Lecture 1 and 2 Flashcards

1
Q

CCD imaging

A

From near infra-red through to UV wavelengths, astronomical data arrives as photons, which trigger a CCD response

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2
Q

What is a CCD

A

A CCD is a semiconductor array of light sensitive pixels typically about 10μm across

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3
Q

Image

A

direct ‘map’ of where photons arrive

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4
Q

How does a CCD work

A

Electron released when photon strikes semiconductor

Bias voltage draws electron into potential well ; stored there during exposure

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5
Q

counts of photons obey

A

Poisson statistics

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6
Q

The number of photons arriving at our detector from a given source will

A

fluctuate

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7
Q

We make certain assumptions (axioms)

A
  1. Photons arrive independently in time
  2. Average photon arrival rate is constant
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8
Q

If observed photons satisfy the axioms the they are said to follow a

A

Poisson distribution

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9
Q

Expectation value

A

E(N) = {N} = Rτ

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10
Q

probability of receiving N photons in time τ

A

p(N) = (Rτ)^N e^-(Rτ) / N!

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11
Q

We can define the variance of N, which is a measure of the spread in the Poisson distribution

A

var(N) = σ^2 = E{[N-E(N)]^2}

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11
Q

We can define the variance of N, which is a measure of the spread in the Poisson distribution

A

var(N) = σ^2 = E{[N-E(N)]^2}

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12
Q

the variance of N is

A

var(N) = Rτ

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13
Q

the standard deviation of N is

A

σ = √Rτ

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14
Q

We estimate the arrival rate as

A

Ř = Nobs / τ

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15
Q

We quote our experimental result for the number count of photons in time interval τ as

A

Nobs ± √Nobs

16
Q

mean =

A

total number / area