Lecture 8: Spectroscopic Instruments Flashcards

(36 cards)

1
Q

chemical composition of stellar body can be

A

determined by observing its spectrum

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2
Q

velocity determined from

A

doppler shift of spectral lines

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3
Q

doppler shift observed in light from stars

A

determine rotation frequency of arms of a spiral galaxy

large planets cause stars to wobble leading to a doppler shift

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4
Q

common components of spectroscopic instruments

A

slit
collimator
diffraction grating
focusing mirror
detector

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5
Q

in general, spectroscopic instruments

A

map wavelength to position on detector

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5
Q

resolving power

A

R= lambda / delta lambda

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6
Q

spectrometer

A

also ‘monochrometer’
entrance and exit slits
tune wavelength by rotating grating

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7
Q

spectrograph

A

also ‘spectroscope’
entrance slit
spectrum recorded on camera or CCD array

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8
Q

diffraction gratings - light transmitted by

A

gaps between lines - apertures

each acts as an independent source

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9
Q

diffraction gratings- secondary wavelets (circular waves) emanate from

A

each gap

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10
Q

diffraction grating - constructive interference at

A

certain angles (diffraction orders)

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11
Q

diffraction angle depends on

A

wavelength

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12
Q

grating equation

A

sin thetam - sin thetai = m lambda/a

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13
Q

angular dispersion equation

A

D= dthetam/d lambda = m/a cos thetam

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14
Q

instrumental width equation

A

delta theta = lambda / Na cos theta m

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15
Q

resolving power equation

A

R=lambda / delta lambda = mN

16
Q

free spectral range equation

A

delta lambda_FSR = lambda/m

17
Q

intensity maxima occur at

A

diffraction angles when the path length difference is equal to an integer number of wavelengths

18
Q

angular dispersion of the grating is the

A

rate at which the angle changes with wavelength

19
Q

angular dispersion is derived by

A

differentiating the grating equation with respect to wavelength

20
Q

getting from angular to linear dispersion

A

small angle approx x=Ltheta

dx/dlambda = L d theta/dlambda
sub in angular dispersion

21
Q

limit of resolution is when

A

first min of lambda1 coincides with the max of lambda 2

rayleigh criterion

22
Q

instrumental width delta theta

A

angular separation to the first min

23
Q

first min occurs for a phase

24
min resolvable difference in wavelength corresponds to
an angular separation given by the instrumental width
25
resolving power derivation
equation instrumental width and angular dispersion
26
at high orders, the spectra
start to overlap blue from higher order overlaps with red from lower order
27
free spectral range is
the difference in wavelength for which you start to get an overlap of adjacent orders
28
constructive interference where phase difference between adjacent rulings is
an integer multiple of 2pi
29
0th order is
direct reflection from surface or specular reflection
30
grating is described mathematically as a
convolution of a single slit of width b with an array of delta functions spaced apart by a
31
32
diffraction pattern is fourier transform of
grating transfer function (by convolution theorem in product of fourier transforms of the individual funcs)
33
intensity maximum at
zeroth order falls off going away from zeroth order
34
reflection grating inefficient
most light directed to 0th order which is undispersed and not useful only around 10% at 1st order need some means of directing all light to order of interest
35