{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:U44XMCHKTYVYQFTI3COEAJD24A","short_pith_number":"pith:U44XMCHK","canonical_record":{"source":{"id":"1609.00938","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-04T14:06:34Z","cross_cats_sorted":[],"title_canon_sha256":"a47d07a2598685296942c7068d507054927f3d1e98856338f5f54687f25b7f49","abstract_canon_sha256":"52fbd9ab82a8ae6f20f22521af8c12cbb0f330c93351dc5b0147918171d65a9e"},"schema_version":"1.0"},"canonical_sha256":"a7397608ea9e2b881668d89c40247ae02d1784cf8afdb6e5d786f739785df050","source":{"kind":"arxiv","id":"1609.00938","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.00938","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"arxiv_version","alias_value":"1609.00938v1","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.00938","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"pith_short_12","alias_value":"U44XMCHKTYVY","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_16","alias_value":"U44XMCHKTYVYQFTI","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_8","alias_value":"U44XMCHK","created_at":"2026-05-18T12:30:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:U44XMCHKTYVYQFTI3COEAJD24A","target":"record","payload":{"canonical_record":{"source":{"id":"1609.00938","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-04T14:06:34Z","cross_cats_sorted":[],"title_canon_sha256":"a47d07a2598685296942c7068d507054927f3d1e98856338f5f54687f25b7f49","abstract_canon_sha256":"52fbd9ab82a8ae6f20f22521af8c12cbb0f330c93351dc5b0147918171d65a9e"},"schema_version":"1.0"},"canonical_sha256":"a7397608ea9e2b881668d89c40247ae02d1784cf8afdb6e5d786f739785df050","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:19.502068Z","signature_b64":"CW2o3qDhmv+CQMn6dOiY/FWlLQ8xJYJsiztJzqWklB7zFwnjn6gUsUQpjgs7rYpcVoM8xa7FjgOYil1B1UcaBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a7397608ea9e2b881668d89c40247ae02d1784cf8afdb6e5d786f739785df050","last_reissued_at":"2026-05-18T01:06:19.501481Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:19.501481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.00938","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":"2026-05-18T01:06:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6LMEQs5uIrAg5F2BupOel8CU8BmRVtGLxuxIIgELJwiiAmHpGYj2P5WL0VYs17MaPYeEijmUgvFv5Vr921dPBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:03:33.884662Z"},"content_sha256":"63b5f68bbb622390deea7261e59c99faf7db987360f79569703a025245b4e392","schema_version":"1.0","event_id":"sha256:63b5f68bbb622390deea7261e59c99faf7db987360f79569703a025245b4e392"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:U44XMCHKTYVYQFTI3COEAJD24A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Shear dynamics of an inverted nematic emulsion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"A. Tiribocchi, D. Marenduzzo, E. Orlandini, M. Da Re","submitted_at":"2016-09-04T14:06:34Z","abstract_excerpt":"Here we study theoretically the dynamics of a 2D and a 3D isotropic droplet in a nematic liquid crystal under a shear flow. We find a large repertoire of possible nonequilibrium steady states as a function of the shear rate and of the anchoring of the nematic director field at the droplet surface. We first discuss homeotropic anchoring. For weak anchoring, we recover the typical behaviour of a sheared isotropic droplet in a binary fluid, which rotates, stretches and can be broken by the applied flow. For intermediate anchoring, new possibilities arise due to elastic effects in the nematic flui"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.00938","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":"2026-05-18T01:06:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QaKwE8PI8pNurnMUgPddqeDflRBon8BpMaaGk72XHOHWTH5pIO12SW0NcMybs2ajZRoh1qLrJmZU1/s9sid+Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T05:03:33.885038Z"},"content_sha256":"18156499b26f2665f91fb9db9951f006cdae342d0a95402b9f9bf2bf05d596e8","schema_version":"1.0","event_id":"sha256:18156499b26f2665f91fb9db9951f006cdae342d0a95402b9f9bf2bf05d596e8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/U44XMCHKTYVYQFTI3COEAJD24A/bundle.json","state_url":"https://pith.science/pith/U44XMCHKTYVYQFTI3COEAJD24A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/U44XMCHKTYVYQFTI3COEAJD24A/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":"2026-05-28T05:03:33Z","links":{"resolver":"https://pith.science/pith/U44XMCHKTYVYQFTI3COEAJD24A","bundle":"https://pith.science/pith/U44XMCHKTYVYQFTI3COEAJD24A/bundle.json","state":"https://pith.science/pith/U44XMCHKTYVYQFTI3COEAJD24A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/U44XMCHKTYVYQFTI3COEAJD24A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:U44XMCHKTYVYQFTI3COEAJD24A","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":"52fbd9ab82a8ae6f20f22521af8c12cbb0f330c93351dc5b0147918171d65a9e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-04T14:06:34Z","title_canon_sha256":"a47d07a2598685296942c7068d507054927f3d1e98856338f5f54687f25b7f49"},"schema_version":"1.0","source":{"id":"1609.00938","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.00938","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"arxiv_version","alias_value":"1609.00938v1","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.00938","created_at":"2026-05-18T01:06:19Z"},{"alias_kind":"pith_short_12","alias_value":"U44XMCHKTYVY","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_16","alias_value":"U44XMCHKTYVYQFTI","created_at":"2026-05-18T12:30:46Z"},{"alias_kind":"pith_short_8","alias_value":"U44XMCHK","created_at":"2026-05-18T12:30:46Z"}],"graph_snapshots":[{"event_id":"sha256:18156499b26f2665f91fb9db9951f006cdae342d0a95402b9f9bf2bf05d596e8","target":"graph","created_at":"2026-05-18T01:06:19Z","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":"Here we study theoretically the dynamics of a 2D and a 3D isotropic droplet in a nematic liquid crystal under a shear flow. We find a large repertoire of possible nonequilibrium steady states as a function of the shear rate and of the anchoring of the nematic director field at the droplet surface. We first discuss homeotropic anchoring. For weak anchoring, we recover the typical behaviour of a sheared isotropic droplet in a binary fluid, which rotates, stretches and can be broken by the applied flow. For intermediate anchoring, new possibilities arise due to elastic effects in the nematic flui","authors_text":"A. Tiribocchi, D. Marenduzzo, E. Orlandini, M. Da Re","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-04T14:06:34Z","title":"Shear dynamics of an inverted nematic emulsion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.00938","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":"sha256:63b5f68bbb622390deea7261e59c99faf7db987360f79569703a025245b4e392","target":"record","created_at":"2026-05-18T01:06:19Z","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":"52fbd9ab82a8ae6f20f22521af8c12cbb0f330c93351dc5b0147918171d65a9e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2016-09-04T14:06:34Z","title_canon_sha256":"a47d07a2598685296942c7068d507054927f3d1e98856338f5f54687f25b7f49"},"schema_version":"1.0","source":{"id":"1609.00938","kind":"arxiv","version":1}},"canonical_sha256":"a7397608ea9e2b881668d89c40247ae02d1784cf8afdb6e5d786f739785df050","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a7397608ea9e2b881668d89c40247ae02d1784cf8afdb6e5d786f739785df050","first_computed_at":"2026-05-18T01:06:19.501481Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:19.501481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CW2o3qDhmv+CQMn6dOiY/FWlLQ8xJYJsiztJzqWklB7zFwnjn6gUsUQpjgs7rYpcVoM8xa7FjgOYil1B1UcaBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:19.502068Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.00938","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:63b5f68bbb622390deea7261e59c99faf7db987360f79569703a025245b4e392","sha256:18156499b26f2665f91fb9db9951f006cdae342d0a95402b9f9bf2bf05d596e8"],"state_sha256":"9964c64de88edd4964b76d374ce7d81e70fb334bb2bfc5446c1bae1a43099a12"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZKc8Zt+OqR4T0vgCcFFE0tNLGprhc+CGxqyCM5P62jQ3eK4E49cTl7ZbALtW9RYQVOTmIqrxlTQvUajQ9QJCDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T05:03:33.887159Z","bundle_sha256":"6bf2c6fd3b8b6e9ebe411a4220bd373c6f104ccba8143eef3f7d8bf9c113b462"}}