The refractive index and thermo-optic coefficient (dn/dT) of linear polyurethanes and UV-cured polyacrylates were determined over a range of near infrared (NIR )wavelengths. Three different linear polyurethanes were prepared from the polycondensation of isophorone diisocyanate (IPDI) and novel diols containing cyclic substituents, such as 1,3-dithiane, cyclic O,S-acetal and 1,3-dithiolane. The polymers exhibited a glass transition at 71-131 1C and were stable up to B250 1C. Urethane-diacrylate was prepared via a reaction of IPDI and 2-hydroxyethyl methacrylate, and a urethane-acrylate polymer film was produced under UV-irradiation. The urethane content of the UV-polymers was adjusted using composite films from a diacrylate-derived from 1,3-dithiane-attached diol. The linear polyurethane provided a high thermo-optic coefficient (dn/dT) of À3.63 Â 10 À4 1C À1 (1550 nm). The coefficient was dependent on the urethane content of the UV-composite films, which exhibited a larger thermooptic effect than the pure UV-acrylate films because of the urethane group. All the urethane-polymer films exhibited a very low birefringence (o0.0004). The presence of N-H in the urethane backbones rarely resulted in additional absorption loss as waveguide materials at specific wavelengths of 1100, 1310 and 1550 nm. A urethane-acrylate composite film exhibited propagation losses of 0.09 (1100 nm), 0.244 (1310 nm) and 0.288 dB cm À1 (1550 nm). The losses (1310 and 1550 nm) were reduced to o0.09 dB cm À1 in the deuterium-exchanged film.
INTRODUCTIONData transmission along optical fibers has progressed with increasing speed, data quality and decreasing cost. Planar waveguide devices offer the advantages of a cost-effective fabrication process, easy integration and compactness. 1,2 These waveguide devices potentially offer high reliability because unlike micro-opto-electromechanical systems, there are no moving parts, and the devices are driven by a change in the refractive index. 3 Polymer waveguide materials have attracted increasing interest in the design of thermally operating devices, such as optical switches, optical splitters, optical attenuators and optical filters. 4,5 These devices should be designed and fabricated to achieve better performance in terms of low power consumption, low switching voltage and rapid response. The device performance is based on the thermo-optic effect of the composing material. A large thermo-optic coefficient (TOC) of a material means that a small temperature change is needed for the necessary change in refractive index, which reduces the power consumption for device operation. 6 Many thermo-optic waveguide devices have been fabricated using polymer materials because of their large TOCs, which are much greater than those of inorganic materials, such as silica (1.1 Â 10 À5 K À1 ) or lithium niobate (4 Â 10 À5 K À1 ). 6-8 Conventional poly(methyl methacrylate) has a TOC of À1.2 Â 10 À4 K À1 . The polymer TOC provides a negative sign,