{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:UIZG7H2MX5ETQIPF64VNLGN45U","short_pith_number":"pith:UIZG7H2M","canonical_record":{"source":{"id":"1904.11386","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-25T14:41:17Z","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"title_canon_sha256":"c8c1e60d77c1e7cf8e7d61c658d2840f92ced3cca61fbc4df33a400f8ae2749c","abstract_canon_sha256":"f16d7d92c0a8a1e33cdaa1e527542881bc5da31ad53b46c8451d6adfc2dc51e4"},"schema_version":"1.0"},"canonical_sha256":"a2326f9f4cbf493821e5f72ad599bced264b538da8b5d48d387f12f8e6a222a8","source":{"kind":"arxiv","id":"1904.11386","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.11386","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"arxiv_version","alias_value":"1904.11386v3","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.11386","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_12","alias_value":"UIZG7H2MX5ET","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_16","alias_value":"UIZG7H2MX5ETQIPF","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_8","alias_value":"UIZG7H2M","created_at":"2026-07-05T00:06:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:UIZG7H2MX5ETQIPF64VNLGN45U","target":"record","payload":{"canonical_record":{"source":{"id":"1904.11386","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-25T14:41:17Z","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"title_canon_sha256":"c8c1e60d77c1e7cf8e7d61c658d2840f92ced3cca61fbc4df33a400f8ae2749c","abstract_canon_sha256":"f16d7d92c0a8a1e33cdaa1e527542881bc5da31ad53b46c8451d6adfc2dc51e4"},"schema_version":"1.0"},"canonical_sha256":"a2326f9f4cbf493821e5f72ad599bced264b538da8b5d48d387f12f8e6a222a8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:06:41.773872Z","signature_b64":"RQfD86tzad82u2mgqpmBIfYiv5fLMjZZwJ4imHEuwrgRp4mkR60ShhGxFf7mhwIZJjX2NoHJ6jdp5a/N7qvdCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a2326f9f4cbf493821e5f72ad599bced264b538da8b5d48d387f12f8e6a222a8","last_reissued_at":"2026-07-05T00:06:41.773430Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:06:41.773430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1904.11386","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T00:06:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3fom8KlscVoCSufZm2XBBLgHIlaEf72F5y2Fk+BO9LL32oB6MKN3qcqSz9Vu3G23oVvjcSNqXA5XjFI0kd7rCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T17:03:00.250241Z"},"content_sha256":"fd23e282b9f15f42b9d565f1cb4b9d181fe0b42d510b46a0cc97c7523ae01a59","schema_version":"1.0","event_id":"sha256:fd23e282b9f15f42b9d565f1cb4b9d181fe0b42d510b46a0cc97c7523ae01a59"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:UIZG7H2MX5ETQIPF64VNLGN45U","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Mesoscale simulation of soft particles with tunable contact angle in multi-component fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.flu-dyn"],"primary_cat":"physics.comp-ph","authors_text":"Jens Harting, Maarten Wouters, Othmane Aouane, Timm Krueger","submitted_at":"2019-04-25T14:41:17Z","abstract_excerpt":"Soft particles at fluid interfaces play an important role in many aspects of our daily life, such as the food industry, paints and coatings, and medical applications. Analytical methods are not capable of describing the emergent effects of the complex dynamics of suspensions of many soft particles, whereas experiments typically either only capture bulk properties or require invasive methods. Computational methods are therefore a great tool to complement experimental work. However, an efficient and versatile numerical method is needed to model dense suspensions of many soft particles. In this a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.11386","kind":"arxiv","version":3},"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/1904.11386/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":"2026-07-05T00:06:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uEGEBNhpbxHLFxthqxiPqe6/p3i9ZOU0jkeJ8xBMWdLm3nNZ/A0Jzsyh/DgNA82vOu7DxhCeGz79nJuE71QTDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T17:03:00.251008Z"},"content_sha256":"becc0d65e3a20bcc00576ec58e6a679f783fa117c0c63c0885a6019f87ffe31a","schema_version":"1.0","event_id":"sha256:becc0d65e3a20bcc00576ec58e6a679f783fa117c0c63c0885a6019f87ffe31a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UIZG7H2MX5ETQIPF64VNLGN45U/bundle.json","state_url":"https://pith.science/pith/UIZG7H2MX5ETQIPF64VNLGN45U/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UIZG7H2MX5ETQIPF64VNLGN45U/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":"2026-08-04T17:03:00Z","links":{"resolver":"https://pith.science/pith/UIZG7H2MX5ETQIPF64VNLGN45U","bundle":"https://pith.science/pith/UIZG7H2MX5ETQIPF64VNLGN45U/bundle.json","state":"https://pith.science/pith/UIZG7H2MX5ETQIPF64VNLGN45U/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UIZG7H2MX5ETQIPF64VNLGN45U/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:UIZG7H2MX5ETQIPF64VNLGN45U","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":"f16d7d92c0a8a1e33cdaa1e527542881bc5da31ad53b46c8451d6adfc2dc51e4","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-25T14:41:17Z","title_canon_sha256":"c8c1e60d77c1e7cf8e7d61c658d2840f92ced3cca61fbc4df33a400f8ae2749c"},"schema_version":"1.0","source":{"id":"1904.11386","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.11386","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"arxiv_version","alias_value":"1904.11386v3","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.11386","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_12","alias_value":"UIZG7H2MX5ET","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_16","alias_value":"UIZG7H2MX5ETQIPF","created_at":"2026-07-05T00:06:41Z"},{"alias_kind":"pith_short_8","alias_value":"UIZG7H2M","created_at":"2026-07-05T00:06:41Z"}],"graph_snapshots":[{"event_id":"sha256:becc0d65e3a20bcc00576ec58e6a679f783fa117c0c63c0885a6019f87ffe31a","target":"graph","created_at":"2026-07-05T00:06:41Z","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/1904.11386/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Soft particles at fluid interfaces play an important role in many aspects of our daily life, such as the food industry, paints and coatings, and medical applications. Analytical methods are not capable of describing the emergent effects of the complex dynamics of suspensions of many soft particles, whereas experiments typically either only capture bulk properties or require invasive methods. Computational methods are therefore a great tool to complement experimental work. However, an efficient and versatile numerical method is needed to model dense suspensions of many soft particles. In this a","authors_text":"Jens Harting, Maarten Wouters, Othmane Aouane, Timm Krueger","cross_cats":["cond-mat.soft","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-25T14:41:17Z","title":"Mesoscale simulation of soft particles with tunable contact angle in multi-component fluids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.11386","kind":"arxiv","version":3},"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:fd23e282b9f15f42b9d565f1cb4b9d181fe0b42d510b46a0cc97c7523ae01a59","target":"record","created_at":"2026-07-05T00:06:41Z","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":"f16d7d92c0a8a1e33cdaa1e527542881bc5da31ad53b46c8451d6adfc2dc51e4","cross_cats_sorted":["cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-25T14:41:17Z","title_canon_sha256":"c8c1e60d77c1e7cf8e7d61c658d2840f92ced3cca61fbc4df33a400f8ae2749c"},"schema_version":"1.0","source":{"id":"1904.11386","kind":"arxiv","version":3}},"canonical_sha256":"a2326f9f4cbf493821e5f72ad599bced264b538da8b5d48d387f12f8e6a222a8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a2326f9f4cbf493821e5f72ad599bced264b538da8b5d48d387f12f8e6a222a8","first_computed_at":"2026-07-05T00:06:41.773430Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:06:41.773430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RQfD86tzad82u2mgqpmBIfYiv5fLMjZZwJ4imHEuwrgRp4mkR60ShhGxFf7mhwIZJjX2NoHJ6jdp5a/N7qvdCw==","signature_status":"signed_v1","signed_at":"2026-07-05T00:06:41.773872Z","signed_message":"canonical_sha256_bytes"},"source_id":"1904.11386","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd23e282b9f15f42b9d565f1cb4b9d181fe0b42d510b46a0cc97c7523ae01a59","sha256:becc0d65e3a20bcc00576ec58e6a679f783fa117c0c63c0885a6019f87ffe31a"],"state_sha256":"9b2ba31bf1ee0cf8eece770fe5d35213cd3610caed7ae28b2dbe7601f06ce3c8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"58qi1spHIbAqd9MbKptKcA7CkzyOPHtaBG078UwFHv6lH0gzsNHqbM6MYGNxXkBlbJ26mWcUBiXH4rq6eo0LDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T17:03:00.256811Z","bundle_sha256":"adf83c724a4374096cf7538ddb040f5c4f0046ca62e152f7ccf4582b18007596"}}