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Published byDora Dalton Modified over 9 years ago
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Semiconductor pn junctions
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Built-in potential defined by equilibrium and levels N A, N D far from metallurgical junction 0 = V T ln[n n0 /n p0 ] = V T ln [(N D × N A )/ n i 2 ]
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Existence of 0 implies E-field and acknowledges impurity sites uncovered by equilibrium process.
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Simplest case, uniform impurity levels, abrupt transition from N A to N D
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Analysis of abrupt junction
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E MAX = Q S / S Qs = qN D x n = qN A x p = qN B W Debye length E MAX = 2 J /W
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Diffused junction (a.k.a. linearly-graded) junction
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Analysis of linearly-graded junction
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E MAX = (qaW 2 /8)/ S = Q S / S a ≡ grading coefficient = (N A + N D )/d J = qaW 3 /12 S = (qaW 2 /8)W/1.5 S= = Q S W/1.5 E MAX = W =
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Junction Capacitance
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pn junction incremental capacitance
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pn junction capacitance CJ =CJ == C J0 = zero bias capacitanceMJ = grading coeffficient
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Doping profile: Courtesy of voltage slope of reciprocal capacitance Y-axis intercept consistent with (1/4pF) 2 Constant slope consistent with (elected) MJ = 0.5
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