I see - thank you for adding that context, I think that this title change is in itself quite interesting… Because then they did intend to use a sensationalist title, and only changed it later.
I have double-checked out of curiosity and I do see that your post’s title is the title indexed by google:
I am sorry for jumping into the assumption that you had changed the title yourself.
EDIT: Ah! After sending this answer I saw jorge’s answer!! So this answer is redundant, but at least you can see that two people arrived at virtually the same conclusion 😀
We need to define a threshold of energy that we consider “ionizing radiation”, and we also need to a more precise definition of “starlight”.
I will arbitrarily select the ionizing radiation threshold to be at 10 eV (124 nm). As for “starlight”, let’s just say that we want to push the 750 nm red light all the way until the point where it becomes ionizing. One thing to consider is that in this situation you will also push infra-red light from the stars towards the visible, so if a star emits a lot infrared this IR light will become “starlight”. So the answer can be muddled up by all of these definitions as well as the emission properties of the star.
To keep it simple… Let’s shift 750 nm red light to 124 nm ionizing radiation. You can rearrange the Doppler expression from this website to solve for the “v” to get the velocity needed to transform 750 nm to 124 nm. The solution I get is -284,035,329 m/s, with the “-” sign indicating movement of the receiver towards the source.
You can double-check by inputting 750 nm as the wavelength from the light emitted by the source, -284,035,329 m/s as the velocity, and the speed of light as “c”:
Then, if you agree with the assumptions, definitions, and the analysis, the receiver needs to move at about 94.68% the speed of light to shift the redder starlight into the ionizing radiation range.