In non-relativistic quantum mechanics, the normal condition for position eigenstates is $$\langle y|x\rangle=\delta(y-x).$$ However, this condition is not Lorentz-invariant. I have never seen a textbook on relativistic quantum mechanics address this normalization issue. It seems to me like this is a very important issue. If the normalization of the position eigenstates is not invariant, the inner product of any state vectors is also not necessarily invariant (and hence probability is not conserved under a Lorentz transformation).
How is this issue resolved? Is it necessary to resort to quantum field theory, or is there a way to redefine the position eigenstate normalization condition to make it Lorentz-invariant?