Lecture 1 and 2 Flashcards
CCD imaging
From near infra-red through to UV wavelengths, astronomical data arrives as photons, which trigger a CCD response
What is a CCD
A CCD is a semiconductor array of light sensitive pixels typically about 10μm across
Image
direct ‘map’ of where photons arrive
How does a CCD work
Electron released when photon strikes semiconductor
Bias voltage draws electron into potential well ; stored there during exposure
counts of photons obey
Poisson statistics
The number of photons arriving at our detector from a given source will
fluctuate
We make certain assumptions (axioms)
- Photons arrive independently in time
- Average photon arrival rate is constant
If observed photons satisfy the axioms the they are said to follow a
Poisson distribution
Expectation value
E(N) = {N} = Rτ
probability of receiving N photons in time τ
p(N) = (Rτ)^N e^-(Rτ) / N!
We can define the variance of N, which is a measure of the spread in the Poisson distribution
var(N) = σ^2 = E{[N-E(N)]^2}
We can define the variance of N, which is a measure of the spread in the Poisson distribution
var(N) = σ^2 = E{[N-E(N)]^2}
the variance of N is
var(N) = Rτ
the standard deviation of N is
σ = √Rτ
We estimate the arrival rate as
Ř = Nobs / τ