1.Department of Electrical and Computer Engineering, University of Utah, Salt Lake City, UT 84112, USA
2.Tata Institute for Fundamental Research, Mumbai 400005, India
A Nahata, Email: nahata@ece.utah.edu
纸质出版日期:2017-06,
网络出版日期:2016-09-27,
收稿日期:2016-03-14,
修回日期:2016-09-14,
录用日期:2016-09-26
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Direct observation of Anderson localization in plasmonic terahertz devices[J]. LSA, 2017,6(2).
Pandey, S. et al. Direct observation of Anderson localization in plasmonic terahertz devices. Light: Science & Applications, 6, e16232 (2017).
Direct observation of Anderson localization in plasmonic terahertz devices[J]. LSA, 2017,6(2). DOI: 10.1038/lsa.2016.232.
Pandey, S. et al. Direct observation of Anderson localization in plasmonic terahertz devices. Light: Science & Applications, 6, e16232 (2017). DOI: 10.1038/lsa.2016.232.
We present the first experimental observation of Anderson localization in the terahertz frequency range using plasmonic structures. To accomplish this goal
we designed THz waveguides consisting of a one-dimensional array of rectangular apertures that were fabricated in a freestanding metal foil. Disorder is introduced into the waveguide by offsetting the position of each aperture by a random distance within a prescribed range. For example
for a waveguide with apertures spaced by 250 μm in a periodic waveguide
10% disorder would correspond to the apertures being shifted by a random value between ±25 μm along the waveguide axis. We find that for disorder levels below 25%
there is only an increase in the propagation loss along the device. However
for two specific waveguides with 25% disorder
we observe a spatially localized mode that lies just within the stop band of the device and exhibits a double-sided exponential spatial decay away from the maximum.
Anderson localizationdisordered medium1D aperiodic latticeterahertz plasmonicsterahertz waveguidestime domain spectroscopy
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