Cargando…

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...

Descripción completa

Detalles Bibliográficos
Autores principales: Ghaffari, Abbas, Kashani, Somayeh, Do, Kevin, Weninger, Keith, Riehn, Robert
Formato: Online Artículo Texto
Lenguaje:English
Publicado: IOP Publishing 2023
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
_version_ 1784889004459556864
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
work_keys_str_mv AT ghaffariabbas ananophotonicinterferometer
AT kashanisomayeh ananophotonicinterferometer
AT dokevin ananophotonicinterferometer
AT weningerkeith ananophotonicinterferometer
AT riehnrobert ananophotonicinterferometer
AT ghaffariabbas nanophotonicinterferometer
AT kashanisomayeh nanophotonicinterferometer
AT dokevin nanophotonicinterferometer
AT weningerkeith nanophotonicinterferometer
AT riehnrobert nanophotonicinterferometer