M. Tonouchi et al., CLASSICAL EDGE MAGNETOPLASMON IN A GAAS ALGAAS 2-DIMENSIONAL ELECTRON-SYSTEM/, Journal of the Physical Society of Japan, 63(12), 1994, pp. 4499-4505
We have studied the edge magnetoplasmon (EMP) in a GaAs/AlGaAs two-dim
ensional electron gas (2DEG) system under conditions where the quantum
Hall effect (QHE) is not observed; we call this a classical EMP. The
classical EMP's are excited in a 2DEG disk by radio frequency electric
field excitation (less than or equal to 1 GHz) in a high magnetic fie
ld B (less than or equal to 5 T) with the 2DEG sheet carrier density n
(s) between 2 x 10(15) m(-2) and 1 x 10(16) m(-2). The resonant freque
ncy is found to be almost proportional to n(s) and inversely proportio
nal to B, which agrees quantitatively with the theory proposed by Volk
ov and Mikhailov, Sov. Phys.-JETP 67 (1988) 1639 by assuming the effec
tive die-lectric constant <(epsilon)over cap>=(1+epsilon(GaAs))/2 wher
e epsilon(GaAs) is appropriate to the GaAs. A comparison of the experi
mental results with the calculations revealed that the electron mobili
ty plays an important role in the definition of the EMP frequency.