This research is focused on the temperature sensing ability of perovskite SrZrO 3 :Eu 3+ hollow spheres synthesized via the sol-gel method followed by heating. The Rietveld refinement indicated that the precursors annealed at 1100 °C were crystallized to form orthorhombic SrZrO 3 . SrZrO 3 particles exhibited non-agglomerated hollow spherical morphology with an average particle size of 300 nm. The UV-excited photoluminescence spectrum of SrZrO 3 :Eu 3+ consisted of two regions. One region was associated with SrZrO 3 trap emission, and the other one was related to the emission of Eu 3+ ions. The intensity ratio of the emission of Eu 3+ ions to the host emission (FIR) and the emission lifetime of Eu 3+ ions were measured in the temperature range of 300-550 K. The sensitivity obtained via the lifetime method was 7.3× lower than that measured via the FIR. Within the optimum temperature range of 300-460 K, the as-estimated sensor sensitivity was increased from 0.0013 to 0.028 K −1 . With a further increase in temperatures, the sensitivity started to decline. A maximum relative sensitivity was estimated to be 2.22%K −1 at 460 K. The resolutions in both methods were below 1K in the above temperature range. The results indicated the suitability of SrZrO 3 :Eu 3+ for the distinct high temperature sensing applications.In daily human life, temperature is recognized as one of the most important measured physical quantities. An accurate and consistent measurement of temperature is essential for the devices related to chemistry, medicine, biology and metrology owing to the cooling and heating phenomena. In the modern world, temperature sensors are widely used, accounting for about 75-80% of the overall sensor market. The conventional temperature sensing measurement mainly depends on the ability of materials in response to heat. Direct contact of the instrument with the heated objects is the main requirement for making such thermometric measurements [1][2][3] . Nowadays, non-contact specific thermometry with high resolution for sensing temperatures in nanoscale environments has emerged as a very dynamic field of research 4 . Among the non-invasive thermometric methods, luminescence thermometry has been established as the key alternative and an accurate technique with high detection sensitivity, spatial resolution and short acquisition times [5][6][7] . The temperature sensors using luminescent materials are based on the change in photoluminescence properties as a function of temperatures. The photoluminescence properties include the emission intensity, peak position, full width at half maxima of the emission spectrum and the characteristic lifetime of the excited state 8,9 .