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A nanophotonic interferometer
The transmission of light through sub-wavelength apertures (zero-mode waveguides, ZMW) in metal films is well-explored. It introduces both an amplitude modulation as well as a phase shift to the oscillating electromagnetic field. We propose a nanophotonic interferometer by bringing two ZMW (∼100 nm...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
IOP Publishing
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9930208/ https://www.ncbi.nlm.nih.gov/pubmed/36652697 http://dx.doi.org/10.1088/1361-6528/acb443 |
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author | Ghaffari, Abbas Kashani, Somayeh Do, Kevin Weninger, Keith Riehn, Robert |
author_facet | Ghaffari, Abbas Kashani, Somayeh Do, Kevin Weninger, Keith Riehn, Robert |
author_sort | Ghaffari, Abbas |
collection | PubMed |
description | The transmission of light through sub-wavelength apertures (zero-mode waveguides, ZMW) in metal films is well-explored. It introduces both an amplitude modulation as well as a phase shift to the oscillating electromagnetic field. We propose a nanophotonic interferometer by bringing two ZMW (∼100 nm diameter) in proximity and monitoring the distribution of transmitted light in the back-focal plane of collecting microscope objective (1.3 N.A.). We demonstrate that both an asymmetry induced by the binding of a quantum dot in one of the two ZMW, as well as an asymmetry in ZMW diameter yield qualitatively similar transmission patterns. We find that the complex pattern can be quantified through a scalar measure of asymmetry along the symmetry axis of the aperture pair. In a combined experimental and computational exploration of detectors with differing ZMW diameters, we find that the scalar asymmetry is a monotonous function of the diameter difference of the two apertures, and that the scalar asymmetry measure is higher if the sample is slightly displaced from the focal plane of the collecting microscope objective. An optimization of the detector geometry determined that the maximum response is achieved at an aperture separation that is comparable to the wavelength on the exit side of the sensor. For small separations of apertures, on the order of a quarter of the wavelength and less, the signal is strongly polarization dependent, while for larger separations, on the order of the wavelength or larger, the signal becomes essentially polarization-independent. |
format | Online Article Text |
id | pubmed-9930208 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | IOP Publishing |
record_format | MEDLINE/PubMed |
spelling | pubmed-99302082023-02-16 A nanophotonic interferometer Ghaffari, Abbas Kashani, Somayeh Do, Kevin Weninger, Keith Riehn, Robert Nanotechnology Paper The transmission of light through sub-wavelength apertures (zero-mode waveguides, ZMW) in metal films is well-explored. It introduces both an amplitude modulation as well as a phase shift to the oscillating electromagnetic field. We propose a nanophotonic interferometer by bringing two ZMW (∼100 nm diameter) in proximity and monitoring the distribution of transmitted light in the back-focal plane of collecting microscope objective (1.3 N.A.). We demonstrate that both an asymmetry induced by the binding of a quantum dot in one of the two ZMW, as well as an asymmetry in ZMW diameter yield qualitatively similar transmission patterns. We find that the complex pattern can be quantified through a scalar measure of asymmetry along the symmetry axis of the aperture pair. In a combined experimental and computational exploration of detectors with differing ZMW diameters, we find that the scalar asymmetry is a monotonous function of the diameter difference of the two apertures, and that the scalar asymmetry measure is higher if the sample is slightly displaced from the focal plane of the collecting microscope objective. An optimization of the detector geometry determined that the maximum response is achieved at an aperture separation that is comparable to the wavelength on the exit side of the sensor. For small separations of apertures, on the order of a quarter of the wavelength and less, the signal is strongly polarization dependent, while for larger separations, on the order of the wavelength or larger, the signal becomes essentially polarization-independent. IOP Publishing 2023-04-30 2023-02-15 /pmc/articles/PMC9930208/ /pubmed/36652697 http://dx.doi.org/10.1088/1361-6528/acb443 Text en © 2023 The Author(s). Published by IOP Publishing Ltd https://creativecommons.org/licenses/by/4.0/Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence (https://creativecommons.org/licenses/by/4.0/) . Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. |
spellingShingle | Paper Ghaffari, Abbas Kashani, Somayeh Do, Kevin Weninger, Keith Riehn, Robert A nanophotonic interferometer |
title | A nanophotonic interferometer |
title_full | A nanophotonic interferometer |
title_fullStr | A nanophotonic interferometer |
title_full_unstemmed | A nanophotonic interferometer |
title_short | A nanophotonic interferometer |
title_sort | nanophotonic interferometer |
topic | Paper |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9930208/ https://www.ncbi.nlm.nih.gov/pubmed/36652697 http://dx.doi.org/10.1088/1361-6528/acb443 |
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