Nathan Warford said:
I understand that the Standard Model of QFT treats elementary particles like the electron, quark, photon, muon, etc. as point-like objects. But I've also heard that a "point-like particle" is nothing more than an idealization of a particle. Elementary particles can be treated as point-like objects in experiments because they have no detectable size, but just because we can't detect their size doesn't mean that they have some finite size smaller than what we can detect (I've heard that this scale is about 10-18 meters).
Some string theorists have said that elementary particles have a size on the scale of the Planck Length. But "on the scale of" means nothing more than a size that can be expressed in Planck units, as opposed to a specific, well-defined number of Planck units. Are there any theoretical models that predict the sizes of the various elementary particles?
There is more than one sensible definition of the term "size" with respect to an elementary particle.
For example, if all particles had truly point-like properties for all purposes, in the limit, nothing would ever interact with anything else, because all Standard Model forces involve carrier bosons interacting with fermions (and sometimes with other carrier bosons as well) in a contact-like manner. But, for purposes of figuring out if a particle moving in the general direction of another particle will "scatter" due to one of the forces in the Standard Model, a particle has a finite size, often within a few orders of magnitude of femtometers, that is part of the equation governing the likelihood that the particles will interact. A description of some of these concepts (there are several similar such concepts) is found in the Wikipedia article on
Compton wavelength.
Another important concept to keep in mind when trying to make sense of the size of a fundamental particle is the uncertainty principle, which provides that one can't know both a particle's location and momentum at the same time at a combined precision greater than that permitted by an equation proportional to Planck's constant. Basically, the harder you look, the more something gets out of focus, not just from a practical perspective, but fundamentally as a intrinsic feature of Nature itself.
Also, special relativity further messes with our normal conception of even basic concepts like length, which turns out to be a function of velocity relative to the speed of light (in a way that nonetheless is not frame dependent).
And, the point-like nature of a fundamental particle is also messed with by the quantum mechanical concept that an unobserved particle is in some sense not in any single place at one time, instead, it is smeared as a probability distribution over all places it could possibly be at once.
Further, while it is contrary to our ordinary intuition, point-like fundamental particles that are not scalars (i.e. spin-0) have directional properties that our ordinary life experience can't make sense of outside a non-point-like topology in an object. (And, indeed, most physics textbooks illustrate these particles as non-point-like in order to explain these properties for heuristic reasons.)
Thus, while to say that fundamental particle is point-like isn't really a category error (there are lots of mathematical purposes for which treating it as point-like is the correct treatment), being point-like doesn't have all of the intuitive implications that it would for an object in your daily life that you could observe unaided.
Somewhat related is the trichotomy of reality, causality and locality in quantum mechanics. The intuition in your question hinges heavily upon the "reality" of a fundamental particle, but in quantum mechanics we know that there are circumstances where all three of those concepts can't be simultaneously true, which is basically a problem with the concepts themselves, as much as it is a statement about what properties Nature has or lacks.