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Showing posts with label L. Schell. Show all posts
Showing posts with label L. Schell. Show all posts
Friday, September 15, 2017
Abstract-Magnetoresistance oscillations induced by high-intensity terahertz radiation
T. Herrmann, Z. D. Kvon, I. A. Dmitriev, D. A. Kozlov, B. Jentzsch, M. Schneider, L. Schell, V. V. Bel’kov, A. Bayer, D. Schuh, D. Bougeard, T. Kuczmik, M. Oltscher, D. Weiss, and S. D. Ganichev
https://journals.aps.org/prb/accepted/7a079Oe8S5a1573025948ef2a7974268293e8629a
We report on observation of pronounced terahertz radiation-induced magneto-resistivity oscillations in AlGaAs/GaAs two-dimensional electron systems, the THz analog of the microwave induced resistivity oscillations (MIRO). Applying high power radiation of a pulsed molecular laser we demonstrate that MIRO, so far observed at low power only, are not destroyed even at very high intensities. Experiments with radiation intensity ranging over five orders of magnitude from 0.1 W/cm2 to 104 W/cm2 reveal high-power saturation of the MIRO amplitude, which is well described by an empirical fit function I/(1+I/I_s)^\beta with \beta~\sim 1. The saturation intensity I_s is of the order of tens of W/cm2and increases by six times by increasing the radiation frequency from 0.6 to 1.1~THz. The results are discussed in terms of microscopic mechanisms of MIRO and compared to nonlinear effects observed earlier at significantly lower excitation frequencies.
Labels:
A. Bayer,
B. Jentzsch,
D. A. Kozlov,
D. Bougeard,
D. Schuh,
D. Weiss,
I. A. Dmitriev,
L. Schell,
M. Oltscher,
M. Schneider,
S. D. Ganichev,
T. Herrmann,
T. Kuczmik,
V. V. Bel’kov,
Z. D. Kvon
Sunday, June 25, 2017
Abstract-Magneto-resistance oscillations induced by high-intensity terahertz radiation
T. Herrmann, Z. D. Kvon, I. A. Dmitriev, D. A. Kozlov, B. Jentzsch, M. Schneider, L. Schell, V. V. Bel'kov, A. Bayer, D. Schuh, D. Bougeard, T. Kuczmik, M. Oltscher, D. Weiss, S. D. Ganichev
(Submitted on 22 Jun 2017)
We report on observation of pronounced terahertz radiation-induced magneto-resistivity oscillations in AlGaAs/GaAs two-dimensional electron systems, the THz analog of the microwave induced resistivity oscillations (MIRO). Applying high power radiation of a pulsed molecular laser we demonstrate that MIRO, so far observed at low power only, are not destroyed even at very high intensities. Experiments with radiation intensity ranging over five orders of magnitude from0.1 W/cm2 to104 W/cm2 reveal high-power saturation of the MIRO amplitude, which is well described by an empirical fit functionI/(1+I/Is)β withβ∼1 . The saturation intensity Is is of the order of tens of W/cm2 and increases by six times by increasing the radiation frequency from0.6 to1.1 THz. The results are discussed in terms of microscopic mechanisms of MIRO and compared to nonlinear effects observed earlier at significantly lower excitation frequencies.
Monday, August 24, 2015
Abstract-Helicity sensitive terahertz radiation detection by dual-grating-gate high electron mobility transistors
P. Faltermeier1, P. Olbrich1, W. Probst1, L. Schell1, T. Watanabe2, S. A. Boubanga-Tombet2, T. Otsuji2 and S. D. Ganichev1
We report on the observation of a radiation helicity sensitive photocurrent excited by terahertz (THz) radiation in dual-grating-gate (DGG) InAlAs/InGaAs/InAlAs/InP high electron mobility transistors (HEMT). For a circular polarization, the current measured between source and drain contacts changes its sign with the inversion of the radiation helicity. For elliptically polarizedradiation, the total current is described by superposition of the Stokes parameters with different weights. Moreover, by variation of gate voltages applied to individual gratings, the photocurrentcan be defined either by the Stokes parameter defining the radiation helicity or those for linearpolarization. We show that artificial non-centrosymmetric microperiodic structures with a two-dimensional electron system excited by THz radiation exhibit a dc photocurrent caused by the combined action of a spatially periodic in-plane potential and spatially modulated light. The results provide a proof of principle for the application of DGG HEMT for all-electric detection of the radiation's polarization state.
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