I'm a one-boxer. It seems obvious: in Newcomb's problem, I'm a millionaire as a one-boxer, but would get much less as a two-boxer.
But what I want to communicate is something like... a perspective from which two-boxing seems obvious.
Nozick's "Newcomb's Problem and Two Principles of Choice" says
According to expected value, you should one-box
According to dominance, you should two-box
Well, I want a high expected value of money, so I should one-box, is that all there is to it?
The issue is that this seems like nonsense. The dominant choice necessarily has higher expected value. At least, that's so in what I'll call "classical decision theory", for which my reference is Savage.
So the perspective I need to communicate is the one where classical decision theory seems perfectly adequate. Not just that, but obvious, even trivial.
And I think this is basically the same perspective where you manage not to worry about quantum interpretations your whole life. Which is not some kind of intellectual uncuriosity, but just that you think of quantum mechanics as something you do with explicit models.
Asking questions like, will anthracene have color? It's basically three fused benzene rings. You have a description that specifies the position of every atom, and then you can simulate it in an oscillating electric field, and ask if it absorbs energy. Anthracene won't throughout frequencies corresponding to the whole visible spectrum, but alizarin will (just anthracene with a few substitutions), which is why it's a red dye.
Those are calculations "in the gas phrase", or rather, simulations of a molecule in empty space. If we want to know about the tube of alizarin in our lab, that's in some organic solvent–usually we just modify the dielectric constant in the simulation, rather than explicitly including solvent molecules. That's how far we are from including the observer, or even the measuring device–we're not even including the solvent.
Classical decision theory makes physical sense to me in the same way. To Savage, acts are functions from states to consequences. He says "states of the world", but defines the world as "the object of interest", so it's really states of the system. Like, if the tube has anthracene, it won't absorb blue light, but if it has alizarin, it will. So I see Savage's "act" function as just the dynamics of the system.
There's no conflict between free will and determinism in classical decision theory. Different initial states evolve to different final states. How does it get in one of those initial states and not the other? Well, we don't include the guy putting the molecule into the tube into our simulation software, and in Savage's decision theory, we don't worry about it any more than we do in physics.
That turns out to make all the difference in quantum interpretations, and in Newcomb's problem, but it's easy to overlook it, as I think Savage does. Because we're not explicitly avoiding inclusion of the observer/decider, we're just only explicitly including whatever we can actually describe precisely enough to calculate with.
So we get to Newcomb's problem. Two possible states of the system: money in both boxes or money in one. So you can make a dominance argument. Or you can make an expected value argument, and you'll conclude that regardless of the probability of the two states, two-boxing has higher expected value. (Which is actually the correct derivation that two-boxing is better vs any random opponent, btw)