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ECE 874: Physical Electronics

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Presentation on theme: "ECE 874: Physical Electronics"— Presentation transcript:

1 ECE 874: Physical Electronics
Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University

2 Lecture 27, 04 Dec 12 Chp. 06: Carrier transport current contributions
VM Ayres, ECE874, F12

3 Review of Diffusion HW06 Prs. 6.3, 6.4, 6.7 involve diffusion
Review of diffusion taken from pp , Streetman and Banerjee, available on class website VM Ayres, ECE874, F12

4 Expected behavior of a pulse of electrons generated at x = 0 & t = 0, over later times: t1, t2, t3….. -L L VM Ayres, ECE874, F12

5 Closer look at electrons spreading out in space over time
Break distance into average chunks lbar More technically, lbar is the distance an electron can go between scattering events: the mean free path VM Ayres, ECE874, F12

6 Closer look at electrons spreading out in space over time
VM Ayres, ECE874, F12

7 Accurate description:
Electrons moving right: ½(n1lbarA) Electrons moving left: ½(n2lbarA) Therefore: the net number of electrons moving from x = 0 to, for example, x = L is: Net electrons = ½(lbarA)[n1 – n2] VM Ayres, ECE874, F12

8 fn(x) = Net electrons = ½(lbarA)[n1 – n2]
Definition of electron flux fn(x): net number of electrons moving from x = 0 to x = L per time The right time to use is the average time between scattering events: the mean free time: tbar fn(x) = Net electrons = ½(lbarA)[n1 – n2] Area tbar VM Ayres, ECE874, F12

9 Goal: re-cast n1 – n2 as a derivative:
VM Ayres, ECE874, F12

10 Now plug n1 – n2 back in to re-cast fn(x) as a derivative:
And take the limit as Dx becomes very small: Dx -> 0: VM Ayres, ECE874, F12

11 VM Ayres, ECE874, F12

12 Converting to diffusion current Jdiff:
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13 Review of drift: HW06 Prs. 6.3 also involves mobility related to drift current Review of drift taken from pp , Streetman and Banerjee, available on class website VM Ayres, ECE874, F12

14 Force of the electric field on the electrons
Decelerations due to collisions balance VM Ayres, ECE874, F12

15 Can think of this as: the probability of staying un-scattered is
exponentially decreasing Interval of time t  dt VM Ayres, ECE874, F12

16 VM Ayres, ECE874, F12

17 VM Ayres, ECE874, F12

18 Use in Pr. 6.3 VM Ayres, ECE874, F12

19 Pr. 6.3: VM Ayres, ECE874, F12

20 Review of Poisson’s equation:
VM Ayres, ECE874, F12

21 Example problem: Calculate r Sketch charge density and E (x) to scale
5 Given equilibrium (300K). Calculate r Sketch charge density and E (x) to scale VM Ayres, ECE874, F12

22 Given: VM Ayres, ECE874, F12

23 Find r: where is it? VM Ayres, ECE874, F12

24 Find r: where is it: in the depletion region:
Where do you want to put the junction? W VM Ayres, ECE874, F12

25 Find r: where is it: in the depletion region: on both sides
xp0 xn0 W VM Ayres, ECE874, F12

26 Find r: charge density:
Also could do this directly: r = qNA = q(1 x 1018) VM Ayres, ECE874, F12

27 Find r: charge density:
Also could do this directly: r = qND = q(5 x 1015) VM Ayres, ECE874, F12

28 Sketch charge density and E (x) to scale
VM Ayres, ECE874, F12

29 Pr. 6. 7 (i): use a Taylor expansion Pr. 6
Pr. 6.7 (i): use a Taylor expansion Pr. 6.9 (e): use simple diagram way of getting E, similar to Pr. 4.11 VM Ayres, ECE874, F12

30 VM Ayres, ECE874, F12

31 Steady state: Chp. 05: rN = rP versus equilibrium rN = 0 and rP = 0
BUT… VM Ayres, ECE874, F12

32 Steady state: Chp. 05: rN = rP versus equilibrium rN = 0 and rP = 0
Steady state: Chp. 06: dn/dt = dp/dt = 0 Useful in Pr. 6.9 (g) VM Ayres, ECE874, F12


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