Your thread title says it all. A 50mm lens with a 100mm aperture provides a paraxial f/# of 0.5, but the working f/# is significantly slower due to cos^4 law roll-off even on-axis, where f/# is usually specified. At f/0.5 the on-axis marginal rays intercept the image plane at 45 degrees, at which angle relative illumination is down 25% for the marginal rays due to cos^4 law. Quick and dirty estimation tells me that, on-axis, the effective speed is thus actually around f/0.9-f/1.0, but with exponentially worse image quality compared to an actual f/0.9 lens due to aberration dependency on f/#. The same rough calculation says Kubrick’s f/0.7 lens was effectively f/0.85 or so (marginal ray illumination is down to about 47% on-axis)
Off-axis it’s even worse, as at some point the ray angles exceed Brewster’s angle (about 54 degrees for digital camera cover plates, 56.5 degrees for gelatin) and simply reflect off the imaging media, where they then bounce around inside the camera and then contribute to veiling glare and loss of contrast. Effective f/# off-axis would drop to f/4 or less even without vignetting.
An *effective* f/0.5 cannot be achieved, as Brewster angle and cos^4 limits effective f/# to 0.7 or so..it’s an asymptotic approach iirc.
So there you go. Note this limit has nothing to do with technology to fabricate / assemble, practicality of using a lens, nor even image quality. Technology and practically do not limit design work. Laws of physics, however, cannot be broken and create a true limit.
Once you can follow what I wrote, you will no longer have to say you don’t understand why they don’t make a 50mm f/0.5 lens.
-Jason