{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:A62LWZBBKACBA2GU5ZE6RECVQN","short_pith_number":"pith:A62LWZBB","canonical_record":{"source":{"id":"2605.14395","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T05:20:24Z","cross_cats_sorted":[],"title_canon_sha256":"19f0ed399e1897649e91fdd35ad7ebd411ebd2fa77f1e564defe5c71fb0add3a","abstract_canon_sha256":"0668cda4244c27f9f2fe276eab480f25a2edb01528c592a18aae9e94c99591fb"},"schema_version":"1.0"},"canonical_sha256":"07b4bb642150041068d4ee49e89055837a6942b53884b0f7de773ef6d3fd03ac","source":{"kind":"arxiv","id":"2605.14395","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14395","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14395v1","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14395","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"pith_short_12","alias_value":"A62LWZBBKACB","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"A62LWZBBKACBA2GU","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"A62LWZBB","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:A62LWZBBKACBA2GU5ZE6RECVQN","target":"record","payload":{"canonical_record":{"source":{"id":"2605.14395","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T05:20:24Z","cross_cats_sorted":[],"title_canon_sha256":"19f0ed399e1897649e91fdd35ad7ebd411ebd2fa77f1e564defe5c71fb0add3a","abstract_canon_sha256":"0668cda4244c27f9f2fe276eab480f25a2edb01528c592a18aae9e94c99591fb"},"schema_version":"1.0"},"canonical_sha256":"07b4bb642150041068d4ee49e89055837a6942b53884b0f7de773ef6d3fd03ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:07.565370Z","signature_b64":"5XBhsAX4HuGSnsTBE2u07CuDLQJ8U7UHenwmsePUp3NkdPa0R0FI9fGOyByC3o6Wk/Aol95DDdOrgmn4UbPmDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07b4bb642150041068d4ee49e89055837a6942b53884b0f7de773ef6d3fd03ac","last_reissued_at":"2026-05-17T23:39:07.564718Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:07.564718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.14395","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k/oIFsLX1ubNXFyxt2ZLqGzPAKkQiAvI7Ty7EITavpfWwBbU3eQRRllqhc68z4uLlseiUK7wE7X/CbLIdfqwBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T03:04:33.319698Z"},"content_sha256":"4981cc236115404a22f70969d1a30902ccaca922a523c35f8197152eafd65569","schema_version":"1.0","event_id":"sha256:4981cc236115404a22f70969d1a30902ccaca922a523c35f8197152eafd65569"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:A62LWZBBKACBA2GU5ZE6RECVQN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Interference visibility as a witness of preparation contextuality via overlap inequalities","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities.","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Mohd Asad Siddiqui","submitted_at":"2026-05-14T05:20:24Z","abstract_excerpt":"We show that standard multi-path interferometry, using only pairwise visibility measurements, provides an operational route to tests of preparation noncontextuality. Under ideal symmetric conditions, interference visibility directly encodes state overlaps, without requiring tomography or SWAP tests. For three paths, any jointly diagonalizable (coherence-free) description must satisfy ${V}_{12}^2+{V}_{23}^2-{V}_{13}^2\\le 1$, where ${V}_{ij}$ are two-path visibilities. Pure qubit detector states violate this bound, achieving a maximal value of $5/4$. We generalize to arbitrary $n$-path interfero"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Under ideal symmetric conditions, interference visibility directly encodes state overlaps, and for three paths any jointly diagonalizable description must satisfy V12² + V23² - V13² ≤ 1, with pure qubit states achieving 5/4; generalized to Sn^max = n cos²(π/2n) - 1 for n ≥ 3.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The operational equivalences used in overlap-based generalized noncontextuality frameworks hold, and the description is jointly diagonalizable (coherence-free) for the bound to apply.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Pairwise visibilities in n-path interferometers yield inequalities violated by qubit states that witness preparation contextuality under operational equivalences.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"ca4bd2db11e66894589f75df2dc89060acf8f501d6b6f1da825c78abf4e413b7"},"source":{"id":"2605.14395","kind":"arxiv","version":1},"verdict":{"id":"6778f4bf-1418-4da1-8204-8a2c8a219bae","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-15T02:28:03.912126Z","strongest_claim":"Under ideal symmetric conditions, interference visibility directly encodes state overlaps, and for three paths any jointly diagonalizable description must satisfy V12² + V23² - V13² ≤ 1, with pure qubit states achieving 5/4; generalized to Sn^max = n cos²(π/2n) - 1 for n ≥ 3.","one_line_summary":"Pairwise visibilities in n-path interferometers yield inequalities violated by qubit states that witness preparation contextuality under operational equivalences.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The operational equivalences used in overlap-based generalized noncontextuality frameworks hold, and the description is jointly diagonalizable (coherence-free) for the bound to apply.","pith_extraction_headline":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities."},"references":{"count":24,"sample":[{"doi":"","year":2014,"title":"T. Baumgratz, M. Cramer, and M. B. Plenio, Quantify- ing coherence, Phys. Rev. Lett.113, 140401 (2014)","work_id":"44cdf2c1-6d3e-4ecf-b7ba-b945ecca2aa3","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2021,"title":"S. Designolle, R. Uola, K. Luoma, and N. Brunner, Set coherence: Basis-independent quantification of quantum coherence, Phys. Rev. Lett.126, 220404 (2021)","work_id":"7a907172-b9c1-46ea-9404-38d9ee00d886","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2020,"title":"E. F. Galv˜ ao and D. J. Brod, Quantum and classical bounds for two-state overlaps, Phys. Rev. A101, 062110 (2020)","work_id":"db212007-697e-40df-b33f-9fdeb99b0ef2","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2024,"title":"R. Wagner, R. S. Barbosa, and E. F. Galv˜ ao, Inequali- ties witnessing coherence, nonlocality, and contextuality, Phys. Rev. A109, 032220 (2024)","work_id":"38781d95-085f-469c-92d6-1bbef0aba2bd","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2005,"title":"R. W. Spekkens, Contextuality for preparations, trans- formations, and unsharp measurements, Phys. Rev. A 71, 052108 (2005)","work_id":"9e04b31f-73ae-48ff-95df-b86396729e29","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":24,"snapshot_sha256":"cc200fe3927ad2c21179c1ea27eed4c97e60962aab18497713c29509108d19b4","internal_anchors":0},"formal_canon":{"evidence_count":2,"snapshot_sha256":"c1195dfad4f450b805b3b80f0ff5c611c80dad3b897566be5f4644e2e1844b4a"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"6778f4bf-1418-4da1-8204-8a2c8a219bae"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nKBcuR5oK5pvawTEdIVjTDqEP30bMns237kBy/xKpVhhCE/GitKeYuPMTk1aqevbqR89FOfY/B9Oj/Wwg+tdAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T03:04:33.320478Z"},"content_sha256":"1442b1835e66dcc6fefb5083a35fe8e1fa457533643ab98e41a854b5951315df","schema_version":"1.0","event_id":"sha256:1442b1835e66dcc6fefb5083a35fe8e1fa457533643ab98e41a854b5951315df"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A62LWZBBKACBA2GU5ZE6RECVQN/bundle.json","state_url":"https://pith.science/pith/A62LWZBBKACBA2GU5ZE6RECVQN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A62LWZBBKACBA2GU5ZE6RECVQN/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":"2026-05-22T03:04:33Z","links":{"resolver":"https://pith.science/pith/A62LWZBBKACBA2GU5ZE6RECVQN","bundle":"https://pith.science/pith/A62LWZBBKACBA2GU5ZE6RECVQN/bundle.json","state":"https://pith.science/pith/A62LWZBBKACBA2GU5ZE6RECVQN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A62LWZBBKACBA2GU5ZE6RECVQN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:A62LWZBBKACBA2GU5ZE6RECVQN","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":"0668cda4244c27f9f2fe276eab480f25a2edb01528c592a18aae9e94c99591fb","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T05:20:24Z","title_canon_sha256":"19f0ed399e1897649e91fdd35ad7ebd411ebd2fa77f1e564defe5c71fb0add3a"},"schema_version":"1.0","source":{"id":"2605.14395","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14395","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14395v1","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14395","created_at":"2026-05-17T23:39:07Z"},{"alias_kind":"pith_short_12","alias_value":"A62LWZBBKACB","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"A62LWZBBKACBA2GU","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"A62LWZBB","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:1442b1835e66dcc6fefb5083a35fe8e1fa457533643ab98e41a854b5951315df","target":"graph","created_at":"2026-05-17T23:39:07Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"Under ideal symmetric conditions, interference visibility directly encodes state overlaps, and for three paths any jointly diagonalizable description must satisfy V12² + V23² - V13² ≤ 1, with pure qubit states achieving 5/4; generalized to Sn^max = n cos²(π/2n) - 1 for n ≥ 3."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The operational equivalences used in overlap-based generalized noncontextuality frameworks hold, and the description is jointly diagonalizable (coherence-free) for the bound to apply."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Pairwise visibilities in n-path interferometers yield inequalities violated by qubit states that witness preparation contextuality under operational equivalences."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities."}],"snapshot_sha256":"ca4bd2db11e66894589f75df2dc89060acf8f501d6b6f1da825c78abf4e413b7"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"c1195dfad4f450b805b3b80f0ff5c611c80dad3b897566be5f4644e2e1844b4a"},"paper":{"abstract_excerpt":"We show that standard multi-path interferometry, using only pairwise visibility measurements, provides an operational route to tests of preparation noncontextuality. Under ideal symmetric conditions, interference visibility directly encodes state overlaps, without requiring tomography or SWAP tests. For three paths, any jointly diagonalizable (coherence-free) description must satisfy ${V}_{12}^2+{V}_{23}^2-{V}_{13}^2\\le 1$, where ${V}_{ij}$ are two-path visibilities. Pure qubit detector states violate this bound, achieving a maximal value of $5/4$. We generalize to arbitrary $n$-path interfero","authors_text":"Mohd Asad Siddiqui","cross_cats":[],"headline":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T05:20:24Z","title":"Interference visibility as a witness of preparation contextuality via overlap inequalities"},"references":{"count":24,"internal_anchors":0,"resolved_work":24,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"T. Baumgratz, M. Cramer, and M. B. Plenio, Quantify- ing coherence, Phys. Rev. Lett.113, 140401 (2014)","work_id":"44cdf2c1-6d3e-4ecf-b7ba-b945ecca2aa3","year":2014},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"S. Designolle, R. Uola, K. Luoma, and N. Brunner, Set coherence: Basis-independent quantification of quantum coherence, Phys. Rev. Lett.126, 220404 (2021)","work_id":"7a907172-b9c1-46ea-9404-38d9ee00d886","year":2021},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"E. F. Galv˜ ao and D. J. Brod, Quantum and classical bounds for two-state overlaps, Phys. Rev. A101, 062110 (2020)","work_id":"db212007-697e-40df-b33f-9fdeb99b0ef2","year":2020},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"R. Wagner, R. S. Barbosa, and E. F. Galv˜ ao, Inequali- ties witnessing coherence, nonlocality, and contextuality, Phys. Rev. A109, 032220 (2024)","work_id":"38781d95-085f-469c-92d6-1bbef0aba2bd","year":2024},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"R. W. Spekkens, Contextuality for preparations, trans- formations, and unsharp measurements, Phys. Rev. A 71, 052108 (2005)","work_id":"9e04b31f-73ae-48ff-95df-b86396729e29","year":2005}],"snapshot_sha256":"cc200fe3927ad2c21179c1ea27eed4c97e60962aab18497713c29509108d19b4"},"source":{"id":"2605.14395","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-15T02:28:03.912126Z","id":"6778f4bf-1418-4da1-8204-8a2c8a219bae","model_set":{"reader":"grok-4.3"},"one_line_summary":"Pairwise visibilities in n-path interferometers yield inequalities violated by qubit states that witness preparation contextuality under operational equivalences.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via overlap inequalities.","strongest_claim":"Under ideal symmetric conditions, interference visibility directly encodes state overlaps, and for three paths any jointly diagonalizable description must satisfy V12² + V23² - V13² ≤ 1, with pure qubit states achieving 5/4; generalized to Sn^max = n cos²(π/2n) - 1 for n ≥ 3.","weakest_assumption":"The operational equivalences used in overlap-based generalized noncontextuality frameworks hold, and the description is jointly diagonalizable (coherence-free) for the bound to apply."}},"verdict_id":"6778f4bf-1418-4da1-8204-8a2c8a219bae"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:4981cc236115404a22f70969d1a30902ccaca922a523c35f8197152eafd65569","target":"record","created_at":"2026-05-17T23:39:07Z","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":"0668cda4244c27f9f2fe276eab480f25a2edb01528c592a18aae9e94c99591fb","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T05:20:24Z","title_canon_sha256":"19f0ed399e1897649e91fdd35ad7ebd411ebd2fa77f1e564defe5c71fb0add3a"},"schema_version":"1.0","source":{"id":"2605.14395","kind":"arxiv","version":1}},"canonical_sha256":"07b4bb642150041068d4ee49e89055837a6942b53884b0f7de773ef6d3fd03ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"07b4bb642150041068d4ee49e89055837a6942b53884b0f7de773ef6d3fd03ac","first_computed_at":"2026-05-17T23:39:07.564718Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:07.564718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5XBhsAX4HuGSnsTBE2u07CuDLQJ8U7UHenwmsePUp3NkdPa0R0FI9fGOyByC3o6Wk/Aol95DDdOrgmn4UbPmDg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:07.565370Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.14395","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4981cc236115404a22f70969d1a30902ccaca922a523c35f8197152eafd65569","sha256:1442b1835e66dcc6fefb5083a35fe8e1fa457533643ab98e41a854b5951315df"],"state_sha256":"05cfe2e1fecb271decaba6a88c10107b0fa1bbf9e3c67ed769386774ab401f15"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t+WzA3Su68RKKZ/ypbNskOlmdcZwdjcRDYFD83yqtEBRZfhqIamxnYC0pEm33niWoKXEp+Hn6UP+x5Nc7pFHDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T03:04:33.325558Z","bundle_sha256":"e3c4940114c0e797838ee5e6a6e0f832f51861b79ac598104faf59a169fc834b"}}