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Tailoring Second-Harmonic Emission from (111)-GaAs Nanoantennas.
Sautter, Jürgen D; Xu, Lei; Miroshnichenko, Andrey E; Lysevych, Mykhaylo; Volkovskaya, Irina; Smirnova, Daria A; Camacho-Morales, Rocio; Zangeneh Kamali, Khosro; Karouta, Fouad; Vora, Kaushal; Tan, Hoe H; Kauranen, Martti; Staude, Isabelle; Jagadish, Chennupati; Neshev, Dragomir N; Rahmani, Mohsen.
Afiliación
  • Sautter JD; Nonlinear Physics Centre, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 Australia.
  • Xu L; Institute of Applied Physics, Abbe Center of Photonics , Friedrich Schiller University Jena , 07745 Jena , Germany.
  • Miroshnichenko AE; School of Engineering and Information Technology , University of New South Wales , Canberra , ACT 2600 , Australia.
  • Lysevych M; School of Engineering and Information Technology , University of New South Wales , Canberra , ACT 2600 , Australia.
  • Volkovskaya I; Department of Electronic Materials Engineering, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 , Australia.
  • Smirnova DA; Institute of Applied Physics , Russian Academy of Sciences , Nizhny Novgorod 603950 , Russia.
  • Camacho-Morales R; Nonlinear Physics Centre, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 Australia.
  • Zangeneh Kamali K; Nonlinear Physics Centre, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 Australia.
  • Karouta F; Nonlinear Physics Centre, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 Australia.
  • Vora K; Department of Electronic Materials Engineering, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 , Australia.
  • Tan HH; Department of Electronic Materials Engineering, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 , Australia.
  • Kauranen M; Department of Electronic Materials Engineering, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 , Australia.
  • Staude I; Photonics Laboratory, Physics Unit , Tampere University , P.O. Box 692, FI-33014 Tampere , Finland.
  • Jagadish C; Institute of Applied Physics, Abbe Center of Photonics , Friedrich Schiller University Jena , 07745 Jena , Germany.
  • Neshev DN; Department of Electronic Materials Engineering, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 , Australia.
  • Rahmani M; Nonlinear Physics Centre, Research School of Physics and Engineering , The Australian National University , Canberra , ACT 2601 Australia.
Nano Lett ; 19(6): 3905-3911, 2019 06 12.
Article en En | MEDLINE | ID: mdl-31136193
ABSTRACT
Second-harmonic generation (SHG) in resonant dielectric Mie-scattering nanoparticles has been hailed as a powerful platform for nonlinear light sources. While bulk-SHG is suppressed in elemental semiconductors, for example, silicon and germanium due to their centrosymmetry, the group of zincblende III-V compound semiconductors, especially (100)-grown AlGaAs and GaAs, have recently been presented as promising alternatives. However, major obstacles to push the technology toward practical applications are the limited control over directionality of the SH emission and especially zero forward/backward radiation, resulting from the peculiar nature of the second-order nonlinear susceptibility of this otherwise highly promising group of semiconductors. Furthermore, the generated SH signal for (100)-GaAs nanoparticles depends strongly on the polarization of the pump. In this work, we provide both theoretically and experimentally a solution to these problems by presenting the first SHG nanoantennas made from (111)-GaAs embedded in a low index material. These nanoantennas show superior forward directionality compared to their (100)-counterparts. Most importantly, based on the special symmetry of the crystalline structure, it is possible to manipulate the SHG radiation pattern of the nanoantennas by changing the pump polarization without affecting the linear properties and the total nonlinear conversion efficiency, hence paving the way for efficient and flexible nonlinear beam-shaping devices.
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Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: Nano Lett Año: 2019 Tipo del documento: Article

Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: Nano Lett Año: 2019 Tipo del documento: Article