{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:RCOPXRNVOWNGDQMYYEGCBPVDKT","short_pith_number":"pith:RCOPXRNV","canonical_record":{"source":{"id":"1609.05777","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-19T15:25:53Z","cross_cats_sorted":[],"title_canon_sha256":"658085c177895f0f34e1382ecc5faead059f3f927854aa29521a31287ad3e1ab","abstract_canon_sha256":"284a4e37ffc3d35c5b74b3750c64308c8e9030c6161c3497507f4d269db816ec"},"schema_version":"1.0"},"canonical_sha256":"889cfbc5b5759a61c198c10c20bea354ea160ba82556270268dde9eaf853621e","source":{"kind":"arxiv","id":"1609.05777","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.05777","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"arxiv_version","alias_value":"1609.05777v1","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.05777","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"pith_short_12","alias_value":"RCOPXRNVOWNG","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RCOPXRNVOWNGDQMY","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RCOPXRNV","created_at":"2026-05-18T12:30:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:RCOPXRNVOWNGDQMYYEGCBPVDKT","target":"record","payload":{"canonical_record":{"source":{"id":"1609.05777","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-19T15:25:53Z","cross_cats_sorted":[],"title_canon_sha256":"658085c177895f0f34e1382ecc5faead059f3f927854aa29521a31287ad3e1ab","abstract_canon_sha256":"284a4e37ffc3d35c5b74b3750c64308c8e9030c6161c3497507f4d269db816ec"},"schema_version":"1.0"},"canonical_sha256":"889cfbc5b5759a61c198c10c20bea354ea160ba82556270268dde9eaf853621e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:25.340903Z","signature_b64":"Uod+T7zAhZuTI6O3o563sccKNpN+JpN1IlGmOYwxEW910UKFukN6uyNZIGWmIIOX/j24BLDbxRlmbyMItgpPDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"889cfbc5b5759a61c198c10c20bea354ea160ba82556270268dde9eaf853621e","last_reissued_at":"2026-05-18T01:04:25.340252Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:25.340252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.05777","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":"2026-05-18T01:04:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2fP5H75h4SnDqqxZvYEn0A134Jv+dGDQsIBtr7KXowFn9iqWHwjJc36pegLwHv50xtPkb2Eg3e8hPIBc8xgGCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T05:21:32.228358Z"},"content_sha256":"2b607f589c71fddc5cde87d0c0bb7827e285a4141022b5a0c3a43271f421e45c","schema_version":"1.0","event_id":"sha256:2b607f589c71fddc5cde87d0c0bb7827e285a4141022b5a0c3a43271f421e45c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:RCOPXRNVOWNGDQMYYEGCBPVDKT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polarization-tailored Fano interference in plasmonic crystals: A Mueller matrix model of anisotropic Fano resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"A. K. Singh, A. Kumar, A. Mandal. S. Misra, N. Ghosh, P. Mitra, S. Chandel, S.K. Ray","submitted_at":"2016-09-19T15:25:53Z","abstract_excerpt":"We present a simple yet elegant Mueller matrix approach for controlling the Fano interference effect and engineering the resulting asymmetric spectral line shape in anisotropic optical system. The approach is founded on a generalized model of anisotropic Fano resonance, which relates the spectral asymmetry to two physically meaningful and experimentally accessible parameters of interference, namely, the Fano phase shift and the relative amplitudes of the interfering modes. The differences in these parameters between orthogonal linear polarizations in an anisotropic system are exploited to desi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.05777","kind":"arxiv","version":1},"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":"2026-05-18T01:04:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yct9YUbozgyes9u3FRIZmUtAHQ22nhbUcQ08uORHPC7fSm9n1ELamv290T+4Sx38PxkzkKbf+ZYr6Gu8q1ZDCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T05:21:32.228713Z"},"content_sha256":"902ff90ac7c944dea53a1a152e7efd2220acd4adda4130b6e2c9024412fd443d","schema_version":"1.0","event_id":"sha256:902ff90ac7c944dea53a1a152e7efd2220acd4adda4130b6e2c9024412fd443d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/bundle.json","state_url":"https://pith.science/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/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":"2026-06-01T05:21:32Z","links":{"resolver":"https://pith.science/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT","bundle":"https://pith.science/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/bundle.json","state":"https://pith.science/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RCOPXRNVOWNGDQMYYEGCBPVDKT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:RCOPXRNVOWNGDQMYYEGCBPVDKT","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":"284a4e37ffc3d35c5b74b3750c64308c8e9030c6161c3497507f4d269db816ec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-19T15:25:53Z","title_canon_sha256":"658085c177895f0f34e1382ecc5faead059f3f927854aa29521a31287ad3e1ab"},"schema_version":"1.0","source":{"id":"1609.05777","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.05777","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"arxiv_version","alias_value":"1609.05777v1","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.05777","created_at":"2026-05-18T01:04:25Z"},{"alias_kind":"pith_short_12","alias_value":"RCOPXRNVOWNG","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RCOPXRNVOWNGDQMY","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RCOPXRNV","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:902ff90ac7c944dea53a1a152e7efd2220acd4adda4130b6e2c9024412fd443d","target":"graph","created_at":"2026-05-18T01:04:25Z","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 present a simple yet elegant Mueller matrix approach for controlling the Fano interference effect and engineering the resulting asymmetric spectral line shape in anisotropic optical system. The approach is founded on a generalized model of anisotropic Fano resonance, which relates the spectral asymmetry to two physically meaningful and experimentally accessible parameters of interference, namely, the Fano phase shift and the relative amplitudes of the interfering modes. The differences in these parameters between orthogonal linear polarizations in an anisotropic system are exploited to desi","authors_text":"A. K. Singh, A. Kumar, A. Mandal. S. Misra, N. Ghosh, P. Mitra, S. Chandel, S.K. Ray","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-19T15:25:53Z","title":"Polarization-tailored Fano interference in plasmonic crystals: A Mueller matrix model of anisotropic Fano resonance"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.05777","kind":"arxiv","version":1},"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":"sha256:2b607f589c71fddc5cde87d0c0bb7827e285a4141022b5a0c3a43271f421e45c","target":"record","created_at":"2026-05-18T01:04:25Z","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":"284a4e37ffc3d35c5b74b3750c64308c8e9030c6161c3497507f4d269db816ec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-19T15:25:53Z","title_canon_sha256":"658085c177895f0f34e1382ecc5faead059f3f927854aa29521a31287ad3e1ab"},"schema_version":"1.0","source":{"id":"1609.05777","kind":"arxiv","version":1}},"canonical_sha256":"889cfbc5b5759a61c198c10c20bea354ea160ba82556270268dde9eaf853621e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"889cfbc5b5759a61c198c10c20bea354ea160ba82556270268dde9eaf853621e","first_computed_at":"2026-05-18T01:04:25.340252Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:25.340252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Uod+T7zAhZuTI6O3o563sccKNpN+JpN1IlGmOYwxEW910UKFukN6uyNZIGWmIIOX/j24BLDbxRlmbyMItgpPDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:25.340903Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.05777","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2b607f589c71fddc5cde87d0c0bb7827e285a4141022b5a0c3a43271f421e45c","sha256:902ff90ac7c944dea53a1a152e7efd2220acd4adda4130b6e2c9024412fd443d"],"state_sha256":"f6b6d526926957d8209994c494b8517733a729fb88646281abce0e784e0be2d5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+CQ0ztM2rtxNzwFp/i+Tupk/0ljECj6UFzPgrZ02auBGGy+dnZ2Bl9fC1VRWldZ1WTCTSrjUdvtuAH/tkwAzCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T05:21:32.231158Z","bundle_sha256":"7b0a6b6c47b5a7a0db9c8a2e5dcb482d85c27750f69f78f2325aedc316d10038"}}