SkepticalScience said:
I asked about QM before - and have since read a bit more about the topic. I still have 2 questions though:
1. Can scientists "see" the particles that make up protons and things? Meaning - do scientists have some sort of super-duper microscope that can actually see these particles? If not - how do we know they exist really??
I'll give a little more detail about what BDZ said. If you whack protons and neutrons hard enough in particle accelerators, you can break them. These collisions are extremely energetic, and the resulting particles are detected in large particle detectors as trajectories, from which you can infer things about them such as their charge and their energy. It gets quite tricky, because you're not only breaking apart the particles, you're also often forming new particle/antiparticle pairs. So analyzing all this gets quite complicated. But by looking at conserved quantities (such as charge and energy/mass), you can infer quite a bit. One of the things they've infered is the existence of quarks: three quarks make up protons and neutrons (the combination determining which you get), but you can also have exotic particles with only two quarks (though I think they decay fairly quickly). But you NEVER see solitary quarks. We infer their existence because of the way the properties they have (such as mass and charge) get conserved across all the different products of collisions.
2. At the quantum level, are the motions of the sub-atomic particles TRULY random - or is it that we don't know what controls it yet??
I would say that this isn't really a well-formed question in the quantum mechanical sense. Quantum mechanics is completely deterministic: the waev function for a system evolves according to an equation with no randomness involved. The problem comes from the measurement process: what exactly does the wave function mean? If we want to measure the position of a particle, we can treat the wave function as a probability distribution and say that the rest is just randomness, but that's not satisfactory. We can also postulate that there are some hidden variables (what you allude to), factors which, if we could know them, would completely determine things unambiguously. But that's actually not satisfactory either, since it's been proven that any possible hidden variables theory is necessarily non-local (shorthand: there's still weirdness going on). And besides, we have no idea where to start with such a theory, so it really doesn't get us any farther.
But there's even a third point that I think gets brushed under the rug far too often. Namely, quantum mechanics makes no distinction between microscopic and macroscopic systems. Our measurement apparatus, in quantum mechanics, is some EXTREMELY complicated system with LOTS of particles. Modelling it with quantum mechanics is, practically speaking, an impossibility, but that doesn't mean it couldn't be done in principle (if, for example, we had a truly infinite and infinitely fast computer, and we could somehow know the exact initial quantum mechanical state of our instrument). IF you could do so, then the complications that arrise from our single particle interacting with this massively many-bodied system (which, due to thermal fluctuations, is never going to be in the same initial state for any two measurements) might make what looks initially like randomness turn out to be not so random after all. But unfortunately, we really can't do that, so this too is kind of just speculation, although I find it much more satisfying than hidden variables (since there's only a practical, not an in-principle, obstacle).
So as a practical matter, we're kind of left with our first option. It does look like there's some inherent randomness in quantum mechanics, but we only need to address it if we do a measurement. The time evolution of a wave function in quantum mechanics is not, itself, random at all.