{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:VCMNL5ZAUFBQJUC6GB5RNBA4LR","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":"04580cfb69cfbb9596128af0d58384586a0a9a089fd29fe904140e7d7d5eb59e","cross_cats_sorted":["physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-07T07:11:23Z","title_canon_sha256":"9f3bbd7173cd53d857f5732bd48a351f22d7c4fed87f1c5b5beb1971c91e43de"},"schema_version":"1.0","source":{"id":"1007.1065","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.1065","created_at":"2026-05-18T03:59:37Z"},{"alias_kind":"arxiv_version","alias_value":"1007.1065v1","created_at":"2026-05-18T03:59:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.1065","created_at":"2026-05-18T03:59:37Z"},{"alias_kind":"pith_short_12","alias_value":"VCMNL5ZAUFBQ","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VCMNL5ZAUFBQJUC6","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VCMNL5ZA","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:9c7df20a16dda5d5e6346386c35d9e8e83f070974c86fd8ee2269511c2936f3c","target":"graph","created_at":"2026-05-18T03:59:37Z","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":"We consider the Casimir-Polder potential of particles placed inside a metallic cylindrical cavity at finite temperatures, taking account of thermal non-equilibrium effects. In particular, we study how the resonant (thermal non-equilibrium) potential and transition rates can be enhanced by fine-tuning the radius of the cavity to match the transition wavelength of the dominant transition of the particle. Numerical calculations show that the CP potential acting atoms prepared in low-lying Rydberg states can be enhanced beyond 30 kHz, which is within the range of observability of modern experiment","authors_text":"Simen {\\AA}. Ellingsen, Stefan Scheel, Stefan Yoshi Buhmann","cross_cats":["physics.atom-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-07T07:11:23Z","title":"Casimir-Polder potential and transition rate in resonating cylindrical cavities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.1065","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:dd662ddb1de23ee7b2fc3d5190129156812383afa5f932abe237776d5f38caed","target":"record","created_at":"2026-05-18T03:59:37Z","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":"04580cfb69cfbb9596128af0d58384586a0a9a089fd29fe904140e7d7d5eb59e","cross_cats_sorted":["physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-07T07:11:23Z","title_canon_sha256":"9f3bbd7173cd53d857f5732bd48a351f22d7c4fed87f1c5b5beb1971c91e43de"},"schema_version":"1.0","source":{"id":"1007.1065","kind":"arxiv","version":1}},"canonical_sha256":"a898d5f720a14304d05e307b16841c5c7d06d2513341c60c3793f21324ce5c96","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a898d5f720a14304d05e307b16841c5c7d06d2513341c60c3793f21324ce5c96","first_computed_at":"2026-05-18T03:59:37.012071Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:59:37.012071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sSpgyrbWxpqp4u85VoVDHlYY7zkEmtSfYLNx9e+v6dwtkBGJvA1z+PDIJFxlc14oWEsGaLjDlLkwiHANKj53Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:59:37.012794Z","signed_message":"canonical_sha256_bytes"},"source_id":"1007.1065","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dd662ddb1de23ee7b2fc3d5190129156812383afa5f932abe237776d5f38caed","sha256:9c7df20a16dda5d5e6346386c35d9e8e83f070974c86fd8ee2269511c2936f3c"],"state_sha256":"1ec04d998b09b273dc1f69c2a0e6a08891d7f3c7ddf7a36bbdb55a6920df0923"}