Polarization effects on population transfer by stimulated Raman transition using overlapping time dependent pump and Stokes
laser pulses from the ground
X
1Σ
g
/+
(
v
g=0,
J
g=1) level of H
2 to the final
X
1Σ
g
/+
(
v
f=1,
J
f=1) level via the intermediate
B
1Σ
u
/+
(
v
i=14,
J
i=0,2),
C
1Π
u
/+
(
v
i=3,
J
i=2) and
C
1Π
u
/−
(
v
i=3,
J
i=1) levels have been theoretically investigated by applying the density matrix formalism. We have studied in detail the dependence
of the population transfer on time delay between two pulses for the cases of on-resonance excitations considering linear parallel
and same-sense circular polarizations of the fields. The pump and Stokes fields are taken as having Gaussian pulse shapes
with peak intensities
I
P
/0
(
I
S
/0
)=2 × 10
6 and 1 × 10
7 W/cm
2. Density matrix equations have been solved for each value of the magnetic quantum number
M
g(0, ±1) of the initial ground level taking into account the
M
g dependence of the Rabi frequencies.
M
g — averaged population transfer to the final level has also been calculated. For resonance excitations to the
B(14, 0) or
C(3, 1) levels, appreciable population transfer is achieved for intuitive pulse order for some particular values of
M
g and
M
i (magnetic quantum number of the resonant intermediate level) depending on the nature of polarizations. The calculated values
of
M
g — averaged population transfer for the two cases of polarizations show that for on-resonance excitation to the
B(14, 0) or the
C(3, 1) level, linear parallel polarization of the laser fields yield more transfer efficiency whereas for resonance excitation
to the
B(14, 2) level, larger population transfer results from the same-sense circular polarizations. For resonance excitation to
the
C(3, 2) level,
M
g — averaged population is found to be almost polarization independent. The calculations for the six-level H
2 system reveal some interesting features of polarization effects on the population transfer efficiency.
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