Phase-sensitive above-threshold ionization of Rydberg atoms at 8 GHz

We have observed the phase dependence of microwave above-threshold ionization (ATI) of Rydberg potassium atoms at a microwave intensity of 3×${10}^4$ W ${\mathrm{cm}}^{\mathrm{-}2}$. By using 5-ps pulses derived from a mode-locked tunable dye laser to create the initial Rydberg state, and phase locking the microwave field to a high harmonic of the mode-locking frequency, we are able to excite the atom at a specific phase of the microwave field. Measurement of the ejected electrons’ energy as a function of the initial Rydberg state and the phase of the microwave field show that it is the phase of the field at which the electron becomes free of the atom that determines its kinetic energy. The energy dependence is described by a simple, classical theory that reveals the relationship between the so-called ‘‘quiver’’ and ‘‘drift’’ terms in the electron energy previously observed in ATI experiments at higher frequencies.