Mathematically this comes from the fact that (x+y)^2 is not equal to x^2 + y^2.
In terms of Feynman's "adding arrows" I'm assuming that the dark lines in an interference pattern represent areas where the probability amplitudes of a photon from one slit arriving 180 out of phase with a photon from the other slit are greatest. However, I don't know if that is right since he doesn't specifically talk about double slit interference in the chapters on photons in QED.
He discusses a single slit, and explains why the smaller the slit the more the light seems to spread out, which is that the narrower slit increases the probability of photons with the same bias (phase) arriving adjacently everywhere. The narrow slit selects out a group of adjacent paths, which, all being similar in time, are similar in bias. Being similar in bias, they don't interfere, don't cancel each other out. The apparent spreading, he seems to be saying, is not actually new behaviour, light is always doing this, it's just that now the impediment to seeing it (canceling by out of phase photons) has been removed. (This is all roughly, on pages 53-56 of the paperback edition of QED)
Imagine a horizontal slit in a vertical piece of flat metal parallel to a wall. Light comes through the slit and shines on the wall. My thinking about what happens next (Feynman doesn't explicitly say) is that, as all the selected 'in phase" light fans out from the slit, the arrows (that designate where the stopwatch pointer would be pointing when they hit the wall) are pointing in a slighly more advanced position for each bit of distance you go vertically up the wall, or down the wall from a horizontal line on the wall level with the slit in the metal through which the light is coming.
Each unit distance up or down the wall from the reference line represents a longer path, and the stopwatch will turn a little farther before the photon hits. And what we end up with is a very neat, smooth gradation of phase up and down from the original stopwatch position to the final one. Any given photon will be pretty much exactly in phase with the others on the same horizontal line, and will be only slightly out of phase with the ones that are, say, a thousandth of an inch above or below it. The ones an inch away, above and below are much more out of phase, and so on.
Adding a second slit, by this reasoning, superimposes a similar fan of photons, precisely graduated by phase, onto the first. The stopwatch pointers of alternate bands of them will naturally fall into "in phase" and "out of phase" categories. The out of phase ones cancel each other out, and the in phase ones reinforce each other. Since all horizontal lines from each individual slit are in phase, the net result is "bands" of light and dark.
Feynman, however, doesn't explicitly say anything about what happens when you put a second slit next to the first, so I'm not sure if I've reasoned this out correctly.