Introduction Flashcards

1
Q

very weak signals and incorrect assumptions leads to

A

systematic errors

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2
Q

a new probe of the universe - gravitational waves

A

will give us a different, non EM view of the universe, and open a new spectrum for observation

complementary information

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3
Q

from near-infrared through to UV wavelengths, astronomical data arrives as

A

photons, which trigger a CCD response

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4
Q

a CCD is a

A

semiconductor array of light-sensitive pixels - typically about 10 micrometers across

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5
Q

CCDs - electrons released when

A

photon strikes semiconductor

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6
Q

CCDs - bias voltage draws…

A

electron into potential well, stored there during exposure

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7
Q

a great deal of astronomical data consists of counts of photons, these obey

A

poisson statistics

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8
Q

the number of photons arriving at a detector from a given source will

A

fluctuate

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9
Q

we can treat the arrival rate of photons statistically which means

A

we can calculate the average number of photons which we expect to arrive in a given time interval

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10
Q

axioms for a poisson distribution

A
  1. photons arrive independently in time
  2. average photon arrival rate is constant
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11
Q

expectation value of number of photons

A

E=<N>=Rt</N>

R is arrival rate
t is exposure time

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12
Q

If we made a series of observations, each of time seconds, we
wouldn’t expect to receive <N> photons every time, but the
average number of counts should equal</N>

A

<N>=Rt
</N>

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13
Q

probability of receiving N photons in time t

A

(Rt)^Ne^-Rt / N!

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14
Q

probability of N events given an expectation value of μ

A

p(N)=μ^Ne^-μ / N!

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15
Q

as Rt increases…

A

the shape of the poisson distribution becomes more symmetrical

(it tends to a normal or gaussian distribution)

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16
Q

variance of N

A

a measure of the spread in the poisson distribution

var(N)=σ=E{[N-E(n)]^”}

17
Q

for a poisson distribution, var(N)=

A

Rt

18
Q

for a poisson distribution, the standard deviation of N is

A

σ=sqrt(Rt)

19
Q

in practice, we usually only observe for one period of t seconds during which

A

we receive a count of Nobs photons

20
Q

estimated arrival rate

A

R hat = Nobs/t

21
Q

we take Nobs as our

A

best estimate for <N> with error sqrt(Nobs)</N>

22
Q

we quote our experimental result for the number count of photons in time interval t as

A

Nobs +/- sqrt(Nobs)

23
Q

raw image includes

A

hot pixels, readout noise, fixed pattern noise (combination of random and systematic uncertainties)

careful calibration needed to extract data

24
Q

corrected image -

A

bias, dark and flat frames
accurate photometry can now begin

25
Q
A