{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:LYPWMW4BRK63VWKTBMEADRLIPN","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":"40eb5351d52d59441b8452d3ade07453776efa44a2397fcaf0d1ed74d8467baf","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-08-17T04:47:57Z","title_canon_sha256":"bbc8087ae6a7b76e3dc65e3c5ddc1dc968fbe898944f43a52b414a4244a8fcc8"},"schema_version":"1.0","source":{"id":"1008.2816","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1008.2816","created_at":"2026-05-18T02:05:47Z"},{"alias_kind":"arxiv_version","alias_value":"1008.2816v2","created_at":"2026-05-18T02:05:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.2816","created_at":"2026-05-18T02:05:47Z"},{"alias_kind":"pith_short_12","alias_value":"LYPWMW4BRK63","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"LYPWMW4BRK63VWKT","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"LYPWMW4B","created_at":"2026-05-18T12:26:10Z"}],"graph_snapshots":[{"event_id":"sha256:272fc3f43bdeb6ca5966fcb31a6dc229f7d05591c6470cb664e971614bc77201","target":"graph","created_at":"2026-05-18T02:05:47Z","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 summarize the results of our comprehensive analytical and numerical studies of the effects of polarization on the Anderson localization of classical waves in one-dimensional random stacks. We consider homogeneous stacks composed entirely of normal materials or metamaterials, and also mixed stacks composed of alternating layers of a normal material and metamaterial. We extend the theoretical study developed earlier for the case of normal incidence [A. A. Asatryan et al, Phys. Rev. B 81, 075124 (2010)] to the case of off-axis incidence. For the general case where both the refractive indices a","authors_text":"Ara A. Asatryan, Ilya V. Shadrivov, Lindsay C. Botten, Michael A. Byrne, Ross C. McPhedran, Sergey A. Gredeskul, Valentin D. Freilikher, Yuri S. Kivshar","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-08-17T04:47:57Z","title":"Effects of polarization on the transmission and localization of classical waves in weakly scattering metamaterials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.2816","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":"sha256:7ed776647b23eca8ca9509490b4a2ad2afc2c65cb1a1785af49baaa3611e3762","target":"record","created_at":"2026-05-18T02:05:47Z","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":"40eb5351d52d59441b8452d3ade07453776efa44a2397fcaf0d1ed74d8467baf","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-08-17T04:47:57Z","title_canon_sha256":"bbc8087ae6a7b76e3dc65e3c5ddc1dc968fbe898944f43a52b414a4244a8fcc8"},"schema_version":"1.0","source":{"id":"1008.2816","kind":"arxiv","version":2}},"canonical_sha256":"5e1f665b818abdbad9530b0801c5687b670d313adff1ea3dd501faca0093ffb1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5e1f665b818abdbad9530b0801c5687b670d313adff1ea3dd501faca0093ffb1","first_computed_at":"2026-05-18T02:05:47.622256Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:05:47.622256Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"38neB6Dpu8GSvmRdu0oyE6Qmitoa3o2/t4/jie7hpZispyuU9Jihc3DGgy49++Em/49eMs8ru5qHOaUhKl6jCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:05:47.622952Z","signed_message":"canonical_sha256_bytes"},"source_id":"1008.2816","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7ed776647b23eca8ca9509490b4a2ad2afc2c65cb1a1785af49baaa3611e3762","sha256:272fc3f43bdeb6ca5966fcb31a6dc229f7d05591c6470cb664e971614bc77201"],"state_sha256":"1842afd3f6ced29609cdb9fb4ad86e304e23e127196e05eae46183fcf3c7d698"}