
1.Physikalisches Institut, Johann Wolfgang Goethe-Universität, Max-von-LaueStr. 1, D-60438 Frankfurt am Main, Germany
2.Institut für Angewandte Physik, Technische Universität Dresden, Nöthnitzer Str. 61, D-01187 Dresden, Germany
3.Department of Microtechnology and Nanoscience, Chalmers University of Technology, SE-41296 Gothenburg, Sweden
4.Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstraße 400, D-01328 Dresden, Germany
5.Complexity and Topology in Quantum Matter (CT.QMAT), Cluster of Excellence EXC 2147, Dresden/ Würzburg, Germany
6.Present address: Department of Electronics and Nanoengineering, Aalto University, Tietotie 3, 02150, Espoo, Finland
Amin Soltani (soltani@physik.uni-frankfurt.de)
Hartmut G. Roskos (roskos@physik.uni-frankfurt.de)
Published:2020,
Published Online:04 June 2020,
Received:09 July 2019,
Revised:27 March 2020,
Accepted:22 April 2020
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Soltani, A. et al. Direct nanoscopic observation of plasma waves in the channel of a graphene field-effect transistor. Light: Science & Applications, 9, 867-873 (2020).
Soltani, A. et al. Direct nanoscopic observation of plasma waves in the channel of a graphene field-effect transistor. Light: Science & Applications, 9, 867-873 (2020). DOI: 10.1038/s41377-020-0321-0.
Plasma waves play an important role in many solid-state phenomena and devices. They also become significant in electronic device structures as the operation frequencies of these devices increase. A prominent example is field-effect transistors (FETs)
that witness increased attention for application as rectifying detectors and mixers of electromagnetic waves at gigahertz and terahertz frequencies
where they exhibit very good sensitivity even high above the cut-off frequency defined by the carrier transit time. Transport theory predicts that the coupling of radiation at THz frequencies into the channel of an antenna-coupled FET leads to the development of a gated plasma wave
collectively involving the charge carriers of both the two-dimensional electron gas and the gate electrode. In this paper
we present the first direct visualization of these waves. Employing graphene FETs containing a buried gate electrode
we utilize near-field THz nanoscopy at room temperature to directly probe the envelope function of the electric field amplitude on the exposed graphene sheet and the neighboring antenna regions. Mapping of the field distribution documents that wave injection is unidirectional from the source side since the oscillating electrical potentials on the gate and drain are equalized by capacitive shunting. The plasma waves
excited at 2 THz
are overdamped
and their decay time lies in the range of 25–70 fs
. Despite this short decay time
the decay length is rather long
i.e.
0.3-0.5 μm
because of the rather large propagation speed of the plasma waves
which is found to lie in the range of 3.5–7 × 10
6
m/s
in good agreement with theory. The propagation speed depends only weakly on the gate voltage swing and is consistent with the theoretically predicted
$$ \frac{1}{4}$$
power law.
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