Electrical oscillations induced by the metal-insulator transition in VO2

  • Hyun-Tak Kim
    ETRI 1 Metal-Insulator Transition Laboratory, , Daejeon 305-350, Republic of Korea
  • Bong-Jun Kim
    ETRI 1 Metal-Insulator Transition Laboratory, , Daejeon 305-350, Republic of Korea
  • Sungyoul Choi
    ETRI 1 Metal-Insulator Transition Laboratory, , Daejeon 305-350, Republic of Korea
  • Byung-Gyu Chae
    ETRI 1 Metal-Insulator Transition Laboratory, , Daejeon 305-350, Republic of Korea
  • Yong Wook Lee
    ETRI 1 Metal-Insulator Transition Laboratory, , Daejeon 305-350, Republic of Korea
  • T. Driscoll
    University of California-San Diego 3 Department of Physics, , La Jolla, California 92093, USA
  • M. M. Qazilbash
    University of California-San Diego 3 Department of Physics, , La Jolla, California 92093, USA
  • D. N. Basov
    University of California-San Diego 3 Department of Physics, , La Jolla, California 92093, USA

説明

<jats:p>We systematically investigate the characteristics of an electrical oscillation observed in two-terminal vanadium dioxide (VO2) devices. These oscillations are observed at room temperature in a simple electrical circuit without inductive components. The circuit is composed only of a dc voltage source, the VO2 device, and a standard resistor connected in series with the device. We explain why the observed oscillations are a result of the percolative metal-to-insulator transition (MIT) of VO2 and the coexistence of the metal and insulating phases. Specifically, oscillations are attributed to the construction and destruction of capacitive regions composed of regions of the semiconducting phase, (as dielectric material) and metallic phase electron carriers, induced by the MIT (as capacitor electrodes). Since the coexistence of these phases—and thus the capacitive regions—is destroyed by elevated temperature, the MIT oscillation is not explained in terms of significant heat input but rather in terms of a voltage-triggered effect. It is also discussed whether the current jump at the onset of the oscillations is driven by Mott physics or by Peierls physics relying on a structural phase transition. Furthermore, the electrical parameter space surrounding these oscillations is explored, and a generation window is identified. Within this generation window, the oscillation frequency can be continuously tuned by adjusting applied voltage or by an external circuit component, such as resistor or added capacitor. The frequency of oscillations can be increased up to &gt;1 MHz.</jats:p>

収録刊行物

被引用文献 (11)*注記

もっと見る

詳細情報 詳細情報について

問題の指摘

ページトップへ