The 80th JSAP Autumn Meeting 2019

Presentation information

Oral presentation

13 Semiconductors » 13.6 Nanostructures, quantum phenomena, and nano quantum devices

[19p-C309-1~16] 13.6 Nanostructures, quantum phenomena, and nano quantum devices

Thu. Sep 19, 2019 1:45 PM - 6:30 PM C309 (C309)

Toshiyuki Ihara(NICT), Toshihiro Nakaoka(Sophia Univ.)

1:45 PM - 2:30 PM

[19p-C309-1] [INVITED] Resonantly Excited Excitons for Second-Order Optical Non-Linearity and Realisation of a Broadly Tuneable THz Source and Absorption Spectrometer

Richard Hogg1, Avan Majeed2, Pavlo Ivanov1, Benjamin Stevens2, Edmund Clarke3, Iain Butler1, David Childs1, Osamu Kojima4 (1.James Watt School of Engineering, University of Glasgow, UK, 2.EEE Department, University of Sheffield, UK, 3.EPSRC National Epitaxy Facility, University of Sheffield, UK, 4.Graduate School of Engineering, Kobe University, Japan)

Keywords:Resonant Excitonic, THz source, Tuneable

A broadly tunable THz source is realized via difference frequency generation utilising resonant excitation of GaAs/AlAs quantum well excitons at room temperature. Resonant excitation results in an enhancement to χ(3). Symmetry breaking of the electronic wavefunctions is made by utilizing a built-in electric-field across a p–i–n junction, resulting in effective χ(2) processes derived from χ(3).
Nonlinear processes occur at ~4 W cm−2 enabling area and power scaling of the THz emitter. Phase matching is realized laterally through normal incidence excitation, akin to two colour interference.
Collimated 130 mW continuous wave (CW) semiconductor lasers with ~1mm beam diameters are used, with one resonant with the heavy-hole exciton, whilst the other is tuned through the excitonic absorption bands.
A THz signal is generated from 0.2–6 THz and efficiencies of ~3 × 10–5, realising ~9 μW of THz power.
We show transmission spectroscopy of atmospheric features, indicating ~20GHz linewidths.