{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:GN3TBVYIWNF5MOK2PM5Z2JJBU3","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":"fbfa3537148bc5bd9143ea5c9c5df572daa93669fabced37638d8806ba0a5061","cross_cats_sorted":["cs.CE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-06-10T04:50:23Z","title_canon_sha256":"1e9fdd18cc3255fd4c5f890a9a124378a031fa57448975a2f30944272ef80cc3"},"schema_version":"1.0","source":{"id":"2106.05494","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.05494","created_at":"2026-07-05T03:51:28Z"},{"alias_kind":"arxiv_version","alias_value":"2106.05494v2","created_at":"2026-07-05T03:51:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.05494","created_at":"2026-07-05T03:51:28Z"},{"alias_kind":"pith_short_12","alias_value":"GN3TBVYIWNF5","created_at":"2026-07-05T03:51:28Z"},{"alias_kind":"pith_short_16","alias_value":"GN3TBVYIWNF5MOK2","created_at":"2026-07-05T03:51:28Z"},{"alias_kind":"pith_short_8","alias_value":"GN3TBVYI","created_at":"2026-07-05T03:51:28Z"}],"graph_snapshots":[{"event_id":"sha256:f0cdd4c683967c6b97fb008c90abaee51ca2135e7197177bfc83d8a2078c652e","target":"graph","created_at":"2026-07-05T03:51:28Z","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/2106.05494/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Coulomb interaction, following an inverse-square force-law, quantifies the amount of force between two stationary and electrically charged particles. The long-range nature of Coulomb interactions poses a major challenge to molecular dynamics simulations which are major tools for problems at the nano-/micro- scale. Various algorithms are developed to calculate the pairwise Coulomb interactions to a linear scaling but the poor scalability limits the size of simulated systems. Here, we conduct an efficient molecular dynamics algorithm with the random batch Ewald method on all-atom systems where t","authors_text":"Jiuyang Liang, Lei Li, Liang Hong, Pan Tan, Shi Jin, Yue Zhao, Zhenli Xu","cross_cats":["cs.CE"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-06-10T04:50:23Z","title":"Superscalability of the random batch Ewald method"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.05494","kind":"arxiv","version":2},"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:f8b01ba41c47ed752cee4683934801abf9e83ddd6882bff57d640f8506128567","target":"record","created_at":"2026-07-05T03:51:28Z","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":"fbfa3537148bc5bd9143ea5c9c5df572daa93669fabced37638d8806ba0a5061","cross_cats_sorted":["cs.CE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2021-06-10T04:50:23Z","title_canon_sha256":"1e9fdd18cc3255fd4c5f890a9a124378a031fa57448975a2f30944272ef80cc3"},"schema_version":"1.0","source":{"id":"2106.05494","kind":"arxiv","version":2}},"canonical_sha256":"337730d708b34bd6395a7b3b9d2521a6d4661f14abc2ef84f0a5aaac358d5281","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"337730d708b34bd6395a7b3b9d2521a6d4661f14abc2ef84f0a5aaac358d5281","first_computed_at":"2026-07-05T03:51:28.607291Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:51:28.607291Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AzCZ6eYO7VNL2KzhUiUsR9oe5P2cxM/zRyIQRIaHC/ZRjRJRImkM/TMMUuBOWdFU5J3PIDdorhMm3821rmO7Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T03:51:28.608011Z","signed_message":"canonical_sha256_bytes"},"source_id":"2106.05494","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f8b01ba41c47ed752cee4683934801abf9e83ddd6882bff57d640f8506128567","sha256:f0cdd4c683967c6b97fb008c90abaee51ca2135e7197177bfc83d8a2078c652e"],"state_sha256":"5eb84726d296a12f52c0ae5d0de75d805a850c4b9fd1394162f8c3b3d5f20bd1"}