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纳米LED远场辐射强度与出光角度的优化仿真

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纳米LED有望应用于超高分辨率微型显示器件,减小纳米LED的出光角度对于降低相邻像素的光串扰具有重要意义.为了获得较小出光角度的氮化镓基纳米LED,本文采用有限元方法,研究了纳米LED形状、量子阱中氮化镓厚度,以及包裹电介质层对其远场辐射强度和出光角度的影响.仿真结果显示,柱形纳米LED结构可以实现约57°的垂直出光角度;通过调整量子阱中氮化镓的厚度为3 nm,在不影响远场强度的情况下可以进一步将垂直出光角度降低至52°.此外,在纳米LED外围包裹折射率为1.5、宽度为200~300 nm的电介质层,可以有效抑制纳米柱侧面出光,使远场强度提升40%.本研究为氮化镓基纳米LED的设计和优化提供了仿真实验支持,有望推动基于纳米LED的超高分辨率显示技术的发展.
Optimized Simulation of Nano-LED Far-Field Radiation Intensity and Emission Angle
Objective Nano-light emitting diodes(nano-LEDs)offer significant potential for ultra-high-resolution display applications.A key challenge in enhancing these displays is minimizing the emission angle of nano-LEDs to reduce optical crosstalk between adjacent pixels.This study addresses this issue by investigating the influence of various parameters on the emission characteristics of GaN-based nano-LEDs.Specifically,it explores the influences of nano-LED shape,the thickness of the GaN layer in the quantum well,and the surrounding dielectric layer on far-field radiation intensity and light emission angle.The objective is to provide a comprehensive simulation-based analysis that can guide the design and optimization of nano-LEDs for improved performance in high-resolution displays.Methods The study employs the finite element method(FEM)to simulate the optical behavior of GaN-based nano-LEDs.Several parameters are adjusted to analyze their effects on emission characteristics.First,different nano-LEDs are tested to determine their influence on the emission angle.Next,the thickness of the GaN layer within the quantum well is varied.Finally,the influence of a dielectric layer encasing the nano-LED is studied.Simulations are performed to evaluate both far-field radiation intensity and the vertical emission angle under these different configurations.The parameters are systematically adjusted to identify the optimal configuration that minimizes the emission angle and enhances the far-field radiation intensity.Results and Discussions To analyze the influence of nano-LED shape on emission properties,we compare the emission effects of nano-LEDs with various top diameters(D).As shown in Figs.1(d)-1(f),an electric field distribution for D=0,400,and 500 nm reveals that a top diameter of 500 nm results in a more focused electric field.The vertical emission angle of the cylindrical nano-LED,where the top and bottom diameters are equal,is smaller,indicating superior optical performance.Figures 1(g)-1(i)demonstrate that the far-field radiation intensity is maximized,and the vertical emission angle minimized when D=500 nm.This relationship is summarized in Figs.1(j)-1(k).Thus,a diameter of 500 nm is chosen for further optimization.Next,the effect of GaN thickness in the quantum well on the electroluminescence of cylindrical nano-LEDs with a diameter of 500 nm is examined.As shown in Figs.2(a)-2(d),increasing GaN thickness(T)enhances electron-hole recombination efficiency,leading to an expanded emission range,The electric field distribution for T=3,5,and 7 nm suggests that a thinner GaN layer(T=3 nm)maintains strong far-field intensity while minimizing the emission angle,as shown in Fig.2(e),which is ideal for achieving a smaller vertical emission angle.The addition of a dielectric layer around the nano-LED controls the effective emission area,focusing the light and improving its directionality.Figures 3(a)-3(d)show the electric field distribution for different dielectric layer widths(W=50,100,and 200 nm).A dielectric layer width of 200-300 nm is found to effectively absorb side-emitted light,reducing the emission angle and increasing far-field intensity by approximately 30%[Figs.3(e)-3(g)].The optimal width for minimizing the emission angle and maximizing intensity is found to be 70 nm.Further simulations investigate the effect of the dielectric layer's refractive index on emission properties.Figures 4(a)-4(d)illustrate the electric field distribution and far-field intensity for refractive indices ranging from n=1.3 to n=1.8,with W=200 nm.The optimal refractive index of n=1.5 provides the most focused far-field distribution and the smallest emission angle.A similar trend is observed for W=300 nm[Figs.4(e)-4(h)],where n=1.5 provides the best performance.Ultimately,cylindrical nano-LEDs with a dielectric layer of n=1.5 and W=300 nm demonstrate a significantly narrower emission angle and a 40%increase in far-field radiation intensity[Figs.5(a)and 5(b)].This configuration effectively absorbs side-emitted light and concentrates the emission,highlighting its potential for high-resolution display applications.Conclusions We analyze the factors influencing the emission characteristics of GaN-based nano-LEDs.Through FEM simulation,it is found that the top diameter,GaN layer thickness,and dielectric layer properties significantly affect far-field radiation intensity and emission angle.The optimal configuration,which includes a top diameter of 500 nm,a GaN layer thickness of 3 nm,a dielectric layer refractive index of 1.5,and a dielectric layer width of 300 nm,results in a 40%increase in far-field radiation intensity and a significantly reduced emission angle.These findings offer valuable insights for the design of high-performance nano-LEDs in ultra-high-resolution display applications.

nano-LEDfar-field radiationemission angle optimizationoptical simulation

张志鹏、苏昊、李文豪、张树钱、郭焱民、龚正、郭太良、吴朝兴

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福州大学物理与信息工程学院,福建 福州 350108

中国福建光电信息科学与技术创新实验室,福建 福州 350108

纳米LED 远场辐射 出光角度优化 光学仿真

2024

光学学报
中国光学学会 中国科学院上海光学精密机械研究所

光学学报

CSTPCD北大核心
影响因子:1.931
ISSN:0253-2239
年,卷(期):2024.44(22)