{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:DDLKLJTSELGJ747NKVFMFMQG7N","short_pith_number":"pith:DDLKLJTS","canonical_record":{"source":{"id":"1105.4934","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-05-25T04:47:59Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"16b4bbf56318b2c27c68294af5ee361cca9705be1ed81b091ea1afa52de34c06","abstract_canon_sha256":"21b68be67af70250a59b580494f582b7bb6563eb07aa0d9ee1f0e479549386a7"},"schema_version":"1.0"},"canonical_sha256":"18d6a5a67222cc9ff3ed554ac2b206fb7dcc57c01286356356e5c8e92eda1421","source":{"kind":"arxiv","id":"1105.4934","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.4934","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"arxiv_version","alias_value":"1105.4934v1","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.4934","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"pith_short_12","alias_value":"DDLKLJTSELGJ","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_16","alias_value":"DDLKLJTSELGJ747N","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_8","alias_value":"DDLKLJTS","created_at":"2026-05-18T12:26:26Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:DDLKLJTSELGJ747NKVFMFMQG7N","target":"record","payload":{"canonical_record":{"source":{"id":"1105.4934","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-05-25T04:47:59Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"16b4bbf56318b2c27c68294af5ee361cca9705be1ed81b091ea1afa52de34c06","abstract_canon_sha256":"21b68be67af70250a59b580494f582b7bb6563eb07aa0d9ee1f0e479549386a7"},"schema_version":"1.0"},"canonical_sha256":"18d6a5a67222cc9ff3ed554ac2b206fb7dcc57c01286356356e5c8e92eda1421","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:21.070167Z","signature_b64":"0CTFCrR+s78z90w3g0X+oMosYuQQs5/fEoSVOdZUWYWiXdkcvGzPgm5SechMaGKFzy0jpjcL3k6t12eG/XeUBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18d6a5a67222cc9ff3ed554ac2b206fb7dcc57c01286356356e5c8e92eda1421","last_reissued_at":"2026-05-18T04:21:21.069689Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:21.069689Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.4934","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":"2026-05-18T04:21:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DQ8Zl3bapKHEIi8ZjMf/NtGiiGMfDTE+KrbqmGbQ2lzS0pOXc2p4qqMQ0Eb2zZGn8VwrCc5W7YQIpyJIeYV1DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T13:42:46.300328Z"},"content_sha256":"60e8a160fa28292a5d14a0dbbf0bfa0f4afcb903982c0a194308a422ff82f2d9","schema_version":"1.0","event_id":"sha256:60e8a160fa28292a5d14a0dbbf0bfa0f4afcb903982c0a194308a422ff82f2d9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:DDLKLJTSELGJ747NKVFMFMQG7N","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modeling of electromagnetic wave propagation and spectra of optical excitations in complex media using 4x4 matrix formalism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"physics.optics","authors_text":"A. A. Sirenko, M. Kotelyanskii, P. D. Rogers","submitted_at":"2011-05-25T04:47:59Z","abstract_excerpt":"Using 4x4 matrix formalism we analyzed electromagnetic wave propagation and Jones matrix components for reflectivity and transmittivity in bi-anisotropic materials. Analytic formulas for complex reflection and transmission coefficients for bi-anisotropic materials in both semi-infinite and thin-film configurations have been derived. The obtained results are applicable for analysis of the optical spectra of multiferroic crystals and metamaterials. The Adjusted Oscillator Strength Matching Condition (AOSM) for hybrid magnetic- and electric-dipole excitations in anisotropic multiferroics is deriv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.4934","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":"2026-05-18T04:21:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mhxA/qPcEEW4E+FgRY5aR4uEsY9fTe4F6SjkEpp3ThbAznmpZ+KbSqIYOug5J63VL/WcYRPRGddO4gdH2EDdAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T13:42:46.301049Z"},"content_sha256":"21cc94bf67c0960f7846dae561804e305b5289f08da6633a03bf2b4dae3cd0cd","schema_version":"1.0","event_id":"sha256:21cc94bf67c0960f7846dae561804e305b5289f08da6633a03bf2b4dae3cd0cd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DDLKLJTSELGJ747NKVFMFMQG7N/bundle.json","state_url":"https://pith.science/pith/DDLKLJTSELGJ747NKVFMFMQG7N/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DDLKLJTSELGJ747NKVFMFMQG7N/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":"2026-06-10T13:42:46Z","links":{"resolver":"https://pith.science/pith/DDLKLJTSELGJ747NKVFMFMQG7N","bundle":"https://pith.science/pith/DDLKLJTSELGJ747NKVFMFMQG7N/bundle.json","state":"https://pith.science/pith/DDLKLJTSELGJ747NKVFMFMQG7N/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DDLKLJTSELGJ747NKVFMFMQG7N/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:DDLKLJTSELGJ747NKVFMFMQG7N","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":"21b68be67af70250a59b580494f582b7bb6563eb07aa0d9ee1f0e479549386a7","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-05-25T04:47:59Z","title_canon_sha256":"16b4bbf56318b2c27c68294af5ee361cca9705be1ed81b091ea1afa52de34c06"},"schema_version":"1.0","source":{"id":"1105.4934","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.4934","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"arxiv_version","alias_value":"1105.4934v1","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.4934","created_at":"2026-05-18T04:21:21Z"},{"alias_kind":"pith_short_12","alias_value":"DDLKLJTSELGJ","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_16","alias_value":"DDLKLJTSELGJ747N","created_at":"2026-05-18T12:26:26Z"},{"alias_kind":"pith_short_8","alias_value":"DDLKLJTS","created_at":"2026-05-18T12:26:26Z"}],"graph_snapshots":[{"event_id":"sha256:21cc94bf67c0960f7846dae561804e305b5289f08da6633a03bf2b4dae3cd0cd","target":"graph","created_at":"2026-05-18T04:21:21Z","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":"Using 4x4 matrix formalism we analyzed electromagnetic wave propagation and Jones matrix components for reflectivity and transmittivity in bi-anisotropic materials. Analytic formulas for complex reflection and transmission coefficients for bi-anisotropic materials in both semi-infinite and thin-film configurations have been derived. The obtained results are applicable for analysis of the optical spectra of multiferroic crystals and metamaterials. The Adjusted Oscillator Strength Matching Condition (AOSM) for hybrid magnetic- and electric-dipole excitations in anisotropic multiferroics is deriv","authors_text":"A. A. Sirenko, M. Kotelyanskii, P. D. Rogers","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-05-25T04:47:59Z","title":"Modeling of electromagnetic wave propagation and spectra of optical excitations in complex media using 4x4 matrix formalism"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.4934","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":"sha256:60e8a160fa28292a5d14a0dbbf0bfa0f4afcb903982c0a194308a422ff82f2d9","target":"record","created_at":"2026-05-18T04:21:21Z","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":"21b68be67af70250a59b580494f582b7bb6563eb07aa0d9ee1f0e479549386a7","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2011-05-25T04:47:59Z","title_canon_sha256":"16b4bbf56318b2c27c68294af5ee361cca9705be1ed81b091ea1afa52de34c06"},"schema_version":"1.0","source":{"id":"1105.4934","kind":"arxiv","version":1}},"canonical_sha256":"18d6a5a67222cc9ff3ed554ac2b206fb7dcc57c01286356356e5c8e92eda1421","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18d6a5a67222cc9ff3ed554ac2b206fb7dcc57c01286356356e5c8e92eda1421","first_computed_at":"2026-05-18T04:21:21.069689Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:21:21.069689Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0CTFCrR+s78z90w3g0X+oMosYuQQs5/fEoSVOdZUWYWiXdkcvGzPgm5SechMaGKFzy0jpjcL3k6t12eG/XeUBg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:21:21.070167Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.4934","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:60e8a160fa28292a5d14a0dbbf0bfa0f4afcb903982c0a194308a422ff82f2d9","sha256:21cc94bf67c0960f7846dae561804e305b5289f08da6633a03bf2b4dae3cd0cd"],"state_sha256":"7bf852ec83ca1b9560d684b8543b3477121727f118f8d69f4b9e6b88da2fef99"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yybik/nsUZHvS1jnC8L+4cLRTTu3n3+ijcC++UXfMMkC5MbT29SC1cm0T5sx/gYC/J7cWBqHWyEpkwbO+15oCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T13:42:46.304974Z","bundle_sha256":"328e2963dbf17ba53e23cec9ec8fb29bc6fb7971d16750f0d526620d811e86bb"}}