Second-Harmonic Generation in Mie-Resonant GaAs Nanowires
We investigate the enhancement of second-harmonic generation in cylindrical GaAs nanowires. Although these nanostructures confine light in two dimensions, power conversion efficiencies on the order of <inline-formula> <math display="inline"> <semantics> <mrow> <m...
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doaj-906ec2535e324618aa4c93f049d123c12020-11-25T01:02:13ZengMDPI AGApplied Sciences2076-34172019-08-01916338110.3390/app9163381app9163381Second-Harmonic Generation in Mie-Resonant GaAs NanowiresDomenico de Ceglia0Luca Carletti1Maria Antonietta Vincenti2Costantino De Angelis3Michael Scalora4Department of Information Engineering, University of Padova, 35131 Padova, ItalyDepartment of Information Engineering, University of Padova, 35131 Padova, ItalyDepartment of Information Engineering, University of Brescia, 25123 Brescia, ItalyDepartment of Information Engineering, University of Brescia, 25123 Brescia, ItalyCharles M. Bowden Research Lab, US Army AMRDEC, Huntsville, AL 35898, USAWe investigate the enhancement of second-harmonic generation in cylindrical GaAs nanowires. Although these nanostructures confine light in two dimensions, power conversion efficiencies on the order of <inline-formula> <math display="inline"> <semantics> <mrow> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>5</mn> </mrow> </msup> </mrow> </semantics> </math> </inline-formula> with a pump peak intensity of <inline-formula> <math display="inline"> <semantics> <mrow> <mo>~</mo> <mn>1</mn> <mo> </mo> <mi>GW</mi> <mo>/</mo> <msup> <mrow> <mi>cm</mi> </mrow> <mn>2</mn> </msup> </mrow> </semantics> </math> </inline-formula> are possible if the pump and the second-harmonic fields are coupled to the Mie-type resonances of the nanowire. We identify a large range of nanowire radii in which a double-resonance condition, i.e., both the pump and the second-harmonic fields excite normal modes of the nanowire, induces a high-quality-factor peak of conversion efficiency. We show that second-harmonic light can be scattered with large efficiency even if the second-harmonic photon energy is larger than 1.42 eV, i.e., the electronic bandgap of GaAs, above which the material is considered opaque. Finally, we evaluate the efficiency of one-photon absorption of second-harmonic light and find that resonant GaAs nanowires absorb second-harmonic light in the near-field region almost at the same rate at which they radiate second-harmonic light in the far-field region.https://www.mdpi.com/2076-3417/9/16/3381nanophotonicsnonlinear opticssecond-harmonic generationMie resonances |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Domenico de Ceglia Luca Carletti Maria Antonietta Vincenti Costantino De Angelis Michael Scalora |
spellingShingle |
Domenico de Ceglia Luca Carletti Maria Antonietta Vincenti Costantino De Angelis Michael Scalora Second-Harmonic Generation in Mie-Resonant GaAs Nanowires Applied Sciences nanophotonics nonlinear optics second-harmonic generation Mie resonances |
author_facet |
Domenico de Ceglia Luca Carletti Maria Antonietta Vincenti Costantino De Angelis Michael Scalora |
author_sort |
Domenico de Ceglia |
title |
Second-Harmonic Generation in Mie-Resonant GaAs Nanowires |
title_short |
Second-Harmonic Generation in Mie-Resonant GaAs Nanowires |
title_full |
Second-Harmonic Generation in Mie-Resonant GaAs Nanowires |
title_fullStr |
Second-Harmonic Generation in Mie-Resonant GaAs Nanowires |
title_full_unstemmed |
Second-Harmonic Generation in Mie-Resonant GaAs Nanowires |
title_sort |
second-harmonic generation in mie-resonant gaas nanowires |
publisher |
MDPI AG |
series |
Applied Sciences |
issn |
2076-3417 |
publishDate |
2019-08-01 |
description |
We investigate the enhancement of second-harmonic generation in cylindrical GaAs nanowires. Although these nanostructures confine light in two dimensions, power conversion efficiencies on the order of <inline-formula> <math display="inline"> <semantics> <mrow> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>5</mn> </mrow> </msup> </mrow> </semantics> </math> </inline-formula> with a pump peak intensity of <inline-formula> <math display="inline"> <semantics> <mrow> <mo>~</mo> <mn>1</mn> <mo> </mo> <mi>GW</mi> <mo>/</mo> <msup> <mrow> <mi>cm</mi> </mrow> <mn>2</mn> </msup> </mrow> </semantics> </math> </inline-formula> are possible if the pump and the second-harmonic fields are coupled to the Mie-type resonances of the nanowire. We identify a large range of nanowire radii in which a double-resonance condition, i.e., both the pump and the second-harmonic fields excite normal modes of the nanowire, induces a high-quality-factor peak of conversion efficiency. We show that second-harmonic light can be scattered with large efficiency even if the second-harmonic photon energy is larger than 1.42 eV, i.e., the electronic bandgap of GaAs, above which the material is considered opaque. Finally, we evaluate the efficiency of one-photon absorption of second-harmonic light and find that resonant GaAs nanowires absorb second-harmonic light in the near-field region almost at the same rate at which they radiate second-harmonic light in the far-field region. |
topic |
nanophotonics nonlinear optics second-harmonic generation Mie resonances |
url |
https://www.mdpi.com/2076-3417/9/16/3381 |
work_keys_str_mv |
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1725206022551764992 |