A thin polarized-light emitting film is fabricated by aligning nanorods in an electric field and subsequent polymerization. A polarization ratio of 0.60 is obtained with this method. The thickness of the film is in the order of a few micrometer, and the method is compatible with largescale processing on cheap, flexible, and transparent substrates. The process can be realized in a roll-to-roll process as in a printing process, when one substrate is flexible and passes over a roll with electrodes.Liquid crystal displays have a limited transmission, on the order of 10%. This is mainly due to the absorbing polarizers and color filters. In a conventional backlight, the emitted light is unpolarized because it originates for LEDs or phosphor materials. Because an LCD is designed to work with polarized light [1], the polarizer typically absorbs half of the light.Light emission is usually the result of a dipole transition in an atom, molecule, or quantum dot. Recently, the development of red and green quantum dots has improved the color saturation of LCDs [2]. Anisotropic emitters can have characteristics that are close to that of a dipole antenna. If the emitters are aligned parallel to the electric field of the light that is transmitted by the polarizer, most of the light that is emitted will pass the polarizer and contribute to the emission of the LCD display as shown in Figure 1. We propose a method for the fabrication of a thin polarized-light emitting film in which an electric field aligns 50-nm long semiconductor nanorods (NRs) in a preferred direction in a polymerized film. Figure 2 shows a photograph of the resulting film with 10 mm thickness.NRs can emit saturated colors and the absorption and emission from these CdSe/CdS nanorods are highly polarized [3]. We have recently shown that NRs can be aligned effectively by applying an electric field [4].Fluorescence microscopy images of thin polarized-light emitting NR film show the emission for the orientation of the polarizer parallel ( Figure 3a) or perpendicular (Figure 3b) to the applied electric field. The ITO electrodes have a width of 6 mm and a spacing of 20 mm. The strongest photoluminescence is observed when the polarizer is parallel to the electric field, indicating that the NRs are aligned along the electric field lines. This is in agreement with earlier polarization measurements on individual NRs and aligned NR arrays [5]. The polarization ratio is defined as:in which I w and I ? are the average photoluminescent intensity over the gap area between two electrodes, when the polarizer is oriented, respectively, parallel and perpendicular to the line electrodes. The polarization ratio for regions with NRs aligned according to the above procedure is about 0.6.