The high-pressure mesomorphic behavior of a chiral liquid crystalline polyacrylate has been studied by x-ray diffraction in situ. The results show the existence of monolayer smectic-A* and bilayer smectic-C* mesophases that coexist in the thermally untreated sample over a well-defined range of temperatures, from ambient pressure up to 133 MPa. Hydrostatic pressures of the order of 100-220 MPa are found to affect strongly the polymorphic behavior of the sample. The smectic-A* mesophase, which at ambient pressure coexists with an interdigitated smectic-C* structure, is stabilized over a temperature range which increases with pressure, whereas the formation of the smectic-C* phase is inhibited above 220 MPa. The pressure increment is found to introduce static positional disorder, and to reduce the long-range positional order in the smectic structure strongly. A transition sequence from the isotropic melt through the smectic-A* phase to a new crystalline structure is found by cooling isobarically down to room temperature. The proposed pressuretemperature phase diagram suggests the occurrence of peculiar disorder-order-disorder transitions as pressure is reduced isothermally.

High-pressure mesomorphic behavior of a chiral polyacrylate by x-ray diffraction in situ

B Paci;
1997

Abstract

The high-pressure mesomorphic behavior of a chiral liquid crystalline polyacrylate has been studied by x-ray diffraction in situ. The results show the existence of monolayer smectic-A* and bilayer smectic-C* mesophases that coexist in the thermally untreated sample over a well-defined range of temperatures, from ambient pressure up to 133 MPa. Hydrostatic pressures of the order of 100-220 MPa are found to affect strongly the polymorphic behavior of the sample. The smectic-A* mesophase, which at ambient pressure coexists with an interdigitated smectic-C* structure, is stabilized over a temperature range which increases with pressure, whereas the formation of the smectic-C* phase is inhibited above 220 MPa. The pressure increment is found to introduce static positional disorder, and to reduce the long-range positional order in the smectic structure strongly. A transition sequence from the isotropic melt through the smectic-A* phase to a new crystalline structure is found by cooling isobarically down to room temperature. The proposed pressuretemperature phase diagram suggests the occurrence of peculiar disorder-order-disorder transitions as pressure is reduced isothermally.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/136385
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