{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:IHHFMALN7YXU6RMGX7WAFK57UY","short_pith_number":"pith:IHHFMALN","canonical_record":{"source":{"id":"1203.6167","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-03-28T05:38:43Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"68c57bdbd4fd948f598e3259906b86fa01c8c9fbd2dcb2db6fa846a31d31354d","abstract_canon_sha256":"ae1551fb79e65eb9ef09f9ebdc9d8edb410a4885843604e36f295fb7d3d3ce5f"},"schema_version":"1.0"},"canonical_sha256":"41ce56016dfe2f4f4586bfec02abbfa61866e1087923b1393405e822cc4f63e7","source":{"kind":"arxiv","id":"1203.6167","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.6167","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"arxiv_version","alias_value":"1203.6167v1","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.6167","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"pith_short_12","alias_value":"IHHFMALN7YXU","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_16","alias_value":"IHHFMALN7YXU6RMG","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_8","alias_value":"IHHFMALN","created_at":"2026-05-18T12:27:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:IHHFMALN7YXU6RMGX7WAFK57UY","target":"record","payload":{"canonical_record":{"source":{"id":"1203.6167","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-03-28T05:38:43Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"68c57bdbd4fd948f598e3259906b86fa01c8c9fbd2dcb2db6fa846a31d31354d","abstract_canon_sha256":"ae1551fb79e65eb9ef09f9ebdc9d8edb410a4885843604e36f295fb7d3d3ce5f"},"schema_version":"1.0"},"canonical_sha256":"41ce56016dfe2f4f4586bfec02abbfa61866e1087923b1393405e822cc4f63e7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:01.151823Z","signature_b64":"5muD8YmW99AnfpLcIJ9MgSsuffJa9F94ajh9cU1n1OtzdG/ZIrTdH7Fmu6OBYpQLgyoO7Qeb903MuW0emUJ6DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"41ce56016dfe2f4f4586bfec02abbfa61866e1087923b1393405e822cc4f63e7","last_reissued_at":"2026-05-18T01:58:01.151349Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:01.151349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1203.6167","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":"2026-05-18T01:58:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uk1u82Y4UKdfzRFI03JWTr/Sf3pf85Hqw2dylbVCut3qGV37/EgDnp5Ahz7nlb25ujkFQh63ceF4Pv4GFCvUDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:35:55.188993Z"},"content_sha256":"152b6bd23c16f950c6a89f45cca4afd2bb14125446e28c76cff6d7059f1af02e","schema_version":"1.0","event_id":"sha256:152b6bd23c16f950c6a89f45cca4afd2bb14125446e28c76cff6d7059f1af02e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:IHHFMALN7YXU6RMGX7WAFK57UY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Full vectorial analysis of polarization effects in optical nanowires","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"physics.optics","authors_text":"M. A. Lohe, Shahraam Afshar V., Tanya M. Monro, Wen Qi Zhang","submitted_at":"2012-03-28T05:38:43Z","abstract_excerpt":"We develop a full theoretical analysis of the nonlinear interactions of the two polarizations of a waveguide by means of a vectorial model of pulse propagation which applies to high index subwavelength waveguides. In such waveguides there is an anisotropy in the nonlinear behavior of the two polarizations that originates entirely from the waveguide structure, and leads to switching properties. We determine the stability properties of the steady state solutions by means of a Lagrangian formulation. We find all static solutions of the nonlinear system, including those that are periodic with resp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.6167","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":"2026-05-18T01:58:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FojmlUoc58YiRW4t6IBRJCaQ7w/SBbfPLdjCSbOk0QcfmliyRbLmEt9/gPOkzzESpKne32RhfK3hFPF6mB+gCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:35:55.189691Z"},"content_sha256":"543ba32bad6e6594d983e0f403c632e4696ee6c384e8845233c6be76681bcc0c","schema_version":"1.0","event_id":"sha256:543ba32bad6e6594d983e0f403c632e4696ee6c384e8845233c6be76681bcc0c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IHHFMALN7YXU6RMGX7WAFK57UY/bundle.json","state_url":"https://pith.science/pith/IHHFMALN7YXU6RMGX7WAFK57UY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IHHFMALN7YXU6RMGX7WAFK57UY/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":"2026-05-27T16:35:55Z","links":{"resolver":"https://pith.science/pith/IHHFMALN7YXU6RMGX7WAFK57UY","bundle":"https://pith.science/pith/IHHFMALN7YXU6RMGX7WAFK57UY/bundle.json","state":"https://pith.science/pith/IHHFMALN7YXU6RMGX7WAFK57UY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IHHFMALN7YXU6RMGX7WAFK57UY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:IHHFMALN7YXU6RMGX7WAFK57UY","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":"ae1551fb79e65eb9ef09f9ebdc9d8edb410a4885843604e36f295fb7d3d3ce5f","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-03-28T05:38:43Z","title_canon_sha256":"68c57bdbd4fd948f598e3259906b86fa01c8c9fbd2dcb2db6fa846a31d31354d"},"schema_version":"1.0","source":{"id":"1203.6167","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.6167","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"arxiv_version","alias_value":"1203.6167v1","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.6167","created_at":"2026-05-18T01:58:01Z"},{"alias_kind":"pith_short_12","alias_value":"IHHFMALN7YXU","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_16","alias_value":"IHHFMALN7YXU6RMG","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_8","alias_value":"IHHFMALN","created_at":"2026-05-18T12:27:09Z"}],"graph_snapshots":[{"event_id":"sha256:543ba32bad6e6594d983e0f403c632e4696ee6c384e8845233c6be76681bcc0c","target":"graph","created_at":"2026-05-18T01:58:01Z","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 develop a full theoretical analysis of the nonlinear interactions of the two polarizations of a waveguide by means of a vectorial model of pulse propagation which applies to high index subwavelength waveguides. In such waveguides there is an anisotropy in the nonlinear behavior of the two polarizations that originates entirely from the waveguide structure, and leads to switching properties. We determine the stability properties of the steady state solutions by means of a Lagrangian formulation. We find all static solutions of the nonlinear system, including those that are periodic with resp","authors_text":"M. A. Lohe, Shahraam Afshar V., Tanya M. Monro, Wen Qi Zhang","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-03-28T05:38:43Z","title":"Full vectorial analysis of polarization effects in optical nanowires"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.6167","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":"sha256:152b6bd23c16f950c6a89f45cca4afd2bb14125446e28c76cff6d7059f1af02e","target":"record","created_at":"2026-05-18T01:58:01Z","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":"ae1551fb79e65eb9ef09f9ebdc9d8edb410a4885843604e36f295fb7d3d3ce5f","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-03-28T05:38:43Z","title_canon_sha256":"68c57bdbd4fd948f598e3259906b86fa01c8c9fbd2dcb2db6fa846a31d31354d"},"schema_version":"1.0","source":{"id":"1203.6167","kind":"arxiv","version":1}},"canonical_sha256":"41ce56016dfe2f4f4586bfec02abbfa61866e1087923b1393405e822cc4f63e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"41ce56016dfe2f4f4586bfec02abbfa61866e1087923b1393405e822cc4f63e7","first_computed_at":"2026-05-18T01:58:01.151349Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:01.151349Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5muD8YmW99AnfpLcIJ9MgSsuffJa9F94ajh9cU1n1OtzdG/ZIrTdH7Fmu6OBYpQLgyoO7Qeb903MuW0emUJ6DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:01.151823Z","signed_message":"canonical_sha256_bytes"},"source_id":"1203.6167","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:152b6bd23c16f950c6a89f45cca4afd2bb14125446e28c76cff6d7059f1af02e","sha256:543ba32bad6e6594d983e0f403c632e4696ee6c384e8845233c6be76681bcc0c"],"state_sha256":"de6da942a8fede92f19dd899d34cf81a4638a52878aa0c06121550843d43759c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DarO48v904MyHmXKeVxMmmioXKbUHcHdiznUNh/WIh6cIuazfPwBGX4j1WwkvTxadqkIq3z62k7SKiLn9FJeAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T16:35:55.193511Z","bundle_sha256":"ba6f7120d38a34350e2c02ef23f022dba1dfdcd64ecedae106232f1506be7d1c"}}