{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:IBEPU76RE2MHJZFECHZGDFUABI","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":"02d6b1c62716177cb0a3bc37104b5239fe377939ab26c259a2c1b34299604773","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-29T11:16:40Z","title_canon_sha256":"26a6a3c4956e9c782f0d54335be5085eca6dd7be63aa7ab5478fd7d17eaac963"},"schema_version":"1.0","source":{"id":"1310.7758","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.7758","created_at":"2026-05-18T01:46:47Z"},{"alias_kind":"arxiv_version","alias_value":"1310.7758v1","created_at":"2026-05-18T01:46:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.7758","created_at":"2026-05-18T01:46:47Z"},{"alias_kind":"pith_short_12","alias_value":"IBEPU76RE2MH","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"IBEPU76RE2MHJZFE","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"IBEPU76R","created_at":"2026-05-18T12:27:46Z"}],"graph_snapshots":[{"event_id":"sha256:14916e33b9cb6ef1761b083118271c5f2bbffb69fdde1ce8a376d4bf2953e4c5","target":"graph","created_at":"2026-05-18T01:46:47Z","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 Kelvin-Helmholtz (KH) instability is studied in a non-Newtonian dusty plasma with an experimentally verified model [Phys. Rev. Lett. {\\bf 98}, 145003 (2007)] of shear flow rate dependent viscosity. The shear flow profile used here is a parabolic type bounded flow. Both the shear thinning and shear thickening properties are investigated in compressible as well as incompressible limits using a linear stability analysis. Like the stabilizing effect of compressibility on the KH instability, the non-Newtonian effect in shear thickening regime could also suppress the instability but on the contr","authors_text":"D. Banerjee, M. S. Janaki, N. Chakrabarti, S. Garai","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-29T11:16:40Z","title":"Kelvin-Helmholtz Instability in non-Newtonian Complex Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.7758","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":"sha256:85db2055c51843d468ab24ec3d77234d81f27a0fa547f34aa0e1fe9c99267f6f","target":"record","created_at":"2026-05-18T01:46:47Z","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":"02d6b1c62716177cb0a3bc37104b5239fe377939ab26c259a2c1b34299604773","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-29T11:16:40Z","title_canon_sha256":"26a6a3c4956e9c782f0d54335be5085eca6dd7be63aa7ab5478fd7d17eaac963"},"schema_version":"1.0","source":{"id":"1310.7758","kind":"arxiv","version":1}},"canonical_sha256":"4048fa7fd1269874e4a411f26196800a2092d061b568580da3814c4e7269d943","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4048fa7fd1269874e4a411f26196800a2092d061b568580da3814c4e7269d943","first_computed_at":"2026-05-18T01:46:47.934493Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:46:47.934493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h4XGBkawlfbVHFYtxqRQt5Q4kZvaYW60bm/n1aSYlhn60kmNMoQS/1TehiKjwzbv7vJC/WQoNAkIwwoA0iTyDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:46:47.935123Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.7758","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:85db2055c51843d468ab24ec3d77234d81f27a0fa547f34aa0e1fe9c99267f6f","sha256:14916e33b9cb6ef1761b083118271c5f2bbffb69fdde1ce8a376d4bf2953e4c5"],"state_sha256":"63df414e2830bba657040e0df0cfddd4366b89132a495e9f26219c3e527c61c5"}