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H. Dicke, Coherence in spontaneous radiation processes, Phys. Rev.93, 99 (1954)","work_id":"5905f19c-0b04-4972-a708-b575c815f22f","year":1954}],"snapshot_sha256":"1d36833ae59a14bef0e18ecfbec22b0f364b992a1644bbf85344e296a0891e95"},"source":{"id":"2510.13671","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-18T07:06:34.283044Z","id":"ad359af5-16db-42a5-a5e7-89f702745db4","model_set":{"reader":"grok-4.3"},"one_line_summary":"Superradiant emission remains asymptotically robust to strong disorder in waveguide QED arrays because atoms spontaneously self-organize their spin states to optimize constructive interference.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The hallmark N squared scaling of superradiant emission remains asymptotically robust to strong spatial and spectral disorder in a one-dimensional waveguide.","strongest_claim":"the key signature of superradiance remains asymptotically robust under strong spatial and spectral disorder, but also exhibits subtle finite-size scaling toward this limit","weakest_assumption":"The semiclassical approximation used in the large-scale simulations accurately captures the collective decay dynamics even under strong disorder, without significant quantum corrections that would alter the observed robustness or ordering."}},"verdict_id":"ad359af5-16db-42a5-a5e7-89f702745db4"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:cdd6beb8615ecb0732cd824f56670677da741c894afecda21338c72edeeda0de","target":"record","created_at":"2026-07-14T02:21:23Z","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":"e371796cac924a1f490e30c79ef6e25899b7a6a14b027614cbabbe2b1c38542d","cross_cats_sorted":["physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-10-15T15:30:30Z","title_canon_sha256":"704c573e80ef5fbc8d2815d381d0282fd882f565e42a99b7ac44570df1a70f9b"},"schema_version":"1.0","source":{"id":"2510.13671","kind":"arxiv","version":3}},"canonical_sha256":"a8ee9f3d49d8aaa94dd2e34ddff6b6e548bcd70b972a36b9827cc31310fffb8d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a8ee9f3d49d8aaa94dd2e34ddff6b6e548bcd70b972a36b9827cc31310fffb8d","first_computed_at":"2026-07-14T02:21:23.912293Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-14T02:21:23.912293Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f63bYUxxY05zChUmEQSoB9CRoScH53Ybv8BKm+sWk8OaHVCS7u5vvoDwTJWNZTn20+BWn7OI3MmttkTBvJMABw==","signature_status":"signed_v1","signed_at":"2026-07-14T02:21:23.913206Z","signed_message":"canonical_sha256_bytes"},"source_id":"2510.13671","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cdd6beb8615ecb0732cd824f56670677da741c894afecda21338c72edeeda0de","sha256:1dc3fefe7fa6e3ecff922ed62fb9b8659f4e1f979ba4d922afee998fe0b10a27"],"state_sha256":"a368cef82cd15ea50199d2578fd742f9cfa590b65bb54809d43540b209e5753b"}