Lecture 2 Flashcards

1
Q

Describe the basic structure of a direct bandgap semiconductor

A

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*.

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2
Q

For a direct bandgap semiconductor, the top of the valence band and the bottom of the conduction band are at ___ _____ k-vector.

A

The same

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3
Q

For an indirect bandgap semiconductor, the top of the valence band and the bottom of the conduction band are at ___________ k-vectors.

A

Different

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4
Q

Describe the basic structure of an indirect bandgap semiconductor

A
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5
Q

What happens to a direct semiconductor when a photon (of energy equal to/greater than the bandgap) is fired at it?

A

The photon is absorbed and an electron crosses the bandgap from the valence band to the conduction band. This creates an electron-hole pair.

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6
Q

How can semiconductor bandgaps be measured?

A

By measuring the optical absorption of photons by the semiconductor as a function of photon energy.

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7
Q

What is the difference in k from the top of the valence band to the bottom of the conduction band in an indirect semiconductor?

A

~ π/a (where a = lattice constant)

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8
Q

What must be conserved when electrons move from the valence band to the conduction band?

A
  • Energy
  • Wavevector, k
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9
Q

Is photon absorption alone possible in an indirect semiconductor?

A

No

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10
Q

Conservation of the wavevector, k, can be thought of the conservation of ‘________ ________’.

A

Effective momentum

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11
Q

Give the equation for the ‘effective momentum’ (i.e. the wavevector) of an electron

A

k = wavevector
m* = effective mass
v = velocity

ℏk = p = momentum

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12
Q

Give the equation for the energy of a photon

A

E = hf = hc/λ

E = energy
f = frequency
c = speed of light
λ = wavelength

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13
Q

Give the equation for the wavevector of a photon

A

k = photon wavevector
ε = photon energy
c = speed of light

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14
Q

What is a phonon?

A

A quantum of lattice vibrational energy.

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15
Q

Why are phonons supplied to/emitted from indirect semiconductors?

A

To supply the additional k-vector needed for an indirect transition of an electron from the valence band to the conduction band.

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16
Q

Give the equation for the energy of a phonon

A

ε = phonon energy
k_B = Boltzmann’s constant
T = temperature

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17
Q

Give the equation for the wavevector of a phonon

A

k = phonon wavevector
ε = phonon energy
v_s = velocity of sound

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18
Q

The energy of a phonon is _____ _______ than the energy of the bandgap.

A

Much smaller

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19
Q

The energy of a photon is ____________ _______ to the energy of the bandgap.

A

Approximately equal

20
Q

The wavevector of a phonon is ____________ _______ to the change in the wavevector of the bandgap.

A

Approximately equal

21
Q

The energy of a photon is _____ _______ than the change in the wavevector of the bandgap.

A

Much smaller

22
Q

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

A

E_g = bandgap energy
ε = energy

23
Q

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

A

∆k = change in wavevector
k = wavevector

24
Q

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

A

E_g = bandgap energy
ε = energy

25
Give the equation for the change in the wavevector when an electron in the valence band absorbs a photon and emits a phonon to move to the conduction band
∆k = change in wavevector k = wavevector
26
Describe the transition of an electron across an indirect band gap when both a photon and a phonon are absorbed
27
Describe the transition of an electron across an indirect band gap when both a photon is absorbed and a phonon is emitted
28
________ gap semiconductors like _____ are required for efficient optoelectronics.
Direct GaAs
29
What is the other name for conduction electron density?
Electron carrier density
30
Describe the relationship between the electron carrier density and temperature
Electron number density depends approximately exponentially on temperature.
31
Give the equation for the electron density in intrinsic (pure) semiconductors
n = electron density E_g = bandgap energy k_B = Boltzmann's constant T = temperature
32
For intrinsic semiconductors, the number of electrons in the __________ band is ______ __ the number of holes in the _______ band.
Conduction Equal to Valence
33
Give the equation for the energy of an electron state in the conduction band
ε = energy of electron state E_g = bandgap energy k = wavevector m_e* = effective mass of an electron
34
Give the equation for the energy of a hole state in the valence band
ε = energy of hole state k = wavevector m_h* = effective mass of a hole
35
Give the equation for the number density of electron states in the conduction band
g_e(ε) = number density m_e* = effective mass of an electron ε = energy of electron state E_g = bandgap energy
36
Give the equation for the number density of hole states in the valence band
g_h(ε) = number density m_h* = effective mass of a hole ε = energy of electron state
37
What does the Fermi-Diract distribution describe?
The probability that a conduction band electron state is occupied.
38
Give the equation for the probability that a conduction band electron state is occupied
f_e(ε) = electron probability function ε = energy of electron state µ = chemical potential k_B = Boltzmann's constant T = temperature
39
Give the equation that a valence band state is 'occupied by a hole' (i.e. the probability that the state is not occupied by an electron)
f_h(ε) = hole probability function f_e(ε) = electron probability function
40
Give the equation for the number density of occupied electron states in the conduction band
n(ε) = number density of occupied states f_e(ε) = electron probability function g_e(ε) = electron number density
41
Give the equation for the number density of occupied hole states in the valence band
p(ε) = number density of occupied states f_h(ε) = hole probability function g_h(ε) = hole number density
42
What is chemical potential?
The chemical potential, µ(T), is the energy for which f(µ) = 1/2.
43
Where is the chemical potential when the hole effective mass equals the electron effective mass
In the middle of the bandgap
44
What is the Fermi energy?
The chemical potential at T = 0K (i.e. µ(0))
45
What is the Fermi level?
The chemical potential at any temperature (i.e. µ(T))