A point: I would remind the OP that there are two scales of answer to the question. If you are asking about what you would see on a photon by photon basis then for each photon observation you don't see an interference pattern, that only manifests in the aggregate of many observations. In the aggregate you get the same behavior as for a classical wave, i.e. whatever interference pattern should emerge.
Here is how you calculate both the probability distribution of what you see photon by photon and in the aggregate. Keep in mind you perceive direction based on the location that the photon is absorbed on the retina (or camera's film, CCD, or CMOS chip). So you would take a point on the retina, "sum over all paths" back to the source through each slit. What you are summing is amplitude as it propagates with phase over the path. Some issues are the aperture (how dilated is your pupal?) relative to wavelength and slit dimensions.
...pause to consider...
Firstly if you have a nearly pinhole camera, aperture comparable to slit size and wavelength of the light, you will get the equivalent of a single pinhole interference pattern on your retina at the amplitude for the value of the regular double slit interference pattern at the position of the aperture. That would mean you would see for many photons, the light coming from a wide range of angles concentrated near the front and with ring interference pattern. On a photon by photon basis you see random photons (speckles in the dark) distributed with probabilities following the mentioned pinhole interference pattern.
In the case of a very large aperture relative to the wavelength (more typical) you would get ...[ pause to calculate...] well I balked at doing the full derivation, I have tests to grade. But I might work this out when I have time. My intuition says you get an image of the slits hence you would see photon by photon, a 50 50 chance of it appearing for each slit, as mentioned by other posts.
In the intermediate case you should get an overlay of the two cases, your aperture diffraction smeared over the classical image of the two slits so you'd see the blurred image of two slits with some fringing determined by aperture diffraction. But again, photon by photon a point speckle randomly distributed over the mentioned patterns.
[edit: Reminder to all, the quantum behavior will always be probabilistic point observations with distribution matching the classical wave diffraction behavior.]