Tunable laser emission is a highly desirable feature in modern technologies such as fiber optics for communications. Polymeric materials are interesting candidates for integrated laser devices, due to their mechanical properties and the possibility of low-cost fabrication schemes. It has been shown in the literature that lasers made of organic materials as the gain medium can be realized in a variety of device configurations.[1±3] Possibly the most straightforward approach is inscribing of a distributed feedback (DFB) grating [4,5] into either the substrate or directly into the organic layer. While DFB structures can be easily produced using fabrication methods such as lithography or imprinting techniques, [6] they generally lack the tunability provided by, e.g., an external cavity. Current research is aimed at electrically tunable DFB lasers [7] and mechanically tunable devices. As an example, truly tunable DFB lasing in liquid-crystalline elastomers [8] has been demonstrated recently.In previous papers we demonstrated DFB structures produced via interference lithography in films of the copolymer poly[styrene-co-(4-vinylbenzyl thiocyanate)]. In these structures the change of the refractive index caused by the UV-induced isomerization of thiocyanate (±SCN) to isothiocyanate (±NCS) groups was employed to provide the required feedback for lasing. [9,10] Using this method, we have shown that two-dimensional gratings of different periods can be easily inscribed, providing limited tunability of the emission wavelength by rotating the substrate. [11] In the present contribution we extend the aforementioned approach by combining the photoreactivity of benzylthiocyanate units with the mechanical properties of a styrene±butadiene rubber (SBR). This allows us to fabricate elastic DFB structures whose grating period can be varied by mechanical strain (elongation/compression). Due to the elastic properties of the material, the mechanical deformation is fully reversible. The emission wavelength of the laser is correlated to the mechanical elongation and can thereby be tuned continuously within a certain range.To synthesize the elastomer, the monomer 4-vinylbenzyl thiocyanate (VBT) was prepared according to a method described earlier.[12] The monomer was then copolymerized with butadiene using a hot emulsion polymerization with K 2 S 2 O 8 as initiator. [13] This strategy was chosen as it provides a convenient and rapid preparation of a UV-sensitive elastomer suitable for holographic recording. The structure of the photo-sensitive elastomer poly[butadiene-co-(4-vinylbenzyl thiocyanate)] (PBco-VBT) is given in Scheme 1. Due to the free-radical reaction, the butadiene units are both (1,2) and (1,4) linked, with the (1,4) units being dominant.
1H NMR data showed 67 ± 2 mol-% of 1,4-linked butadiene, 12 ± 2 mol-% 1,2-linked butadiene, and 21 ± 2 mol-% of VBT units in the copolymer. This was further confirmed by elemental analysis (C, H, N, S). These data, as well as FTIR spectra, showed that no isomerization of the thiocyanate gro...