Abstract:Thin free-standing films (FSFs) of an antiferroelectric liquid crystal (AFLC) were investigated by transmission ellipsometry. The phase difference between p-polarized and s-polarized light was measured as a function of the temperature and the incidence angle of the light beam. It was found that the structure of an FSF with two layers is anticlinic (SmC*
A) throughout the temperature range investigated whereas the bulk sample shows several phases, from SmC*
A to SmA phases. T… Show more
“…A freely suspended film of chiral smectics is a very interesting and useful system to elucidate not only the film ordering itself but the property of a bulk phase [1][2][3][4][5][6][7][8][9][10]. By a study of such system, the phase structure free from an anchoring effect because of boundary walls can be observed [9,10].…”
Section: Introductionmentioning
confidence: 99%
“…By a study of such system, the phase structure free from an anchoring effect because of boundary walls can be observed [9,10]. On the other hand, surface layers of the film are known to order at a temperature higher than the bulk critical temperature for both ferroelectric [1][2][3][4][5] and antiferroelectric [6,7] smectics. Now, a ferroelectric material 4-(3-methyl-2-chloropentanoyloxy)-4 0 -heptyloxy-biphenyl (C7) shows a first-order phase transition from a smectic A phase (SmA) to a smectic C phase (SmC Ã ) [11], whereas most of ferroelectric smectics exhibit a second-order phase transition.…”
The method to study phase transitions of thin systems on the basis of a bulk phase diagram is applied to a freely suspended film of ferroelectric smectics showing a first-order phase transition in the bulk, where an ordering effect resulting from surface layers is replaced by an effective field that is conjugate to the order parameter. In the framework of a phenomenological free energy whose coefficients are determined form the experimental evidence about C7, the behavior of the transition is being clarified, which coincides with experimental findings, and especially the small shift of transition temperature from the bulk one is elucidated. The mechanism of the continuous change occurring in the system of thickness just below a critical thickness is clarified, where an unstable state that is never realized in the bulk appears at the interior layers. The behavior of this continuous change discloses the difference between the ordering effects resulting from the boundaries and the external fields.
“…A freely suspended film of chiral smectics is a very interesting and useful system to elucidate not only the film ordering itself but the property of a bulk phase [1][2][3][4][5][6][7][8][9][10]. By a study of such system, the phase structure free from an anchoring effect because of boundary walls can be observed [9,10].…”
Section: Introductionmentioning
confidence: 99%
“…By a study of such system, the phase structure free from an anchoring effect because of boundary walls can be observed [9,10]. On the other hand, surface layers of the film are known to order at a temperature higher than the bulk critical temperature for both ferroelectric [1][2][3][4][5] and antiferroelectric [6,7] smectics. Now, a ferroelectric material 4-(3-methyl-2-chloropentanoyloxy)-4 0 -heptyloxy-biphenyl (C7) shows a first-order phase transition from a smectic A phase (SmA) to a smectic C phase (SmC Ã ) [11], whereas most of ferroelectric smectics exhibit a second-order phase transition.…”
The method to study phase transitions of thin systems on the basis of a bulk phase diagram is applied to a freely suspended film of ferroelectric smectics showing a first-order phase transition in the bulk, where an ordering effect resulting from surface layers is replaced by an effective field that is conjugate to the order parameter. In the framework of a phenomenological free energy whose coefficients are determined form the experimental evidence about C7, the behavior of the transition is being clarified, which coincides with experimental findings, and especially the small shift of transition temperature from the bulk one is elucidated. The mechanism of the continuous change occurring in the system of thickness just below a critical thickness is clarified, where an unstable state that is never realized in the bulk appears at the interior layers. The behavior of this continuous change discloses the difference between the ordering effects resulting from the boundaries and the external fields.
“…We simulated the phase difference D between the p-polarized and s-polarized light outgoing from the FSFs of MHPOBC [1], so as to investigate the layer structure of FSFs in smectic phase, where refractive indices were assumed to be the same as those of the bulk sample (n e ¼ 1.64, n o ¼ 1.50 [5]). Because the FSFs is composed of a tremendous numbers of molecules in each layer of FSFs, therefore the physical concept of refractive index may hold even in such thin films.…”
The refractive indices of free-standing films (FSFs) of an antiferroelectric liquid crystal MHPOBC and a conventional smectic liquid crystal 8CB were studied by means of transmission and reflection ellipsometry. When the FSF thickness of MHPOBC is thicker than 260 nm, the refractive indices of FSFs appear to be the same as those of bulk smectic layers. In the case of thin FSFs of 8CB with a small numbers of layers, birefringence could not be obtained clearly by means of reflection ellipsometry.
“…For example, ellipsometry (e.g. [36,64,66,67,[77][78][79][80]) and X-ray investigations [17, 19-21, 27, 45, 54, 61, 62, 71, 80-86] have been successfully applied.…”
Section: Introductionmentioning
confidence: 99%
“…Directly related to the structure of the films is their ferroelectric, antiferroelectric and ferrielectric behavior [23,36,66,[77][78][79][80][87][88][89][90][91][92][93][94]. In films of a few molecular layers, these properties can change dramatically with respect to the bulk samples.…”
Abstract. Free-standing smectic films are unique fluid objects with an exceptionally large surface-to-volume ratio. They are excellently suited for studies of surface and interface properties of liquids. We describe surface tension measurements in the smectic and isotropic phases, with particular emphasis on anomalies near the phase transitions. A model that considers the excess surface entropy of ordered surface layers is applied to describe the experimental observations qualitatively and quantitatively. From the geometrical properties of isotropic droplets in free-standing films and from the forces acting on these droplets, interface tensions between the smectic and isotropic phases are derived. Finally, we report measurements of the gas permeation through smectic films and develop a model for the description of the film-thickness dependence of the permeation coefficient.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.