Role of surface order on the total electric conduction in NLC samples

被引:12
作者
Alexe-Ionescu, AL
Ionescu, AT
Barna, ES
Scaramuzza, N
Strangi, G
机构
[1] Univ Calabria, Dipartmento Fis, I-87036 Arcavacata Di Rende, Cosenza, Italy
[2] INFM, UdR, I-87036 Arcavacata Di Rende, Cosenza, Italy
[3] Univ Politehn Bucuresti, Dept Fiz, RO-77206 Bucharest, Romania
[4] Univ Bucuresti, Fac Fiz, RO-76900 Bucharest, Romania
关键词
D O I
10.1021/jp034462l
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Current vs voltage measurements have revealed two different conduction zones in a NLC sample. A standard sandwich type sample was filled with K18 (6CB) which was aligned (approximately) homeotropically by the two ITO surfaces previously cleaned in orthochromic mixture. On two opposite sides of the cell, the NLC was limited by two Mylar stripes acting as spacers. The other two sides were left open, and the liquid crystal had two free surfaces (limited only by air) in the form of a cylindrical meniscus. The overall conductivity of the cell depended strongly on the length of the free surface. For the same area, samples with a larger free surface experienced a higher overall conductivity. In the absence of an electric field, we considered the order in the free surface zone to be planar with n being normal to LC-air interface. For small electric fields the conduction along director n in the bulk is less than the conduction perpendicular to n on the free zone. At higher fields, the Freedericksz transition which operates on the free zone reduces the overall conductivity. This reduced conductivity was practically equal to that obtained when ITO electrodes were completely immersed in liquid crystal; that is, the free surfaces do not contribute to the conduction. Considering the measured values, we have concluded that the order in the free surface zone was planar for a depth of about 50 mum.
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页码:5487 / 5490
页数:4
相关论文
共 4 条
[1]  
[Anonymous], 1993, ELECTROOPTIC EFFECTS
[2]  
DEGENNES PG, 1993, PHYSICS LIQUID CRYST
[3]   Microscopic structure and dynamics of a partial bilayer smectic liquid crystal [J].
Lansac, Y ;
Glaser, MA ;
Clark, NA .
PHYSICAL REVIEW E, 2001, 64 (05) :12-051703
[4]   Determination of the nematic alignment and anchoring strength at the curved nematic-air interface [J].
Slavinec, M ;
Crawford, GD ;
Kralj, S ;
Zumer, S .
JOURNAL OF APPLIED PHYSICS, 1997, 81 (05) :2153-2156