Chemistry Reference
In-Depth Information
Fig. 7.11 Typical Z-scan
profiles of the [Ni( L ) 2 Br]Br 2 /
PMMA film in the open and
closed aperture condition.
The solid lines show the
theoretical fits. Adapted
from [ 5 ]
image in Fig. 7.10a . The photograph of the film on a CaF 2 substrate is shown in
Fig. 7.10b .
Figure 7.10c shows the absorption (
) spectrum of the [Ni( L ) 2 Br]Br 2 film,
together with the spectrum of a single crystal of [Ni(chxn) 2 Br]Br 2 . The latter is
obtained as the sum (
a
a , which
were calculated from the polarized reflectivity spectra for the electric field of light
parallel and perpendicular to b , respectively, through the KK transformation. The
spectral shape of
a // +2
a ) of the polarized absorption spectra
a // and
in the [Ni( L ) 2 Br]Br 2 film is in good agreement with that in the
[Ni(chxn) 2 Br]Br 2 single crystal. No significant enhancement of the background due
to light scattering is observed even in the higher energy region (~4 eV), suggesting
the high quality of the film as an optical media.
Typical Z-scan profiles of the [Ni( L ) 2 Br]Br 2 film are presented in Fig. 7.11 . The
measurements were carried out with the light pulse of the optical communication
wavelength
a
l ¼
m
ho ¼
:
80 eV ). The upper panel
shows the nonlinear increase in the absorption (decrease of the transmittance)
around the focal plane ( z ¼
1.55
m (the photon energy
0
0) in the open aperture condition. The one-photon
absorption is negligible at 0.8 eV so that the observed nonlinear signal can be
attributed to two-photon absorption (TPA). The profile in the partially closed
aperture condition includes the TPA component as well as the component for the
optical Kerr effect described by Re
w ð 3 Þ ðo; o; o; oÞ
. By dividing the profile in
the partially closed aperture condition by that in the open aperture condition, the
profile for the optical Kerr effect alone was obtained, which exhibits a plus-minus
structure characteristic of self-defocusing, as shown in the lower panel of Fig. 7.11 .
The two profiles in Fig. 7.11 were well reproduced by the theoretical profiles
predicted for the third-order nonlinear optical response, as shown by thin solid
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