This is inspired by a recent post on why a free electron can't absorb a photon, though my question below is about something considerably more general.
The argument in the accepted answer goes (in essence) like this:
Taking $c=1$, and working in the rest frame of the electron, let $p\neq 0$ be the momentum (and hence the energy) of the photon and let $m\neq 0$ be the mass (and hence the energy) of the electron. Then the combined particle must have momentum $p$ and energy $m+p$, which means that its mass $\hat{m}$ must satisfy $\hat{m}^2=(p+m)^2-p^2=m^2+2mp$.
Now if we suppose that the combined particle has the mass of the original electron, we get $2mp=0$, which is a contradiction.
This shows that the combined particle cannot be an electron. It does not, by itself, show that the combined particle cannot exist. This leads me to wonder how the argument can be completed, and to the more general question of how one shows that a given particle cannot exist. (I expect this is a very naive question.)
It's been suggested (in comments on the referenced post) that the argument for non-existence can be completed by invoking additional conservation laws, such as conservation of lepton number. But I don't see how this can possibly suffice, as we can always suppose that the lepton number of the combined particle is the sum of the lepton numbers of the electron and the photon, and likewise for any other quantity that needs to be conserved.
In the end, then, we have a particle with a prescribed mass and prescribed values for a bunch of other conserved quantities.
My question is: What tells us that this particle can't exist?
My guess is that this comes down to some exercise in representation theory, where the particle would have to correspond to some (provably non-existent) representation of the Poincare group.
Is this guess right, or is there either more or less to it than that?