M. K. Liou

Anatomy of the soft photon approximation in hadron-hadron bremsstrahlung

A modified Low procedure for constructing soft-photon amplitudes has been used to derive two general soft-photon amplitudes, a two-s\char21{}two-t special amplitude

Pauli principle in the soft-photon approach to proton-proton bremsstrahlung.

{\mathit{M}}_{\mathrm{\ensuremath{\mu}}}^{\mathit{T}\mathit{s}\mathit{T}\mathit{t}\mathit{s}}

Bremsstrahlung from /sup 16/O+p near the 2. 66-MeV resonance

and a two-u\char21{}two-t special amplitude

Comment on "Validity of certain soft photon amplitudes"

{\mathit{M}}_{\mathrm{\ensuremath{\mu}}}^{\mathit{T}\mathit{u}\mathit{T}\mathit{t}\mathit{s}}

Bremsstrahlung from /sup 12/C+p near the 461-keV resonance

, where s, t, and u are the Mandelstam variables.

Pion-proton bremsstrahlung calculation and the experimental'' magnetic moment of. Delta. sup ++ (1232)

{\mathit{M}}_{\mathrm{\ensuremath{\mu}}}^{\mathit{T}\mathit{s}\mathit{T}\mathit{t}\mathit{s}}

Nucleon-nucleon bremsstrahlung : Anomalous magnetic moment effects

depends only on the elastic T matrix evaluated at four sets of (s,t) fixed by the requirement that the amplitude be free of derivatives (\ensuremath{\partial}T/\ensuremath{\partial}s and/or \ensuremath{\partial}T/\ensuremath{\partial}t). Likewise

Soft-photon analysis of pion-proton bremsstrahlung and the experimental'' magnetic moment of. Delta. sup ++ (1232)

{\mathit{M}}_{\mathrm{\ensuremath{\mu}}}^{\mathit{T}\mathit{u}\mathit{T}\mathit{t}\mathit{s}}

Proton-proton bremsstrahlung calculation : Comparison with recent high-precision experimental results

depends only on the elastic T matrix evaluated at four sets of (u,t) also fixed by the requirement that the amplitude

Noncoplanarity effects in proton-proton bremsstrahlung

{\mathit{M}}_{\mathrm{\ensuremath{\mu}}}^{\mathit{T}\mathit{u}\mathit{T}\mathit{t}\mathit{s}}