Nanowire Optoelectronics
Semiconductor nanowires have been used in a variety of passive and active optoelectronic devices including waveguides, photodetectors, solar cells, light-emitting diodes (LEDs), lasers, sensors, and optical antennas. We review the optical properties of these nanowires in terms of abso...
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2015-12-01
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Online Access: | https://doi.org/10.1515/nanoph-2015-0025 |
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doaj-f5b16ba791fa4ffa962dd6fd7b2328eb2021-09-06T19:20:29ZengDe GruyterNanophotonics2192-86062192-86142015-12-014449150210.1515/nanoph-2015-0025nanoph-2015-0025Nanowire OptoelectronicsWang Zhihuan0Nabet Bahram1Drexel University, Electrical and Computer Engineering Department, Philadelphia, PA, USA, 19104Drexel University, Electrical and Computer Engineering Department, Philadelphia, PA, USA, 19104Semiconductor nanowires have been used in a variety of passive and active optoelectronic devices including waveguides, photodetectors, solar cells, light-emitting diodes (LEDs), lasers, sensors, and optical antennas. We review the optical properties of these nanowires in terms of absorption, guiding, and radiation of light, which may be termed light management. Analysis of the interaction of light with long cylindrical/hexagonal structures with subwavelength diameters identifies radial resonant modes, such as Leaky Mode Resonances, or Whispering Gallery modes. The two-dimensional treatment should incorporate axial variations in “volumetric modes,”which have so far been presented in terms of Fabry–Perot (FP), and helical resonance modes. We report on finite-difference timedomain (FDTD) simulations with the aim of identifying the dependence of these modes on geometry (length, width), tapering, shape (cylindrical, hexagonal), core–shell versus core-only, and dielectric cores with semiconductor shells. This demonstrates how nanowires (NWs) form excellent optical cavities without the need for top and bottommirrors. However, optically equivalent structures such as hexagonal and cylindrical wires can have very different optoelectronic properties meaning that light management alone does not sufficiently describe the observed enhancement in upward (absorption) and downward transitions (emission) of light inNWs; rather, the electronic transition rates should be considered. We discuss this “rate management” scheme showing its strong dimensional dependence, making a case for photonic integrated circuits (PICs) that can take advantage of the confluence of the desirable optical and electronic properties of these nanostructures.https://doi.org/10.1515/nanoph-2015-0025nanowire photonics resonant modes light absorption spontaneous and stimulated emission transition rates core–shell nanowires |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Wang Zhihuan Nabet Bahram |
spellingShingle |
Wang Zhihuan Nabet Bahram Nanowire Optoelectronics Nanophotonics nanowire photonics resonant modes light absorption spontaneous and stimulated emission transition rates core–shell nanowires |
author_facet |
Wang Zhihuan Nabet Bahram |
author_sort |
Wang Zhihuan |
title |
Nanowire Optoelectronics |
title_short |
Nanowire Optoelectronics |
title_full |
Nanowire Optoelectronics |
title_fullStr |
Nanowire Optoelectronics |
title_full_unstemmed |
Nanowire Optoelectronics |
title_sort |
nanowire optoelectronics |
publisher |
De Gruyter |
series |
Nanophotonics |
issn |
2192-8606 2192-8614 |
publishDate |
2015-12-01 |
description |
Semiconductor nanowires have been used in a variety of passive and active
optoelectronic devices including waveguides, photodetectors, solar cells,
light-emitting diodes (LEDs), lasers, sensors, and optical antennas. We review
the optical properties of these nanowires in terms of absorption, guiding, and
radiation of light, which may be termed light management. Analysis of the
interaction of light with long cylindrical/hexagonal structures with
subwavelength diameters identifies radial resonant modes, such as Leaky Mode
Resonances, or Whispering Gallery modes. The two-dimensional treatment should
incorporate axial variations in “volumetric modes,”which have so far been
presented in terms of Fabry–Perot (FP), and helical resonance modes. We report
on finite-difference timedomain (FDTD) simulations with the aim of identifying
the dependence of these modes on geometry (length, width), tapering, shape
(cylindrical, hexagonal), core–shell versus core-only, and dielectric cores with
semiconductor shells. This demonstrates how nanowires (NWs) form excellent
optical cavities without the need for top and bottommirrors. However, optically
equivalent structures such as hexagonal and cylindrical wires can have very
different optoelectronic properties meaning that light management alone does not
sufficiently describe the observed enhancement in upward (absorption) and
downward transitions (emission) of light inNWs; rather, the electronic
transition rates should be considered. We discuss this “rate management” scheme
showing its strong dimensional dependence, making a case for photonic integrated
circuits (PICs) that can take advantage of the confluence of the desirable
optical and electronic properties of these nanostructures. |
topic |
nanowire photonics resonant modes light absorption spontaneous and stimulated emission transition rates core–shell nanowires |
url |
https://doi.org/10.1515/nanoph-2015-0025 |
work_keys_str_mv |
AT wangzhihuan nanowireoptoelectronics AT nabetbahram nanowireoptoelectronics |
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1717776749732823040 |