Download presentation
Presentation is loading. Please wait.
Published byCecil Greer Modified over 9 years ago
1
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu
2
VM Ayres, ECE875, S14 Chp 03: metal-semiconductor junction Currents: I-V / J-V measurements: discussion of part b (not assigned) in Pr. 3.08 on board to introduce thermionic emission model for I-V (or J-V) Thermionic emission model: where from Lecture 23, 10 Mar 14
3
Pr. 3.08: Use: X 1/10 10 VM Ayres, ECE875, S14
4
Thermionic emission model for J
5
VM Ayres, ECE875, S14 Chp 03: metal-semiconductor junction Currents: I-V / J-V measurements: discussion of part b (not assigned) in Pr. 3.08 on board to introduce thermionic emission model for I-V (or J-V) Thermionic emission model: where from Lecture 23, 10 Mar 14
6
Width Height Barrier width versus height maximally affect different types of transport which are energy-dependant VM Ayres, ECE875, S14
7
1. Thermionic emission (enough energy compared with height: q Bn is critical) 2. Tunnelling (W D is critical) Dotted line: Both 1. and 2. can be going on at the same time VM Ayres, ECE875, S14
8
3. J rec 4. diffusion of electrons 5. diffusion of holes VM Ayres, ECE875, S14
9
5. diffusion of holes VM Ayres, ECE875, S14 4. diffusion of electrons
10
Thermionic emission model for transport: VM Ayres, ECE875, S14 enough energy above E C compared with barrier height q n is critical
11
Start: ECEC Need to put dn in terms of v x
12
N(E): 3Df(E): “hot”: non-degenerate
13
So far: dn is now in terms of dv
14
v is 3D: e- moving in any direction. Still need to pick out the transport direction in x
15
See next slide for helpful integrals Note that k = k B = 1.38 x 10 -23 J/K
17
Are you done? No. You need to re-write the contact potential in terms of the barrier height Requirement on the KE/velocity in the transport direction x:
18
Note: current direction is going the other way. No bias on metal side: V = 0 Current density from metal into semiconductor:
19
J TE = J TE-sat = J TE = J s->m + J m->s Total Thermionic Current density: = {J TE-sat } Now you are done.
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.