Chapter 9: Semiconductors Flashcards
1
Q
Semiconductors Basics
(3 points)
A
- Conductivity highly dependent on T,E,B
- Metallic or insulator like properties
- Filled valence band, so technically an insulator
2
Q
Semiconductor Classification
(4 points)
A
- Intrinsic semiconductors are “naturally” occurring and have low conductivity
- Extrinsic semiconductors are doped intrinsic semiconductors
- A direct semiconductor has the minimum of the conduction and the maximum of the valence band at same k
- An indirect semiconductor has the minimum of the conduction band and the maximum of the valence band at different k
3
Q
Temperature Dependence of Band Gap
(5 points)
A
- As temperature increases, band gap decreases
- Because interatomic spacing increases with temperature, so potential felt by electron decreases
- Described by Varhsni Equation (see below)
- Parabolic at low T
- Linear at high T
4
Q
Temperature Dependence of Band Gap
(Graph)
A
5
Q
Optical Absorption in Semiconductors
(4 points)
A
- Photon delivers only energy
- Optically transparent for (h-bar)ω < Eg
- Phonon delivers momentum
- Required for indirect band gap
6
Q
Doped Semiconductors
(7 points)
A
- Types:
- Donor: Impurity that adds electron to conduction band
- Acceptor: Impurity that adds hole to valence band
- Binding energy can be estimated with Bohr model (meV
- Classification:
- Doped with more donors → n-type
- Doped with more acceptors → p-type
7
Q
Temperature Dependence of Chemical Potential
(Regimes: 4 points)
A
- Compensation Regime
- Impurity Reserve Regime
- Saturtion of Impurities
- Intrinsic Regime
8
Q
Compensation Regime
(5 points)
A
- kBT <<< Ed
- Donors not ionized
- For T → 0, then µ = Ed
- As T increases, electrons excited into conduction band, because acceptors are saturated
- µ shifts towards Ec and nC increases exponentially (−Ed/kBT)
9
Q
Impurity Reserve Regime
(3 points)
A
- kBT ≪ Ed
- Donors start to contribute to conduction band, but not all
- µ approximately in the middle of Ed and Ec
10
Q
Saturation of Impurities
(3 points)
A
- kBT ≥ Ed
- Temperature ionizes all donors, but still too small to excited a large enough number of VB electrons
- µ moves with increasing T towards middle of band gap
11
Q
Intrinsic Regime
(3 points)
A
- kBT >> Ed
- VB excitations become important
- µ moves to middle of band gap
12
Q
pn-Junction in Thermal Equilibrium
(Before Contact: 2 points)
A
- µn < Ed (n-type)
- µp > Ea (p-type)
13
Q
pn-Junction in Thermal Equilibrium
(After Contact: 5 points)
A
- µn = µp
- Diffusion of electrons in p-side (or holes into n-side)
- Creates space charge separation
- Creates electric field
- Induces drift current in opposition to diffusion current
14
Q
Schottky Approximation
(3 points)
A
- Space charge approximated as step-functions
- Electric field determined from E ∝ \int ρ dx
- Potential determined from V ∝ − \int E dl
15
Q
pn-Junction Under Forward Bias
(4 points)
A
- Bands “squished” together (∆E = e(Vo − Vapp))
- Electron Fermi energy raises
- Induced electric field diminishes → Drift current weaker → diffusion current dominates
- IV characteristic: forward bias region (below)