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In the past decade there have been many versions of visual spectroscopes made available to the amateur market. One such device is the Rainbow Optics Star Spectroscope, a device that consists of a transmission grating housed in a 1.25" diameter filter cell, and a lens assembly that fits over the telescope eyepiece. Using this device, any amateur can see spectroscopic details in bright stars using modest telescopic equipment. In a 106mm scope, one can make out detailed absorbtion lines in stars down to magnitude 4 pretty easily. Now, place the grating of this unit in front of a CCD camera; Just screw it into the CCD's nosepiece. You now have a spectrograph capable of recording spectra from any subject that you can normally image. The possibilities are virtually endless.
The distance the grating resides from the imager chip determines the spread of the spectrum, and to some extent, the resolution offered by the system. Since the nosepiece of the MX-5C is so long, the spectrum fills the width of the CCD image, and the star (0 order image) is not visible in the same frame. That is a setback, since having the star within the field of the image helps to callibrate spectral lines later on in the process.
In a later evening, I discovered that the grating could be screwed into the empty hole in the SBIG CFW-8 color filter wheel. This brings the grating closer to the chip and presents an image of the star (0 order) along with the 1st order spectrum all in the same field of an ST-7.
First, the object to be imaged is centered on the CCD chip, and the scope's drive is kept running. Using slow motions, the star is moved to one side of the chip which brings the first order spectrum into view of the chip. Now you should be able to take a quick 2-3 second integration of the star and its first order spectrum. Some time must then be spent on focus. Be sure to focus on the spectrum, not the star, as the spectrum is created at a steep angle to the focal plane. Note that a sharp focus can only be achieved on one section of the spectrum at a time.
Once the star is focused, set the CCD software to take a ten second integration. Once set, turn off the mount's tracking power letting the star drift in RA. Now, activate the integration. When complete, turn the drive back on again. This process can be repeated two to four times without having to re-center the star's image on the chip.

Also, keeping the grating aligned with the CCD's pixel rows helps to keep things oriented better for these operations. I used some teflon tape on the filter threads to tighten the grating up in the proper orientation when I placed it into the CFW-8. Once aligned, the images will look more like the following:

This is a 10 second integration of the star Arcturus, also using the FSQ-106n and the ST-7. The grating was properly aligned to the pixels, and the pixels were properly aligned to the RA drift direction. All went well here. Note the varying brightnesses of the horizontal lines. These are caused by scintillation, the star's twinkling in the atmosphere. Even though the seeing conditions were not the best, a fine spectrum is captured. This makes for another reason to do spectroscopy ;-)
Below is a chart of all the spectra I obtained on a couple of evenings. They are arranged such that their 0-order star image is in line from image to image, and they are all to the same scale (raw unprocessed FITS images converted to JPEG). They are also ordered such that the younger stars are at the top, and older stars are at the bottom. Note how the spectrum itself migrates towards the red and infra-red as the stars get older and redder. This is just as one would expect.

Those looking for more precision should investigate the following two software packages, both free:
IRAF (UNIX flavors only)
VSpec (MS Windows, in French and English)
These will handle more complicated spectral analysis including the typical non-linear Angstrom-Pixel relationships you will discover. They will also help to identify various spectral lines.
When processing the spectrum, try to avoid complicated image processing algorythms that might alter the brightness levels of the image. Linear (screen) stretches are ok, but nonlinear ones complicate the analysis. Sometimes an unsharp mask helps to better define faint absorbtion lines. Both IRAF and VSpec will create graphs representing intensity vs. X-pixel-position (Wavelength).
This design can be greatly improved by adding a wedge prism to the grating. This "lenses" are available from Edmund Scientific and will help to reduce various abberations (coma). See a wonderful explanation online at Christian Buil's website: The Theory of Diffractive Gratings in Converging Optical Beams. He goes into marvelous detail about the theory, construction and use of grisms for spectrography. This article is a "must" for those wishing to improve their systems.
Christian Buil's Home Page
The Spectrography Bookmark
The Spectra of Gas Discharges
The Forum for Amateur Spectroscopy
Worcester Park Observatory: Maurice Gavin
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Last Modified: 3/19/03 8:55p
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