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Wavelength-scale errors in optical localization due to spin-orbit coupling of light

Far-field optical imaging techniques allow the determination of the position of point-like emitters and scatterers [1–3]. Although the optical wavelength sets a fundamental limit to the image resolution of unknown objects, the position of an individual emitter can in principle be estimated from the...

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Detalles Bibliográficos
Autores principales: Araneda, G., Walser, S., Colombe, Y., Higginbottom, D. B., Volz, J., Blatt, R., Rauschenbeutel, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6398575/
https://www.ncbi.nlm.nih.gov/pubmed/30854021
http://dx.doi.org/10.1038/s41567-018-0301-y
Descripción
Sumario:Far-field optical imaging techniques allow the determination of the position of point-like emitters and scatterers [1–3]. Although the optical wavelength sets a fundamental limit to the image resolution of unknown objects, the position of an individual emitter can in principle be estimated from the image with arbitrary precision. This is used for example in the determination of stars position [4] or in optical super-resolution microscopy [5]. Furthermore, precise position determination is an experimental prerequisite for the manipulation and measurement of individual quantum systems, such as atoms, ions, and solid-state-based quantum emitters [6–8]. Here we demonstrate that spin-orbit coupling of light in the emission of elliptically polarized emitters can lead to systematic, wavelength-scale errors in the estimation of the emitters position. Imaging a single trapped atom as well as a single sub-wavelength-diameter gold nanoparticle, we demonstrate a shift between the emitters measured and actual positions which is comparable to the optical wavelength. For certain settings, the expected shift can become arbitrarily large. Beyond optical imaging techniques, our findings could be relevant for the localization of objects using any type of wave that carries orbital angular momentum relative to the emitters position with a component orthogonal to the direction of observation.