Hi Bruce,
first, I would like to briefly explain (very simplified) where the effect comes from. Everybody knows the diffraction pattern of some typical apertures in astrophotography. So, the diffraction pattern of a round aperture is the Airy disk. The diffraction pattern of a Newtonian telescope is a superposition of the Airy disk with the typical spikes by the spider od the secondary. Also pretty much everybody knows the diffraction pattern of the Bahtinov mask. I have shown all three in the first figure. The diffraction pattern (below) is the 2D Fourier transform of the aperture shape (above).

Refractors should actually always show each star as an Airy disk. However, the telescope does not consist of only one lens, but usually of several lenses (front lens and reducer for example). In addition there are apertures like the dew shield (like Jay said before). If a star is not imaged on the optical axis, but further out at the edge of the image, then the projection of the telescope aperture is no longer a circle, but a superposition of two circles. I have tried to show this schematically.

The Fourier transformation of this aperture shape then results in the inverse lighthouse, as in your image.

The whole thing might be handeled in the image post-processing somehow (I can't do that) or it can be avoided from the beginning, if the star is not too far away from the optical axis or if the outermost projection of the aperture is circular by a clever arrangement of apertures. But the latter means: Either you use small camera chips or increase the f-stop number. But nobody really wants that. I hope I was able to help out a little.
Clear skies
Thorsten