We present an in situ method for the simultaneous determination of wafer curvature and true growth temperature during metalorganic vapor phase epitaxy of group-III-nitrides on silicon. The measurement configuration allows determining the wafer curvature by the reflections of parallel laser beams, and at the same time, the wafer temperature is measured by emissivity-corrected pyrometry. The bending of the substrates due to strained layers and unequal thermal expansions coefficients causes a change in the surface temperature of the wafer, although the monitored process temperature is constant. Thereby both kinds of curvatures, concave and convex, lead to an opposed temperature variation. Thus, by growing LED structures on silicon a temperature shift up to 45 K with respect to the susceptor was observed.One of the most important parameters in metalorganic vapor phase epitaxy (MOVPE) is the growth temperature, because it strongly influences, e.g., surface diffusion, composition, growth rates, and the crystallographic structure of epilayers. For this reason, the knowledge of the exact wafer temperature is essential for growing high quality devices. The process temperature in a MOVPE reactor is usually obtained from a light-pipe or a thermocouple, which measures the temperature on or below the susceptor, which might be different from the true wafer temperature. In addition, in the case of strained layers a wafer bending arises which causes lateral temperature variations across the wafer because the wafer looses contact to the susceptor either in the center or at the edges, depending on a convex or concave bowing, respectively. In recent years, experimental methods have been developed, which allow the in situ determination of film stress during thin film deposition [1]. Among these techniques most attention has been drawn to a quasi "direct" measurement of stress by the wafer curvature method during the deposition of thin solid films. This technique is based on the measurement of the substrate curvature κ induced by the mismatch. The wafer curvature κ can be used as a means to determine the amount of stress via the mismatch strain ε m . In the simplest case of linear stress-thickness dependence, the stress can be determined via the well-known Stoney equation [2]; in the case of a non-linear dependence numerical [3] or quasi-analytical solutions exist [4]. The curvature method has already been successfully applied to follow the stress evolution during metal organic vapor phase epitaxy of GaN or AlGaN on sapphire [5,6] or silicon [7]. However, to the best of our knowledge, up to now, no direct attention has been drawn to the impact of wafer bending on the substrate temperature. It is expected, that the different types of curvatures, concave or convex, lead to an increase or to a decrease of the temperature at the surface in the center of the wafer, respectively, and thus to temperature inhomogeneities across the wafer. In this report, in addition to curvature measurements we simultaneously measured in situ the impact