Superluminal mode commutator
does not go on-shell for any value of the momentum. 2 that the theory contains one spin 3/2 and one spin 1/2 positive-norm physical particle, together with their antiparticles, while the other, longitudinal spin 1/2 component does not propagate, i.e. The Rarita-Schwinger vector-spinor contains two spin 1/2 irreducible components, the undesirable longitudinal p μ ψ μ and the physical transverse γ μ ψ μ. The difference is that we relax one of the Pauli-Fierz constraints, which are necessary to get rid of the reducible spin 1/2 components. The equations analyzed in this paper are almost exactly those of the standard Rarita-Schwinger spin 3/2 theory Rarita:1941mf. In the canonical formalism it is only necessary to choose the physical vacuum as the highest-weight state with respect to the spin 1/2 operators in order to correctly reproduce both the unusual residues and locations of the poles. The canonically quantized field is causal, and the equal-time anti-commutator has positive definite form. The propagator contains poles of the spin 1/2 modes above the real axis for the positive and below the real axis for the negative frequency modes, while the residues at those poles are also of the sign opposite to the usual altogether this leads to a unitary S-matrix, the forward amplitude ⟨ p | p ⟩ being positive for all modes. It is found that the retarded part appropriately propagates the positive energy solutions forward in time, while the advanced part propagates the negative energy solutions back in time so long as the parameters are chosen such that the positive frequency modes have the same parity. the positive frequency modes have negative energy. Classically, for spin 1/2 modes the energy is of the opposite sign to frequency, i.e. The unfamiliar feature of the theory is that the charge matrix is not positive definite it is positive definite on the space of spin 3/2 solutions, and negative definite on the space of spin 1/2 solutions. We then quantize the theory using the appropriate Grassmann-variable path integral and study the poles of the propagator. We find that the interaction is consistent and does not lead to superluminal propagation for a range of the mass of the spin 1/2 particle, except for the special point where the spin 1/2 particle is infinitely massive. This is done by allowing a more general form for the mass term, while leaving the kinetic terms untouched. Electromagnetic interactions of the spin 3/2 particle are investigated while allowing the propagation of the transverse spin 1/2 component present in the reducible Rarita-Schwinger vector-spinor.