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Astronomical Techniques ILecture 12
Yogesh Wadadekar
Jan-Feb 2015
IUCAA-NCRA Grad School 1 / 27
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Objective prism imagers: place prism over telescopeprimary
IUCAA-NCRA Grad School 2 / 27
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Principle of diffraction gratings
Maxima in the output intensity occur at a sequence of anglessin θn = nλ/d .
IUCAA-NCRA Grad School 3 / 27
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Diffraction grating contains many slits. Order 1onwards, separation happens!
gratings contain hundreds to thousands of grooves/mm.IUCAA-NCRA Grad School 4 / 27
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proof of grating equation with reflection grating
nλ = d(sinα+ sinβn)
IUCAA-NCRA Grad School 5 / 27
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reflection grating
Sign convention: α and β have opposite signs if they are on oppositesides of the grating normal.
for m = 0 grating acts as a mirror α = −βfor m > 0, β > −αfor m < 0 β < −α
IUCAA-NCRA Grad School 6 / 27
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Blazed grating -Littrow configuration
2d sin θB = mλ
IUCAA-NCRA Grad School 7 / 27
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Reflection and transmission gratings
How is this transmission grating different from a prism?
IUCAA-NCRA Grad School 8 / 27
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Pattern for many slits - monochromatic light
The addition of slits increases the sharpness and brightness of thepeaks but leaves the locations of the orders unchanged. Of course,slight peak offset for slightly differing wavelength.
IUCAA-NCRA Grad School 9 / 27
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But different orders overlap!
IUCAA-NCRA Grad School 10 / 27
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Resolution of grating
If grating is illuminated by polychromatic light. In a given order, redderlight is diffracted to larger angles than blue light. The maxima foradjacent wavelengths in a given order are offset slightly. Spectralresolution for order n is determined by the wavelength shift needed toplace the diffraction pattern maximum for λ+ δλ on the first minimumin the pattern for λ. The resolution is:
< =λ
δλ= nN
so it depends both on the order and on the total number of slitsilluminated on the grating N.
IUCAA-NCRA Grad School 11 / 27
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Angular dispersion
in order n is given by:dθdλ
=n
d cos θHigher dispersion corresponds to larger values of this quantity.Echelles take advantage of both n and θ dependence to maximizedispersion.
IUCAA-NCRA Grad School 12 / 27
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Astronomers working definition of dispersion
Astronomers often use the word dispersion to refer to dλ/dx in thespectrograph focal plane, usually quoted in Å per mm. This is moreproperly called the “linear reciprocal dispersion”. It is inversely relatedto the angular dispersion, so lower values correspond to higherwavelength dispersion. e.g. Sloan Survey has 3 Å per pixel (24 µm).
IUCAA-NCRA Grad School 13 / 27
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Advantages of gratings
Dispersion same for all wavelengths in given orderLarge dispersions/resolutions possible (large n)Transmission or reflection gratings availableHigh UV throughputs possible (with proper reflection coating)Grating technology highly developed, extensive customizationpossible
IUCAA-NCRA Grad School 14 / 27
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Disadvantages of gratings
Size limited by capacity of ruling engine. Use of mosaic gratingswith large beam telescopes possible but performancecompromised.Order superposition: red light of a given order is spatiallycoincident with blue light from a higher order. In echellespectrographs, use a second grating as a cross-disperser.Low efficiency: Gratings distribute light across a large number oforders (including the zeroth order, which has no dispersion). Fluxdecreases rapidly with order. Solution: Blazed reflection gratings,in which the facets of the slits are cut at an angle that places themaximum of the single-aperture pattern at a chosen wavelengthand order.
IUCAA-NCRA Grad School 15 / 27
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Echelle grating and cross disperser
IUCAA-NCRA Grad School 16 / 27
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How gratings are manufactured
a master is prepared with a diamond tool making closely spacedgrooves on metal - high cost.many replicas can be made with plastic using the metal grating asmaster.these can be mounted on glass to form a transmission grating orcoated with a reflective material to form reflection grating.
IUCAA-NCRA Grad School 17 / 27
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Grism - Prism + Diffraction grating
A grism is a combination of a prism and grating arranged to keep lightat a chosen central wavelength undeviated as it passes through acamera.
IUCAA-NCRA Grad School 18 / 27
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Spectrograph variants: Double spectrographs
IUCAA-NCRA Grad School 19 / 27
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Spectrograph variants: Fiber fed multi-objectspectrographs (1D)
IUCAA-NCRA Grad School 20 / 27
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SDSS plugplate
IUCAA-NCRA Grad School 21 / 27
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Long slit spectroscopy (2D)
IUCAA-NCRA Grad School 22 / 27
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Long slit spectroscopy
Which way is the galaxy rotating?
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All detector imaging steps apply for spectroscopy
Bias subtraction, Dark subtraction, flat fielding, cosmic ray removal,bad pixel interpolation etc. are required for spectroscopic data.
IUCAA-NCRA Grad School 24 / 27
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Integral field spectrograph (3D)
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Tiling a galaxy with lenslets
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Integral field spectrograph
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