138
M. Jasiurkowska-Delaporte
Fig. 12 Kissinger and Augis and Bennett plots for non-isothermal cold crystallization of a Cr1 in
the nematic phase of 5P-EtFLEt-P5 and b Cr2 in isotropic phase of 5P-Am*FLAm*-P5. The figure
presents unpublished data for 5P-EtFLEt-P5 and data for 5P-Am*FLAm*-P5 taken with permission
(The European Physical Journal (EPJ)) from Ref [30]
this is absent [47]. The existence of both SmB phases in BBOA was confirmed by
X-ray studies. Molecular dynamics investigations by BDS revealed that the transition
from SmB hex to SmB Cr is also characterized by retardation of the rotational motions
of molecules around their short axis and an increase in corresponding activation
energy [9]. Moreover, the glass transition in the highly ordered SmB Cr phase is
M. Jasiurkowska-Delaporte
Fig. 12 Kissinger and Augis and Bennett plots for non-isothermal cold crystallization of a Cr1 in
the nematic phase of 5P-EtFLEt-P5 and b Cr2 in isotropic phase of 5P-Am*FLAm*-P5. The figure
presents unpublished data for 5P-EtFLEt-P5 and data for 5P-Am*FLAm*-P5 taken with permission
(The European Physical Journal (EPJ)) from Ref [30]
this is absent [47]. The existence of both SmB phases in BBOA was confirmed by
X-ray studies. Molecular dynamics investigations by BDS revealed that the transition
from SmB hex to SmB Cr is also characterized by retardation of the rotational motions
of molecules around their short axis and an increase in corresponding activation
energy [9]. Moreover, the glass transition in the highly ordered SmB Cr phase is