Photonics - Topic 5 Flashcards

1
Q

What are Pyroelectric detectors?

A

Photon energy converted to heat

uses pyroelectric crystal - Radiation falling on the detector changes its temperature and reduces its polarisation, which changes the charge on its surface.

This can be detected as a transient voltage.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

Photoconductivity in semiconductors

A
  • An electron-hole pair (EHP) can be generated in a semiconductor by an incoming photon with energy β„Žπ‘“ > 𝐸𝑔, where 𝐸𝑔 is the bandgap energy of the semiconductor.
    • Increases the conductivity of the semiconductor.
      • If there is an electric field across the semiconductor, there will be an increase in current
        • (the electric field will separate the EHP, causing them to move in opposite directions).
    • Known as photoconductivity.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

What bias does a photodiode (pn junction) need to perform as a photodetector?

A

Reverse bias

The reverse bias increases the potential barrier in the depletion region, resulting in a very small reverse current (the dark current) when there is no light incident on the photodiode.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

How is current generated in a photodiode (pn junction)?

A

Thus we can expect the photocurrent due to the light falling on the photodiode to be due to EHPs generated in (or close to) the depletion region.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

Effect of illumination on the I-V curve of a photodiode

A

As the optical power incident on the junction is increased more electron hole pairs are created resulting in a larger negative current:

I = -Is - I0(P0)

Is is dark curent

P0 is photocurent

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Explain what happens for increasing optical power on a photodiode in reverse bias

A
  • When the diode is reverse biased, photogenerated EHPs cause a current to flow from n to p, i.e. in the reverse direction.
  • Increasing optical power will lead to more EHPs being generated, so the current increases with increasing optical power.
    • Since the number of EHPs generated is proportional to the number of incident photons, which is proportional to the power, the photocurrent in the reverse biased region increases linearly with power.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

What happens if a photodiode is under forward bias?

A
  • If the diode is forward biased, the potential barrier will be lowered and forward current will flow. As the forward voltage is increased, the forward current will eventually dominate over the reverse photocurrent, and the 𝐼 βˆ’ 𝑉 characteristic will follow that for the unilluminated diode.
  • At a certain forward bias, the forward current will balance the reverse photocurrent, so no net current flows. Thus a voltage (π‘‰π‘œπ‘) will appear across an open-circuit photodiode that has light falling on it. For 0 < 𝑉 < π‘‰π‘œπ‘ the diode operates in photovoltaic mode. It is in this region that pn diode solar cells operate.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Eq: Outline Photodiode absorption characteristics

A

At the interface between the air and photodiode, the power entering the semiconductor is 𝑃0(1 βˆ’ 𝑅).

Inside the semiconductor, the power is assumed to decay exponentially, with absorption (or loss) coefficient 𝛼, so that overall the power at a distance π‘₯ into the semiconductor is given by:

𝑃(π‘₯) = 𝑃0 (1 βˆ’ 𝑅) e(βˆ’π›Όπ‘₯)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Eq: Outline Photocurrent in Photdiode

A

From the fact that power decays exponentially across the semiconductor, we can see that the _power absorbed in the depletion regio_n, which will lead to the generation of photocurrent, is given by:

𝑃(π‘₯1 ) βˆ’ 𝑃(π‘₯2) = 𝑃0(1 βˆ’ 𝑅)[e(βˆ’π›Όπ‘₯1) βˆ’ e(βˆ’π›Όπ‘₯2)]

where π‘₯1 and π‘₯2 are the positions of the top and bottom of the depletion region.

If the fraction of absorbed photons that generate an EHP that contributes to the photocurrent is πœ‚π‘–π‘›π‘‘ (the internal quantum efficiency), the photocurrent generated is

πΌπ‘œ = (π‘’πœ‚π‘–π‘›π‘‘ / β„Žπ‘“) 𝑃0(1 βˆ’ 𝑅)[e(βˆ’π›Όπ‘₯1) βˆ’ e(βˆ’π›Όπ‘₯2)]

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Eq: What is the responsivity of a photodiode?

A

The responsivity of a photodiode is the ratio of generated photocurrent to optical power incident on the detector.

mA.mW-1

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Eq: What is the external quantum efficiency?

A

Compares the number of electrons generated to the number of photons incident on the photodiode. The number of photons incident per second is 𝑃0/β„Žπ‘“, and the number of electrons flowing per second is 𝐼0/𝑒.

πœ‚π‘’π‘₯𝑑 = 𝑅𝑠 (β„Žπ‘ / 𝑒λ)

πœ‚π‘’π‘₯𝑑 can be expressed as:

πœ‚π‘’π‘₯𝑑 = πœ‚π‘–π‘›π‘‘(1 βˆ’ 𝑅)[e(βˆ’π›Όπ‘₯1 ) βˆ’ e(βˆ’π›Όπ‘₯2)]

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

What is the Spectral Response of a photodiode?

A
  • Rearranging πœ‚π‘’π‘₯𝑑 = 𝑅𝑠 (β„Žπ‘ / 𝑒λ) we can see that responsivity is proportional to the wavelength.
    • only true for photons with energy greater than the bandgap energy
  • Real case
    • The real responsivity deviates from the ideal at short wavelengths due to the wavelength dependence of the absorption coefficient in the external quantum efficiency
    • At long wavelengths below the bandgap energy the responsivity tails off in a smooth way due to the continuous nature of band edge _(_i.e. cut off of the band gap energy is not abrupt in real materials).
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

p-i-n junction diagam, energy plot, fixed charge density plot and electric field plot

A
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Eq: Poisson’s equation for pin junction

A

Where ND is the charge density

and the denominator consists of the permittivity constants.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

p-i-n junction design considerations: increasing the length of the depletion region

A
  • The external quantum efficiency can be increased to almost 100% by increasing the length of the depletion region.
    • In practice: ldepletion >> 1 / Ξ±
      • where 1 / Ξ± is the attenuation length scale
  • However, increasing he length will also affect the bandwidth of the photodiode:
    • It increases the response time as the photo-generated carriers have further to drift
    • It reduces the capacitance of the photodiode, which will increase the bandwidth
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

What is carrier transit time and what does it depend on?

A
  • It is the time taken for the photogenerated carriers to cross the depletion region and enter the doped region where they are majority carriers.
    • The transit time depend on β†’ drift velocity, which depends on β†’ electric field in the intrinsic region.
    • drift velocity β†’ increased
      • high reverse bias across the pin photodiode.
17
Q

Eq: Carrier velocity and drift time in phototiode

A

Carrier velocity:

𝑣 = μ𝐸 = μ𝑉/x

ΞΌ is the Carrier mobility (m2 /V/s)

Drift time:

𝑑𝑐 = π‘₯ / 𝑣 = π‘₯ 2 / μ𝑉

x is the Junction width (m)

18
Q

What happens to the drift velocity at high electric fields?

A

𝑑𝑐 = π‘₯ / π‘£π‘ π‘Ž<em>t</em>

Drift velocity saturates at large electric field values and electron and hole velocities become similar.

Saturated velocity β‡’ shortest drift time (and hence highest bandwidth).

19
Q

What is the Photodiode equivalent circuit

A
  • The space charge regions of a pin photodiode are like charges on the plates of a capacitor, so the photodiode can be modelled as a current source in parallel with a capacitor with capacitance:
    • 𝐢𝑗 = πœ€π‘Ÿπœ€0𝐴 / π‘₯
  • Photodiode will be connected to a load with resistance 𝑅L
  • Forms a low-pass filter, with time constant 𝑅L𝐢𝑗
20
Q

Photodiode junction discharge time

A
21
Q

Eq: Photodiode junction diffusion time

A

𝑑𝑑 = 𝑙2 / 2 De

22
Q

How is diffusion time minimised in photodiodes?

A

In well designed photodiodes the diffusion time is minimised by using a thin top p-region such that

td << tc

23
Q

How is the overall bandwidth of the phototdiode determined?

A
  • The overall bandwidth of a photodiode is determined by the combination of the responses due to the drift, diffusion and RC times
    • not simple to calculate the combined effect
    • by comparing the drift, diffusion and RC times it may be possible to identify a dominant factor
24
Q

Design guidelines for photodiode

A
  • Design guidelines (for overall bandwidth ):
    • Use thin p-layer to so that diffusion time 𝑑𝑑 << 1/B
    • Chose intrinsic layer width such that drift time 𝑑𝑐 < 1 / (2B)
    • Chose junction capacitance (PD area) so that 𝑑RC < 1 / (2Ο€B)
    • Note that there is a trade-off between junction capacitance (𝑑RC) and drift time
25
Q

pin photodiode structure (top entry)

A
  • Thin p-region
  • Anti-reflection (AR) coating to reduce reflections at air semiconductor interface
  • Thick intrinsic region (depletion region) to maximise absorption
  • Small area to reduce junction capacitance