{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:BZMQZRM2YIA2LOZOQQYQGHGXCG","short_pith_number":"pith:BZMQZRM2","schema_version":"1.0","canonical_sha256":"0e590cc59ac201a5bb2e8431031cd711ab52fd2a4a7df0f63db01d1f16371473","source":{"kind":"arxiv","id":"0906.0479","version":1},"attestation_state":"computed","paper":{"title":"Electric field Induced Patterns in Soft Visco-elastic films: From Long Waves of Viscous Liquids to Short Waves of Elastic Solids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Ashutosh Sharma, Hemant M. Dixit, Indrani Banerjee, K. S. Narayan, N. Arun, Partho S. G. Pattader","submitted_at":"2009-06-02T13:16:16Z","abstract_excerpt":"We show that the electric field driven surface instability of visco-elastic films has two distinct regimes: (1) The visco-elastic films behaving like a liquid display long wavelengths governed by applied voltage and surface tension, independent of its elastic storage and viscous loss moduli, and (2) the films behaving like a solid require a threshold voltage for the instability whose wavelength always scales as ~ 4 x film thickness, independent of its surface tension, applied voltage, loss and storage moduli. Wavelength in a narrow transition zone between these regimes depends on the storage m"},"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":"0906.0479","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2009-06-02T13:16:16Z","cross_cats_sorted":[],"title_canon_sha256":"07dc9a437171ef45929c3c7e73c9a9a8deb241a96fe60a40e0f3f8011f9458af","abstract_canon_sha256":"064a74c1f1186f2aea36596dd86ae9c37c8fee56554844ebfc0e7ffffbb4bddf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:13:29.759753Z","signature_b64":"u1/ohXIF1L315r1WVLcYCIUuNhuIE6+obXo/+ZXDsGCPo7m5sxNeCJVIDQBkayCthHgKCzDF8DPjWObDvLmfAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e590cc59ac201a5bb2e8431031cd711ab52fd2a4a7df0f63db01d1f16371473","last_reissued_at":"2026-05-18T02:13:29.759129Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:13:29.759129Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electric field Induced Patterns in Soft Visco-elastic films: From Long Waves of Viscous Liquids to Short Waves of Elastic Solids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Ashutosh Sharma, Hemant M. Dixit, Indrani Banerjee, K. S. Narayan, N. Arun, Partho S. G. Pattader","submitted_at":"2009-06-02T13:16:16Z","abstract_excerpt":"We show that the electric field driven surface instability of visco-elastic films has two distinct regimes: (1) The visco-elastic films behaving like a liquid display long wavelengths governed by applied voltage and surface tension, independent of its elastic storage and viscous loss moduli, and (2) the films behaving like a solid require a threshold voltage for the instability whose wavelength always scales as ~ 4 x film thickness, independent of its surface tension, applied voltage, loss and storage moduli. Wavelength in a narrow transition zone between these regimes depends on the storage m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0906.0479","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":"0906.0479","created_at":"2026-05-18T02:13:29.759234+00:00"},{"alias_kind":"arxiv_version","alias_value":"0906.0479v1","created_at":"2026-05-18T02:13:29.759234+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0906.0479","created_at":"2026-05-18T02:13:29.759234+00:00"},{"alias_kind":"pith_short_12","alias_value":"BZMQZRM2YIA2","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_16","alias_value":"BZMQZRM2YIA2LOZO","created_at":"2026-05-18T12:25:58.837520+00:00"},{"alias_kind":"pith_short_8","alias_value":"BZMQZRM2","created_at":"2026-05-18T12:25:58.837520+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/BZMQZRM2YIA2LOZOQQYQGHGXCG","json":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG.json","graph_json":"https://pith.science/api/pith-number/BZMQZRM2YIA2LOZOQQYQGHGXCG/graph.json","events_json":"https://pith.science/api/pith-number/BZMQZRM2YIA2LOZOQQYQGHGXCG/events.json","paper":"https://pith.science/paper/BZMQZRM2"},"agent_actions":{"view_html":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG","download_json":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG.json","view_paper":"https://pith.science/paper/BZMQZRM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0906.0479&json=true","fetch_graph":"https://pith.science/api/pith-number/BZMQZRM2YIA2LOZOQQYQGHGXCG/graph.json","fetch_events":"https://pith.science/api/pith-number/BZMQZRM2YIA2LOZOQQYQGHGXCG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG/action/storage_attestation","attest_author":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG/action/author_attestation","sign_citation":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG/action/citation_signature","submit_replication":"https://pith.science/pith/BZMQZRM2YIA2LOZOQQYQGHGXCG/action/replication_record"}},"created_at":"2026-05-18T02:13:29.759234+00:00","updated_at":"2026-05-18T02:13:29.759234+00:00"}