{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:SPHLR2FBRAHS6ROY6XSIXWEEHJ","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":"aac40ddfd6620fb87f0e81fe6d893365416d896f2455002acc58c90fb99cc22d","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-07-14T17:11:18Z","title_canon_sha256":"54d566788a8ae78a4ae0ed00c517c5a2c7d16b9ff713840b45f198e322f7f291"},"schema_version":"1.0","source":{"id":"2507.10645","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.10645","created_at":"2026-07-05T11:36:57Z"},{"alias_kind":"arxiv_version","alias_value":"2507.10645v1","created_at":"2026-07-05T11:36:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.10645","created_at":"2026-07-05T11:36:57Z"},{"alias_kind":"pith_short_12","alias_value":"SPHLR2FBRAHS","created_at":"2026-07-05T11:36:57Z"},{"alias_kind":"pith_short_16","alias_value":"SPHLR2FBRAHS6ROY","created_at":"2026-07-05T11:36:57Z"},{"alias_kind":"pith_short_8","alias_value":"SPHLR2FB","created_at":"2026-07-05T11:36:57Z"}],"graph_snapshots":[{"event_id":"sha256:277914c5c9a314379f4cb24d2bac4bfec2be9838f644ddcc4a9ca0dd891d13f2","target":"graph","created_at":"2026-07-05T11:36:57Z","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/2507.10645/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Connecting plasma processing parameters to the resultant film microstructure remains a fundamental challenge in materials synthesis, one that has largely confined process design to empirical approaches. To bridge this gap, we develop a predictive analysis of coupling by applying a renormalization group (RG) analysis to an effective Hamiltonian for the stochastic dynamics of the plasma-surface interface, derived systematically from microscopic principles. The central result from this formalism is the system's exhibition of asymptotic freedom; the effective dimensionless coupling, $g$, between t","authors_text":"Hasitha Mahabaduge, Joel Saucedo, Uday Lamba","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-07-14T17:11:18Z","title":"Scaling Relations, Morphological Stability, and Asymptotic Freedom of Plasma-Surface Deposition Dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.10645","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:c622dc1bbc8ea52a8f469875535c63c0796bef66175e64864da4513e7b6e9187","target":"record","created_at":"2026-07-05T11:36:57Z","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":"aac40ddfd6620fb87f0e81fe6d893365416d896f2455002acc58c90fb99cc22d","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-07-14T17:11:18Z","title_canon_sha256":"54d566788a8ae78a4ae0ed00c517c5a2c7d16b9ff713840b45f198e322f7f291"},"schema_version":"1.0","source":{"id":"2507.10645","kind":"arxiv","version":1}},"canonical_sha256":"93ceb8e8a1880f2f45d8f5e48bd8843a7d1b1505b7f2c0d4e365dd8ed38d6182","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"93ceb8e8a1880f2f45d8f5e48bd8843a7d1b1505b7f2c0d4e365dd8ed38d6182","first_computed_at":"2026-07-05T11:36:57.993112Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:36:57.993112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h7UmPQuQfJWEwl+DqZZiB6YZ8+R9AJZrJ3l6oo0dOOns6149MTGMD6AumxQqovYND8Ev8B6eVRmji90vxXmvAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:36:57.993581Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.10645","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c622dc1bbc8ea52a8f469875535c63c0796bef66175e64864da4513e7b6e9187","sha256:277914c5c9a314379f4cb24d2bac4bfec2be9838f644ddcc4a9ca0dd891d13f2"],"state_sha256":"6951b24095f3dec9c2f2d26299e22993535da89b52441098d5c8615417ee8380"}