The doughnut-shaped bokeh you get from the central obstruction in a mirror lens (aka catadioptric lens) is always a nice artistic touch.
It's challenging to make a long focal length lens with a low focal ratio using glass. The focal ratio (f-stop) is the area of clear aperture of the lens divided into the focal length. That means in order for a 500mm lens to offer f/4 the area of clear aperture has to divide into the focal length four times... which requires a diameter of 125mm (about 5").
When a "glass" lens is used, problems with chromatic aberration become severe at that size and you have to use exotic low dispersion elements and achromatic doublets in an attempt to "reduce" the impact. This means the lens is not only physically large, but it's also going to be heavy. Canon likes to use fluorite crystal for their low dispersion elements. Fluorite has to be synthetically "grown" in a kiln and in order to make a crystal large enough to grind into a optical grade lens requires a very long time in a kiln.
Basically there's no "cheap" way to do this and get a lens that isn't garbage. The "long" glass telephoto lenses tend to be f/5.6 (because split-prism & phase-detect focusing still works at f/5.6) but much above that and it basically doesn't work anymore. I have an old 35mm camera with manual focusing and the split prism focus aid. You can't even focus that above f/5.6 because half of the mirror will almost always be black. You can only look at the image and try to visually make the image as good as possible.
A catadioptric lens (basically works like a Schmidt-Cassegrain or Mak-Cas telescope) uses parabolic mirrors to focus light rather than passing the light through a lens. Since the light only "bounces" off a mirror rather than passing through a lens, it doesn't have a CA problem (thank Isaac Newton for discovering this.)
Catadioptric scopes work fabulously on deep space objects (no bokeh). But not so well on terrestrial objects because the "blur" always takes on the shape of the clear aperture. Catadioptric scopes always have a central obstruction. This means the area of "clear" aperture is always in the shape of a doughnut -- so you get circular "bokeh" with a black center.