{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:3ILWT7HMGLMP7XKDAXNJ3OAOGP","short_pith_number":"pith:3ILWT7HM","canonical_record":{"source":{"id":"2406.06256","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-06-10T13:36:29Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"c5999f9e8e108a18c01db3414b1cd0cddc1e36a7a885c8e215206fff4a77bcae","abstract_canon_sha256":"f17c4473afa573df95560cf5aab7800af970b9a099e01f973e041b93c0bd1689"},"schema_version":"1.0"},"canonical_sha256":"da1769fcec32d8ffdd4305da9db80e33cb715eafe19a0c197e81e8893c59d12b","source":{"kind":"arxiv","id":"2406.06256","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.06256","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"arxiv_version","alias_value":"2406.06256v1","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.06256","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_12","alias_value":"3ILWT7HMGLMP","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"3ILWT7HMGLMP7XKD","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"3ILWT7HM","created_at":"2026-07-05T08:29:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:3ILWT7HMGLMP7XKDAXNJ3OAOGP","target":"record","payload":{"canonical_record":{"source":{"id":"2406.06256","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-06-10T13:36:29Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"c5999f9e8e108a18c01db3414b1cd0cddc1e36a7a885c8e215206fff4a77bcae","abstract_canon_sha256":"f17c4473afa573df95560cf5aab7800af970b9a099e01f973e041b93c0bd1689"},"schema_version":"1.0"},"canonical_sha256":"da1769fcec32d8ffdd4305da9db80e33cb715eafe19a0c197e81e8893c59d12b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:29:39.841630Z","signature_b64":"wrU7rB4CKokffvQik642EdYEr4a/sxVRIwj9vF5YYeKlGwwyXYl/syTqfO1ad3Np20Nvr9AbzbtSYWUbxAjdBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da1769fcec32d8ffdd4305da9db80e33cb715eafe19a0c197e81e8893c59d12b","last_reissued_at":"2026-07-05T08:29:39.841208Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:29:39.841208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2406.06256","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":"2026-07-05T08:29:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H9yOEPcLa9dlw8A+Up1GS2g27Up3guGnIT5qmitwku8ExKtfhQQZs/mKvA/ClPipw+1EyawkayY31r+MGaooAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T23:11:00.374796Z"},"content_sha256":"1436afaaa6fbf3f650298d588d53bcd015d1765eea0f034d53e952cfd5977e7b","schema_version":"1.0","event_id":"sha256:1436afaaa6fbf3f650298d588d53bcd015d1765eea0f034d53e952cfd5977e7b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:3ILWT7HMGLMP7XKDAXNJ3OAOGP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Study on Kelvin Helmholtz shear flows subjected to differential rotation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Devendra Sharma, Prince Kumar","submitted_at":"2024-06-10T13:36:29Z","abstract_excerpt":"A numerical simulation of Kelvin-Helmholtz Instability (KHI) in parallel shear flows subjected to external rotation is carried out using a pseudo-spectral technique. The Coriolis force, arising in a rotation frame under the beta plane approximation, tends to suppress the growth of KHI modes. The numerical results show a close qualitative agreement with the analytical results obtained for a step-wise shear flow profile. Experimental evidence demonstrates that particles in a rotating frame experience the Coriolis force, mathematically equivalent to the Lorentz force. Therefore, the Coriolis forc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.06256","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.06256/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T08:29:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1WQmlZnJ90I1q5BS4QAoiDEO7G9SZ+jw79QEXTy0LzT2VuUs3ndD2HAFccjKS8KMxv7TUWB4dsKVDxcUgempDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-06T23:11:00.375166Z"},"content_sha256":"bdd941cd106cd4e46cddc9a3df83a832c2919723ed882b0d7971ce5979fbe1f7","schema_version":"1.0","event_id":"sha256:bdd941cd106cd4e46cddc9a3df83a832c2919723ed882b0d7971ce5979fbe1f7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/bundle.json","state_url":"https://pith.science/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/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":"2026-07-06T23:11:00Z","links":{"resolver":"https://pith.science/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP","bundle":"https://pith.science/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/bundle.json","state":"https://pith.science/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3ILWT7HMGLMP7XKDAXNJ3OAOGP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:3ILWT7HMGLMP7XKDAXNJ3OAOGP","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":"f17c4473afa573df95560cf5aab7800af970b9a099e01f973e041b93c0bd1689","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-06-10T13:36:29Z","title_canon_sha256":"c5999f9e8e108a18c01db3414b1cd0cddc1e36a7a885c8e215206fff4a77bcae"},"schema_version":"1.0","source":{"id":"2406.06256","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.06256","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"arxiv_version","alias_value":"2406.06256v1","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.06256","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_12","alias_value":"3ILWT7HMGLMP","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"3ILWT7HMGLMP7XKD","created_at":"2026-07-05T08:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"3ILWT7HM","created_at":"2026-07-05T08:29:39Z"}],"graph_snapshots":[{"event_id":"sha256:bdd941cd106cd4e46cddc9a3df83a832c2919723ed882b0d7971ce5979fbe1f7","target":"graph","created_at":"2026-07-05T08:29:39Z","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/2406.06256/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A numerical simulation of Kelvin-Helmholtz Instability (KHI) in parallel shear flows subjected to external rotation is carried out using a pseudo-spectral technique. The Coriolis force, arising in a rotation frame under the beta plane approximation, tends to suppress the growth of KHI modes. The numerical results show a close qualitative agreement with the analytical results obtained for a step-wise shear flow profile. Experimental evidence demonstrates that particles in a rotating frame experience the Coriolis force, mathematically equivalent to the Lorentz force. Therefore, the Coriolis forc","authors_text":"Devendra Sharma, Prince Kumar","cross_cats":["physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-06-10T13:36:29Z","title":"Study on Kelvin Helmholtz shear flows subjected to differential rotation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.06256","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":"sha256:1436afaaa6fbf3f650298d588d53bcd015d1765eea0f034d53e952cfd5977e7b","target":"record","created_at":"2026-07-05T08:29:39Z","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":"f17c4473afa573df95560cf5aab7800af970b9a099e01f973e041b93c0bd1689","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-06-10T13:36:29Z","title_canon_sha256":"c5999f9e8e108a18c01db3414b1cd0cddc1e36a7a885c8e215206fff4a77bcae"},"schema_version":"1.0","source":{"id":"2406.06256","kind":"arxiv","version":1}},"canonical_sha256":"da1769fcec32d8ffdd4305da9db80e33cb715eafe19a0c197e81e8893c59d12b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"da1769fcec32d8ffdd4305da9db80e33cb715eafe19a0c197e81e8893c59d12b","first_computed_at":"2026-07-05T08:29:39.841208Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:29:39.841208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wrU7rB4CKokffvQik642EdYEr4a/sxVRIwj9vF5YYeKlGwwyXYl/syTqfO1ad3Np20Nvr9AbzbtSYWUbxAjdBg==","signature_status":"signed_v1","signed_at":"2026-07-05T08:29:39.841630Z","signed_message":"canonical_sha256_bytes"},"source_id":"2406.06256","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1436afaaa6fbf3f650298d588d53bcd015d1765eea0f034d53e952cfd5977e7b","sha256:bdd941cd106cd4e46cddc9a3df83a832c2919723ed882b0d7971ce5979fbe1f7"],"state_sha256":"5d525c97043044c1a26ff08b19b390e5a956e75f1bda554eec6040160cc45906"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6DzAs8ryFHD+ZIlTwpmzDhJI48U/vzf51xdOFfBGk570ZZuZ8NnL3WhB8ENhrjoXV2Gec09XepNUfo5xL39FBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-06T23:11:00.377406Z","bundle_sha256":"b4d94933d2933be0278d96901033c998ff51e7d68457a12edcfbef1a02d53bd3"}}