{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:WF2RFWRKGYX4HN4ZIOYWC7UKWD","short_pith_number":"pith:WF2RFWRK","canonical_record":{"source":{"id":"1701.07935","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-01-27T03:44:34Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"title_canon_sha256":"4d73f86784649e7314a0eff280cdf8ad709ce0e98c6adfd6222dfbf310543b69","abstract_canon_sha256":"78c95da6443c0f3f0e9df7ec979aac69c818c19798fe091f259139346021c6fb"},"schema_version":"1.0"},"canonical_sha256":"b17512da2a362fc3b79943b1617e8ab0dbc9cb6697ce4538f932d4441e9bbc3b","source":{"kind":"arxiv","id":"1701.07935","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.07935","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"arxiv_version","alias_value":"1701.07935v3","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.07935","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"pith_short_12","alias_value":"WF2RFWRKGYX4","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WF2RFWRKGYX4HN4Z","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WF2RFWRK","created_at":"2026-05-18T12:31:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:WF2RFWRKGYX4HN4ZIOYWC7UKWD","target":"record","payload":{"canonical_record":{"source":{"id":"1701.07935","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-01-27T03:44:34Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"title_canon_sha256":"4d73f86784649e7314a0eff280cdf8ad709ce0e98c6adfd6222dfbf310543b69","abstract_canon_sha256":"78c95da6443c0f3f0e9df7ec979aac69c818c19798fe091f259139346021c6fb"},"schema_version":"1.0"},"canonical_sha256":"b17512da2a362fc3b79943b1617e8ab0dbc9cb6697ce4538f932d4441e9bbc3b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:36.042955Z","signature_b64":"mg7gfYioW8tknqTNSWRXVDXt5TbQm1p4QHfFpB/5/tYWxMPukNOWMwPrTU+OAsrnZzFYFJXuvHQPaZB/xTF9BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b17512da2a362fc3b79943b1617e8ab0dbc9cb6697ce4538f932d4441e9bbc3b","last_reissued_at":"2026-05-18T00:37:36.042305Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:36.042305Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1701.07935","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NijS5Sl6lJWoPTJjvLSGS1ViLmyAVLPNyuTzdpNE9KcW41orpsqyb1k0RsUwEjN/GFRXwrFW9ouXyWsb1W8wAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:19:49.539137Z"},"content_sha256":"94e6ffbbf7887a2876409ff9abd1d130f7d55bccbbc8f71044e1da910a4f1516","schema_version":"1.0","event_id":"sha256:94e6ffbbf7887a2876409ff9abd1d130f7d55bccbbc8f71044e1da910a4f1516"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:WF2RFWRKGYX4HN4ZIOYWC7UKWD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Cutoff-free Circuit Quantum Electrodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"primary_cat":"quant-ph","authors_text":"Alexandru Petrescu, Hakan E. T\\\"ureci, Moein Malekakhlagh","submitted_at":"2017-01-27T03:44:34Z","abstract_excerpt":"Any quantum-confined electronic system coupled to the electromagnetic continuum is subject to radiative decay and renormalization of its energy levels. When coupled to a cavity, these quantities can be strongly modified with respect to their values in vacuum. Generally, this modification can be accurately captured by including only the closest resonant mode of the cavity. In the circuit quantum electrodynamics architecture, where the coupling strengths can be substantial, it is however found that the radiative decay rates are strongly influenced by far off-resonant modes. A multimode calculati"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.07935","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+O+HxXvuGfZEdQDhZxvmeIgtRnPodV/RMJFYSewVLcX+S/8xHjKCUTgN89JhpWtYcXzg64RL8pBNtp0QM65/DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:19:49.539863Z"},"content_sha256":"43710be767b32d6f764f8ab14b3424ae40ed55a6838fbc69eac25f9be87b61a5","schema_version":"1.0","event_id":"sha256:43710be767b32d6f764f8ab14b3424ae40ed55a6838fbc69eac25f9be87b61a5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/bundle.json","state_url":"https://pith.science/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/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":"2026-05-25T19:19:49Z","links":{"resolver":"https://pith.science/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD","bundle":"https://pith.science/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/bundle.json","state":"https://pith.science/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WF2RFWRKGYX4HN4ZIOYWC7UKWD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:WF2RFWRKGYX4HN4ZIOYWC7UKWD","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":"78c95da6443c0f3f0e9df7ec979aac69c818c19798fe091f259139346021c6fb","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-01-27T03:44:34Z","title_canon_sha256":"4d73f86784649e7314a0eff280cdf8ad709ce0e98c6adfd6222dfbf310543b69"},"schema_version":"1.0","source":{"id":"1701.07935","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.07935","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"arxiv_version","alias_value":"1701.07935v3","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.07935","created_at":"2026-05-18T00:37:36Z"},{"alias_kind":"pith_short_12","alias_value":"WF2RFWRKGYX4","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WF2RFWRKGYX4HN4Z","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WF2RFWRK","created_at":"2026-05-18T12:31:53Z"}],"graph_snapshots":[{"event_id":"sha256:43710be767b32d6f764f8ab14b3424ae40ed55a6838fbc69eac25f9be87b61a5","target":"graph","created_at":"2026-05-18T00:37:36Z","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":"Any quantum-confined electronic system coupled to the electromagnetic continuum is subject to radiative decay and renormalization of its energy levels. When coupled to a cavity, these quantities can be strongly modified with respect to their values in vacuum. Generally, this modification can be accurately captured by including only the closest resonant mode of the cavity. In the circuit quantum electrodynamics architecture, where the coupling strengths can be substantial, it is however found that the radiative decay rates are strongly influenced by far off-resonant modes. A multimode calculati","authors_text":"Alexandru Petrescu, Hakan E. T\\\"ureci, Moein Malekakhlagh","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-01-27T03:44:34Z","title":"Cutoff-free Circuit Quantum Electrodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.07935","kind":"arxiv","version":3},"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":"sha256:94e6ffbbf7887a2876409ff9abd1d130f7d55bccbbc8f71044e1da910a4f1516","target":"record","created_at":"2026-05-18T00:37:36Z","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":"78c95da6443c0f3f0e9df7ec979aac69c818c19798fe091f259139346021c6fb","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-01-27T03:44:34Z","title_canon_sha256":"4d73f86784649e7314a0eff280cdf8ad709ce0e98c6adfd6222dfbf310543b69"},"schema_version":"1.0","source":{"id":"1701.07935","kind":"arxiv","version":3}},"canonical_sha256":"b17512da2a362fc3b79943b1617e8ab0dbc9cb6697ce4538f932d4441e9bbc3b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b17512da2a362fc3b79943b1617e8ab0dbc9cb6697ce4538f932d4441e9bbc3b","first_computed_at":"2026-05-18T00:37:36.042305Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:36.042305Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mg7gfYioW8tknqTNSWRXVDXt5TbQm1p4QHfFpB/5/tYWxMPukNOWMwPrTU+OAsrnZzFYFJXuvHQPaZB/xTF9BA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:36.042955Z","signed_message":"canonical_sha256_bytes"},"source_id":"1701.07935","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:94e6ffbbf7887a2876409ff9abd1d130f7d55bccbbc8f71044e1da910a4f1516","sha256:43710be767b32d6f764f8ab14b3424ae40ed55a6838fbc69eac25f9be87b61a5"],"state_sha256":"4754fe8840816301fb521e83fe17e5bfbd58c94b40e6a4a557c0e438edb1b462"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bLGrnPLry1ncL+309cwyGnhZq2N38Ook9gKCEFHXiOC2QHJZpu/iapHJjETPw2rXSHY/0O5sUlYcgiwRJ84LBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T19:19:49.543943Z","bundle_sha256":"d92353c247efc6b6a0c0c43b15fd95d824d6965bb057f5cf6c5f9fba0c02132a"}}