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from
10 to +101C shows the existence of 1:2 reciprocal ratios of the first and
the second diffraction orders; the intensity decreases with increase in the
temperature, but at 10 1C the second peak could not be seen. Close examination
of the SAXS diffractions in the temperature range 8-221C reveals the coexist-
ence of two mesophases, the Q
L
phase and the lamellar phase. The Q
L
phase
was discussed in our earlier report.
16
Once the sample reaches 231C, the ratio of the reciprocal spacing changes in
good agreement with a typical Q
L
phase. The WAXS diffractogram exhibits a
broad peak centred at 4.6A
˚
[Figure 3(a)]. The lamellar and Q
L
phases were
further analysed by the SAXS synchrotron between 0 and 401C. It was found
that, from 8 to 201C, the intensity from the lamellar mesophases becomes
gradually reduced and a transformation to the Q
L
phase occurs. The Q
L
mesophase peaks progressively become more pronounced and they have higher
intensities, as shown in Figure 4. The progressive thermal transformation is
strongly consistent with a gradual disordering of the L
a
phase. This can be seen
from the disappearance of the peaks related to the L
a
phase, which is accom-
panied by the appearance of the Q
L
peaks.
These overall findings are in good agreement with the study of Cherezov
et al.
34
on the phase transition from L
a
to the inverse bicontinuous cubic phase
Figure 4 Synchrotron SAXS intensity as function of temperature. (a) L
b
and L
a
(
'
)
and Q
L
(
J
) mesophases at 0-401C. (b) Expanded plot for L
a
mesophases. (c)
Expanded plot for Q
L
mesophases
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