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CHAPTER 4 – THE SEMICONDUCTOR IN EQUILIBRIUM

PHYSICAL ELECTRONICS(ECE3540)Brook Abegaz, Tennessee Technological University, Fall 2013 Friday, September 20, 2013 Tennessee Technological University1 CHAPTER 4 THE SEMICONDUCTOR IN EQUILIBRIUMC hapter 4 The SEMICONDUCTOR in EQUILIBRIUM CHAPTER 3: considering a general crystal andapplying to it the concepts of quantum mechanicsin order to determine a few of the characteristics ofelectrons in a single-crystal lattice. CHAPTER 4:apply these concepts specifically to asemiconductor material. CHAPTER 4:use thedensity of quantum statesin theconduction bandand thedensity of quantum statesin thevalence bandalong with theFer mi-Diracprobability functionto determine theconcentrationof electrons and holesin the conduction andvalence bandsFriday, September 20, 2013 Tennessee Technological University2 EQUILIBRIUM , or thermal EQUILIBRIUM , implies thatno externalforcessuch as voltages, electric fields, magnetic fields, ortemperature gradients are acting on the SEMICONDUCTOR .

Chapter 4: use the density of quantum states in the conduction band and the density of quantum states in the valence band along with the Fermi-Dirac probability function to determine the concentration of electrons and holes in the conduction and valence bands ... atoms or defects.

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