{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:3LZ6Q2XKU5OZZCEKRBUHAAPPA7","short_pith_number":"pith:3LZ6Q2XK","canonical_record":{"source":{"id":"1902.08499","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2019-02-22T14:13:32Z","cross_cats_sorted":[],"title_canon_sha256":"b13f69ae7da19a011bbdd9c8d482655d581b822a0dcba383a063bf787cc9c2fd","abstract_canon_sha256":"5f80140e1c5ebe33e001c03ed70f9e278cf089e2078f2de52245692a311cd508"},"schema_version":"1.0"},"canonical_sha256":"daf3e86aeaa75d9c888a88687001ef07ca697da19a1529d9e1e7f0335cac45ba","source":{"kind":"arxiv","id":"1902.08499","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.08499","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"arxiv_version","alias_value":"1902.08499v1","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.08499","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"pith_short_12","alias_value":"3LZ6Q2XKU5OZ","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"3LZ6Q2XKU5OZZCEK","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"3LZ6Q2XK","created_at":"2026-05-18T12:33:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:3LZ6Q2XKU5OZZCEKRBUHAAPPA7","target":"record","payload":{"canonical_record":{"source":{"id":"1902.08499","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2019-02-22T14:13:32Z","cross_cats_sorted":[],"title_canon_sha256":"b13f69ae7da19a011bbdd9c8d482655d581b822a0dcba383a063bf787cc9c2fd","abstract_canon_sha256":"5f80140e1c5ebe33e001c03ed70f9e278cf089e2078f2de52245692a311cd508"},"schema_version":"1.0"},"canonical_sha256":"daf3e86aeaa75d9c888a88687001ef07ca697da19a1529d9e1e7f0335cac45ba","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:52:57.046698Z","signature_b64":"UkH2AeNsRvB7RNQh3uCcFh24uxT7fi6zNYp2SeDXYWVjOZCW127cygUA6xfnhcgVoVLFSaqLsrRW4V5mJrSKBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"daf3e86aeaa75d9c888a88687001ef07ca697da19a1529d9e1e7f0335cac45ba","last_reissued_at":"2026-05-17T23:52:57.045959Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:52:57.045959Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1902.08499","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":"2026-05-17T23:52:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ROaO4wbm9VYqoJDwTBVC2Xjp5Dc+uCKhuc6ipn6ktKIRnlJJlv6aCOi1PHoZSS0sX5oZXvAktr3bjDvYvHG7CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T16:05:40.039847Z"},"content_sha256":"9d61d62994261e01fe38c4fc7a210438f5fb1483fc77491f4d1f10cc296c65e2","schema_version":"1.0","event_id":"sha256:9d61d62994261e01fe38c4fc7a210438f5fb1483fc77491f4d1f10cc296c65e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:3LZ6Q2XKU5OZZCEKRBUHAAPPA7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rayleigh breakup of a charged viscous drop via tip-streaming","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Neha Gawande, Rochish Thaokar, Y. S. Mayya","submitted_at":"2019-02-22T14:13:32Z","abstract_excerpt":"The experimental observation of D. Duft, T. Achtzehn, R. Muller, B. A. Huber, and T. Leisner, Nature 421, 128 (2003) on the sequential progression of the instability of a charged liquid drop points at the formation of a jet followed by the emission of progeny droplets as a crucial pathway of the Rayleigh fission process. In spite of considerable theoretical progress, a quantitative understanding of this breakup pathway through mathematical models has largely remained inconclusive. This limitation has mainly been due to the fact that the generally applied electrostatic boundary condition of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.08499","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":"2026-05-17T23:52:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YCAMkRx1PnDCp60sW4LIcoNOgJRoh3tFldcuk4m2sv9897vk5R6/lbT6KYIeQZuuZuuHAT2VpSUYYCYKzCNoBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T16:05:40.040180Z"},"content_sha256":"18d17de80a4ce71c121cc1066592b34227960db0673b84f304a7771d3152f0f1","schema_version":"1.0","event_id":"sha256:18d17de80a4ce71c121cc1066592b34227960db0673b84f304a7771d3152f0f1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/bundle.json","state_url":"https://pith.science/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/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":"2026-06-29T16:05:40Z","links":{"resolver":"https://pith.science/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7","bundle":"https://pith.science/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/bundle.json","state":"https://pith.science/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3LZ6Q2XKU5OZZCEKRBUHAAPPA7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:3LZ6Q2XKU5OZZCEKRBUHAAPPA7","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":"5f80140e1c5ebe33e001c03ed70f9e278cf089e2078f2de52245692a311cd508","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2019-02-22T14:13:32Z","title_canon_sha256":"b13f69ae7da19a011bbdd9c8d482655d581b822a0dcba383a063bf787cc9c2fd"},"schema_version":"1.0","source":{"id":"1902.08499","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.08499","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"arxiv_version","alias_value":"1902.08499v1","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.08499","created_at":"2026-05-17T23:52:57Z"},{"alias_kind":"pith_short_12","alias_value":"3LZ6Q2XKU5OZ","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"3LZ6Q2XKU5OZZCEK","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"3LZ6Q2XK","created_at":"2026-05-18T12:33:07Z"}],"graph_snapshots":[{"event_id":"sha256:18d17de80a4ce71c121cc1066592b34227960db0673b84f304a7771d3152f0f1","target":"graph","created_at":"2026-05-17T23:52:57Z","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 experimental observation of D. Duft, T. Achtzehn, R. Muller, B. A. Huber, and T. Leisner, Nature 421, 128 (2003) on the sequential progression of the instability of a charged liquid drop points at the formation of a jet followed by the emission of progeny droplets as a crucial pathway of the Rayleigh fission process. In spite of considerable theoretical progress, a quantitative understanding of this breakup pathway through mathematical models has largely remained inconclusive. This limitation has mainly been due to the fact that the generally applied electrostatic boundary condition of the","authors_text":"Neha Gawande, Rochish Thaokar, Y. S. Mayya","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2019-02-22T14:13:32Z","title":"Rayleigh breakup of a charged viscous drop via tip-streaming"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.08499","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":"sha256:9d61d62994261e01fe38c4fc7a210438f5fb1483fc77491f4d1f10cc296c65e2","target":"record","created_at":"2026-05-17T23:52:57Z","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":"5f80140e1c5ebe33e001c03ed70f9e278cf089e2078f2de52245692a311cd508","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2019-02-22T14:13:32Z","title_canon_sha256":"b13f69ae7da19a011bbdd9c8d482655d581b822a0dcba383a063bf787cc9c2fd"},"schema_version":"1.0","source":{"id":"1902.08499","kind":"arxiv","version":1}},"canonical_sha256":"daf3e86aeaa75d9c888a88687001ef07ca697da19a1529d9e1e7f0335cac45ba","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"daf3e86aeaa75d9c888a88687001ef07ca697da19a1529d9e1e7f0335cac45ba","first_computed_at":"2026-05-17T23:52:57.045959Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:52:57.045959Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UkH2AeNsRvB7RNQh3uCcFh24uxT7fi6zNYp2SeDXYWVjOZCW127cygUA6xfnhcgVoVLFSaqLsrRW4V5mJrSKBA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:52:57.046698Z","signed_message":"canonical_sha256_bytes"},"source_id":"1902.08499","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9d61d62994261e01fe38c4fc7a210438f5fb1483fc77491f4d1f10cc296c65e2","sha256:18d17de80a4ce71c121cc1066592b34227960db0673b84f304a7771d3152f0f1"],"state_sha256":"2ccfc3d6315ebd57f19c9fd8c20351d691f08254a1edffc5ec676d07b523b42d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B6ZC/AurANvHVLO5JtUPznF9vq+/xwYVquv5t7q0ECNA2Z2t9II1WoYc1KrLI0jm3n9xOw+ULl1ARWi/GQwvBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T16:05:40.041928Z","bundle_sha256":"a1d65e590370ec5275752ae888cbfdb5c4940868886a826771619b00127d44b8"}}