{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:FEPICPB5WEYXV7PJARTCIDYM3R","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":"2db7854251bf80282dae668933eedcbd9c30a58df3283b7cd84d4548f4c271c8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-01-01T00:15:13Z","title_canon_sha256":"ba681a437cb6081e26feb5c1f9b6355ab96bd6a4f524f5b177a6efb1f509eba5"},"schema_version":"1.0","source":{"id":"1801.00376","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.00376","created_at":"2026-05-18T00:08:10Z"},{"alias_kind":"arxiv_version","alias_value":"1801.00376v1","created_at":"2026-05-18T00:08:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.00376","created_at":"2026-05-18T00:08:10Z"},{"alias_kind":"pith_short_12","alias_value":"FEPICPB5WEYX","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_16","alias_value":"FEPICPB5WEYXV7PJ","created_at":"2026-05-18T12:32:22Z"},{"alias_kind":"pith_short_8","alias_value":"FEPICPB5","created_at":"2026-05-18T12:32:22Z"}],"graph_snapshots":[{"event_id":"sha256:27e458a65ecbe5eb3d438ad1369edd0117d23faaa7d8c218d2ea199f5aa69edb","target":"graph","created_at":"2026-05-18T00:08:10Z","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"},"paper":{"abstract_excerpt":"Thermal runaway occurs when a rise in system temperature results in heat generation rates exceeding dissipation rates. Here we demonstrate that thermal runaway occurs in thermal radiative systems, given a sufficient level of negative differential thermal emission. By exploiting the insulator-to-metal phase transition of vanadium dioxide, we show that a small increase in heat generation (e.g., 10 nW/mm2) can result in a large change in surface temperature (e.g., ~35 K), as the thermal emitter switches from high emissivity to low emissivity. While thermal runaway is typically associated with cat","authors_text":"Andrej Lenert, David M. Bierman, Evelyn N. Wang, Federico Capasso, Matthew De La Ossa, Mikhail A. Kats, Shriram Ramanathan, Shuyan Zhang, You Zhou","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-01-01T00:15:13Z","title":"Radiative thermal runaway due to negative differential thermal emission across a solid-solid phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.00376","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":"sha256:55d94cd6976ceb6b904b822a8a25ba855b581727b72839a235f3dd66eb565fa6","target":"record","created_at":"2026-05-18T00:08:10Z","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":"2db7854251bf80282dae668933eedcbd9c30a58df3283b7cd84d4548f4c271c8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-01-01T00:15:13Z","title_canon_sha256":"ba681a437cb6081e26feb5c1f9b6355ab96bd6a4f524f5b177a6efb1f509eba5"},"schema_version":"1.0","source":{"id":"1801.00376","kind":"arxiv","version":1}},"canonical_sha256":"291e813c3db1317afde90466240f0cdc7c2c3376c0f7f2afce6706596ae22c3a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"291e813c3db1317afde90466240f0cdc7c2c3376c0f7f2afce6706596ae22c3a","first_computed_at":"2026-05-18T00:08:10.684737Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:08:10.684737Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"D52/RJaLKYJuYcGqr0qTlBFYNc7Fh5GtT+lz6jCfI5L3QP1r9m7jZxx1SfxnetCiEuhH9Yvo2nlYZDfp86yuAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:08:10.685129Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.00376","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:55d94cd6976ceb6b904b822a8a25ba855b581727b72839a235f3dd66eb565fa6","sha256:27e458a65ecbe5eb3d438ad1369edd0117d23faaa7d8c218d2ea199f5aa69edb"],"state_sha256":"c02400d9b37edcc3518743daf877c6c9e27982c5c8f70f298200127602f3fa09"}