2017年第64回応用物理学会春季学術講演会

講演情報

一般セッション(口頭講演)

3 光・フォトニクス » 3.12 ナノ領域光科学・近接場光学

[15p-F202-1~11] 3.12 ナノ領域光科学・近接場光学

3.11と3.12のコードシェアセッションあり

2017年3月15日(水) 14:00 〜 17:00 F202 (F202)

井村 考平(早大)

14:45 〜 15:00

[15p-F202-4] グラフェンにおけるショット雑音のナノスケールイメージング

〇(PC)林 冠廷1、根間 裕史1、翁 銭春1、金 鮮美1、菅原 健太2、尾辻 泰一2、小宮山 進3、梶原 優介1 (1.東大生研、2.東北大通研、3.東大総文)

キーワード:近接場光顕微学、グラフェン、ショット雑音

There have been recently several advanced developments of graphene-based FET devices, such as ultra-high frequency optoelectronic or electron devices. The study of non-equilibrium electron kinetics (e.g. current fluctuation) in graphene devices, especially at the nanoscale, would be an important issue to be tackled at present. So far the vast majority of shot noise measurements have been restricted to the noise integrated in the whole conductor. The detection and the mapping of local shot-noise in real-space has remained to be an attractive and challenging task to be tackled by researchers for decades.
In this study, we present the first shot noise image on bilayer graphene with nanometer resolution, taken by using a passive THz scanning near-field optical microscope. A sharp metal tip scatters fluctuating evanescent fields (~20 THz) generated by the current fluctuation of charge carriers, and the scattered waves are detected by a highly-sensitivity THz detector. The bilayer graphene sheet was epitaxially grown on 4H-SiC (000-1) substrate by thermal decomposition in an argon atmosphere. The bilayer graphene is suggested to be of high quality from the Raman spectroscopy, where both G and G’ bands show very sharp one-peak structure, while the D peak, due to the defects, is much smaller (intensity ratio of D/G ~0.2). The graphene is patterned into a device of a narrow constriction with length 1.4 μm and width 0.7 μm by using e-beam lithography and reactive ion etching. The 2D image of the fluctuating evanescent fields taken with the current of 1.77 mA. The current density is much higher in the constricted region than the outside region. This is why the shot noise, manifesting itself as the fluctuating evanescent fields, shows up only in the constricted region. In the presentation, the dependence of the shot noise profile on the bias-current and the tip height will be discussed.