{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:473OMSAEQCRPXNB7OMJRKPZD56","short_pith_number":"pith:473OMSAE","canonical_record":{"source":{"id":"1707.05946","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-07-19T06:17:13Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"ae31cbf151e694b2191c9a3ce4a46e536d68dc9488e1c7313cb05f85ba3709aa","abstract_canon_sha256":"99b476951fc71c55cfb116ea95698f680117a49e9c743b6e5cb7cbe0e358b523"},"schema_version":"1.0"},"canonical_sha256":"e7f6e6480480a2fbb43f7313153f23efb6b70c92abb71afc34f62fff3108f452","source":{"kind":"arxiv","id":"1707.05946","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.05946","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"arxiv_version","alias_value":"1707.05946v2","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05946","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"pith_short_12","alias_value":"473OMSAEQCRP","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"473OMSAEQCRPXNB7","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"473OMSAE","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:473OMSAEQCRPXNB7OMJRKPZD56","target":"record","payload":{"canonical_record":{"source":{"id":"1707.05946","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-07-19T06:17:13Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"ae31cbf151e694b2191c9a3ce4a46e536d68dc9488e1c7313cb05f85ba3709aa","abstract_canon_sha256":"99b476951fc71c55cfb116ea95698f680117a49e9c743b6e5cb7cbe0e358b523"},"schema_version":"1.0"},"canonical_sha256":"e7f6e6480480a2fbb43f7313153f23efb6b70c92abb71afc34f62fff3108f452","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:31.701751Z","signature_b64":"Kkj8QNmTDOxOvZNJ2FjOM2QvWRWzf4fyZW6ZYguK7KvatQn8tslVWSKDlO3h8UfipcEQui5OEl4qlJ8KG2AQDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7f6e6480480a2fbb43f7313153f23efb6b70c92abb71afc34f62fff3108f452","last_reissued_at":"2026-05-18T00:18:31.701275Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:31.701275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.05946","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":"2026-05-18T00:18:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XYwr3z/DUhj917CTj3sJf3AF4nKsbg8M8UGc7X3RaCjzdMPasXwPB6xNE3sBP35psJ2Rmh+JBJEFxiqcxDJtDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T08:18:17.431455Z"},"content_sha256":"390535fd4234205fec48a1d6b6e869033910e7c145dcadfb6142a355bed8db63","schema_version":"1.0","event_id":"sha256:390535fd4234205fec48a1d6b6e869033910e7c145dcadfb6142a355bed8db63"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:473OMSAEQCRPXNB7OMJRKPZD56","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-Markovian Dynamics of a Qubit Due to Single-Photon Scattering in a Waveguide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"quant-ph","authors_text":"Francesco Ciccarello, Harold U. Baranger, Yao-Lung L. Fang","submitted_at":"2017-07-19T06:17:13Z","abstract_excerpt":"We investigate the open dynamics of a qubit due to scattering of a single photon in an infinite or semi-infinite waveguide. Through an exact solution of the time-dependent multi-photon scattering problem, we find the qubit's dynamical map. Tools of open quantum systems theory allow us then to discuss the general features of this map, find the corresponding non-Linbladian master equation, and assess in a rigorous way its non-Markovian nature. The qubit dynamics has distinctive features that, in particular, do not occur in emission processes. Two fundamental sources of non-Markovianity are prese"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05946","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":"2026-05-18T00:18:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rLQuUF0Mwo2zdLFmOpt0Ilcy7bCQQm2JlqY1o+Ykbu9ZXNC6B5AmG45BSnPn/p22To6ZIzIqM4yOsNJwoHp6Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T08:18:17.431805Z"},"content_sha256":"384aaa71650d122e0ee909f3842f8e1373e9aaa3ba8a20b3699014e15f43c356","schema_version":"1.0","event_id":"sha256:384aaa71650d122e0ee909f3842f8e1373e9aaa3ba8a20b3699014e15f43c356"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/473OMSAEQCRPXNB7OMJRKPZD56/bundle.json","state_url":"https://pith.science/pith/473OMSAEQCRPXNB7OMJRKPZD56/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/473OMSAEQCRPXNB7OMJRKPZD56/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":"2026-05-31T08:18:17Z","links":{"resolver":"https://pith.science/pith/473OMSAEQCRPXNB7OMJRKPZD56","bundle":"https://pith.science/pith/473OMSAEQCRPXNB7OMJRKPZD56/bundle.json","state":"https://pith.science/pith/473OMSAEQCRPXNB7OMJRKPZD56/state.json","well_known_bundle":"https://pith.science/.well-known/pith/473OMSAEQCRPXNB7OMJRKPZD56/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:473OMSAEQCRPXNB7OMJRKPZD56","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":"99b476951fc71c55cfb116ea95698f680117a49e9c743b6e5cb7cbe0e358b523","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-07-19T06:17:13Z","title_canon_sha256":"ae31cbf151e694b2191c9a3ce4a46e536d68dc9488e1c7313cb05f85ba3709aa"},"schema_version":"1.0","source":{"id":"1707.05946","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.05946","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"arxiv_version","alias_value":"1707.05946v2","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05946","created_at":"2026-05-18T00:18:31Z"},{"alias_kind":"pith_short_12","alias_value":"473OMSAEQCRP","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"473OMSAEQCRPXNB7","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"473OMSAE","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:384aaa71650d122e0ee909f3842f8e1373e9aaa3ba8a20b3699014e15f43c356","target":"graph","created_at":"2026-05-18T00:18:31Z","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 investigate the open dynamics of a qubit due to scattering of a single photon in an infinite or semi-infinite waveguide. Through an exact solution of the time-dependent multi-photon scattering problem, we find the qubit's dynamical map. Tools of open quantum systems theory allow us then to discuss the general features of this map, find the corresponding non-Linbladian master equation, and assess in a rigorous way its non-Markovian nature. The qubit dynamics has distinctive features that, in particular, do not occur in emission processes. Two fundamental sources of non-Markovianity are prese","authors_text":"Francesco Ciccarello, Harold U. Baranger, Yao-Lung L. Fang","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-07-19T06:17:13Z","title":"Non-Markovian Dynamics of a Qubit Due to Single-Photon Scattering in a Waveguide"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05946","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":"sha256:390535fd4234205fec48a1d6b6e869033910e7c145dcadfb6142a355bed8db63","target":"record","created_at":"2026-05-18T00:18:31Z","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":"99b476951fc71c55cfb116ea95698f680117a49e9c743b6e5cb7cbe0e358b523","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-07-19T06:17:13Z","title_canon_sha256":"ae31cbf151e694b2191c9a3ce4a46e536d68dc9488e1c7313cb05f85ba3709aa"},"schema_version":"1.0","source":{"id":"1707.05946","kind":"arxiv","version":2}},"canonical_sha256":"e7f6e6480480a2fbb43f7313153f23efb6b70c92abb71afc34f62fff3108f452","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e7f6e6480480a2fbb43f7313153f23efb6b70c92abb71afc34f62fff3108f452","first_computed_at":"2026-05-18T00:18:31.701275Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:31.701275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Kkj8QNmTDOxOvZNJ2FjOM2QvWRWzf4fyZW6ZYguK7KvatQn8tslVWSKDlO3h8UfipcEQui5OEl4qlJ8KG2AQDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:31.701751Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.05946","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:390535fd4234205fec48a1d6b6e869033910e7c145dcadfb6142a355bed8db63","sha256:384aaa71650d122e0ee909f3842f8e1373e9aaa3ba8a20b3699014e15f43c356"],"state_sha256":"2c12f68b0c7ca43d072be380dab1da4a264b768b9af7c76ae48c231c841fef90"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4XiV3HPXfQMd0kJ6UEQP26o/cLNBiFEWT3qJeRxLPX8Xg10a9659PzIcml52Or8OLuzzkzFyFeL1RchMmygdCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T08:18:17.434056Z","bundle_sha256":"8b856729e29e2a6589505f7ee0bb3814ffc328cab6b69dc631a33f26809741f1"}}