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ECE 874: Physical Electronics
Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
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Lecture 12, 09 Oct 12 VM Ayres, ECE874, F12
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Finite Potential Well:
(eV) Electron energy: E > U0 Electron energy: E < U0 (nm) Regions: -∞ to 0 0 to a a to +∞ VM Ayres, ECE874, F12
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Infinite Potential Well:
U (eV) = +∞ U (eV) = +∞ Electron energy: E < U0 (nm) Regions: -∞ to 0 0 to a a to +∞ VM Ayres, ECE874, F12
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For these two situations, found: - y(x) - En
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A) U0 = 0.7 eV = half the size of the bandgap
Lecture 11 Example problem: Find energy levels in a finite model for a SQW: Consider a SQW of width a = 10 nm that is fabricated in GaAs that operates at 300K. The SQW is modelled as a finite well. How many energy levels for an e- exist for: A) U0 = 0.7 eV = half the size of the bandgap B) U0 = 1.4 eV = just under the size of the bandgap C) What is the practical meaning of the limit: x = E/U0, 0 < x < 1? VM Ayres, ECE874, F12
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Finite Potential Well Advantage is: you scale to important parameters: the height U0 and width a. Note: Width a only affects the LHS: the number/spacing of tan curves. Height U0 affects both sides but practical advantage on RHS plot.. VM Ayres, ECE874, F12
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VM Ayres, ECE874, F12
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VM Ayres, ECE874, F12
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Discussion of Matlab solutions for:
ECE874_FiniteWellEnergyLevels_Lec11.m Lecture 11 example problem: examples of two different well heights: U0 = 0.7 ev and U0 = 1.4 eV for a fixed well width and electron energy up to same value as U0 ECE874_FiniteWellEnergyLevels_ThreeVariables.m General three variable set-up allows you to change: well height U0 well width a energy “of” electron compared to well height: z = E/U0 VM Ayres, ECE874, F12
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Last section of Chp. 02 is about the Finite Barrier:
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VM Ayres, ECE874, F12
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Finite barrier Anderson, Modern Physics and Quantum Mechanics
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E > Anderson V0 Pierret U0 VM Ayres, ECE874, F12
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A last look at the finite well, for E > U0 too:
VM Ayres, ECE874, F12
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