{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:YJDZH4QSTIZDMCMXGV5Q2J7A37","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":"8c9720a0c2a0d91fb4628104f5c5dbcf175013fe51f2d8952b6a13d336dd5c22","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-01-16T16:03:03Z","title_canon_sha256":"8a3ee26ed8b3e7e74d0bfb0b3ed29ffac0e48b9c0021afbd302f0754d53e25e1"},"schema_version":"1.0","source":{"id":"2601.11391","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2601.11391","created_at":"2026-07-01T01:17:45Z"},{"alias_kind":"arxiv_version","alias_value":"2601.11391v2","created_at":"2026-07-01T01:17:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2601.11391","created_at":"2026-07-01T01:17:45Z"},{"alias_kind":"pith_short_12","alias_value":"YJDZH4QSTIZD","created_at":"2026-07-01T01:17:45Z"},{"alias_kind":"pith_short_16","alias_value":"YJDZH4QSTIZDMCMX","created_at":"2026-07-01T01:17:45Z"},{"alias_kind":"pith_short_8","alias_value":"YJDZH4QS","created_at":"2026-07-01T01:17:45Z"}],"graph_snapshots":[{"event_id":"sha256:efe56febbaee9661368045bd43e046c58f0bc22f97f8d7f9ae7b81145d84340d","target":"graph","created_at":"2026-07-01T01:17:45Z","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/2601.11391/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present NAVIS (NAnochannel Velocity and thermal Interfacial Slip), a LAMMPS-Python scripted toolkit for computing the Navier (hydrodynamic) friction coefficient and Kapitza (thermal) resistance at arbitrary solid-fluid interfaces. NAVIS is based on equilibrium molecular dynamics (EMD) methods for calculating the linear response friction and thermal resistance at the interface, as well as the corresponding velocity and temperature slips. The methodology is based on our previous studies (Hansen, et al., Phys. Rev. E 84, 016313 (2011); Varghese et al., J. Chem. Phys. 154, 184707 (2021); Alosio","authors_text":"Billy Dean Todd, Jesper Schmidt Hansen, Sleeba Varghese, Sobin Alosious","cross_cats":["physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-01-16T16:03:03Z","title":"NAVIS: A LAMMPS-Python framework for efficient computation of nanochannel velocity and thermal interfacial slip"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2601.11391","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":"sha256:05093027f33e3232a9cf9de6c9688f63ff61e67943e0a94ac0a233990ac7da9b","target":"record","created_at":"2026-07-01T01:17:45Z","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":"8c9720a0c2a0d91fb4628104f5c5dbcf175013fe51f2d8952b6a13d336dd5c22","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-01-16T16:03:03Z","title_canon_sha256":"8a3ee26ed8b3e7e74d0bfb0b3ed29ffac0e48b9c0021afbd302f0754d53e25e1"},"schema_version":"1.0","source":{"id":"2601.11391","kind":"arxiv","version":2}},"canonical_sha256":"c24793f2129a32360997357b0d27e0dfdc1d24d9f9ce10a047b2d3360b5f5df7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c24793f2129a32360997357b0d27e0dfdc1d24d9f9ce10a047b2d3360b5f5df7","first_computed_at":"2026-07-01T01:17:45.566183Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-01T01:17:45.566183Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UhG0duJUflgpk92B0o/DHf5qG2TFbG8NV0w0xDptZ/BNpNAyuhKVN1UPhTBHRFo3t7i0MqSOj8g8A1EltdJUAQ==","signature_status":"signed_v1","signed_at":"2026-07-01T01:17:45.566796Z","signed_message":"canonical_sha256_bytes"},"source_id":"2601.11391","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05093027f33e3232a9cf9de6c9688f63ff61e67943e0a94ac0a233990ac7da9b","sha256:efe56febbaee9661368045bd43e046c58f0bc22f97f8d7f9ae7b81145d84340d"],"state_sha256":"a299076bf06baf595a9782af09cb75363acb2f8507202c800b5fcdd8931a52a0"}