Z","title":"Two fluctuating interfaces with sticking interactions: Invariant measures and dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.20350","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:ca232373a1ba139cdf1d2cac0b8a28a7045f787887d5b2c1cce8fdae913565f0","target":"record","created_at":"2026-07-05T11:44:17Z","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":"b2c58460a544d5d6457bca4d13d2e7a9f50f483c2f74b7a306ac0dc8d1d81a90","cross_cats_sorted":["cond-mat.soft","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2025-07-27T16:38:44Z","title_canon_sha256":"80b52e1bc9adc077c061aaba235c78baf1d4556b306f90b8da78be5d9022d855"},"schema_version":"1.0","source":{"id":"2507.20350","kind":"arxiv","version":1}},"canonical_sha256":"aa98b32dd182ded718ebd9fcd27d97bdeedffd4c28ff099fdc79171cef393fb6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa98b32dd182ded718ebd9fcd27d97bdeedffd4c28ff099fdc79171cef393fb6","first_computed_at":"2026-07-05T11:44:17.603215Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:44:17.603215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rUkLxxiNVx3yv1F11hoIkj6xd1gF9A+7la1pD443N7Fve/PG0yy0GhuJ042BVjjsiTOMldrwvFca4jQzv3DhBg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:44:17.603763Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.20350","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ca232373a1ba139cdf1d2cac0b8a28a7045f787887d5b2c1cce8fdae913565f0","sha256:d3fca35a844a918a6482dd57bf9f626f2a5841a80a856439245cde49ebfa8c2d"],"state_sha256":"11680d2bdb8b165661753820044850d3ccba74b64d61aafc20ff7a9a52c3188c"}