The question "how would the coin have landed if I had guessed tails?" seems to me like a reasonably well-defined physical question about how accurately you can flip a coin without having the result be affected by random noise such as someone saying "heads" or "tails" (as well as quantum fluctuations). It's not clear to me what the answer to this question is, though I would guess that the coin's counterfactual probability of landing heads is somewhere strictly between 0% and 50%.
Oh, interesting. Would your interpretation be different if the guess occurred well after the coinflip (but before we get to see the coinflip)?
Summary: There's a "thin" concept of counterfactual that's easy to formalize and a "thick" concept that's harder to formalize.
Suppose you're trying to guess the outcome of a coinflip. You guess heads, and the coin lands tails. Now you can ask how the coin would have landed if you had guessed tails. The obvious answer is that it would still have landed tails. One way to think about this is that we have two variables, your guess A and the coin C, that are independent in some sense; so we can counterfactually vary A while keeping C constant.
But consider the variable X=A XOR C. If we change A to tails and keep X the same, we conclude that if we had guessed tails, the coin would have landed heads!
Now this is clearly silly. In real life, we have a causal model of the world that tells us that the first counterfactual is correct. But we don't have anything like that for logical uncertainty; the best we have is logical induction, which just give us a joint distribution. Given a joint distribution over A×C, there's no reason to prefer holding C constant rather than holding A XOR C constant. I want a thin concept of counterfactuals that includes both choices. Here are a few definitions, in increasing generality:
1. Given independent discrete random variables A and C, such that C is uniform, a thin counterfactual is a choice of permutation ϕ(a) of C for every a∈A.
2. Given a joint distribution over A and Y, a thin counterfactual is a random variable Z independent of A and an isomorphism of probability spaces A×Z≈A×Y that commutes with the projection to A.
3. Given a probability space A and a probability kernel κ:A→Y, a thin counterfactual is a probability space Z and a kernel λ:A×Z→Y such that ∫Zλdz=κ.
There are often multiple choices of thin counterfactual. When we say that one of the thin counterfactuals is more natural or better than the others, we are using a thick concept of counterfactuals. Pearl's concept of counterfactuals is a thick one. No one has yet formalized a thick concept of counterfactuals in the setting of logical uncertainty.