Title: ECE 802-604: Nanoelectronics
1ECE 802-604Nanoelectronics
- Prof. Virginia Ayres
- Electrical Computer Engineering
- Michigan State University
- ayresv_at_msu.edu
2Lecture 15, 17 Oct 13
In Chapters 02 and 03 in Datta How to correctly
measure I GV Add scattering to
Landauer-Buttiker Buttiker approach for dealing
with incoherent scatterers 2.6 occupied states
as scatterers 3.1 scattering/S matrix
31 Deg, M 1
mR
mL
X
X
O
probe
m
m
4Outline of the solution
Goal V IR, solve for R What is V mA
mB What is I I I1 I2
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6Lec 14
where
Ielectron
7Lec 14 Further benefit from I3 I4 0 with
Unitarity and symmetry, found m
8Lec 14 Used 3 conditions
1/ I3 I4 0
2/
3/
9Datta Sec. 2.6
101 Deg, M 1
mR
mL
X
X
O
probe
m
mA
mB
m
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12NT(E)
13Where from
14Where from
15Where from
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21above mB
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32Datta Sec. 3.1
33What is a scattering S matrix?
34Introduce an S-matrix to describe both probe and
occupied state scattering while maintaining
Landuaer-Buttiker approach of treating all
terminals alike
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36Datta, Sec. 3.1
Two propagating modes into one propagating
mode expect scattering due to occupied states
Game plan for each Si j element determine
is it a reflection or a transmission?
37Start with a more familiar example from a paper
by Engquist
The single in/out channel for the incoherent
scatterer gives an experimentally wrong
resistance. The Buttiker two-channel probe
description turned out to be correct.
38Example find the S-matrix for the diagram shown.
39Example find the S-matrix for the diagram shown.
40Example find the S-matrix for the diagram shown.
41Example find the scattering matrix S for the
Engquist diagram
42Example find the scattering matrix S for the
Engquist diagram
aout
bin
gin
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46Datta Sec. 3.1
47Example find the S-matrix for the diagram shown.
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