R. Uberna et al., PHASE AND AMPLITUDE CONTROL IN THE FORMATION AND DETECTION OF ROTATIONAL WAVE-PACKETS IN THE E(1)SIGMA(-2()(G) STATE OF LI), The Journal of chemical physics, 108(22), 1998, pp. 9259-9274
Femtosecond laser pulse amplitude/phase masking techniques are employe
d to control the formation and detection of rotational wave packets in
the electronic E (1)Sigma(g)(+) state of lithium dimer. The wave pack
ets are prepared by coherent excitation of rovibronic E (1)Sigma(g)(+)
a ( VE,JE) states of Li-2 from a single intermediate state, A (1)Sigm
a(u)(+) (nu(A) = 11, J(A) = 28), and probed by time-resolved photoioni
zation. In the detection step, the wave packet is projected onto the X
(2)Sigma(g)(+) state of Li-2(+). New resonance structure in the X (2)
Sigma(u)(+) ionic state continuum is obtained by measuring the wave pa
cket signal modulation amplitude as a function of the frequencies remo
ved from the spectrally dispersed probe pulse by insertion of a wire m
ask in a single-grating pulse shaper. A split glass phase mask inserte
d into the pulse shaper is used to produce step function changes in th
e spectral phase of the pulse. The phase relation among the wave packe
t states is varied by changing the relative phases of spectral compone
nts in the pump pulse and is monitored by measuring the changes in the
phase of the rotational wave packet recurrences using an unmodified p
robe pulse. By altering the relative phases among the wave packet comp
onents, the spatial distribution of the initial wave packet probabilit
y density is varied, resulting in phase-dependent ''alignment'' of the
probability density in angular space. Phase changes in the signal rec
urrences are also observed when a phase modified pulse is used in the
wave packet detection step after wave packet preparation with an unmod
ified pulse. The formation and detection of the wave packets is discus
sed in terms of quantum interference between different excitation rout
es. The relative phase factors encoded in a single optical pulse (pump
dr probe) are transferred into the interference term of the measured
signal through the molecule-photon interaction. (C) 1998 American Inst
itute of Physics. [S0021-9606(98)00222-0].