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Summary This technique uses a diffraction grating mounted in front of a camera fitted with a long focus lens. It was developed as a simple way to improve the resolution of low dispersion spectra of bright objects using the Star Analyser diffraction grating, compared to the standard configuration. In practise a resolution of typically 15A can be obtained, some 2-3 times better than the alternative simple configuration with the grating mounted in the converging beam between telescope and camera. The peculiar eclipsing binary star Epsilon Aurigae was the original application, (Click here for high resolution spectra of Epsilon Aurigae) however I suspect it has significant potential as an educational tool, providing the simplest possible introduction to practical astronomical spectroscopy and the spectral classification of stars. |
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The
Technique
(Modified
12 May
2009
to include results using
a fixed camera on a
tripod)
Using an Objective Prism (a wedge prism placed in front of the
telescope aperture) is a long established way of
producing low
resolution
spectra. A similar
technique
can be used with a
diffraction
grating, but
large
diameter gratings (and objective prisms) are expensive and
the dispersion produced by even a coarse 100
lines/mm
grating is unmanageably
high with a
typical telescope
focal
length.
Using a
camera lens
instead of
a telescope
however gives
a more reasonable
dispersion and the
smaller objective size of a typical
camera lens means
small
affordable but
efficient 1.25 inch
diameter gratings
such as the Star Analyser can be
used.
Of
course
using
such a small aperture
restricts the
technique
to brighter
objects but
because the light from the star is
already
collimated, it potentially
can give significantly
improved
resolution (typically
3x)
compared with
the alternative simple technique
of placing the
grating in the
converging beam
between the
telescope and
the
camera.
Making the
most
of this potential
increase in resolution requires
a
higher
dispersion than is normally used with
the Star
Analyser, which
means a larger camera
detector if
the full
spectrum plus zero
order is
to be
imaged. (Useful to aid
focusing and calibration,
particularly for
beginners). A large format
monochrome astro
camera
would be an
ideal
but expensive option. Alternatively
Digital Single Lens Reflex cameras such
as the Cannon 350D
etc perform well
under astro imaging conditions and can be
used successfully in this application, though
with
restricted wavelength
range towards the IR unless
the internal IR blocking filter has been
removed or
replaced.
The
choice of lens focal length depends on a number
of
factors:
The
dispersion increases
proportionally with
focal
length but
so does the size of
the star image so the
resolution
is largely
independent of
focal length.
A shorter focal length
means a
shorter, more concentrated
spectrum and therefore
fainter
objects can be
recorded.
With
too short a
focal length however, the star
image will
be
undersampled (ie the
star image
will be smaller than a single pixel,
remembering that for
a colour camera
like a DSLR, the
effective pixel
size is
larger than a single pixel due to
the Bayer pattern of pixel colour coding).
Undersampling
can produce severe
artifacts in the spectrum,
particularly with
colour
cameras.
A short focal
length also means a greater area of sky is
imaged
giving a higher sky
background brightness and an
increased risk of interference from other
stars and their
spectra.
(Note that using this
technique with
short
focal lengths
can be useful for
recording spectra
of fainter
diffuse
objects such
as comets as seen here
bottom of
the page. In extreme cases it also be used
to cover
a wide field at ultra
low
resolution
as in this meteor
spectrum)
Too long
a
focal length and it will not
be
possible to fit
the star
(zero
order) and spectrum in the
frame. Tracking also
becomes
more
critical at higher focal lengths.(Indeed,
with modest
focal lengths it is
possible to produce
"drift
spectra"
with a fixed
camera)

For these tests I used a 100 lines/mm Star Analyser grating with a Canon 350D camera fitted with a 75-300mm zoom lens at 200mm focal length which gives a dispersion of about 3.5A/pixel. It was piggyback mounted on my main telescope. ((It is also possible to used a fixed camera on a tripod, orientating it so the star drifts perpendicular to the dispersion direction.)

To mount the grating, I cut a hole in a lens cap and
screwed the Star Analyser into it. To make it easier to
rotate the grating
independent of
the focusing adjustment,
I added a
blank rotatable filter
cell
(from an
inexpensive
crossed
polarising
filter set) between the lens cap and the
Star
Analyser. An
alternative could be to adapt a
blank
photographic filter
cell the right
size for the
lens.
This could be
orientated by screwing the
assembly in
and out. The small
grating aperture
produced some vignetting but not
so
severe that it could not be removed using a flat
field.
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A typical single 30sec exposure of Epsilon Aurigae
(7th full size) |
Flat field |
Recording the Spectra
If you are using a DSLR camera set it to record RAW images.
(unlike jpegs, these are uncompressed, have a greater bit
depth and do not have
a white
balance setting
applied)
As
well as your target
star spectrum
you
should record darks and
flats and at least once (and
ideally
every
session), a calibration star spectrum (a
bright spectral type A star is best eg
Vega, Altair,
Castor, Regulus,
preferably at similar elevation to your target).
It is a
good idea to take the
calibration star
spectrum
first,
using it to
get the focus and grating
orientation correct and then move to the target
without
disturbing the
settings.
Start by recording an image without the
grating in place. Position the star in the
centre
left of the frame,
leaving
enough
room to the right for
the
spectrum. (A zoom lens is handy
here
as
you can locate
the star and
position it roughly before zooming in.) Check that
there
are no faint stars close
to a line running
horizontally from the star
in
the
region where the
spectrum will
fall and no bright
stars on the same
line
within the frame or
within a frame either side
which
could potentially
produce spectra overlapping
with the wanted spectrum. If there are,
reorientate the
camera so that
the horizontal line is free from such
potential
interference.
Note I
f you are
using the camera on
an undriven mount,
orientate the camera with the horizontal axis of
the camera field pointing at the celestial
pole.
(ie orientate the
spectrum
along the Dec axis). That
way
any star
trailing will
occur
perpendicular to
the direction
of the spectrum. If there is potential
interference
from other stars,
you will be unable to
rotate the
camera to avoid
them but
you could
try running
the spectrum from left to right
instead by
rotating the
grating 180
deg.

A "drift spectrum" of Deneb taken using a fixed camera and 200mm lens on a tripod
Continue to Processing the Spectra >>>