{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:2JXEI7BA5BKQBKOLIAS26CDIT4","short_pith_number":"pith:2JXEI7BA","canonical_record":{"source":{"id":"1605.07395","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-24T11:59:19Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"39c861f631c4ca35f11746ce0df44526389cf9a1f173453aea56180535f196d6","abstract_canon_sha256":"fdc8a76db29ba5d1f392c02d1cfad9df8bca2d2d7671a99981e787c388052528"},"schema_version":"1.0"},"canonical_sha256":"d26e447c20e85500a9cb4025af08689f1d2dcddb5ae07ac5c0fcb01996fdf3a3","source":{"kind":"arxiv","id":"1605.07395","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.07395","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"arxiv_version","alias_value":"1605.07395v1","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.07395","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"pith_short_12","alias_value":"2JXEI7BA5BKQ","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"2JXEI7BA5BKQBKOL","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"2JXEI7BA","created_at":"2026-05-18T12:29:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:2JXEI7BA5BKQBKOLIAS26CDIT4","target":"record","payload":{"canonical_record":{"source":{"id":"1605.07395","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-24T11:59:19Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"39c861f631c4ca35f11746ce0df44526389cf9a1f173453aea56180535f196d6","abstract_canon_sha256":"fdc8a76db29ba5d1f392c02d1cfad9df8bca2d2d7671a99981e787c388052528"},"schema_version":"1.0"},"canonical_sha256":"d26e447c20e85500a9cb4025af08689f1d2dcddb5ae07ac5c0fcb01996fdf3a3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:41.758312Z","signature_b64":"3SS2P4v/+1ezp69dQFARnkU1hsmlN0ihlyfWBkE/ViRv4MhqvYildF6kFda5OAg6giBq4nxoHYLVaxz80eApBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d26e447c20e85500a9cb4025af08689f1d2dcddb5ae07ac5c0fcb01996fdf3a3","last_reissued_at":"2026-05-18T01:12:41.757984Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:41.757984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.07395","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":"2026-05-18T01:12:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"816J5oUccuKMYNi7uoiqqv7Yz/UI7ublYdI27ywfkbPA26xnXhYHXAeo3kVVPpPvfpfKbXzD0OH/Is/OIH0ZCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:55:20.115346Z"},"content_sha256":"698887c004cf054eda73bfea8ef41fe05143d5156c44768fe25ede9a98ff306b","schema_version":"1.0","event_id":"sha256:698887c004cf054eda73bfea8ef41fe05143d5156c44768fe25ede9a98ff306b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:2JXEI7BA5BKQBKOLIAS26CDIT4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stick-jump mode in surface droplet dissolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.flu-dyn","authors_text":"Detlef Lohse, Erik Dietrich, E. Stefan Kooij, Harold J. W. Zandvliet, Xuehua Zhang","submitted_at":"2016-05-24T11:59:19Z","abstract_excerpt":"The analogy between evaporating surface droplets in air to dissolving long-chain alcohol droplets in water is worked out. We show that next to the three known modi for surface droplet evaporation or dissolution (constant contact angle mode, constant contact radius mode, and stick-slide mode), a fourth mode exists for small droplets on supposedly smooth substrates, namely the stick-jump mode: intermittent contact line pinning causes the droplet to switch between sticking and jumping during the dissolution. We present experimental data and compare them to theory to predict the dissolution time i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.07395","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":"2026-05-18T01:12:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tCYE22KosDjTwaEm1ahRo45S1XJuqtuz7us5PYFpHua8WGIwBHSNaZ5q3sNC1oSP0dYFXJt12n/BWoARLN4UDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:55:20.115991Z"},"content_sha256":"d899b067c95c5a7c368d0c1a9e0428e753e972f238cd98dbc7d2f1f2f84283a6","schema_version":"1.0","event_id":"sha256:d899b067c95c5a7c368d0c1a9e0428e753e972f238cd98dbc7d2f1f2f84283a6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/bundle.json","state_url":"https://pith.science/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/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":"2026-05-26T13:55:20Z","links":{"resolver":"https://pith.science/pith/2JXEI7BA5BKQBKOLIAS26CDIT4","bundle":"https://pith.science/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/bundle.json","state":"https://pith.science/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2JXEI7BA5BKQBKOLIAS26CDIT4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:2JXEI7BA5BKQBKOLIAS26CDIT4","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":"fdc8a76db29ba5d1f392c02d1cfad9df8bca2d2d7671a99981e787c388052528","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-24T11:59:19Z","title_canon_sha256":"39c861f631c4ca35f11746ce0df44526389cf9a1f173453aea56180535f196d6"},"schema_version":"1.0","source":{"id":"1605.07395","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.07395","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"arxiv_version","alias_value":"1605.07395v1","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.07395","created_at":"2026-05-18T01:12:41Z"},{"alias_kind":"pith_short_12","alias_value":"2JXEI7BA5BKQ","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"2JXEI7BA5BKQBKOL","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"2JXEI7BA","created_at":"2026-05-18T12:29:55Z"}],"graph_snapshots":[{"event_id":"sha256:d899b067c95c5a7c368d0c1a9e0428e753e972f238cd98dbc7d2f1f2f84283a6","target":"graph","created_at":"2026-05-18T01:12:41Z","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":"The analogy between evaporating surface droplets in air to dissolving long-chain alcohol droplets in water is worked out. We show that next to the three known modi for surface droplet evaporation or dissolution (constant contact angle mode, constant contact radius mode, and stick-slide mode), a fourth mode exists for small droplets on supposedly smooth substrates, namely the stick-jump mode: intermittent contact line pinning causes the droplet to switch between sticking and jumping during the dissolution. We present experimental data and compare them to theory to predict the dissolution time i","authors_text":"Detlef Lohse, Erik Dietrich, E. Stefan Kooij, Harold J. W. Zandvliet, Xuehua Zhang","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-24T11:59:19Z","title":"Stick-jump mode in surface droplet dissolution"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.07395","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":"sha256:698887c004cf054eda73bfea8ef41fe05143d5156c44768fe25ede9a98ff306b","target":"record","created_at":"2026-05-18T01:12:41Z","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":"fdc8a76db29ba5d1f392c02d1cfad9df8bca2d2d7671a99981e787c388052528","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-24T11:59:19Z","title_canon_sha256":"39c861f631c4ca35f11746ce0df44526389cf9a1f173453aea56180535f196d6"},"schema_version":"1.0","source":{"id":"1605.07395","kind":"arxiv","version":1}},"canonical_sha256":"d26e447c20e85500a9cb4025af08689f1d2dcddb5ae07ac5c0fcb01996fdf3a3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d26e447c20e85500a9cb4025af08689f1d2dcddb5ae07ac5c0fcb01996fdf3a3","first_computed_at":"2026-05-18T01:12:41.757984Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:41.757984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3SS2P4v/+1ezp69dQFARnkU1hsmlN0ihlyfWBkE/ViRv4MhqvYildF6kFda5OAg6giBq4nxoHYLVaxz80eApBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:41.758312Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.07395","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:698887c004cf054eda73bfea8ef41fe05143d5156c44768fe25ede9a98ff306b","sha256:d899b067c95c5a7c368d0c1a9e0428e753e972f238cd98dbc7d2f1f2f84283a6"],"state_sha256":"2559c10cd0aa9a827d9417ba9dcf79c0347db8f48f6f7b39615d2b0bbffbd6cf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HlanIpWTMdZ1jyidzzwCatiMjXlwJi9hjdVLiWc9dCB1hTnpy84OL1ynluudVeXz6bn38DlcbNWh5MSu9JPPAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T13:55:20.119513Z","bundle_sha256":"de207acf6258b2fd8211f4dac136c899d2dcdfbcdeb149359613315d04311dac"}}