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ECE 874: Physical Electronics
Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
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Lecture 27, 04 Dec 12 Chp. 06: Carrier transport current contributions
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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
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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
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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
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Closer look at electrons spreading out in space over time
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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
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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
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Goal: re-cast n1 – n2 as a derivative:
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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
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Converting to diffusion current Jdiff:
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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
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Force of the electric field on the electrons
Decelerations due to collisions balance VM Ayres, ECE874, F12
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Can think of this as: the probability of staying un-scattered is
exponentially decreasing Interval of time t dt VM Ayres, ECE874, F12
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Use in Pr. 6.3 VM Ayres, ECE874, F12
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Pr. 6.3: VM Ayres, ECE874, F12
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Review of Poisson’s equation:
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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
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Given: VM Ayres, ECE874, F12
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Find r: where is it? VM Ayres, ECE874, F12
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Find r: where is it: in the depletion region:
Where do you want to put the junction? W VM Ayres, ECE874, F12
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Find r: where is it: in the depletion region: on both sides
xp0 xn0 W VM Ayres, ECE874, F12
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Find r: charge density:
Also could do this directly: r = qNA = q(1 x 1018) VM Ayres, ECE874, F12
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Find r: charge density:
Also could do this directly: r = qND = q(5 x 1015) VM Ayres, ECE874, F12
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Sketch charge density and E (x) to scale
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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
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Steady state: Chp. 05: rN = rP versus equilibrium rN = 0 and rP = 0
BUT… VM Ayres, ECE874, F12
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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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