For a model atom in a flat-top laser pulse, the nondipole shift of multiphoton photoelectron peaks depends on emission angle, dominated by electron recoil, with only a small redshift from retardation.
For the mask function M0(x) we select the same values as above, R1 = 30a0 and R2 = 90a0
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Multiphoton ionization distributions beyond the dipole approximation: Retardation versus recoil corrections
For a model atom in a flat-top laser pulse, the nondipole shift of multiphoton photoelectron peaks depends on emission angle, dominated by electron recoil, with only a small redshift from retardation.