We demonstrate stable wavelength tunable inscription of polymer optical fiber Bragg gratings (FBGs). By straining the fiber during FBG inscription, we linearly tune the center wavelength over 7 nm with less than 1% strain. Above 1% strain, the tuning curve saturates and we show a maximum tuning of 12 nm with 2.25% strain. We use this inscription method to fabricate a dual-FBG strain sensor in a poly (methyl methacrylate) single-mode microstructured polymer optical fiber and demonstrate temperature compensated strain sensing around 850 nm.Index Terms-Fiber Bragg grating, polymer optical fiber, strain sensing, temperature compensation. D UE to the low Young's modulus (about 25 times lower than silica) and high elastic limit of over 10% (about 10 times higher than silica), fiber Bragg gratings (FBGs) in polymer optical fibers (POFs) are attractive for fiber-optical strain sensing [1][2]. POFs are also clinically acceptable, flexible and non-brittle, which makes the POF FBG a candidate for in-vivo biomedical applications [3][4][5][6]. FBGs have been reported in both step index POFs [2,7-9] and microstructured POFs (mPOFs) [9][10][11][12][13].To date the majority of POFs and microstructured POFs (mPOFs) are made of poly (methyl methacrylate) (PMMA), which has a high thermo-optic coefficient and strongly absorbs water. PMMA FBG strain sensors therefore have a large cross-sensitivity to humidity and temperature [1,8,13]. The problem of humidity is strongly reduced by using POF FBGs made of the polymer TOPAS [4,5], which has a humidity sensitivity of less than 38.4 pm/%rH @1565nm [13]. This is more than 50 times less than POF FBGs made of PMMA [10,13]. However, both TOPAS and PMMA POF FBGs are still sensitive to temperature with similar sensitivities [1,13]. This is a major problem for POF (and silica) FBG strain sensors in practical applications, in particular in static strain sensing, where temperature variations occur on the same timescale as the variations in strain.A simple solution is to use a second closely spaced and strain free FBG with a different resonance wavelength to Manuscript provide an independent control of the temperature. The difference in resonance frequency between the two FBGs will then still measure the strain, but be independent of temperature, as was demonstrated for silica FBGs [14].In this letter we demonstrate the concept of dual-FBG temperature compensated strain sensing for POF FBGs. To fabricate two (or more) POF FBGs with closely spaced resonance wavelengths we further demonstrate a simple technique for highly controlled tuning of the resonance wavelength of a POF FBG written with the standard phase-mask technique using the same phase-mask. By straining the POF during writing we can linearly tune the wavelength by 7 nm using only 1% strain. Going into the saturated regime we show 12 nm tuning with 2.25 % strain using a force of only 0.5 N due to the low Young's modulus of PMMA. This tuning range is about 5 times higher than for silica fibers [15] and can prove useful for future multiplexe...