Lecture 2 Flashcards

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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
Q

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

A

∆k = change in wavevector
k = wavevector

26
Q

Describe the transition of an electron across an indirect band gap when both a photon and a phonon are absorbed

A
27
Q

Describe the transition of an electron across an indirect band gap when both a photon is absorbed and a phonon is emitted

A
28
Q

________ gap semiconductors like _____ are required for efficient optoelectronics.

A

Direct
GaAs

29
Q

What is the other name for conduction electron density?

A

Electron carrier density

30
Q

Describe the relationship between the electron carrier density and temperature

A

Electron number density depends approximately exponentially on temperature.

31
Q

Give the equation for the electron density in intrinsic (pure) semiconductors

A

n = electron density
E_g = bandgap energy
k_B = Boltzmann’s constant
T = temperature

32
Q

For intrinsic semiconductors, the number of electrons in the __________ band is ______ __ the number of holes in the _______ band.

A

Conduction
Equal to
Valence

33
Q

Give the equation for the energy of an electron state in the conduction band

A

ε = energy of electron state
E_g = bandgap energy
k = wavevector
m_e* = effective mass of an electron

34
Q

Give the equation for the energy of a hole state in the valence band

A

ε = energy of hole state
k = wavevector
m_h* = effective mass of a hole

35
Q

Give the equation for the number density of electron states in the conduction band

A

g_e(ε) = number density
m_e* = effective mass of an electron
ε = energy of electron state
E_g = bandgap energy

36
Q

Give the equation for the number density of hole states in the valence band

A

g_h(ε) = number density
m_h* = effective mass of a hole
ε = energy of electron state

37
Q

What does the Fermi-Diract distribution describe?

A

The probability that a conduction band electron state is occupied.

38
Q

Give the equation for the probability that a conduction band electron state is occupied

A

f_e(ε) = electron probability function
ε = energy of electron state
µ = chemical potential
k_B = Boltzmann’s constant
T = temperature

39
Q

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)

A

f_h(ε) = hole probability function
f_e(ε) = electron probability function

40
Q

Give the equation for the number density of occupied electron states in the conduction band

A

n(ε) = number density of occupied states
f_e(ε) = electron probability function
g_e(ε) = electron number density

41
Q

Give the equation for the number density of occupied hole states in the valence band

A

p(ε) = number density of occupied states
f_h(ε) = hole probability function
g_h(ε) = hole number density

42
Q

What is chemical potential?

A

The chemical potential, µ(T), is the energy for which f(µ) = 1/2.

43
Q

Where is the chemical potential when the hole effective mass equals the electron effective mass

A

In the middle of the bandgap

44
Q

What is the Fermi energy?

A

The chemical potential at T = 0K (i.e. µ(0))

45
Q

What is the Fermi level?

A

The chemical potential at any temperature (i.e. µ(T))