Lecture 2 Flashcards
Describe the basic structure of a direct bandgap semiconductor
Electron states in the conduction band behave like free electrons but with an effective mass of m_e*.
Holes in the valence band have a single effective mass of m_h*.
For a direct bandgap semiconductor, the top of the valence band and the bottom of the conduction band are at ___ _____ k-vector.
The same
For an indirect bandgap semiconductor, the top of the valence band and the bottom of the conduction band are at ___________ k-vectors.
Different
Describe the basic structure of an indirect bandgap semiconductor
What happens to a direct semiconductor when a photon (of energy equal to/greater than the bandgap) is fired at it?
The photon is absorbed and an electron crosses the bandgap from the valence band to the conduction band. This creates an electron-hole pair.
How can semiconductor bandgaps be measured?
By measuring the optical absorption of photons by the semiconductor as a function of photon energy.
What is the difference in k from the top of the valence band to the bottom of the conduction band in an indirect semiconductor?
~ π/a (where a = lattice constant)
What must be conserved when electrons move from the valence band to the conduction band?
- Energy
- Wavevector, k
Is photon absorption alone possible in an indirect semiconductor?
No
Conservation of the wavevector, k, can be thought of the conservation of ‘________ ________’.
Effective momentum
Give the equation for the ‘effective momentum’ (i.e. the wavevector) of an electron
k = wavevector
m* = effective mass
v = velocity
ℏk = p = momentum
Give the equation for the energy of a photon
E = hf = hc/λ
E = energy
f = frequency
c = speed of light
λ = wavelength
Give the equation for the wavevector of a photon
k = photon wavevector
ε = photon energy
c = speed of light
What is a phonon?
A quantum of lattice vibrational energy.
Why are phonons supplied to/emitted from indirect semiconductors?
To supply the additional k-vector needed for an indirect transition of an electron from the valence band to the conduction band.
Give the equation for the energy of a phonon
ε = phonon energy
k_B = Boltzmann’s constant
T = temperature
Give the equation for the wavevector of a phonon
k = phonon wavevector
ε = phonon energy
v_s = velocity of sound
The energy of a phonon is _____ _______ than the energy of the bandgap.
Much smaller
The energy of a photon is ____________ _______ to the energy of the bandgap.
Approximately equal
The wavevector of a phonon is ____________ _______ to the change in the wavevector of the bandgap.
Approximately equal
The energy of a photon is _____ _______ than the change in the wavevector of the bandgap.
Much smaller
Give the equation for the bandgap energy when an electron in the valence band absorbs a photon and also absorbs a phonon to move to the conduction band
E_g = bandgap energy
ε = energy
Give the equation for the change in the wavevector when an electron in the valence band absorbs a photon and also absorbs a phonon to move to the conduction band
∆k = change in wavevector
k = wavevector
Give the equation for the bandgap energy when an electron in the valence band absorbs a photon and emits a phonon to move to the conduction band
E_g = bandgap energy
ε = energy