{"as_of":"2026-08-17T07:23:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:a3638c25d873db38df332790633466d234497a29e565c9f138cfd780a149cf81","coverage":[{"denominator":28,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":28,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T15:27:21.279127Z","state":"measured"},{"denominator":28,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":28,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1908.01157/citation-record","integrity":"/paper/1908.01157/integrity","json":"/paper/1908.01157/citation-record.json","paper":"/paper/1908.01157"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.567241Z","title":"Chiral plasmonics","venue":null,"work_id":"7b21cd36-430b-41d9-92eb-85a611536df0","year":2017},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.192269Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:45a66d661cace41f32fcf39e38a69253b1d71954f4766f0aa420dd0005d5da2a","observation_id":"2426a68d-ffa6-42b7-b398-6a60487847bb","resolution":{"observed_at":"2026-08-14T15:27:21.570667Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.556145Z","title":"Tailoring enhanced optical chirality: design principles for chiral plasmonic nanostr uctures","venue":null,"work_id":"0eb86f75-541d-4311-8912-87b5d758838d","year":2012},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.195816Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:ba4f6668fd21bffdb7375e75099d2f63a258123ab44dc24ab1217addb9ba3e9e","observation_id":"02f10147-45a6-491b-aacf-c3536ad74b29","resolution":{"observed_at":"2026-08-14T15:27:21.560705Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.545566Z","title":"Chiral light design and detection inspired by optical antenna theory","venue":null,"work_id":"3737d094-f146-47af-b5fa-27fb5b4f379c","year":2018},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.199557Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:31d414832a04fca0c4f61215b8a5d94d1a19cfe0b510e5c83e46b2fd1f65415d","observation_id":"a1b2be24-28a1-4948-955d-b9ad3b27f159","resolution":{"observed_at":"2026-08-14T15:27:21.549884Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.535237Z","title":"Probing t he chiral nature of electromagnetic fields surrounding plasmonic nanostructures","venue":null,"work_id":"5aa8fdbb-70b7-4ad7-acf8-9baa429cf687","year":2013},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.203293Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:cb2caf75f295dcec046e106de3fecef7fd6823ee9b23ac8e0f43fc6221e4a9e4","observation_id":"dd97a19a-6b93-4465-8bc6-ce2c3df827af","resolution":{"observed_at":"2026-08-14T15:27:21.539206Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.524998Z","title":"Taminiau, R","venue":null,"work_id":"95a3e7d1-3bf3-43b7-adc8-799c6aa1556f","year":2007},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.206511Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:b64ddeac5d6b3da3331a2667ef7400685bc14ea04aff7afe766da9c68a71634f","observation_id":"f4a1a190-f280-4e3d-a994-b2a185663110","resolution":{"observed_at":"2026-08-14T15:27:21.528746Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.515471Z","title":"Burresi, D","venue":null,"work_id":"3278606f-a16e-4ae6-aa6c-82ec210b28da","year":2009},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.210251Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:50481c790eb785d4cae5ab5dffbd6bda9ebdcd7903b62ac135b70ad094310048","observation_id":"22cd5bfa-77ef-44f4-949a-046e19a4adcc","resolution":{"observed_at":"2026-08-14T15:27:21.519144Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.506209Z","title":"Hybrid photonic antennas for subnanometer multicolor localization and nanoimaging of s ingle molecules","venue":null,"work_id":"7f4a5cd0-78e0-415b-a212-0b2583f9df55","year":2014},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.214243Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:7ae85f55749bdba6e094179db3f617547611a4a30ce980fd3e1959b05aa8c75b","observation_id":"9b8c71d5-769a-464e-82e0-f0eae6f0ea29","resolution":{"observed_at":"2026-08-14T15:27:21.509771Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.497573Z","title":"Murphy-DuBay, L","venue":null,"work_id":"06a6b741-c7b9-4aa1-bf74-852e2cf64d53","year":2008},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.217348Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:d6cd7c994fb8fa6dd5d1a17286058a617500a8d9d286a0661f001bc5c9b2b018","observation_id":"57606285-fcb9-427b-962e-e7d521f3d4a5","resolution":{"observed_at":"2026-08-14T15:27:21.500783Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.488618Z","title":"Grosjean, I","venue":null,"work_id":"ae4313a0-6734-448a-ad30-2ef9898dc96c","year":2010},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.220327Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:bb1d5b7f8c708ed2e7c41c0b055bdad295b544ca82c5fd4c8860516b06eeade8","observation_id":"6c2c94e7-f908-475a-9c5b-001bd60176ce","resolution":{"observed_at":"2026-08-14T15:27:21.492049Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.479569Z","title":"Near-field probing of slow bloch modes on photonic crystals with a nanoantenna","venue":null,"work_id":"89e84b7c-1e88-4eef-8a7a-f5969fab8097","year":2012},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.223736Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:af3f1a7b31216416c0321ef3467c45174dc00dc18a27de4508d1e27b5bd2f32f","observation_id":"103457a4-977e-4cf3-9496-62c34a60bf13","resolution":{"observed_at":"2026-08-14T15:27:21.482818Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.470578Z","title":"Plas- monic nanofocusing with a metallic pyramid and an integrate d c-shaped aperture","venue":null,"work_id":"280e7742-9bd4-4c9c-b679-7d5a54a6ec29","year":2013},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.226771Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:fdaf943824a891c6e8bf881ab963faf05d518f29057aa448d906391f162b141d","observation_id":"efcba357-6a73-4442-8b88-75b6da53ac4b","resolution":{"observed_at":"2026-08-14T15:27:21.473845Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.461464Z","title":"Doubly resonant photonic antenna for single infrared quantum dot imaging at telecommunication wavelengths","venue":null,"work_id":"5f2eb736-c606-4a2d-a133-f12efc7fa379","year":2017},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.229667Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:716d3c73e471de1286f226d124445b06871f44d77160d96a5aa377bd5cf731cf","observation_id":"df829754-b037-4542-bd3e-fb1f7a0750fb","resolution":{"observed_at":"2026-08-14T15:27:21.464769Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.451808Z","title":"Optical and infrar ed helical metamaterials","venue":null,"work_id":"208a0613-27b2-406b-8844-c4dfa00e6236","year":2016},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.232554Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:2069f173b9c9bdd057ecf0e4a4a0173abff67d9f3550ccaf50cd2671498a697e","observation_id":"b3edf8c7-78f9-4354-a7f4-bc4bb91f2f12","resolution":{"observed_at":"2026-08-14T15:27:21.455203Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.442804Z","title":"Plasmonic nano helix metamaterials with tailorable giant circular dichroism","venue":null,"work_id":"f0b57aa6-d11c-43c3-b923-699ee00b5d50","year":2013},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.236572Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:bc7dfb6984f4a0dacc40723819776d6af4485d3bed11d90fe211d17bbb10bc9c","observation_id":"a1f9ccfc-b928-44f4-b857-a17b915bddea","resolution":{"observed_at":"2026-08-14T15:27:21.446264Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.433902Z","title":"Nanoscale 3d chiral plasmonic helices with circular dichroism at visible frequencies","venue":null,"work_id":"ed929350-29c9-4316-8b20-7d8ec642f478","year":2014},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.239925Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:a444c9335f783a938d8863c8446494af6c6f1f7cf7bf67afa30c2ba4e829d520","observation_id":"fd5bd66f-dac1-43f8-b494-a654b9e824b1","resolution":{"observed_at":"2026-08-14T15:27:21.437431Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.425116Z","title":"Triple-helical nanowires by tomographic rotatory growth for chiral photonics","venue":null,"work_id":"eb438576-6e57-4410-a81b-2a4dbd1bc572","year":2015},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.242918Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:5f7ea77210235b29088128e2d28575a10dcfe6e817eb3a88bbbe2a2c0a524cdf","observation_id":"3f3a0ae2-96d7-450a-9e0e-0aa3a00ba55f","resolution":{"observed_at":"2026-08-14T15:27:21.428381Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.416642Z","title":"Gold helix pho tonic metamaterial as broadband circular polarizer","venue":null,"work_id":"117e8097-bccd-4631-bf86-327e27e5eac8","year":2009},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.245817Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:a22ba24fe9effd1224bcc80127bab56f76c8b9735c56cc1b105bd870d259cbe3","observation_id":"ff9a35cd-54f0-40be-9080-97b424f5412b","resolution":{"observed_at":"2026-08-14T15:27:21.419810Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.407133Z","title":"Core– shell plasmonic nanohelices","venue":null,"work_id":"49f5c245-80c8-4fdc-b149-66540f3e8767","year":2017},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.248824Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:da4de18d9c94d14442a67467c80b863523a4cb1b2f7fa6b8d78b1a7c28a8a8df","observation_id":"4001f76e-c5a3-48ec-934a-cced62032b40","resolution":{"observed_at":"2026-08-14T15:27:21.411012Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.398016Z","title":"Helical plasmonic nanostructures as prototypical chiral near-field sources","venue":null,"work_id":"da2822fc-87f5-4ce1-8f07-d22521a09f86","year":2014},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.251642Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:0f59ddaa348bdcf743a30a647ae42379afd6b22970b306b970275fb339b532e8","observation_id":"020b93d1-5fa2-4aa1-9ccd-3ab6c3dc5c0e","resolution":{"observed_at":"2026-08-14T15:27:21.401469Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.388063Z","title":"Chiroptical response of a single plasmonic na nohelix","venue":null,"work_id":"4f554b94-e92d-4f8f-b755-8016e4320297","year":2018},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.254527Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:11246e90b39334bc4afa1d9f3dc02a5b9a0b450a448d76d0e458b00b845d5d83","observation_id":"2d8c8c42-dda6-4f2a-bf39-7169e920c4f1","resolution":{"observed_at":"2026-08-14T15:27:21.391920Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.378812Z","title":"Interaction of light carrying orbital angular momentum with a chiral dipolar sca tterer","venue":null,"work_id":"7d40d9fa-cf91-4774-8552-d69cffba7ddc","year":2019},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.257461Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:4b7dc1e1d4ec4e924e86c82a70cafe3499264c523c47bdb80e7d9e3213218af7","observation_id":"c5fbd691-6d10-4ce2-b1e8-809bdebca932","resolution":{"observed_at":"2026-08-14T15:27:21.382043Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.06527","last_updated":"2018-12-16T19:45:17Z","snapshot_observed_at":"2026-08-14T17:42:52.000390Z","submitted_at":"2018-12-16T19:45:17Z","title":"Controlling light polarization by swirling surface plasmons","version":1},"cited_work":{"arxiv_id":"1812.06527","doi":null,"metadata_source":"pith","pith_arxiv_id":"1812.06527","snapshot_observed_at":"2026-08-14T15:27:21.306196Z","title":"Controlling light polarization by swirling surface plasmons","venue":"physics.optics","work_id":"98013a7c-d7a8-460f-a493-71eb36d21cd6","year":2018},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.260525Z"},"links":{"cited_paper":"/paper/1812.06527","citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:b4c626bbe4491e9617810c78f9522c396a3e34aae748e9c7a035ae009bd0555a","observation_id":"411a2a2b-95de-413d-a94b-747d8393e9cd","resolution":{"observed_at":"2026-08-14T15:27:21.312783Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.368931Z","title":"Nanoscopic control a nd quantification of enantioselective optical forces","venue":null,"work_id":"0c1ae30e-840c-42a5-8343-0f62f77a8f9f","year":2017},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.263961Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:a0e4023df9452b6d61c8d5a067628d72634c61ba0b5e5d70e6975026fa570d1d","observation_id":"12b2f12c-7b6c-4d3d-b841-433095fae22b","resolution":{"observed_at":"2026-08-14T15:27:21.373030Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.358430Z","title":"Programm able extreme chirality in the visible by helix-shaped metamaterial platform","venue":null,"work_id":"db940877-eb38-4384-92b9-d2bf27100840","year":2016},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.267529Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:7ee0133ff198fcf9bcd29bcbf3e0ee8797ad529d639b9ea5a9d13d9a34d89bba","observation_id":"0f270247-652d-45bf-9ae7-70dd3b3ad823","resolution":{"observed_at":"2026-08-14T15:27:21.362683Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.348541Z","title":null,"venue":null,"work_id":"c18afae0-8a17-433e-b02b-2d1b8fa78824","year":1997},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.270452Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:f7e213f5cb107818c2b3e19caa7311d343af9e2e6e7d432d3f37840f5cbe11d6","observation_id":"a50192f0-a375-4aac-9c99-dfa21f5c8d33","resolution":{"observed_at":"2026-08-14T15:27:21.352002Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.339136Z","title":"Antennas and wave propagation","venue":null,"work_id":"05702981-b033-4245-9016-f7921a451fa9","year":2006},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.273319Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:44a9aee78965bf183cda4d359cf24798a640e5a3c47e34e53a8e792aa7949d45","observation_id":"81b2ebbc-d4a2-44b2-9090-c332e4e5ff32","resolution":{"observed_at":"2026-08-14T15:27:21.342569Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.329202Z","title":"Extraordinary transmis- sion through a single coaxial aperture in a thin metal film","venue":null,"work_id":"1738d26d-d683-499c-9c3c-fe67b5705fd8","year":2010},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.276295Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:2b2f49172cbdbb25e209f6187d7adab0ee1936b6355419bb207f459ae9dc0174","observation_id":"de439bbc-f5fa-40e7-9170-c9233b5b79b6","resolution":{"observed_at":"2026-08-14T15:27:21.332692Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T15:27:21.319341Z","title":"Enhanced transmission through subwavelen gth metallic coaxial apertures by excitation of the TEM mode","venue":null,"work_id":"37dce29a-f9e2-41aa-a55f-d223469da14a","year":2007},"citing_paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T15:27:21.279127Z"},"links":{"citing_paper":"/paper/1908.01157"},"observation_digest":"sha256:538dfccbb8069b9cfbd6e562e94559f2d13106f31bed8601c30016924e846913","observation_id":"4c0c4480-b2ff-4d55-8099-c9e6290731bd","resolution":{"observed_at":"2026-08-14T15:27:21.322899Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"1908.01157","last_updated":"2019-08-03T12:28:17Z","latest_version":1,"primary_category":"physics.optics","snapshot_observed_at":"2026-08-14T15:19:42.380821Z","submitted_at":"2019-08-03T12:28:17Z","title":"Individual plasmonic helix for probing light chirality"},"reference_resolution":{"displayed":28,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":1,"verified_exact":1,"verified_fuzzy":26},"total_outbound_references":28},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 17 August 2026, this Paper Citation Record lists 28 of 28 outbound references and 0 inbound Pith citation observations for arXiv:1908.01157."}