{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:VVABSQPQ4V343Q2QY4PRS7VPJV","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":"5fa1bfc4df5b91f572386260b8523b71808ad87637dad0c9b1774c790efee777","cross_cats_sorted":["cond-mat.other","nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-05-11T16:59:00Z","title_canon_sha256":"781d1159b46799ffb9cf7192dc7771450fc13f7966028ec0843d1d6d0c91aa7f"},"schema_version":"1.0","source":{"id":"1205.3182","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.3182","created_at":"2026-05-18T03:55:36Z"},{"alias_kind":"arxiv_version","alias_value":"1205.3182v1","created_at":"2026-05-18T03:55:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.3182","created_at":"2026-05-18T03:55:36Z"},{"alias_kind":"pith_short_12","alias_value":"VVABSQPQ4V34","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"VVABSQPQ4V343Q2Q","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"VVABSQPQ","created_at":"2026-05-18T12:27:25Z"}],"graph_snapshots":[{"event_id":"sha256:ada0bc307f4529f7463d2171688e92a6447f1b163af868422da31f3c203f5eb0","target":"graph","created_at":"2026-05-18T03:55:36Z","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 demonstrate that soliton-plasmon bound states appear naturally as propagating eigenmodes of nonlinear Maxwell's equations for a metal/dielectric/Kerr interface. By means of a variational method, we give an explicit and simplified expression for the full-vector nonlinear operator of the system. Soliplasmon states (propagating surface soliton-plasmon modes) can be then analytically calculated as eigenmodes of this non-selfadjoint operator. The theoretical treatment of the system predicts the key features of the stationary solutions and gives physical insight to understand the inherent stabili","authors_text":"Albert Ferrando, Carles Mili\\'an, Daniel E. Ceballos-Herrera, Dmitry V. Skryabin","cross_cats":["cond-mat.other","nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-05-11T16:59:00Z","title":"Maxwell's equations approach to soliton excitations of surface plasmonic resonances"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.3182","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":"sha256:6a616ce5403130723bd026114147f933f19d25147cd35a28ee9f99e7603fc01c","target":"record","created_at":"2026-05-18T03:55:36Z","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":"5fa1bfc4df5b91f572386260b8523b71808ad87637dad0c9b1774c790efee777","cross_cats_sorted":["cond-mat.other","nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-05-11T16:59:00Z","title_canon_sha256":"781d1159b46799ffb9cf7192dc7771450fc13f7966028ec0843d1d6d0c91aa7f"},"schema_version":"1.0","source":{"id":"1205.3182","kind":"arxiv","version":1}},"canonical_sha256":"ad401941f0e577cdc350c71f197eaf4d6df4756d42971035a73c42cdc0045693","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ad401941f0e577cdc350c71f197eaf4d6df4756d42971035a73c42cdc0045693","first_computed_at":"2026-05-18T03:55:36.716035Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:55:36.716035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"F6vK3accqoEA9j5GxrgzYS56PstD5RLvvTJn5QuXkNTCaW9+e+6aeMLfqT3DvvScC5Pu95DILSaMwMCiTwjpBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:55:36.716609Z","signed_message":"canonical_sha256_bytes"},"source_id":"1205.3182","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6a616ce5403130723bd026114147f933f19d25147cd35a28ee9f99e7603fc01c","sha256:ada0bc307f4529f7463d2171688e92a6447f1b163af868422da31f3c203f5eb0"],"state_sha256":"d11decb2dabe84df0aa88bd302d81a706009324258e15651b5b58875946b3b18"}