TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK
An analytical expression for evaluating the transmission coefficient and tunnel current of an electron in metal-oxide-semiconductor hetero junction anisotropic material has been derived. The Si(100)/SiO2/Si(100) heterostructure was used to examine the analytic expression. Airy function numerical...
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id-itb.:743562023-07-11T11:40:49ZTRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK Agustina Indonesia Final Project Transmission coefficient, tunnel current INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/74356 An analytical expression for evaluating the transmission coefficient and tunnel current of an electron in metal-oxide-semiconductor hetero junction anisotropic material has been derived. The Si(100)/SiO2/Si(100) heterostructure was used to examine the analytic expression. Airy function numerical method is chosen in calculating the solution of Schrödinger equation for trapezoidal barrier. The transmission coefficient is calculated for electron energy 0.1 eV to 4 eV. The transmission coefficient is superior as the energy of electron higher than 3 eV. By varying the applied bias voltage to the potential barrier, barrier width, electron incident angle, and electron velocity, the different value of transmission coefficient be obtained. The electron effective mass in the oxide layer, electron velocity, and the Fermi energy are three fitting parameters. It is shown that the calculated tunnel current is well fitted to the measured one in low applied bias voltage. text |
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An analytical expression for evaluating the transmission coefficient and tunnel
current of an electron in metal-oxide-semiconductor hetero junction anisotropic
material has been derived. The Si(100)/SiO2/Si(100) heterostructure was used to
examine the analytic expression. Airy function numerical method is chosen in
calculating the solution of Schrödinger equation for trapezoidal barrier. The
transmission coefficient is calculated for electron energy 0.1 eV to 4 eV. The
transmission coefficient is superior as the energy of electron higher than 3 eV. By
varying the applied bias voltage to the potential barrier, barrier width, electron
incident angle, and electron velocity, the different value of transmission coefficient be
obtained. The electron effective mass in the oxide layer, electron velocity, and the
Fermi energy are three fitting parameters. It is shown that the calculated tunnel
current is well fitted to the measured one in low applied bias voltage. |
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Final Project |
author |
Agustina |
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Agustina TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
author_facet |
Agustina |
author_sort |
Agustina |
title |
TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
title_short |
TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
title_full |
TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
title_fullStr |
TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
title_full_unstemmed |
TRANSMITANSI DAN ARUS TEROBOSAN ELEKTRON DI DALAM METAL-OKSIDA-SEMIKONDUKTOR (MOS) SAMBUNGAN HETERO MATERIAL ANISOTROPIK |
title_sort |
transmitansi dan arus terobosan elektron di dalam metal-oksida-semikonduktor (mos) sambungan hetero material anisotropik |
url |
https://digilib.itb.ac.id/gdl/view/74356 |
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