{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:BP6LMYNNJCXSMVICCO5EVTJ3P4","short_pith_number":"pith:BP6LMYNN","schema_version":"1.0","canonical_sha256":"0bfcb661ad48af26550213ba4acd3b7f2b39c5635349c3cf92665c86f6e3f1a8","source":{"kind":"arxiv","id":"1102.5114","version":1},"attestation_state":"computed","paper":{"title":"Morphological instability of the solid-liquid interface in crystal growth under supercooled liquid film flow and natural convection airflow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"K. Ueno, M. Farzaneh","submitted_at":"2011-02-24T22:01:58Z","abstract_excerpt":"Ring-like ripples on the surface of icicles are an example of morphological instability of the ice-water interface during ice growth under supercooled water film flow. The surface of icicles is typically covered with ripples of about 1 cm in wavelength, and the wavelength appears to be almost independent of external temperature, icicle radius, and volumetric water flow rate. One side of the water layer consists of the water-air surface and growing ice is the other. This is one of the more complicated moving phase boundary problems with two interfaces. A recent theoretical work [K. Ueno, Phys. "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1102.5114","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2011-02-24T22:01:58Z","cross_cats_sorted":[],"title_canon_sha256":"0c99e6ef1ea316e01fbeb721acf4a3475cdb28ed3353fb82ad2a4ad5aeadc0d5","abstract_canon_sha256":"85b7a6fef19cc87d2945c11786bb937aa8f203893aee24d8276840852c1f691c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:05.142226Z","signature_b64":"hRkThE2hAS2Pgo1hYWN+t/x8RgXrGFW9ci/9I4f1g1erihtAZEjcmeRHiQsvkTAT8wJuXPWedUG2H7u2PAuzAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0bfcb661ad48af26550213ba4acd3b7f2b39c5635349c3cf92665c86f6e3f1a8","last_reissued_at":"2026-05-18T02:03:05.141277Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:05.141277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Morphological instability of the solid-liquid interface in crystal growth under supercooled liquid film flow and natural convection airflow","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"K. Ueno, M. Farzaneh","submitted_at":"2011-02-24T22:01:58Z","abstract_excerpt":"Ring-like ripples on the surface of icicles are an example of morphological instability of the ice-water interface during ice growth under supercooled water film flow. The surface of icicles is typically covered with ripples of about 1 cm in wavelength, and the wavelength appears to be almost independent of external temperature, icicle radius, and volumetric water flow rate. One side of the water layer consists of the water-air surface and growing ice is the other. This is one of the more complicated moving phase boundary problems with two interfaces. A recent theoretical work [K. Ueno, Phys. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.5114","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1102.5114","created_at":"2026-05-18T02:03:05.141426+00:00"},{"alias_kind":"arxiv_version","alias_value":"1102.5114v1","created_at":"2026-05-18T02:03:05.141426+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.5114","created_at":"2026-05-18T02:03:05.141426+00:00"},{"alias_kind":"pith_short_12","alias_value":"BP6LMYNNJCXS","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_16","alias_value":"BP6LMYNNJCXSMVIC","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_8","alias_value":"BP6LMYNN","created_at":"2026-05-18T12:26:24.575870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4","json":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4.json","graph_json":"https://pith.science/api/pith-number/BP6LMYNNJCXSMVICCO5EVTJ3P4/graph.json","events_json":"https://pith.science/api/pith-number/BP6LMYNNJCXSMVICCO5EVTJ3P4/events.json","paper":"https://pith.science/paper/BP6LMYNN"},"agent_actions":{"view_html":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4","download_json":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4.json","view_paper":"https://pith.science/paper/BP6LMYNN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1102.5114&json=true","fetch_graph":"https://pith.science/api/pith-number/BP6LMYNNJCXSMVICCO5EVTJ3P4/graph.json","fetch_events":"https://pith.science/api/pith-number/BP6LMYNNJCXSMVICCO5EVTJ3P4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4/action/storage_attestation","attest_author":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4/action/author_attestation","sign_citation":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4/action/citation_signature","submit_replication":"https://pith.science/pith/BP6LMYNNJCXSMVICCO5EVTJ3P4/action/replication_record"}},"created_at":"2026-05-18T02:03:05.141426+00:00","updated_at":"2026-05-18T02:03:05.141426+00:00"}