Abstract
The construction of physical transition probabilities in non-Hermitian, effective-Hamiltonian models of multiphoton ionization is analyzed. Eigenstates of the effective Hamiltonians, H^ and H^, are respectively determined to be projected incoming and outgoing states. These models are found to be intrinsically S-matrix models, and the adiabatic eigenstates are used to construct appropriate transition amplitudes. The intermediate-time bound-electron population differs quantitatively from customary norm-of-state constructions.

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