{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:OCN2RJPZYIKOQBYFK6OPLZRYMC","short_pith_number":"pith:OCN2RJPZ","schema_version":"1.0","canonical_sha256":"709ba8a5f9c214e80705579cf5e638609bba7f293cdc3e4db5a0992f3e6095f4","source":{"kind":"arxiv","id":"1305.2488","version":3},"attestation_state":"computed","paper":{"title":"QED with a parabolic mirror","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"G. Alber, G. Leuchs, J. Z. Bern\\'ad, L.L.S\\'anchez-Soto, M. Stobi\\'nska","submitted_at":"2013-05-11T09:48:50Z","abstract_excerpt":"We investigate the quantum electrodynamics of a single two-level atom located at the focus of a parabolic cavity. We first work out the modifications of the spontaneous emission induced by the presence of this boundary in the optical regime, where the dipole and the rotating-wave approximations apply. Furthermore, the single-photon state that leaves the cavity asymptotically is determined. The corresponding time-reversed single-photon quantum state is capable of exciting the atom in this extreme multimode scenario with near-unit probability. Using semiclassical methods, we derive a photon-path"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1305.2488","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-05-11T09:48:50Z","cross_cats_sorted":[],"title_canon_sha256":"4cd3fd29bbe1ea93e109a012cd7cc14aa90b522f28d0206b5477054e41dd8e44","abstract_canon_sha256":"83075c890de008c6dc6ac84efa0aa63078434cb90bdb4825e61c0627c4a04da3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:15:55.601943Z","signature_b64":"CvJV1shybmjROHP5IpVsmt/VhO5aTzRG2yrJkP8bOwiz3V/uHZR9/faiXfAdVraMwfEIeuKYoI1caEN+/PadAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"709ba8a5f9c214e80705579cf5e638609bba7f293cdc3e4db5a0992f3e6095f4","last_reissued_at":"2026-05-18T03:15:55.601059Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:15:55.601059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QED with a parabolic mirror","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"G. Alber, G. Leuchs, J. Z. Bern\\'ad, L.L.S\\'anchez-Soto, M. Stobi\\'nska","submitted_at":"2013-05-11T09:48:50Z","abstract_excerpt":"We investigate the quantum electrodynamics of a single two-level atom located at the focus of a parabolic cavity. We first work out the modifications of the spontaneous emission induced by the presence of this boundary in the optical regime, where the dipole and the rotating-wave approximations apply. Furthermore, the single-photon state that leaves the cavity asymptotically is determined. The corresponding time-reversed single-photon quantum state is capable of exciting the atom in this extreme multimode scenario with near-unit probability. Using semiclassical methods, we derive a photon-path"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.2488","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1305.2488","created_at":"2026-05-18T03:15:55.601211+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.2488v3","created_at":"2026-05-18T03:15:55.601211+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.2488","created_at":"2026-05-18T03:15:55.601211+00:00"},{"alias_kind":"pith_short_12","alias_value":"OCN2RJPZYIKO","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"OCN2RJPZYIKOQBYF","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"OCN2RJPZ","created_at":"2026-05-18T12:27:54.935989+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC","json":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC.json","graph_json":"https://pith.science/api/pith-number/OCN2RJPZYIKOQBYFK6OPLZRYMC/graph.json","events_json":"https://pith.science/api/pith-number/OCN2RJPZYIKOQBYFK6OPLZRYMC/events.json","paper":"https://pith.science/paper/OCN2RJPZ"},"agent_actions":{"view_html":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC","download_json":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC.json","view_paper":"https://pith.science/paper/OCN2RJPZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.2488&json=true","fetch_graph":"https://pith.science/api/pith-number/OCN2RJPZYIKOQBYFK6OPLZRYMC/graph.json","fetch_events":"https://pith.science/api/pith-number/OCN2RJPZYIKOQBYFK6OPLZRYMC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC/action/storage_attestation","attest_author":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC/action/author_attestation","sign_citation":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC/action/citation_signature","submit_replication":"https://pith.science/pith/OCN2RJPZYIKOQBYFK6OPLZRYMC/action/replication_record"}},"created_at":"2026-05-18T03:15:55.601211+00:00","updated_at":"2026-05-18T03:15:55.601211+00:00"}