Abstract

For a general form of the massless boson field of arbitrary spin we show that Lorentz covariance completely determines the tensor-field wave function; the equality of this function and the generator of the little group is established. The general parametrization of the potential is presented. The bispinor representation of fields is introduced and its properties are examined. As an application, several processes involving the graviton bremsstrahlung are considered and simple expressions for the helicity amplitudes are obtained.

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