{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:IWCTBF22DUTBBWHG4WDN2YMHLK","short_pith_number":"pith:IWCTBF22","canonical_record":{"source":{"id":"1703.05928","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-17T09:07:13Z","cross_cats_sorted":[],"title_canon_sha256":"c60e1e72ce43a92cef220a82683520f884638c44d2318864dcdcfb9b23755367","abstract_canon_sha256":"72021b8bfcfe08ce61c42e43528d2635d3c9a45c1c168cfa5016acde240af437"},"schema_version":"1.0"},"canonical_sha256":"458530975a1d2610d8e6e586dd61875ab16d42df9e8e47d0d70ced2069774d7f","source":{"kind":"arxiv","id":"1703.05928","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.05928","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"arxiv_version","alias_value":"1703.05928v2","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05928","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"pith_short_12","alias_value":"IWCTBF22DUTB","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IWCTBF22DUTBBWHG","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IWCTBF22","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:IWCTBF22DUTBBWHG4WDN2YMHLK","target":"record","payload":{"canonical_record":{"source":{"id":"1703.05928","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-17T09:07:13Z","cross_cats_sorted":[],"title_canon_sha256":"c60e1e72ce43a92cef220a82683520f884638c44d2318864dcdcfb9b23755367","abstract_canon_sha256":"72021b8bfcfe08ce61c42e43528d2635d3c9a45c1c168cfa5016acde240af437"},"schema_version":"1.0"},"canonical_sha256":"458530975a1d2610d8e6e586dd61875ab16d42df9e8e47d0d70ced2069774d7f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:10.639606Z","signature_b64":"rgZit0V/KXur5aFFM84aSHe9oz9oqCq1xF8itD9SNTm1KFQxQpvbpHk/kX1p3XT42xl5BFHZSoZNpljxxXcoAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"458530975a1d2610d8e6e586dd61875ab16d42df9e8e47d0d70ced2069774d7f","last_reissued_at":"2026-05-18T00:35:10.639205Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:10.639205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.05928","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7NIEHWn4Ko4aHfi6QrwoBje0SfUvhnamy27qw9ci5LWwHVtDKVXPQTqAKeP6HyC6d+UEtrbV6VYHeKIQUc0MAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T07:30:18.306502Z"},"content_sha256":"cd3d8166e99403fb12ac920bfe87b9a4a9858e06de19dbd6a4d24c6bf5bf142f","schema_version":"1.0","event_id":"sha256:cd3d8166e99403fb12ac920bfe87b9a4a9858e06de19dbd6a4d24c6bf5bf142f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:IWCTBF22DUTBBWHG4WDN2YMHLK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Unraveling Mirror Properties in Time-Delayed Quantum Feedback Scenarios","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Alexander Carmele, Fabian M. Faulstich, Manuel Kraft","submitted_at":"2017-03-17T09:07:13Z","abstract_excerpt":"We derive in the Heisenberg picture a widely used phenomenological coupling element to treat feedback effects in quantum optical platforms. Our derivation is based on a microscopic Hamiltonian, which describes the mirror-emitter dynamics based on a dielectric, a mediating fully quantized electromagnetic field, and a single two-level system in front of the dielectric. The dielectric is modeled as a a system of identical two-state atoms. The Heisenberg equation yields a system of describing differential operator equations, which we solve in the Weisskopf-Wigner limit. Due to a finite round-trip "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05928","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C1rgFBpXdX7pD0jhPmVzZ5VAvqU52ezsPSNnnN7RLQ6/AVxSSr6tmIBW7hrM3yKGK3P264gBsm/SK5w4Ad7fCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T07:30:18.306846Z"},"content_sha256":"9c07ad390dfd68ae312d06862a674db5bd10154ec71a057b603b4644dc8340f2","schema_version":"1.0","event_id":"sha256:9c07ad390dfd68ae312d06862a674db5bd10154ec71a057b603b4644dc8340f2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/bundle.json","state_url":"https://pith.science/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T07:30:18Z","links":{"resolver":"https://pith.science/pith/IWCTBF22DUTBBWHG4WDN2YMHLK","bundle":"https://pith.science/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/bundle.json","state":"https://pith.science/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IWCTBF22DUTBBWHG4WDN2YMHLK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:IWCTBF22DUTBBWHG4WDN2YMHLK","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":"72021b8bfcfe08ce61c42e43528d2635d3c9a45c1c168cfa5016acde240af437","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-17T09:07:13Z","title_canon_sha256":"c60e1e72ce43a92cef220a82683520f884638c44d2318864dcdcfb9b23755367"},"schema_version":"1.0","source":{"id":"1703.05928","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.05928","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"arxiv_version","alias_value":"1703.05928v2","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05928","created_at":"2026-05-18T00:35:10Z"},{"alias_kind":"pith_short_12","alias_value":"IWCTBF22DUTB","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IWCTBF22DUTBBWHG","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IWCTBF22","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:9c07ad390dfd68ae312d06862a674db5bd10154ec71a057b603b4644dc8340f2","target":"graph","created_at":"2026-05-18T00:35:10Z","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":"We derive in the Heisenberg picture a widely used phenomenological coupling element to treat feedback effects in quantum optical platforms. Our derivation is based on a microscopic Hamiltonian, which describes the mirror-emitter dynamics based on a dielectric, a mediating fully quantized electromagnetic field, and a single two-level system in front of the dielectric. The dielectric is modeled as a a system of identical two-state atoms. The Heisenberg equation yields a system of describing differential operator equations, which we solve in the Weisskopf-Wigner limit. Due to a finite round-trip ","authors_text":"Alexander Carmele, Fabian M. Faulstich, Manuel Kraft","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-17T09:07:13Z","title":"Unraveling Mirror Properties in Time-Delayed Quantum Feedback Scenarios"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05928","kind":"arxiv","version":2},"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:cd3d8166e99403fb12ac920bfe87b9a4a9858e06de19dbd6a4d24c6bf5bf142f","target":"record","created_at":"2026-05-18T00:35:10Z","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":"72021b8bfcfe08ce61c42e43528d2635d3c9a45c1c168cfa5016acde240af437","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-17T09:07:13Z","title_canon_sha256":"c60e1e72ce43a92cef220a82683520f884638c44d2318864dcdcfb9b23755367"},"schema_version":"1.0","source":{"id":"1703.05928","kind":"arxiv","version":2}},"canonical_sha256":"458530975a1d2610d8e6e586dd61875ab16d42df9e8e47d0d70ced2069774d7f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"458530975a1d2610d8e6e586dd61875ab16d42df9e8e47d0d70ced2069774d7f","first_computed_at":"2026-05-18T00:35:10.639205Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:10.639205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rgZit0V/KXur5aFFM84aSHe9oz9oqCq1xF8itD9SNTm1KFQxQpvbpHk/kX1p3XT42xl5BFHZSoZNpljxxXcoAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:10.639606Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.05928","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd3d8166e99403fb12ac920bfe87b9a4a9858e06de19dbd6a4d24c6bf5bf142f","sha256:9c07ad390dfd68ae312d06862a674db5bd10154ec71a057b603b4644dc8340f2"],"state_sha256":"b446e2926390d8781986849e77aa1bb6babb2b5bc4447b055c0b5bd6f4387c66"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Cv80oUF66YXji2fBuX4hxG/iPlgODJYSdzwIRhjESiyjV1L8fYphe/nhLDfloBy80aBaNmvdNXJNmNgaFW4dAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T07:30:18.308924Z","bundle_sha256":"6c4f9486630c64031697c28a6133307a5e0293fdb5844328c25186aebb114f33"}}