Enhancement of color rendering index for white light LED lamps by red Y2O3:EU3+ phosphor

APPLIED PHYSICS VOLUME: 14 |NUMBER: 3 |2016 |SEPTEMBER Enhancement of Color Rendering Index for White Light LED Lamps by Red Y2O3:Eu3+ Phosphor Tran Hoang Quang MINH, Nguyen Huu Khanh NHAN, Thoai Phu VO, Nguyen Doan Quoc ANH Department of Electronics and Telecommunications, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, 19 Nguyen Huu Tho Street, Ho Chi Minh City, Vietnam [email protected], nguyenh[email protected], thoaiphuv[email protected], nguyendoanquo[email protected] DOI: 10.15598/aeee.v14i3.1642 Abstract. We present an application of the red Y2O3:Eu3+ dopant phosphor compound for reaching the color rendering index as high as 86. The Multi-Chip White LED lamps (MCW-LEDs) with high Correlated Color Temperatures (CCTs) including 7000 K and 8500 K are employed in this study. Besides, the impacts of the Y2O3:Eu3+ phosphor on the attenuation of light through phosphor layers of the various packages is also demonstrated based on the Beer-Lambert law. Simulation results provide important conclusion for selecting and developing the phosphor materials in MCW-LEDs manufacturing. Keywords Beer-Lambert law, Color Rendering Index, pcWLEDs, Y2O3:Eu3+. 1. Introduction There are many benefits of MCW-LEDs to consumers such as high brightness, low power consumption, long lifetime, fast response, climate impact resistance [1]. Correspondingly, MCW-LEDs are considered to be key lighting devices to replace traditional lamps. Luminous output and Correlated Color Temperature (CCT) uniformity are two main factors of white LED lamps. By adding SiO2powder having the suitable size and concentration, some researchers have reduced spatial CCT deviation without decreasing lumen output significantly. The lumen output of MCW-LEDs can be enhanced significantly after adding the green Ce0.67 Tb0.33 MgAl11 O19:Ce, Tb phosphor to MCW-LEDs [2]. Furthermore, we cannot but mention the Color Rendering Index (CRI) that is considered as one important characteristic of MCW-LEDs. Several previous studies have applied methods that consist of mixing red-phosphors or doping red LEDs to compensate redlight to MCW-LEDs [3], [4], [5], [6], [7]. Besides, Won et al. presented high CRI multi-chip white LEDs, combining blue LEDs and green (Ba,Sr)2SiO4:Eu2+ and red CaAlSiN3:Eu2+ phosphors with the different packages. By doping the missing red component in phosphor-converted MCW-LEDs (pc-WLEDs), the CRI of MCW-LEDs can be enhanced to more than 80, which is an important goal [2]. Red Y2O3:Eu3+ phosphor is one of cathodoluminescent phosphors, which is employed widely in color displays as a red-light-emitting component. However, Y2O3:Eu3+ phosphor has not many applications for improving CRI as yet. In this paper, we introduce the impacts of Y2O3:Eu3+ phosphor particles in multi-chip white light LEDs with conformal phosphor or in-cup phosphor packages to enhance color rendering ability. It has been found that the participation of Y2O3:Eu3+ phosphor particles can dominate the red-light emitting event in pc-WLEDs, so that the LED light distribution can be free from the dispersion incurred by LED packages to yield higher Color Rendering Index. We have divided the work processes into three main stages. The precise MCW-LEDs physical model having average CCTs of 7000 K and 8500 K has been conducted by LightTools software at first. Then, the transmission of light has been decreased after mixing Y2O3:Eu3+ particles, which has demonstrated the Beer-Lambert law. Finally, we have investigated the effects of Y2O3:Eu3+ phosphor particles on the color rendering ability of MCW-LEDs according to the simc 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 340 APPLIED PHYSICS VOLUME: 14 |NUMBER: 3 |2016 |SEPTEMBER ulation results. Based on the results, the proposed method of doping certain amounts of Y2O3:Eu3+ in the LED packages can improve their CRI significantly. 2. Simulation The pc-WLEDs is covered by flat silicone layer, which is simulated by using LightTools 8.1.0 program. The key work consists of pc-WLEDs construction and phosphor concentration adjustment. Firstly, the structures of pc-WLEDs such as the Conformal Phosphor Package (CPP) and the In-cup Phosphor Package (IPP) are introduced with five CCTs of 7000 K and 8500 K, see Fig. 1. Secondly, it is necessary to keep the MCWLEDs work at mean CCTs from 7000 K to 8500 K for achieving the LED product specification. If the weight percentage of the red Y2O3:Eu3+ phosphor increases, that of yellow YAG:Ce phosphor needs to be decreased to maintain the mean CCT values. Silicone lens Gold wire Y O :Eu 23 3+ Reflector Silicone substrate LED chip (a) the conformal phosphor package Silicone lens Y O :Eu 23 3+ Silicone substrate LED chip (b) the in-cup phosphor package Fig. 1: Illustration of MCW-LEDs. The optical properties of reflector of CPP and IPP are similar. The depth, inner, and outer radius of the reflector are 2.07 mm, 8 mm and 9.85 mm, respectively. The CPP and the IPP, with the fixed thickness of 0.08 mm and 2.07 mm in turn, cover the nine chips. The blue Led chip has a dimension of 1.14 ×0.15 mm. The radiant flux of each blue chip is 1.16 W, and the peak wavelength is 453 nm. At the CPP displayed in Fig. 1(a), its phosphor layer is coated conformally on nine LEDs. As for the IPP, its phosphor layer is located in the silicone lens, as displayed in Fig. 1(b). The absorption, emission and scattering of both YAG:Ce and Y2O3:Eu3+ phosphor particles, with the peak wavelengths including blue of 453 nm and greenyellow of 555 nm, can be computed by Mie-scattering theory [2]. The phosphor layers consist of YAG:Ce and Y2O3:Eu3+ powders and the silicone matrix. Their refractive indexes are 1.83, 1.93 and 1.50, respectively. Meanwhile, the mean radii of the phosphor powders are 7.25 µm, which conforms the real particle size. 3. Color Rendering Index In order to verify the improvement of CRI using Y2O3:Eu3+ phosphor, we switch the average CCT among the values of 7000 K and 8500 K and change Y2O3:Eu3+ weight. The corresponding values of CRI are then calculated and displayed on Fig. 2. Figure 2(a) illustrates the impact of Y2O3:Eu3+ concentration on CRI of CPP structures. It can be observed that the CRI grows with the weight percentage of Y2O3:Eu3+ phosphor in the continuous range from 0 % to nearly 10 %. The highest color rendering ability is obtained with the Y2O3:Eu3+ weight range from 8 % to 12 %. In particular, optimal color rendering index that can be achieved exceeds the value of 86 in this case. As for IPP structure, the Y2O3:Eu3+ concentration ranges continuously from 0 % to approximately 0.4 %. From 0.3 % to 0.4 %, the CRI has a decreasing tendency with the increasing of Y2O3:Eu3+ weight beyond a point where the red-light starts to be over-dominant, causing color rendering ability to reduce. The highest color rendering ability with the different CCTs can be obtained when the Y2O3:Eu3+ percentage ranges from 0.24 % to 0.3 %, as shown in Fig. 2(b). The optimal color rendering index of MCW-LEDs can exceed 84 in this case, which is 25.8 % higher than that of the non Y2O3:Eu3+ case, i.e. When the Y2O3:Eu3+ concentration is equal to 0 %. In summary, with the simulated results of CRI, we can demonstrate that the Y2O3:Eu3+ phosphor having proper concentration can be used for increasing the CRI. c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 341 APPLIED PHYSICS VOLUME: 14 |NUMBER: 3 |2016 |SEPTEMBER 0 2 4 6 8 10 12 14 50 55 60 65 70 75 80 85 90 Y2O3 wt. (%) Color Rendering Index 7000 K 8500 K (a) CPP 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 60 65 70 75 80 85 90 Y2O3 wt. (%) Color Rendering Index 7000 K 8500 K (b) IPP Fig. 2: The color rendering index at average CCTs of 7000 K and 8500 K with various Y2O3:Eu3+ weight with two phosphor geometries. 4. Luminous Flux The effect of Y2O3:Eu3+ concentration in phosphor compound on the lumen output is also verified together with the CRI, as shown in Fig. 3. The weight percentage of phosphor compound was varied continuously from 0 % to 14 % and to 0.4 % for CPP and IPP, respectively. At low Y2O3:Eu3+ concentration regime, the extinction coefficient tends to reduce, which results in the enhancement of luminous output. Meanwhile, the luminous flux decreases with the Y2O3:Eu3+ weight enhancement due to the increase of extinction coefficient. To verify these results, the relationship of luminous output to the Y2O3:Eu3+ weight can be formulated according to Mie-scattering theory. The depletion of light is calculated by the Beer-Lambert law: I=I0e−µext L,(1) (a) CPP@7000 K (b) CPP@8500 K Fig. 3: Luminous flux according to computed extinction coefficient of CPPs. where Iis the transmitted light power, I0is the incident light power, µext =N·Cext is the extinction coefficient, Lis the path length and Nis the number of particles per cubic millimeter. According to Mie-scattering theory, the extinction cross section Cext of phosphor particles can be characterized by the following relationship: Cext =2πa2 x2 ∞ X n=1 (2n+ 1)Re(an+bn),(2) where x= 2πa/λ is the size parameter, anand bnare the expansion coefficients with even symmetry and odd symmetry, respectively. The parameters anand bnare defined as: an(x, m) = ψ0 n(mx)ψn(x)−mψn(mx)ψ0 n(x) ψ0 n(mx)ξn(x)−mψn(mx)ξ0 n(x),(3) bn(x, m) = mψ0(mx)ψn(x)−ψn(mx)ψ0 n(x) mψ0 n(mx)ξn(x)−ψn(mx)ξ0 n(x),(4) c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 342 APPLIED PHYSICS VOLUME: 14 |NUMBER: 3 |2016 |SEPTEMBER where ais the spherical particle radius, λis the relative scattering wavelength, mis the refractive index of scattering particles, and ψn(x)and ξn(x)are the Riccati–Bessel functions. The extinction coefficient of the red Y2O3:Eu3+ phosphor is verified for two distinct wavelengths, 555 nm and 453 nm, which are the emission peaks of the YAG:Ce phosphor and the LED chips, respectively. The variation of the mentioned parameters with respect to the Y2O3:Eu3+ concentration according to the above equations are displayed in Fig. 3 and Fig. 4. The simulation results of luminous flux for CPP as shown in Fig. 3 are compared with those for IPP as demonstrated in Fig. 4. It is indicated that the higher lumen output should occur at low Y2O3:Eu3+ concentration, which corresponds to the lower extinction coefficient value. These results can be employed to estimate the influence of Y2O3:Eu3+ concentration on the lumen output from the pc-WLEDs. (a) IPP@7000 K (b) IPP@8500 K Fig. 4: Luminous flux according to computed extinction coefficient of IPPs. 5. Conclusion Summary, both the CRI and the lumen output of MCW-LEDs depend on the red Y2O3:Eu3+ phosphor concentration. Firstly, it is noted that the CRI can be enhanced to 86 and more regardless of the mean CCTs and the phosphor geometries. Next, the luminous flux has a decreasing tendency at large weight range due to the enhancement of the extinction coefficient. However, it is noticeable that the lumen output can be grown after adding Y2O3:Eu3+ with low weight range. Finally, the paper proves the implications of Y2O3:Eu3+ phosphor application for developing the pc-WLEDs of MCW-LEDs manufacturing. References [1] ZHENG, H., X. B. LUO, R. HU, B. CAO, X. FU, Y. WANG and S. LIU. Conformal phosphor coating using capillary microchannel for controlling color deviation of phosphor-converted white light-emitting diodes. Optics Express. 2012, vol. 20, iss. 5, pp. 5092–5098. ISSN 1094-4087. DOI: 10.1364/OE.20.005092. [2] LIU, S. and X. B. LUO. LED Packaging for Lighting Applications: Design, Manufacturing and Testing. Hoboken: John Wiley&Sons, 2011. ISBN 978-0-470-82840-3. [3] LIU, Z. Y., S. LIU, K. WANG and X. 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DOI: 10.1364/OE.15.007572. c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 343 APPLIED PHYSICS VOLUME: 14 |NUMBER: 3 |2016 |SEPTEMBER [7] WANG, K., S. LIU, X. B. LUO, Z. Y. LIU and F. CHEN. Optical Analysis of A 3W LightEmitting Diode (LED) MR16 Lamp. In: International Conference on Electronic Packaging Technology &High Density Packaging. Shanghai: IEEE, 2008, pp. 1–5. ISBN 978-1-4244-2740-6. DOI: 10.1109/ICEPT.2008.4607028. About Authors Tran Hoang Quang MINH defended his Ph.D. thesis at Tomsk Polytechnic University, Tomsk City, Russian Federation. The author’s major fields of study are High-Voltage Power System, Relay Protections and Optoelectronics. He is working as Lecturer in Faculty of Electrical and Electronic Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam. Nguyen Huu Khanh NHAN defended his Ph.D. thesis at Institute of Research and Experiments for Electrical and Electronic Equipment, Moscow, Russian Federation. He is working as Lecturer in Faculty of Electrical and Electronic Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam. His research interests include VLSI, MEMS and LED driver chips. Thoai Phu VO was born in An Giang province, Vietnam. He has been working at the Faculty of Electrical and Electronics Engineering, Ton Duc Thang University. He received his Ph.D. degree from Dayeh University, Taiwan in 2015. His research interests are optoelectronics, fuzzy control, image processing. Nguyen Doan Quoc ANH was born in Khanh Hoa province, Vietnam. He has been working at the Faculty of Electrical and Electronics Engineering, Ton Duc Thang University. Quoc Anh received his Ph.D. degree from National Kaohsiung University of Applied Sciences, Taiwan in 2014. His research interest is optoelectronics (such as Multi-chip white light LEDs, free-form lens, optical material). c 2016 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 344