Abstract
A calculation, to order α, of the phase of the scattering amplitude for charged bosons is shown to involve the double spectral function for the box graph. At small angles the result agrees with a (Bakamjian-Thomas) equivalent-potential calculation and reduces to the potential-scattering-theory result in the nonrelativistic limit; the infrared-divergent part agrees with that obtained for a Yukawa potential, as the shielding radius approaches infinity.

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