{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:RGRNNOYHAAMSEMLYEANG7EAKYG","short_pith_number":"pith:RGRNNOYH","canonical_record":{"source":{"id":"1104.2638","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2011-04-13T22:47:07Z","cross_cats_sorted":[],"title_canon_sha256":"c8d5a63f4fcebebfc6a9a0256d84cf267c5df80ea80f54be6fa0cdf9907e3740","abstract_canon_sha256":"087e358c5f9e5c7ae635241a65effe1d1a1bc31efc7d0e7d364d0e14b8983217"},"schema_version":"1.0"},"canonical_sha256":"89a2d6bb070019223178201a6f900ac18bbc3621c5a8992d5a29b75bbfeb8422","source":{"kind":"arxiv","id":"1104.2638","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.2638","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"arxiv_version","alias_value":"1104.2638v1","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.2638","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"pith_short_12","alias_value":"RGRNNOYHAAMS","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_16","alias_value":"RGRNNOYHAAMSEMLY","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_8","alias_value":"RGRNNOYH","created_at":"2026-05-18T12:26:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:RGRNNOYHAAMSEMLYEANG7EAKYG","target":"record","payload":{"canonical_record":{"source":{"id":"1104.2638","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2011-04-13T22:47:07Z","cross_cats_sorted":[],"title_canon_sha256":"c8d5a63f4fcebebfc6a9a0256d84cf267c5df80ea80f54be6fa0cdf9907e3740","abstract_canon_sha256":"087e358c5f9e5c7ae635241a65effe1d1a1bc31efc7d0e7d364d0e14b8983217"},"schema_version":"1.0"},"canonical_sha256":"89a2d6bb070019223178201a6f900ac18bbc3621c5a8992d5a29b75bbfeb8422","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:24:27.180312Z","signature_b64":"wD+BndEVFXMf5nsmxzGhDpzbMfFiRutxpRknVoB5dEYRcy2OaTLCS6Q0ZqSUhlxCML4lUHbqTcDpmW9ma3iDAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89a2d6bb070019223178201a6f900ac18bbc3621c5a8992d5a29b75bbfeb8422","last_reissued_at":"2026-05-18T04:24:27.179829Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:24:27.179829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1104.2638","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":"2026-05-18T04:24:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WJvhaDffijbOeJ6WPXMEggzi5OCg1XxomqCuQyTGjplXrjQbCK3LjoXQBMBK+EKET4omX2jFHaq+/LdfQoyhCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T16:31:01.421029Z"},"content_sha256":"a10369debadb7748d717a2a023f7699a4ff6e563797c90d7ab855bb8e1bfb8fb","schema_version":"1.0","event_id":"sha256:a10369debadb7748d717a2a023f7699a4ff6e563797c90d7ab855bb8e1bfb8fb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:RGRNNOYHAAMSEMLYEANG7EAKYG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scattering matrix of elliptically polarized waves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.class-ph","authors_text":"E. Casta\\~no, M. Mart\\'inez-Mares","submitted_at":"2011-04-13T22:47:07Z","abstract_excerpt":"We analyze the scattering of elliptically polarized plane waves normally incident at the planar interface between two different materials; we consider two cases: dielectric-dielectric and dielectric-conductor interfaces. The scattering matrix S in both cases is obtained using the boundary conditions and Poynting's theorem. In the dielectric-dielectric case we write S using two different basis, the usual xy and a rotated one. For the dielectric-conductor interface, the use of the rotated basis together with an energy balance argument leads us, in a natural way, to construct a unitary S matrix a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.2638","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":"2026-05-18T04:24:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"49eoGelMkmZZghinnwHoXw/i1B5Bu92GsVvF8A01yLwYSRN/vqnQbHE/EQuIefb2trq7+bBQ5J/aPenS6JvNBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T16:31:01.421387Z"},"content_sha256":"85b51fe369bfc12ae040c4c92fdd930161a4c33f3b1761cce7a874af0145e7c1","schema_version":"1.0","event_id":"sha256:85b51fe369bfc12ae040c4c92fdd930161a4c33f3b1761cce7a874af0145e7c1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/bundle.json","state_url":"https://pith.science/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/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":"2026-06-10T16:31:01Z","links":{"resolver":"https://pith.science/pith/RGRNNOYHAAMSEMLYEANG7EAKYG","bundle":"https://pith.science/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/bundle.json","state":"https://pith.science/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RGRNNOYHAAMSEMLYEANG7EAKYG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:RGRNNOYHAAMSEMLYEANG7EAKYG","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":"087e358c5f9e5c7ae635241a65effe1d1a1bc31efc7d0e7d364d0e14b8983217","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2011-04-13T22:47:07Z","title_canon_sha256":"c8d5a63f4fcebebfc6a9a0256d84cf267c5df80ea80f54be6fa0cdf9907e3740"},"schema_version":"1.0","source":{"id":"1104.2638","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.2638","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"arxiv_version","alias_value":"1104.2638v1","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.2638","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"pith_short_12","alias_value":"RGRNNOYHAAMS","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_16","alias_value":"RGRNNOYHAAMSEMLY","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_8","alias_value":"RGRNNOYH","created_at":"2026-05-18T12:26:41Z"}],"graph_snapshots":[{"event_id":"sha256:85b51fe369bfc12ae040c4c92fdd930161a4c33f3b1761cce7a874af0145e7c1","target":"graph","created_at":"2026-05-18T04:24:27Z","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 analyze the scattering of elliptically polarized plane waves normally incident at the planar interface between two different materials; we consider two cases: dielectric-dielectric and dielectric-conductor interfaces. The scattering matrix S in both cases is obtained using the boundary conditions and Poynting's theorem. In the dielectric-dielectric case we write S using two different basis, the usual xy and a rotated one. For the dielectric-conductor interface, the use of the rotated basis together with an energy balance argument leads us, in a natural way, to construct a unitary S matrix a","authors_text":"E. Casta\\~no, M. Mart\\'inez-Mares","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2011-04-13T22:47:07Z","title":"Scattering matrix of elliptically polarized waves"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.2638","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:a10369debadb7748d717a2a023f7699a4ff6e563797c90d7ab855bb8e1bfb8fb","target":"record","created_at":"2026-05-18T04:24:27Z","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":"087e358c5f9e5c7ae635241a65effe1d1a1bc31efc7d0e7d364d0e14b8983217","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2011-04-13T22:47:07Z","title_canon_sha256":"c8d5a63f4fcebebfc6a9a0256d84cf267c5df80ea80f54be6fa0cdf9907e3740"},"schema_version":"1.0","source":{"id":"1104.2638","kind":"arxiv","version":1}},"canonical_sha256":"89a2d6bb070019223178201a6f900ac18bbc3621c5a8992d5a29b75bbfeb8422","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89a2d6bb070019223178201a6f900ac18bbc3621c5a8992d5a29b75bbfeb8422","first_computed_at":"2026-05-18T04:24:27.179829Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:24:27.179829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wD+BndEVFXMf5nsmxzGhDpzbMfFiRutxpRknVoB5dEYRcy2OaTLCS6Q0ZqSUhlxCML4lUHbqTcDpmW9ma3iDAw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:24:27.180312Z","signed_message":"canonical_sha256_bytes"},"source_id":"1104.2638","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a10369debadb7748d717a2a023f7699a4ff6e563797c90d7ab855bb8e1bfb8fb","sha256:85b51fe369bfc12ae040c4c92fdd930161a4c33f3b1761cce7a874af0145e7c1"],"state_sha256":"3fa3aca2ca6a8c18e2d9a68a310b82b2bf5006f29a6923ae0aad9b31ce9ab9d2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oBuGEZo5Qnp0PjqMNf+fYKMqevN0AT7VUmEOJBAd6aXzRJdj4NpTfFgs3QrCVQ+xQYgnd0Uzg0cqTkwxHrWhBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T16:31:01.423308Z","bundle_sha256":"a6b87134c31f721c6d4ab1fec7c9b0dc18317c3c759e5e1c29cec7a7fdb66031"}}