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Y. C. Chen, C. T. Pan, C. C. Hsieh, C. Y. Su, H. C. Wu, W. C. Li, "Fabrication of Light Extraction Efficiency of Organic Light-Emitting Diodes with 3D Aspherical Microlens by Using Dry Etching Process", Journal of Nanomaterials, vol. 2013, Article ID 797534, 6 pages, 2013. https://doi.org/10.1155/2013/797534
Fabrication of Light Extraction Efficiency of Organic Light-Emitting Diodes with 3D Aspherical Microlens by Using Dry Etching Process
organic light-emitting diode (OLED) can enable a greater artificial contrast ratio and viewing angle compared to liquid crystal display (LCD) because OLED pixels directly emit light. There is a shortcoming that the internal quantum efficiency can reach values close to 100%, but about 80% light disperses because of the difference among the refractive indices of the substrate, anode, indium tin oxide (ITO) film, and air. In this paper, three dimensions aspherical microlens arrays (3D A-MLAs) with substrate modifications are developed to simulate the optical luminous field by using FRED software. This study modified parameters of 3D A-MLAs such as the diameter, fill-factor, aspect ratio, dry etching parameters, and electroforming rates of microlens to improve the extraction efficiency of the OLED. In dry etching, not only the aspect ratio with better extraction rate can be obtained by reactive ion etching (RIE) dry etching, but also an undercutting phenomenon can be avoided. The dimensions of 3D A-MLAs can be accurately controlled in the electroforming process used to make a nickel-cobalt (Ni-Co) metal mold to achieve the designed dimensions. According to the measured results, the average luminance efficacy of the OLEDs with 3D A-MLAs can be enhanced.
In this rapid-growing information era, display has become an indispensable information tool. In the flat panel displays (FPDS), the organic light-emitting diode (OLED) display is attracting considerable interest, because it is much thinner, lighter, and more flexible than liquid crystal display (LCD).
OLED seems to be the perfect technology for all types of displays, but the extraction efficiency of current OLED is generally low due to its total internal reflection, and the internal quantum efficiency is limited because light disperses in different refractive indices [1–3]. Thus, how to increase the OLED extraction efficiency of luminance is worth studying. The extraction efficiency of luminance could be increased by many methods, such as using the resonant cavity , excitation of surface plasmons , insertion of a thin silica aerogel layer of very low refractive index , and 2D SiO2/SiNx photonic crystals  as well as microlens arrays . Among these technologies, the process of microlens arrays is simple and reliable, so this study analyzed the manufacturing and designed parameters of microlens arrays (MLAs). The luminance will be increased as the contact angle and fill-factor of MLA  increase, and the luminance will be decreased as the viewing angle is increases .
Being a commercial fabricating process, it should be of low cost and rapid. But the conventional methods of fabricating A-MLAs such as gray-scale mask, sandblasted diffuser plate, and lithography with SU-8 still have some disadvantages [11–13]. Those processes need highly accurate alignment and control, long process time, high production cost, and special material. To solve these problems, we presented a modified LIGA process. A metal mold is applied to replicate MLA rapidly by using this method, and A-MLAs could be produced with any shape. So far, hexagonal , triangular , and dual-curvature MLAs  were successfully fabricated accurately in our laboratory.
The aspherical microlens shape attached on the OLED can reduce the ratio of total reflection in substrate to improve the efficiency of an OLED when the waveguide phenomenon which occurs between air and glass is reduced. three dimensions aspherical microlens arrays (3D A-MLAS) optical films were fabricated. In electroforming, the Ni-Co alloy was deposited on the seed layer, and it forms a metal mold that is also called the first mold. The second mold was fabricated by polydimethylsiloxane (PDMS), which was replicated from the first mold. The parameters of the process such as diameter of MLA, dry etching, and electroforming rates were analyzed. We used SpectraScan Colorimeter PR-650 to measure the luminance efficiency. The luminance of OLEDs can be enhanced significantly.
2. Materials and Methods
2.1. Design and Simulation
The fill-factor is the ratio of the active refracting area to the total contiguous area occupied by the lens array. And the aspect ratio is the proportional relationship between width and height of MLA. This study used the optical simulation software, FRED, to analyze the variations of the optical characteristics such as the diameter and aspect ratio. This analysis is based on the theory that when the aspect ratios of A-MLAs are higher, the intensity of a light source is higher. The parameters include curves, four layouts, and four diameters. The variations of intensity with respect to diameters are limited in the same layout with different diameters. In the design, fill-factor and aspect ratio are two important factors. The higher fill-factor and aspect ratio an MLA has, the higher extraction rate can be obtained. These experiments focus on how the different parameters of dry etching and electroforming rate influence the formation of A-MLAs with the same diameters. Figure 1 is a gain of luminous intensity of OLED with MLAs film with a spherical curve in different layouts. The simulation results show that luminous intensity of the layout of tangential circle is obviously higher than of the other layouts. For the same aspect ratio of 0.5, the luminous intensity can be enhanced up to 28% which is compared with a bare OLED light source without optical film. Due to the geometric constraints, the maximum aspect ratio of a spherical MLA is 0.5. In order to collect the maximum amount of light, the lens should be as close to 100% as possible .
2.2. Fabrication and Process
The study develops 3D A-MLAs by modified lithographie, galvanoformung, abformung (LIGA) process. The procedure is shown in Figure 2.(1)Dehydrate RCA cleaning removes the organic contaminants, thin oxide layer, and ionic contamination on wafers. (2)Spinning positive photoresist (PR), AZ4620, on wafers. (3)After soft baking, the PR is exposed to a pattern of intense light, as shown in Figure 2(a). The exposure to light causes a chemical change that makes the PR become soluble in the developer when it is exposed, and the pitch and dimensions of mask pattern were 70 μm and 40 μm, respectively, which should be taken into consideration carefully to manufacture an A-MLA.(4)Reflow process can make a column array become a microlens array, as shown in Figure 2(b). We used reactive ion etching (RIE) dry etching to avoid significant undercutting of photoresist pattern, as shown in Figure 2(c). In dry etching, different concentrations of oxygen can obviously influence the shape and surface roughness of microstructures.
Sputtering silver (Ag) layer as a seed layer on the wafer then depositing Ni-Co alloy as an electroforming mold on it is called first mold. In electroforming, various ampere per square decimeter (ASD) (A/dm2) can influence deposition rate and roughness and then replicate the first mold by PDMS [17, 18], as shown in Figure 2(d). Finally, the optical film with A-MLAs by ultraviolet (UV) cured process was fabricated.
3. Results and Discussion
3.1. Dimensions of A-MLAs
The diameters of 3D microlenses are set as 10, 20, 50, and 100 μm modified LIGA process, and the aspect ratios are from 0.1 to 2.5. While the aspect ratio is larger than 1.25, the luminous intensity decreases gradually (Figure 3). The height of a microlens can be achieved by the etching and electroforming process.
3.2. Diameters of A-MLAs
Comparing the diameter of 3D A-MLAs simulated by FRED with the diameter manufactured by UV cured process, the radius decreased from 70 μm to 69.4 μm. The substrate was exposed to UV light. After developing and thermal reflow, a microcolumn array was obtained, and the diameter was 38.4 μm. This error was 4%. Then we used RIE dry etching to avoid significant undercutting of photoresist pattern, and the diameter was 36.3 μm. This error was 5.5%. After dry etching and electroforming process, a microlens array was cast by using PDMS process, and the diameter was 69.5 μm. This error was 0.7%.
3.3. Dry Etching Parameters
RIE with incident oxygen (O2) plasma and sulfur hexafluoride (SF6) was performed to shrink the size of A-MLAs in order to facilitate the etching of photoresist. The RIE was performed on spheres with variable O2 flow rates (10, 5, 1, and 0 sccm). The etching parameter is shown in Table 1. The aspect ratio became worse as the height which was 16.8 μm of A-MLAs was reduced obviously.
The flow rate was set to be 10 sccm with a chamber pressure of 25 mTorr and the power of 40 W in the first experiment, as shown in Figures 4(a) and 4(b). The heights were 21.9 and 22.6 μm in the second and third experiments, as shown in Figures 4(c) and 4(d), and the etching rates were 1 : 1.85 and 1 : 2.1 separately.
Scanning electron microscopic (SEM) images of a 3D A-MLA without O2 dry etching which could not be used because of its low etching efficiency. The study found that the lower O2 concentration is, the much higher and better shape could be obtained, but if O2 concentration was too low (below 1 sccm) as the seventh experiment, the gas would damage the structure seriously, so the concentration should be well controlled.
3.4. Electroforming Rates
Photoresist surface has many defects after RIE etching, and the dimensions are shrunk by etching. Electroforming process can smooth the surface defects by depositing metal layers to replicate PDMS molds. During the electroplating, the lens grows isotropically. The development of a hexagonal microlens array is influenced by the gaps between etching patterns and the diameters of microlenses (Figure 5(a)). Furthermore, the electroplating technology is an important process to fabricate the hexagonal shape. Then, a Ni-Co alloy was cast atop the seed layer, and it formed a microgapless hexagonal microlens array (Figure 5(b)). Therefore the profile of hexagonal lens is spherical, same as the microlens of PR. The metal mold with higher ASD is better than the one with lower ASD, as shown in Figure 6.
3.5. Measurement of the Film Pasted on an OLED
The luminance, current density, and luminance efficiency tested by SpectraScan Colorimeter PR-650 (Photo Research, Inc.) were controlled by a computer and a power supply. The power supply (2400 Source Meter, Keithley) can provide direct current (DC) to an OLED as a light source in this measurement.
For the measurement of A-MLAs, four samples including bare light, A-MLAs with low ASD called low-ASD film, A-MLAs with high ASD called high-ASD film, and an etched optical film without electroforming were used to generate and select suitable items called NE-film (Table 2). The measured data of each film is shown Table 3 is the all calculated results. Comparison between bare light and an OLED with films is obtained, and the largest variation is 15 times the luminance of the bare light.
The luminance and uniformity were measured by nine-point measurement (Figures 7, 8, and 9), and the optical film was attached to an OLED. The measurement of the bare light was used as base data to compare with the others, and the optical film with A-MLAs was 15 times brighter than bare light.
After dry etching process was applied into the LIGA-like process, aspect ratio of 3D A-MLA was improved significantly. By replicating PDMS mold rapidly, the time-wasted microelectroforming process could be removed. There are several advantages in our study.(1)3D A-MLAs with high aspect ratio could be fabricated by using modified LIGA process that combined reflow process and dry etching.(2)By using electroforming technology, 3D A-MLA with high fill-factor could be achieved.(3)The time of process and cost could be reduced by applying the PDMS replicating and UV curing technologies to the process. (4)After 3D A-MLAs were used, the luminance of OLED could be enhanced significantly, and the efficiency of light source was raised as well.
The authors like to thank F. T. Hsu, P. H. Lin, and the National Sun Yat-Sen University for the assistance in this project.
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