It is shown that any regularized helicity amplitude that is known from axiomatic local field theory to satisfy dispersion relations for -t₀≤t≤0 is in fact analytic in the quasi-topological product |t|<R×s in the cut plane with cuts s=C+λ, s=-t-μ+C^', where λ, μ≥0 and R is a fixed number. This is the extension to the scattering of nonzero-spin particles of a result obtained in the scalar case. As a first consequence, the Froissart limits are extended to all helicity amplitudes. Furthermore, it is shown that for -t₀≤t≤0 and s going to infinity, the regularized helicity amplitudes in the t channel, with initial (final) helicities λ₁ and λ₂ (μ₂ and μ₂), are bounded by Cₛ^1-max(|λ|,|μ|)(lns)² if λ+μ is even, or by Cₛ^1-max(|λ|,|μ|)(lns)³ if λ+μ is odd, where λ=λ₁-λ₂ and μ=μ₁-μ₂. This gives superconvergent amplitudes as soon as one of the spins is larger than 1. The case of spin-0-spin-1 scattering is marginal, and in the absence of any detailed dynamical information, one cannot obtain a superconvergent amplitude in that case.
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Mahoux et al. (1968) studied this question.
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