{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:R3GFORRSHPVRS2TZO5K63MZ47H","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":"0dcbea52e72e6c3172162d55afd18fa9b982f9a01bedd47844d116fcc31587cf","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-04-28T12:59:12Z","title_canon_sha256":"c8630a9b294e0c280d4853bdb66c1e6f9ef5740ac7991667392f88e8569922bc"},"schema_version":"1.0","source":{"id":"1504.07456","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1504.07456","created_at":"2026-05-18T02:17:34Z"},{"alias_kind":"arxiv_version","alias_value":"1504.07456v1","created_at":"2026-05-18T02:17:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.07456","created_at":"2026-05-18T02:17:34Z"},{"alias_kind":"pith_short_12","alias_value":"R3GFORRSHPVR","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"R3GFORRSHPVRS2TZ","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"R3GFORRS","created_at":"2026-05-18T12:29:39Z"}],"graph_snapshots":[{"event_id":"sha256:f16051aedd4bd5a72327fdcd595251e85f7e45bf3d69fa375cdcf4363b10b268","target":"graph","created_at":"2026-05-18T02:17:34Z","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":"The response of superconducting pair-breaking detectors is dependent on the details of the quasiparticle distribution. In Kinetic Inductance Detectors (KIDs), where both pair breaking and non-pair breaking photons are absorbed simultaneously, calculating the detector response therefore requires knowledge of the often nonequilibrium distributions. The quasiparticle effective temperature provides a good approximation to these nonequilibrium distributions. We compare an analytical expression relating absorbed power and the quasiparticle effective temperature in superconducting thin films to full ","authors_text":"David J. Goldie, Stafford Withington, Tejas Guruswamy","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-04-28T12:59:12Z","title":"Quasiparticle effective temperature in superconducting thin films illuminated at THz frequencies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.07456","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:c18da90eefff7f94d17141220e0ace56e420a038267ae6a113395aaf458bf203","target":"record","created_at":"2026-05-18T02:17:34Z","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":"0dcbea52e72e6c3172162d55afd18fa9b982f9a01bedd47844d116fcc31587cf","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-04-28T12:59:12Z","title_canon_sha256":"c8630a9b294e0c280d4853bdb66c1e6f9ef5740ac7991667392f88e8569922bc"},"schema_version":"1.0","source":{"id":"1504.07456","kind":"arxiv","version":1}},"canonical_sha256":"8ecc5746323beb196a797755edb33cf9f06256fcad27f6dfc2f699dd9ccafd6e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8ecc5746323beb196a797755edb33cf9f06256fcad27f6dfc2f699dd9ccafd6e","first_computed_at":"2026-05-18T02:17:34.681164Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:17:34.681164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"M7ivTl0v4HhkW3iXOnQ/MSiac6ADtmi1BifAVk3CC9z3a6HCsPfP4UOKjq1EquXhB8+9TLqfIXRWGo0jpBRZDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:17:34.681835Z","signed_message":"canonical_sha256_bytes"},"source_id":"1504.07456","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c18da90eefff7f94d17141220e0ace56e420a038267ae6a113395aaf458bf203","sha256:f16051aedd4bd5a72327fdcd595251e85f7e45bf3d69fa375cdcf4363b10b268"],"state_sha256":"cf48ba1835c9fffbb0e862f032bb0747a61ae1a97ca451ced9545e02d3515707"}