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Computational Solid State Physics 計算物性学特論 第10回 10. Transport properties II: Ballistic transport
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Electron transport properties l e : electronic mean free path l φ : phase coherence length λ F : Fermi wavelength
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Tunneling transport I L
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Current in one-dimension T(k): transmission coefficient
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Total current in one-dimension
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Low bias limit : conductance at low temperatures
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Landauer ’ s formula : transmission coefficient : Conductance : Quantum conductance : Quantum resistance I: current, V: bias
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Two- and four- terminal measurements
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Tow- and four- terminal measurement 2-terminal measurement 4-terminal measurement
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Conductance of a quantum point contact
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Only one channel (n=1) is open. for n=1 Conductance of a quantum point contact Quantization of transverse motion
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Nanowire of Au
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Mechanically Controllable Break Junction
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Histogram of conductance of a relay junction
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Conductance through a quantum dot
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:Lorentzian broadening of resonant tunneling through quantized energy E N of a dot :Thermal broadening Tunneling current via quantum dot
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A bound state and a resonant state
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Transmission coefficient for resonant tunneling If T L =T R
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Transmission coefficient of a resonant-tunneling structure
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Characteristics of resonant tunneling diode
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Resonant tunneling current :wave function :energy
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Large bias and low temperature limit Total resonant tunneling current
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Transmission coefficient for resonant tunneling If T L =T R
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Profile through a three-dimensional resonant-tunnelling diode. The bias increases from (a) to (d), giving rise to the I(V) characteristic shown in (e). The shaded areas on the left and right are the Fermi seas of electrons. Profile through a three-dimensional resonant tunneling diode
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Problems 10 Calculate the density of states for free electrons in one, two and three dimensions. Calculate the ballistic current in two dimensions. Calculate the transmission coefficient for a square barrier potential. Calculate the transmission coefficient for a double square barrier potential.
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