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Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/
Semiconductor Device Modeling and Characterization EE5342, Lecture 12 -Sp 2002 Professor Ronald L. Carter L12 21Feb02
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Bipolar junction transistor (BJT)
E B C VEB VCB Charge neutral Region Depletion Region The BJT is a “Si sandwich” Pnp (P=p+,p=p-) or Npn (N=n+, n=n-) BJT action: npn Forward Active when VBE > 0 and VBC < 0 L12 21Feb02
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BJT coordinate systems
z x”c x” WB WB+WC -WE xB x x’E x’ Charge neutral Region Depletion Region Base Collector Emitter L12 21Feb02
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BJT boundary and injection cond (npn)
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BJT boundary and injection cond (npn)
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IC npn BJT (*Fig 9.2a) L12 21Feb02
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npn BJT bands in FA region
q(VbiE-VBE ) q(VbiC-VBC ) qVBE qVBC injection high field L12 21Feb02
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Coordinate system - prototype npn BJT (Fig 9.8*)
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Notation for npn & pnp BJTs
NE, NB, NC E, B, and C doping (maj) xE, xB, xC E, B, and C CNR widths DE, DB, DC Dminority for E, B, and C LE, LB, LC Lminority for E, B, and C (L2min = Dmin tmin) tE0, tB0, tC0 minority carrier life- times for E, B, and C regions L12 21Feb02
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Notation for npn BJTs only
pEO, nBO, pCO: E, B, and C thermal equilibrium minority carrier conc pE(x’), nB(x), pC(x’’): positional mathe- matical function for the E, B, and C total minority carrier concentrations dpE(x’), dnB(x), dpC(x’’): positional ma- thematical function for the excess minority carriers in the E, B, and C L12 21Feb02
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Notation for pnp BJTs only
nEO, pBO, nCO: E, B, and C thermal equilibrium minority carrier conc nE(x’), pB(x), nC (x’’): positional mathe- matical function for the E, B, and C total minority carrier concentrations dnE(x’), dpB(x), dnC(x’’): positional ma- thematical function for the excess minority carriers in the E, B, and C L12 21Feb02
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npn BJT boundary conditions
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Emitter solution in npn BJT
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Base solution in npn BJT
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Collector solution in npn BJT
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Hyperbolic sine function
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npn BJT regions of operation
VBC Reverse Active Saturation VBE Forward Active Cutoff L12 21Feb02
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npn FA BJT minority carrier distribution (Fig 9.4*)
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npn RA BJT minority carrier distribution (Fig 9.11a*)
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npn cutoff BJT min carrier distribution (Fig 9.10a*)
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npn sat BJT minority carrier distribution (Fig 9.10b*)
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Defining currents in FA mode npn BJT (Fig 9.13*)
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npn BJT currents (F A region, ©RLC)
IC = JCAC IB=-(IE+IC ) JnE JnC IE = -JEAE JRB=JnE-JnC JpE JGC JRE JpC L12 21Feb02
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npn BJT topology x x’ p-Base n-Collector N-Emitter z WB WB+WC -WE x”c
Charge Neutral Region Depletion Region x x’ p-Base n-Collector N-Emitter z WB WB+WC -WE x”c x” xB x’E IE IC IB L12 21Feb02
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E current equations in FA mode npn BJT
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C current equations in FA mode npn BJT
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FA npn figure of merit emitter eff
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FA npn figure of merit base transp
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FA npn figure of merit recomb fact
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E current equations in FA mode npn BJT
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C current equations in FA mode npn BJT
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References * Semiconductor Physics & Devices, by Donald A. Neamen, Irwin, Chicago, 1997. L12 21Feb02
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