Electro‐optical properties and nonlinear response of side chain liquid crystalline polymers

Abstract Among the NLO processes that have been studied, one of the most visually dramatic is the frequency doubling. In the field of optical information storage this process can provide the conversion of near‐infrared laser light from diode lasers into deep blue light. Compared to the more traditional inorganic NLO materials, polymers with polarizable aromatic pendant side groups are increasingly being recognized as the materials of the future. Recently it has been pointed out that the axial ordering spontaneously present in nematic and smectic A polymers can be used to enhance field‐induced polar ordering by elongating the orientational distribution function along the electric field direction. Depending on the value of the microscopic order parameters

2 and

4 , the performance may be improved by a factor of 1 to 5 by using LCPs instead of ordinary amorphous polymers for SHG. 1‐4) Interesting results have been obtained for copolyethers prepared by chemical modification of polyepichlorohydrin with classical 4‐cyano‐4'‐hydroxybiphenyl mesogenic group which possesses NLO properties itself. 5‐8) These copolyethers afford the opportunity to fine‐tune the polymer properties by varying the concentration of the mesogenic side groups. As the concentration is increased, we move from a purely isotropic polymer to a nematic polymer. Spin‐coated films have been activated using the corona poling technique and the order parameters

2 have been determined from optical absorption spectra. The second harmonic coefficients d 33 and d 31 have been measured and compared with different statistical models. In view of the great practical importance, characterization of the wavelength dispersion has been carried out. It agrees well with the two‐level approximation model. The dynamics of optical SHG has been investigated. It has been shown that both the presence of LC character in the material and the temperature at which the films are stored below Tg are important in determining the stability of the SH coefficients. A polyacrylate and a polymethacrylate bearing the same 4‐cyanobiphenyl‐based side groups have also been studied. 7‐8) Of particular interest is the fact that the former is nematic while the latter is purely isotropic at rest, the addition of a methyl group to each structural unit of the polyacrylate backbone creating a higher conformational barrier to mesogen packing. Studies of the temporal and thermal characteristics of the poling process have been performed to: •understand and control the poling process with the intention of maximizing poling induced nonlinearity and stability. •elucidate the influence of the polymer backbone, our data including the use of the same mesogenic unit attached to increasing flexible backbones (e.g. polymethacrylate and polyether). •establish if, in the isotropic cases, noticeable axial order can be induced by the poling field, especially when the system is pulled through nematic/isotropic transition by the electric field.