Then calculate the power per unit solid angle as a function of angle for red, green, and blue light using stackdipole script command and export the ray results.Finally, import the results into Zemax OpticStudio and visualize the farfield results of an arbitrary array of OLED sources.A more efficient approach is to start with a planar OLED or a multilayer stack using the Stack optical solver.Using stackfield, we can optimize the position of a dipole inside OLED design.
The farfield raysets then can be generated using stackdipole script command. Finally results will be imported into Zemax OpticStudio as raysets that can be used to study the incoherent emission from a macroscopic device. An optimal dipole position is the maximum of electric filed in the active layer region to enhance the rate of spontaneous emission. The incoherent superposition of the far fields from three sources are calculated for a 301 array. This is equivalent to running a 1D simulation (with one mesh cell along the x- and z-axis) with a plane wave source traveling along y-axis. ![]() This result is used to generate 3 raysets and saved into a format that can be imported into OpticStudio. As can be seen in the image below, the red pixel shows a large power per unit solid angle at steep angles. In this case the three different sources used mix to form white light. Additionally, in the shaded model of the entire device, layout rays can be added to view a smaller number of rays from the source file. If a larger value is used, the results will be calculated further from the interface. For non-lossy materials, this will not affect the reflected and transmitted power, but it will change phase of the complex coefficients. The size is Ndipoles and thus a combination of polarizations can be set for different dipoles. Roxio easy cd dvd creator 6 free downloadThe changes have to be made in first and second steps to optimize the dipole position and extract raysets for the new geometry. The farfield results of patterned OLED then can be imported into Zemax.
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