  We discuss the processes $\pi \pi \to \pi \pi$ and $\pi \pi \to \pi \pi
\gamma$ from a general quantum field theory (QFT) point of view. We study the
soft-photon limit where the photon energy $\omega \to 0$ and where we have the
theorems due to F.E. Low and S. Weinberg. We consider for the radiative
amplitude the Laurent expansion in $\omega$ and calculate the terms of order
$\omega^{-1}$ and $\omega^{0}$. The pole term $\propto \omega^{-1}$ is given by
Weinberg's soft-photon theorem. Then we calculate the amplitudes for the above
reactions for high center-of-mass energies and small momentum transfers, that
is, in the soft-diffraction regime using the tensor-pomeron model. We identify
places where "anomalous" soft photons could come from. Three soft-photon
approximations (SPAs) are introduced. The corresponding SPA results are
compared to those obtained from the full tensor-pomeron model for
center-of-mass energies $\sqrt{s} = 10$ GeV and 100 GeV. The kinematic regions
where the SPAs are a good representation of the full amplitude are determined.
Finally we make some remarks on the type of fundamental information one could
obtain from high-energy exclusive hadronic reactions without and with soft
photon radiation.
