Abstract:The theory of ``direct'' and ``phonon-assisted'' tunneling is reviewed. Theoretical I–V characteristics are calculated using the constant field model. Generalizations to nonconstant field and more complicated band structure models are discussed briefly.
“…5c. This behavior is characteristic of a tunnel diode [33][34][35][36][37][38][39][40][41] and is consistent with degenerative doping and the introduction of donor states below the conduction band minimum.…”
Remmes, N.; Dowben, Peter A.; Ahmad, A.A.; Ianno, N.J.; Li, J.Z.; and Jiang, H.X., "The incorporation of Nickel and Phosphorus dopants into Boron-Carbon alloy thin films" (1998). Peter Dowben Publications. 105.
“…5c. This behavior is characteristic of a tunnel diode [33][34][35][36][37][38][39][40][41] and is consistent with degenerative doping and the introduction of donor states below the conduction band minimum.…”
Remmes, N.; Dowben, Peter A.; Ahmad, A.A.; Ianno, N.J.; Li, J.Z.; and Jiang, H.X., "The incorporation of Nickel and Phosphorus dopants into Boron-Carbon alloy thin films" (1998). Peter Dowben Publications. 105.
“…20. The active dopant concentrations n ¼ 3:3 Â19 19 cm À3 and p ¼ 1:1 Â 19 19 cm À3 are obtained with Hall measurements and satisfy the previously mentioned requirements for exponential BTBT current. Transmission Electron Microscopy (HR-HAADF-STEM, Fig.…”
The effective bandgap is a crucial design parameter of heterojunction tunneling field-effect transistors. In this letter, we demonstrate a method to measure the effective bandgap directly from the band-to-band tunneling current of a heterojunction Esaki diode, of which we only require knowledge of the electrostatic potential profile. The method is based on a characteristic exponentially increasing current with forward bias, caused by sharp energy filtering at cryogenic temperature. We apply this method experimentally to a n+In0.53Ga0.47As/pGaAs0.5Sb0.5 Esaki diode and define requirements to apply it to other heterojunctions.
“…The tunneling probability, T, is [7]: For simplicity, we will assume that the electric field across the tunneling junction, F, is constant and equal to the peak electric field. The effective mass for tunneling [1,8,9] is * tunnel m 1 , and EG is the band gap.…”
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