{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PCMTDQJFK34RTSMZ47OLB5XSUK","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ab9c531ca8f3107aec56e97c2f16736a338f5695981f6209ce612995a1e03035","cross_cats_sorted":["cs.LG","physics.ao-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"stat.ML","submitted_at":"2026-07-13T18:00:05Z","title_canon_sha256":"2f75dc3ce0bfda98e7ca663e3d162effa41b7557d9e38637f9fdc92fef5dadcb"},"schema_version":"1.0","source":{"id":"2607.18298","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.18298","created_at":"2026-07-22T00:22:40Z"},{"alias_kind":"arxiv_version","alias_value":"2607.18298v1","created_at":"2026-07-22T00:22:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.18298","created_at":"2026-07-22T00:22:40Z"},{"alias_kind":"pith_short_12","alias_value":"PCMTDQJFK34R","created_at":"2026-07-22T00:22:40Z"},{"alias_kind":"pith_short_16","alias_value":"PCMTDQJFK34RTSMZ","created_at":"2026-07-22T00:22:40Z"},{"alias_kind":"pith_short_8","alias_value":"PCMTDQJF","created_at":"2026-07-22T00:22:40Z"}],"graph_snapshots":[{"event_id":"sha256:0de4085d89f7200482cc7153808b3bbcd6bcfb608f9a0da9ba77eba95131b259","target":"graph","created_at":"2026-07-22T00:22:40Z","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/2607.18298/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We show that a single climate realization can be decomposed into forced and internal components by treating external forcing as a dynamical driver within a linear stochastic system, an idea grounded in pullback attractor theory. In doing so, we address a central methodological challenge in climate science with direct implications for climate projection and the detection and attribution of the forced response, disentangling the forced climate response from internal variability in a single observed record. Statistical methods range from approaches trained on large ensembles to techniques operati","authors_text":"Andrei Gavrilov, Gustau Camps-Valls, Nathan Mankovich","cross_cats":["cs.LG","physics.ao-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"stat.ML","submitted_at":"2026-07-13T18:00:05Z","title":"Disentangling Forced and Internal Climate Variability in Single Realizations using Dynamic Mode Decomposition with Control"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.18298","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":"sha256:261b75ffbe7b5cf3dacf7d2e6a7c10a829c35b48fa3501d2d6246fab86f7e629","target":"record","created_at":"2026-07-22T00:22:40Z","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":"ab9c531ca8f3107aec56e97c2f16736a338f5695981f6209ce612995a1e03035","cross_cats_sorted":["cs.LG","physics.ao-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"stat.ML","submitted_at":"2026-07-13T18:00:05Z","title_canon_sha256":"2f75dc3ce0bfda98e7ca663e3d162effa41b7557d9e38637f9fdc92fef5dadcb"},"schema_version":"1.0","source":{"id":"2607.18298","kind":"arxiv","version":1}},"canonical_sha256":"789931c12556f919c999e7dcb0f6f2a283b4a021d01bc8c31ed67ec9655289eb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"789931c12556f919c999e7dcb0f6f2a283b4a021d01bc8c31ed67ec9655289eb","first_computed_at":"2026-07-22T00:22:40.632556Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-22T00:22:40.632556Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fZxo4UGWtSOF9LRxFO7N/HwFF/APeASqnR417T4mEO5fajEo3AiX8BE9HDzKtEnY2L+/DpRYLjIfWVDmeYNGAQ==","signature_status":"signed_v1","signed_at":"2026-07-22T00:22:40.633374Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.18298","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:261b75ffbe7b5cf3dacf7d2e6a7c10a829c35b48fa3501d2d6246fab86f7e629","sha256:0de4085d89f7200482cc7153808b3bbcd6bcfb608f9a0da9ba77eba95131b259","sha256:9e5e5999edb38b3f6998d319946bd64979044e4d74088ac0b5d5d18e0a872020"],"state_sha256":"105295cd3088cdbba2b950763c37b0bfb9ee06841c373b39f8afc9ab5a6d5737"}