A gas of Rb atoms in a static electric field has been photoexcited to just
above the classical ionization threshold by a phase-locked sequence of two
far infrared pulses. A single laser pulse generates a series of ejected ele
ctron packets emerging at the saddle point of the potential; each of the ej
ected packets is characterized by a phase and a chirp. We calculate and mea
sure these phases and chirps using the time dependent interference of the e
lectronic wave function controlled by the delay between the two light pulse
s.