Av. Benderskii et al., Photodynamics in superfluid helium: Femtosecond laser-induced ionization, charge recombination, and preparation of molecular Rydberg states, J CHEM PHYS, 110(3), 1999, pp. 1542-1557
Femtosecond pulses (790 nm) are used for nonresonant laser excitation of su
perfluid liquid helium to prepare ionic and neutral excited states at energ
ies above 18 eV. Measurements of laser-induced fluorescence and photocurren
t enable a detailed description of the primary photoprocesses. A controllab
le excitation regime unique to femtosecond pulses is realized at laser inte
nsities below the dielectric breakdown threshold, I < 5 X 10(13) W/cm(2). A
steady state of the long-lived triplet excimers He-2*((3)a) (lowest Rydber
g state) is established; the concentration decays between laser pulses thro
ugh diffusion-controlled bimolecular annihilation to similar to 10(12) cm(-
3) at a laser repetition rate of 500 Hz. The triplet population is amplifie
d with each pulse in a sequence that involves: (1) ionization of the Rydber
g electron of He-2* via complete Coulomb barrier suppression; (2) cascade e
lectron impact ionization of the ground-state He atoms by the ponderomotive
ly accelerated quasifree electrons in liquid He; (3) localization and therm
alization of the "hot'' electrons and He+ cations to form electron "bubble'
' and He-3(+) "snowball'' states; (4) recombination of these elementary cha
rge carriers to form He-2*. The amplification factor for the triplets M = 2
(m) characterizes the excitation sequence: m is the number of generations i
n the cascade (m = 5 at I = 4.5 X 10(13) W/cm(2)), and m is proportional to
the laser intensity and temporal pulse width. The laser-induced ionization
cascade prepares an inhomogeneous initial distribution of spatially separa
ted ions on three length scales: clumps of positive charges with an interio
nic separation determined by the cascade length of 60 Angstrom; a cloud of
electrons surrounding the clump at the electron thermalization length simil
ar to 10(3) Angstrom; and interclump separation dictated by the concentrati
on of the He-2* precursors, similar to 10(4) Angstrom. (C) 1999 American In
stitute of Physics. [S0021-9606(99)01202-7].