Week 11 Electrons, Holes & Effective Mass Flashcards
how does mass change from the Free Electron Model to the NFEM/TBM
the energy is modified by lattice interactions and the mass is no longer well defined
what is the effective mass equation
m* = ħ^2/[d^2E/dk^2]
what is effective mass
measure of interactions with the lattice
define a hole
empty state near the top of a valence band with positive effective mass and positive charge
what is the Hall field equation
EH = RHjxBz
j is current density
RH is the hall coefficient
what is the Hall coefficient equation and its special case for holes
RH = -1/ne
RH = 1/ρe
ρ is the hole concentration
what can happen to electrons and holes at room temp
some electrons are excited from top of valence band to bottom of the conduction band
electrons at top of conduction band and holes at bottom of valence band are treated as charge carriers
define an intrinsic semi conductor
conductor where conductivity is due to the intrinsic properties of the material itself so contains no impurities
what is the condition for intrinsic semi conductors
n = p
number of conduction electrons = number of holes in valence band
what is the probability of excitation for a charge carrier in an intrinsic semi conductor equation
P = n/N0 = exp[-EG/2kT]
what is the ntype doping equation
ΔED = EC - ED = m*/m ER/ε^2
what is the ptype doping equation
ΔEV = EA - EV