Photonics - Topic 5 Flashcards
What are Pyroelectric detectors?
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.
Photoconductivity in semiconductors
- An electron-hole pair (EHP) can be generated in a semiconductor by an incoming photon with energy βπ > πΈπ, where πΈπ 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).
- If there is an electric field across the semiconductor, there will be an increase in current
- Known as photoconductivity.
- Increases the conductivity of the semiconductor.
What bias does a photodiode (pn junction) need to perform as a photodetector?
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 is current generated in a photodiode (pn junction)?
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.
Effect of illumination on the I-V curve of a photodiode
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
Explain what happens for increasing optical power on a photodiode in reverse bias
- 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.
What happens if a photodiode is under forward bias?
- 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 πΌ β π 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 (πππ) will appear across an open-circuit photodiode that has light falling on it. For 0 < π < πππ the diode operates in photovoltaic mode. It is in this region that pn diode solar cells operate.
Eq: Outline Photodiode absorption characteristics
At the interface between the air and photodiode, the power entering the semiconductor is π0(1 β π ).
Inside the semiconductor, the power is assumed to decay exponentially, with absorption (or loss) coefficient πΌ, so that overall the power at a distance π₯ into the semiconductor is given by:
π(π₯) = π0 (1 β π ) e(βπΌπ₯)
Eq: Outline Photocurrent in Photdiode
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:
π(π₯1 ) β π(π₯2) = π0(1 β π )[e(βπΌπ₯1) β e(βπΌπ₯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 ππππ‘ (the internal quantum efficiency), the photocurrent generated is
πΌπ = (πππππ‘ / βπ) π0(1 β π )[e(βπΌπ₯1) β e(βπΌπ₯2)]
Eq: What is the responsivity of a photodiode?
The responsivity of a photodiode is the ratio of generated photocurrent to optical power incident on the detector.
mA.mW-1
Eq: What is the external quantum efficiency?
Compares the number of electrons generated to the number of photons incident on the photodiode. The number of photons incident per second is π0/βπ, and the number of electrons flowing per second is πΌ0/π.
πππ₯π‘ = π π (βπ / πΞ»)
πππ₯π‘ can be expressed as:
πππ₯π‘ = ππππ‘(1 β π )[e(βπΌπ₯1 ) β e(βπΌπ₯2)]
What is the Spectral Response of a photodiode?
- Rearranging πππ₯π‘ = π
π (βπ / πΞ») 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).
p-i-n junction diagam, energy plot, fixed charge density plot and electric field plot
Eq: Poissonβs equation for pin junction
Where ND is the charge density
and the denominator consists of the permittivity constants.
p-i-n junction design considerations: increasing the length of the depletion region
- 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
- In practice: ldepletion >> 1 / Ξ±
- 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