ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu
Lecture 16, 23 Oct 12 VM Ayres, ECE874, F12
Effective mass: How: practical discussion: VM Ayres, ECE874, F12
Reminder: how you got the E-k curves: Kronig-Penney model allowed energy levels, Chp. 03: LHS RHS Graphical solution for number and values of energy levels E1, E2,…in eV. a = width of well, b = width of barrier, a + b = Block periodicity aBl VM Ayres, ECE874, F12
k = 0 k = ± p a + b VM Ayres, ECE874, F12
(b) VM Ayres, ECE874, F12
(b) VM Ayres, ECE874, F12
Matlab can do numerical derivatives Get: the E-k curves. Matlab can do numerical derivatives Note that the effective mass m* isn’t a single number. Note also that a + b = aBl varies depending on what direction you move in, so there are more curves than are on this single ± direction chart. VM Ayres, ECE874, F12
Which band has the sharpest curvature d2E/dk2? Get: the E-k curves. Region of biggest change of tangent = greatest curvature: the parabolas shown. Example problem: Which band has the sharpest curvature d2E/dk2? Which band has the lightest effective mass? Which band has the heaviest effective mass? Where in k-space, for both? VM Ayres, ECE874, F12
Which band has the sharpest curvature d2E/dk2? Band 4 Get: the E-k curves. Region of biggest change of tangent = greatest curvature: the parabolas shown. Example problem: Which band has the sharpest curvature d2E/dk2? Band 4 Which band has the lightest effective mass? Which band has the heaviest effective mass? Band 1: broadest = least curvature divide by smallest number = heaviest m* Where in k-space, for both? At k= 0 called the G point VM Ayres, ECE874, F12
VM Ayres, ECE874, F12
Where in k-space, for both? VM Ayres, ECE874, F12
Where in k-space, for both? m*A at G k = 0 m*B at about ½ way between G and X in [100] direction: k = 0 VM Ayres, ECE874, F12
k = p/aBl = p/aLC at end of Zone 1 a + b = aBl aBl for [100] = aLC k = p/aBl = p/aLC at end of Zone 1 This is X for [100] VM Ayres, ECE874, F12
Where in k-space, for both? m*A at G k = 0 m*B at about ½ way between G and X in [100] direction at k = p/2 aLC k = 0 VM Ayres, ECE874, F12
Assume T = 300K and it doesn’t change Ec = Egap = constant at a given T Hint: compare the answers for b = 0 and b ≠ 0 in (a) VM Ayres, ECE874, F12
Pick correct curve: VM Ayres, ECE874, F12
Pick conduction or valence bands:: E – Ec (eV) VM Ayres, ECE874, F12
Pick conduction minima. Where in k-space are they? E – EV (eV) <111> L G X <100> VM Ayres, ECE874, F12
Pick conduction minima. Where in k-space are they? G at k = 0 L at k = p/aBl for <111> Could work out the aBl distance between atomic cores in a <111> direction if needed. Not needed to finish answering the question. E – EV (eV) <111> L G X <100> VM Ayres, ECE874, F12
Note that the effective mass m* isn’t a single number. Go back to here: Note that the effective mass m* isn’t a single number. Note also that a + b = aBl varies depending on what direction you move in, so there are more curves than are on this single ± direction chart. VM Ayres, ECE874, F12
VM Ayres, ECE874, F12
VM Ayres, ECE874, F12
VM Ayres, ECE874, F12
VM Ayres, ECE874, F12
(From practical to fundamental!) VM Ayres, ECE874, F12
In 3 D: VM Ayres, ECE874, F12
Write this in 2D: all three parts. Integrate a -> v -> r. Vector r (t) is the direction. The final answer contains time t. VM Ayres, ECE874, F12
Then a = dv/dt for dvx/dt and dvy/dt Start with [m*ij] Then F = qE Then a = dv/dt for dvx/dt and dvy/dt Integrate with respect to time, 2x’s, to get x(t) and y(t). VM Ayres, ECE874, F12
k = 0 VM Ayres, ECE874, F12
1D: Any one of these parabolas could be modelled as: Region of biggest change of tangent = greatest curvature: the parabolas shown. 1D: Any one of these parabolas could be modelled as: VM Ayres, ECE874, F12
For any of these parabolas: Region of biggest change of tangent = greatest curvature: the parabolas shown. 3D: <111> + <100> E – EV (eV) <111> L G X <100> For any of these parabolas: There’s a major axis but also two minor ones VM Ayres, ECE874, F12
E – EV (eV) <111> L G X <100> Same: truncate 1/2 VM Ayres, ECE874, F12
k = 0 VM Ayres, ECE874, F12