弱磁场中向列相液晶TEB30A薄膜自衍射现象研究

刘桂香; 王雁冰

doi:10.3788/YJYXS20163106.0547

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弱磁场中向列相液晶TEB30A薄膜自衍射现象研究

材料与器件 | 更新时间：2020-08-12

- 弱磁场中向列相液晶TEB30A薄膜自衍射现象研究
- Self-diffraction effect of nematic liquid TEB 30 A film in weak magnetic field
- 液晶与显示 2016年31卷第6期页码：547-552
- 作者机构：
  
  内蒙古科技大学包头师范学院,内蒙古包头,014030
- 作者简介：
- 基金信息：
  
  内蒙古自治区教育厅科学研究项目(No.NJZY12203)()
- DOI：10.3788/YJYXS20163106.0547
  中图分类号： O436
- 收稿日期：2016-02-27，
  
  修回日期：2016-03-11，
  
  纸质出版日期：2016-06-05
- 稿件说明：
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刘桂香, 王雁冰,. 弱磁场中向列相液晶TEB30A薄膜自衍射现象研究[J]. 液晶与显示, 2016,31(6): 547-552

LIU Gui-xiang, WANG Yan-bin,. Self-diffraction effect of nematic liquid TEB 30 A film in weak magnetic field[J]. , 2016,31(6): 547-552
刘桂香, 王雁冰,. 弱磁场中向列相液晶TEB30A薄膜自衍射现象研究[J]. 液晶与显示, 2016,31(6): 547-552 DOI： 10.3788/YJYXS20163106.0547.

LIU Gui-xiang, WANG Yan-bin,. Self-diffraction effect of nematic liquid TEB 30 A film in weak magnetic field[J]. , 2016,31(6): 547-552 DOI： 10.3788/YJYXS20163106.0547.

摘要

采用1.5 mW低功率的He-Ne激光(632.8 nm)正入射向列相液晶TEB30A薄膜

研究向列相液晶TEB30A薄膜在不同强度的弱磁场(0、0.4649、0.5062和0.5185 T)中的远场衍射特性。实验结果表明

向列相液晶TEB30A薄膜在4种不同强度的弱磁场(0

0.4649

0.5062和0.5185 T)中都能产生远场衍射。衍射图样会随磁场强度的增加而发生明显的变化。衍射环的数目增加

衍射环宽度变宽

衍射场向外拓展。当磁场强度为0.5062 T时

衍射环上出现了近似相互平行的干涉直条纹。当磁场强度达到0.5185 T时

干涉直条纹更加明显的趋于平行。在弱磁场的作用下

激光束在远场的散度变得明显。基于Kirchhoff-Fraunhofer衍射积分原理的理论模拟结果表明

当激光通过处在弱磁场中的向列相液晶TEB30A薄膜时

横向非线性相移会增大。随着弱磁场强度由0 T增加到0.5185 T

非线性相移也由4 增加到20 。弱磁场引起样品非线性相移增大

导致其远场衍射图样发生了变化。远场衍射光强图样的变化也是透射光能量分布的改变

因此

可将弱磁场调控向列相液晶这一技术应用于磁控光开关及光限幅等领域。

Abstract

The far-field diffraction characteristics was studied in the different weak magnetic fields(0

0.4649

0.5062 and 0.5185 T)with the low power He-Ne laser of 1.5 mW(632.8 nm)being normal incident on the film of nematic liquid crystals TEB30A.The experiment results showed that the film of nematic liquid crystals TEB30A can produce diffraction in the four weak magnetic fields of 0

0.4649

0.5062 and 0.5185.The diffraction pattern could obviously be changed with the increasing of the magnetic strength. The number of diffraction rings increased

the width of diffraction rings became wide

and the diffraction field expanded outward. At the magnetic strength of 0.5062 T

the interference stripes appeared on the diffracting rings. While the magnetic strength increased to 0.5185 T

the interference stripes was becoming parallel. Under the effect of the weak magnetic field

the divergence of the laser beam was changed drastically in the far-field. Based on the Kirchhoff-Fraunhofer diffraction integral

the theoretical simulation results showed that

when the laser beam passed through the film of nematic liquid crystals TEB30A in the weak magnetic field

the transverse nonlinear phase would increase. With the weak magnetic strength increasing from 0 T to 0.5185 T

the nonlinear phase increased from 4 to20 .The weak magnetic field caused the nonlinear phase

resulting in the change of the far-field diffraction pattern. The change of the far-field diffraction pattern is also the change of the distribution of the transmitted light energy. Therefore

the technology of the weak magnetic field modulating the nematic liquid crystals can be applied to the areas of magnetic-optical switch and magnetic-optical limiters.

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references

OLYAEEFAR B, KHOSHSIMA H. Faster electro optical switching with a highly viscous nematic liquid crystal mixture[J].Optical and Quantum Electronics, 2014, 46(2):357-363.

CHERNYSHUKS B. High-order elastic terms,boojums and general paradigm of the elastic interaction between colloidal particles in the nematicliquid crystals[J]. The European Physical Journal E, 2014, 37(1):6.

MICHAEL J, MACNEIL L, SMYTHN F, et al. Exact and approximate solutions for optical solitary waves in nematic liquid crystals[J].Physica D:Nonlinear Phenomena, 2014, 284:1-15.

KHOO I C. Nonlinear optics, active plasmonics and metamaterials with liquid crystals[J]. Progress in Quantum Electronics, 2014, 38(2):77-117.

NOROOZI N,GRECOV D. Numerical simulation of three-dimensional flow-induced microstructure in a simplified prosthetic hip joint with nematic liquid crystal lubricant[J].RheologicaActa, 2014, 53(5/6):457-465.

ZOLOT'KOA S, KITAEVAV F, KROON, et al. The effect of an optical field on the nematic phase of the liquid crystal[J].JETPLetters, 1980, 32(2):158-162.

DURBINS D, ARAKELIANS F, SHENY R. Laser-induced diffraction rings from a nematic-liquid-crystal film[J]. Optics Letters, 1981, 6(9):411-413.

SANTAMATO E, SHENY R. Field-curvature effect on the diffraction ring pattern of a laser beam dressed by spatial self-phase modulation in a nematic film[J]. Optics Letters, 1984, 9(12):564-566.

BLOISI F, VICARI L, SIMONI F, et al. Self-phase modulation in nematic liquid-crystal films:detailed measurements and theoretical calculations[J].Journal of the Optical Society of America B, 1988, 5(12):2462-2466.

HSIUNG H, SHIL P, SHENY R. Transient laser-induced molecular reorientation and laser heating in a nematic liquid crystal[J]. Physical Review A, 1984, 30(3):1453-1460.

KHOOI C, FINNG M, MICHAELR R, et al. Passive optical self-limiter using laser-induced axially asymmetric and symmetric transverse self-phase modulations in nematic liquid crystals[J].Optics Letters, 1986, 11(4):227-229.

任常愚,孙秀冬,刘正君,等.C60掺杂向列相液晶薄膜的激光诱导自衍射现象研究[J].光学学报,2009,29(3):772-777. REN C Y, SUN X D, LIU Z J, et al.Investigation of self-diffraction effect in C60-doped nematic liquid crystals induced by Gaussian beam[J].Acta Optica Sinica, 2009, 29(3):772-777. (in Chinese)

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