It's been published many times over the past two and half centuries (not by me of course) and you'll find it in any textbook treatment of waves.
Crawford's "Waves" is volume 3 of the Berkeley Physics series, a standard textbook for the third semester of a undergraduate physics program and a good starting point - I'm partial to it because it's the one my professor used so I have a copy on my bookshelf.
But, repeating myself, this is not quantum mechanics. It is classical wave behavior and a prerequisite to quantum mechanics (which started for me in the fourth semester). The quantum mechanical double slit experiment works more like:
The probability of a photon landing at any given point on the screen is calculated by considering all possible paths between the photon source and that point. Each path makes either a positive or a negative contribution to that probability, and we sum all of these to get the total probability (the actual probability is the square of this sum).
When two slits are open a photon can pass through either slit. There will be some areas of the screen where the contribution from paths through one slit will be positive while that from the other is negative and they cancel; in others both will have the same sign and they reinforce one another; and we get the alternating regions of high and low probability that make an interference pattern after enough photons have made their dots on the screen.
But when we close a one slit, or place a detector at a slit, then any given photon can only have gone through one slit or the other, so we only have the contributions from the path through that one slit. There’s no opposite sign contribution from the other slit to cancel or reinforce it, so no interference pattern. There still is a bit of pattern, usually called a “diffraction pattern”, that comes from having some paths through the left-hand side of the single slit and others through the right-hand side.
The connection to classical electromagnetic waves, Young's double-slit experiment, and other "let's make an interference pattern with laser light" demonstrations is that the probability amplitudes in the quantum mechanical experiments obey a wave equation similar to the classical wave equation. Thus we need the mathematical techniques of Crawford's book or equivalent before we can start in on the quantum mechanical problem, and we can use our intuition from the classical waves as an analogy to get a feel for how the quantum mechanical probabilities behave. And if we're trying for a layman-friendly math-free explanation, that analogy is all we have.... but it leads to confusion when people hear it, mistake the analogy for the real thing, and come away believing that Young and subsequent optical demonstrations are showing quantum mechanical behavior.
Feynman’s non-serious layman-friendly book “QED: The strange theory of light and matter” is worth reading. It is no substitute for learning the math, but it goes into more interesting examples of this “contributions from all paths” model.