In this paper we describe a unified R-matrix-Floquet theory which can be us
ed to analyse both multiphoton ionization of diatomic molecules and laser-a
ssisted electron-diatomic molecule scattering. Our treatment is non-perturb
ative and can be applied to arbitrary multi-electron diatomic molecules. We
assume that the laser field is monochromatic, monomode, spacially homogene
ous and linearly polarized, where the molecular axis can be oriented in an
arbitrary direction relative to this polarization direction. The theory tak
es advantage of the natural division of configuration space into internal a
nd external regions occurring in the R-matrix method, to choose the most ap
propriate form of the interaction Hamiltonian in each region. This enables
standard multi-centre electron-molecule scattering programs to be modified
in a straightforward way to solve the problem in the internal region and si
ngle-centre atomic multiphoton propagator programs to be extended to solve
the problem in the external region. We illustrate our theory by considering
the form of the equations for homonuclear diatomic molecules. We also pres
ent results for H-2 using a simple target wavefunction which provides an im
portant test of the theory and the computer programs and illustrates the ro
le of resonances in two-photon ionization.