LED用石墨烯复合透明电极厚度组合的仿真与优化

为降低石墨烯(Gr)透明电极与p-GaN之间的肖特基势垒与接触电阻,进行了将银、金、镍和铂四种金属或氧化镍作为中间层引入它们两者之间的尝试。使用有限元方法模拟研究了Gr与金属或氧化镍的不同厚度组合对LED的光、热和电特性的影响。发现:透明导电层的透光率和LED芯片的表面温度均随石墨烯和金属或氧化镍厚度的增加而降低;1.5nm的Ag、Ni、Pt,1nm Au或1nm的NiO_x分别与3层(3L)Gr复合时为优化厚度组合,其中,1.5nm Ni/3L Gr为最佳Gr/金属复合透明电极。     

电极耦合层对GaN基蓝光LED出光特性的影响

光提取效率的提高对GaN基蓝光LED的广泛应用有重要的影响.计算了以Ni/Au基金属化方法形成的p型GaN电极的折射率,通过分析电极层中的能流传输情况在电极上设计高折射率的耦合层来减少电极层对光的吸收以及提高光的透射,耦合层通过采用圆台结构来减少光在空气/耦合层界面上的全反射以提高GaN基蓝光LED的光提取效率.应用传输矩阵法计算的结果表明,光学厚度为π/2,折射率为2.02的ITO耦合层能使450 nm的蓝光在膜系上的透射率提高到75%.     

Ni层厚度对p-GaN/Ni/Au欧姆接触特性的影响

对p-GaN/Ni/Au欧姆接触特性与Ni金属层厚度之间的相关性进行了对比实验研究,利用XRD衍射结果与表面金相显微分析手段对Ni/Au双层金属电极在合金退火过程中的行为特性进行了细致探讨。分析结果表明:在Ni/Au电极结构中,由双层互扩散机制与NiO氧化反应机理决定,Ni层与Au层之间的厚度比率对p型GaN欧姆接触特性的优劣有重要影响,在Ni、Au层厚度相当时可获得最佳的p型欧姆接触。     

大功率倒装结构GaN LED p电极研究

从接触电阻、反射率、电流扩展等方面对Ni/Au/Ag,ITO/Ag,Ag等多种倒装结构p电极金属体系进行分析比较,给出了实现倒装结构大功率GaN LED p电极的多种设计方案.指出Ni/Au金属化体系在大功率LED应用中存在的热稳定性问题及Ru,Ir等新型金属体系实现GaN p电极接触的潜在优势.     

大功率倒装结构GaN LED p电极研究

从接触电阻、反射率、电流扩展等方面对Ni/Au/Ag,ITO/Ag,Ag等多种倒装结构p电极金属体系进行分析比较,给出了实现倒装结构大功率GaN LED p电极的多种设计方案.指出Ni/Au金属化体系在大功率LED应用中存在的热稳定性问题及Ru,Ir等新型金属体系实现GaN p电极接触的潜在优势.     

大功率倒装结构GaN LED p电极研究

从接触电阻、反射率、电流扩展等方面对Ni/Au/Ag,ITO/Ag,Ag等多种倒装结构p电极金属体系进行分析比较，给出了实现倒装结构大功率GaN LED p电极的多种设计方案. 指出Ni/Au金属化体系在大功率LED应用中存在的热稳定性问题及Ru,Ir等新型金属体系实现GaN p电极接触的潜在优势.     

GaAs吸收衬底生长的立方相GaN发光二极管的工艺设计与实现

利用光学薄膜原理,计算了采用晶片键合技术来提高以GaAs为衬底的立方相GaN的出光效率的理论可行性.以Ni为粘附层,Ag为反射层的Ni/Ag/Au薄膜体系可以使立方GaN的出光效率从理论上提高2.65倍左右.实验结果证实,利用键合方法实现的以Ni/Ag/Au作为反射膜的样品的光反射率比未做键合的GaN/GaAs样品的光反射率在理论计算的459.2nm处提高了2.4倍.     

GaAs吸收衬底生长的立方相GaN发光二极管的工艺设计与实现

利用光学薄膜原理,计算了采用晶片键合技术来提高以GaAs为衬底的立方相GaN的出光效率的理论可行性.以Ni为粘附层,Ag为反射层的Ni/Ag/Au薄膜体系可以使立方GaN的出光效率从理论上提高2.65倍左右.实验结果证实,利用键合方法实现的以Ni/Ag/Au作为反射膜的样品的光反射率比未做键合的GaN/GaAs样品的光反射率在理论计算的459.2nm处提高了2.4倍.     

垂直结构GaN基LED用Ni/Ag反射镜电极

Ni/Ag/Ti/Au金属系反射镜电极广泛用于GaN基垂直结构发光二极管(LED)的传统制造工艺.这种电极需要进行高温长时间整体退火才能获得高质量的欧姆接触,但对电极的反射率和器件性能影响较大.介绍了一种新工艺方法,该方法将电极分解为接触层和反射层,降低反射层经历的退火温度和时间,获得了拥有良好的欧姆接触特性和高反射率的反射镜电极,解决了传统电极光学性能和电学性能相互制约的问题.首先生长极薄的Ni/Ag作为接触层,对接触层进行高温长时间退火后再生长厚层Ag作为反射层,之后再进行一次低温退火.使得对反射起主要作用的反射层免于高温长时间退火,相较于传统Ni/Ag/Ti/Au电极,该方法在获得更优良的欧姆接触的同时,提升了电极的反射率.在氧气氛围下进行500℃接触层退火3 min,400℃整体退火1 min后,电极的比接触电阻率为1.7×l0-3Ω·cm2,同时在450 nm处反射率为93％.     

用于紫外探测器的AlGaN/GaN异质结构的Ti/Al/Ni/Au欧姆接触特性

采用Ti/Al/Ni/Au多层金属体系在Al0.27Ga0.73N/GaN异质结构上制备了欧姆接触. 分别采用线性传输线方法(LTLM)和圆形传输线方法(CTLM)对其电阻率进行了测试. 当Ti(10nm)/Al(100nm)/Ni(40nm)/Au(100nm)金属体系在650℃高纯N2气氛中退火30s时,测量得到的最小比接触电阻率为1.46E-5Ω·cm2. 并制备了Al0.27Ga0.73N/GaN光导型紫外探测器,通过测试发现探测器的暗电流-电压曲线呈线性分布. 实验结果表明在Al0.27Ga0.73N/GaN异质结构上获得了好的欧姆接触,能够满足制备高性能AlGaN/GaN紫外探测器的要求.     

Nanomeshed Pt(Au) Transparent Contact to p-GaN of Light-Emitting Diode

This study examines nanomeshed Pt and Pt(Au) thin films formed by a dewetting process on a p-GaN surface. With prolonged annealing, the Pt(Au) layer shows more stable contact resistance to p-GaN and lower sheet resistance than the Pt layer. L–I curves show that the GaN light-emitting diode (LED) with the Pt(Au) transparent conducting layer (TCL) produces more light output power than the GaN LED with the Pt TCL. The higher light output of the LED with the Pt(Au) TCL is attributed to the lower sheet resistance, which improves current spreading in the active region.     

InGaN/GaN light emitting diodes with Ni/Au mesh p-contacts

In order to improve the light transmittance and output efficiency of the InGaN/GaN multi-quantum well (MQW) light emitting diodes (LEDs), we proposed a novel Ni/Au mesh p-contact. As compared with the traditional Ni/Au film p-contact, the proposed Ni/Au mesh p-contact has the less light blocking nature yet still keeps well ohmic contact. Our lab result shows that for 470 nm wavelength the Ni/Au mesh p-contact has 95% light transmittance and 11.3 mW output power at a 20 mA injection current. In contrast, at the same 470 nm wavelength, the traditional Ni/Au film p-contact has 72% light transmittance and 8.12 mW output power at a 20 mA injection current.     

Low-operation voltage of InGaN-GaN light-emitting diodes withSi-doped In0.3Ga0.7N/GaN short-period superlatticetunneling contact layer

InGaN/GaN multiple-quantum-well light-emitting diode (LED) structures including a Si-doped In_0.23Ga_0.77N/GaN short-period superlattice (SPS) tunneling contact were grown by metalorganic vapor phase epitaxy. In_0.23Ga_0.77N/GaN(n⁺)-GaN(p) tunneling junction, the low-resistivity n⁺-In_0.3Ga_0.77 N/GaN SPS instead of high-resistivity p-type GaN as a top contact layer, allows the reverse-biased tunnel junction to form an “ohmic” contact. In this structure, the sheet electron concentration of Si-doped In_0.23Ga_0.77N/GaN SPS is around 1×10¹⁴/cm², leading to an averaged electron concentration of around 1×10²⁰/cm³. This high-conductivity SPS would lead to a low-resistivity ohmic contact (Au/Ni/SPS) of LED. Experimental results indicate that the LEDs can achieve a lower operation voltage of around 2.95 V, i.e., smaller than conventional devices which have an operation voltage of about 3.8 V     

Effects of p-type GaN thickness on optical properties of GaN-based light-emitting diodes

The influence of p-type Ga N(p Ga N) thickness on the light output power(LOP) and internal quantum efficiency(IQE) of light emitting diode(LED) was studied by experiments and simulations. The LOP of Ga N-based LED increases as the thickness of p Ga N layer decreases from 300 nm to 100 nm, and then decreases as the thickness decreases to 50 nm. The LOP of LED with 100-nm-thick pG a N increases by 30.9% compared with that of the conventional LED with 300-nm-thick p Ga N. The variation trend of IQE is similar to that of LOP as the decrease of Ga N thickness. The simulation results demonstrate that the higher light efficiency of LED with 100-nm-thick p Ga N is ascribed to the improvements of the carrier concentrations and recombination rates.     

Influence of Ni Schottky contact thickness on two-dimensional electron-gas sheet carrier concentration of strained AI0.3Ga0.7N/GaN heterostructures

Ni/Au Schottky contacts with thicknesses of either 50(A)/50(A) or 600 (A)/2000(A) were deposited on strained Al0.3Ga0.7N/GaN heterostructures.Using the measured C-V curves and Ⅰ-Ⅴ characteristics at room temperature,the calculated density of the two-dimensional electron-gas (2DEG) of the 600(A)/2000(A) thick Ni/Au Schottky contact is about 9.13 x 1012 cm-2 and that of the 50(A)/50(A) thick Ni/Au Schottky contact is only about 4.77 ×1012 cm-2.The saturated current increases from 60.88 to 86.34 mA at a bias of 20 V as the thickness of the Ni/Au Schottky contact increases from 50(A)/50(A)to 600(A)/2000(A).By self-consistently solving Schrodinger's and Poisson's equations,the polarization charge sheet density of the two samples was calculated,and the calculated results show that the polarization in the AIGaN barrier layer for the thick Ni/Au Schottky contact is stronger than the thin one.Thus,we attribute the results to the increascd biaxial tensile stress in the Al0.3Ga0.7N barrier layer induced by the 600(A)/2000(A)thick Ni/Au Schottky contact.     

Formation of Ta/Ti/Al/Mo/Au ohmic contacts to an AlGaN/AlN/GaN heterostructure grown on a silicon substrate

The features of the formation of Ta/Ti/Al/Mo/Au ohmic contacts to a Al_0.26Ga_0.74N/AlN/GaN heterostructure grown on semi-insulating Si(111) substrates are studied. The dependences of the contact resistance on the Al (90, 120, 150, 180 nm) and Ti (15, 30 nm) layer thickness and optimal temperature-time annealing conditions are determined for each studied metallization scheme. It is shown that the minimum achievable contact resistance monotonically increases from 0.43 to 0.58 Ω mm as the Al layer thickness increases from 90 to 180 nm at unchanged Ta, Ti, Mo, Au layer thicknesses. A change in the Ti layer thickness from 15 to 30 nm has no significant effect on the minimum contact resistance. The least contact resistance of 0.4 Ω mm is achieved for Ta/Ti/Al/Mo/Au layers with thicknesses of 10/15/90/40/25 nm, respectively. The optimal annealing temperature for this metallization variant is 825°C at a process duration of 30 s. The grown ohmic contacts have smooth contact-area edges and flat morphology of their surface.     

High brightness InGaN green LEDs with an ITO on n/sup ++/-SPS upper contact

Indium tin oxide (ITO) (260 nm) and Ni (5 nm)/Au (10 nm) films were deposited onto glass substrates, p-GaN layers, n/sup +/-InGaN/GaN short-period-superlattice (SPS), n/sup ++/-SPS and nitride-based green light-emitting diodes (LEDs). It was found that ITO could provide us an extremely high transparency (i.e., 95% at 520 nm). It was also found that the 1.03/spl times/10/sup -3/ /spl Omega/cm/sup 2/ specific contact resistance of ITO on n/sup ++/-SPS was reasonably small. Although the forward voltage of the LED with ITO on n/sup ++/-SPS upper contacts was slightly higher than that of the LED with Ni/Au on n/sup ++/-SPS upper contacts, the 20 mA output power and external quantum efficiency of the former could reach 4.98 mW and 8.2%, respectively, which were much larger than the values observed from the latter. The reliability of ITO on n/sup ++/-SPS upper contacts was also found to be reasonably good.