{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:ULYQO2XT2FSIT7WQF6S6RTERMU","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":"1a7950657b4c4dad65795d9526fd88b3e58f0ffa670a1f062f37a95b27366ce7","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-09-05T04:42:24Z","title_canon_sha256":"f93e3ca51e31864cce83e9090949b373f43737d6d14140192160f31b759cc245"},"schema_version":"1.0","source":{"id":"2409.03241","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.03241","created_at":"2026-07-05T09:03:28Z"},{"alias_kind":"arxiv_version","alias_value":"2409.03241v1","created_at":"2026-07-05T09:03:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.03241","created_at":"2026-07-05T09:03:28Z"},{"alias_kind":"pith_short_12","alias_value":"ULYQO2XT2FSI","created_at":"2026-07-05T09:03:28Z"},{"alias_kind":"pith_short_16","alias_value":"ULYQO2XT2FSIT7WQ","created_at":"2026-07-05T09:03:28Z"},{"alias_kind":"pith_short_8","alias_value":"ULYQO2XT","created_at":"2026-07-05T09:03:28Z"}],"graph_snapshots":[{"event_id":"sha256:e79d3b91c6e36bb555ad4a85b1021cfe744f98e7e6f7d60b86a7c69293b4109e","target":"graph","created_at":"2026-07-05T09:03:28Z","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/2409.03241/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The solution for non-linear, complex partial differential Equations (PDEs) is achieved through numerical approximations, which yield a linear system of equations. This approach is prevalent in Computational Fluid Dynamics (CFD), but it restricts the mesh size since the solution of the linear system becomes computationally intractable when the mesh resolution increases. The reliance on the ability of High-Performance Computers (HPC) to scale up and meet these requirements is myopic; such very high-fidelity simulations require a paradigm shift in computing. This paper presents an exploration of ","authors_text":"Abhishek Chopra, Dhamotharan S, Ferdin Sagai Don Bosco, Rut Lineswala","cross_cats":["quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-09-05T04:42:24Z","title":"Demonstration of Scalability and Accuracy of Variational Quantum Linear Solver for Computational Fluid Dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.03241","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":"sha256:2d1fcd8abc92cdecc7fb37f0ce126bc93c9232d11d6549a47a94a22ad216e1b1","target":"record","created_at":"2026-07-05T09:03:28Z","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":"1a7950657b4c4dad65795d9526fd88b3e58f0ffa670a1f062f37a95b27366ce7","cross_cats_sorted":["quant-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-09-05T04:42:24Z","title_canon_sha256":"f93e3ca51e31864cce83e9090949b373f43737d6d14140192160f31b759cc245"},"schema_version":"1.0","source":{"id":"2409.03241","kind":"arxiv","version":1}},"canonical_sha256":"a2f1076af3d16489fed02fa5e8cc916510233c24802a5128f16871e7c7ff73be","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a2f1076af3d16489fed02fa5e8cc916510233c24802a5128f16871e7c7ff73be","first_computed_at":"2026-07-05T09:03:28.340452Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:03:28.340452Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fJda8w3KYBTO/KbNoEHRHbHqRcc80AdXPjspCNXNkWc2Qoekh+xjh6H5U58M+y90PCuf1lsosWwI97ShPYwIAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:03:28.340964Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.03241","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2d1fcd8abc92cdecc7fb37f0ce126bc93c9232d11d6549a47a94a22ad216e1b1","sha256:e79d3b91c6e36bb555ad4a85b1021cfe744f98e7e6f7d60b86a7c69293b4109e"],"state_sha256":"02b13289e26e6f5523648d1aef17a5da6473bf89090b7acefee71f4e7a85596a"}