Table of Contents
ISRN Optics
Volume 2013, Article ID 385345, 5 pages
Research Article

Combined Experimental and Monte-Carlo Ray-Tracing Approach for Optimizing Light Extraction in LED COB Modules

CEA-Leti, Minatec Campus, 17 rue des Martyrs, 38054 Grenoble Cedex 9, France

Received 6 May 2013; Accepted 26 June 2013

Academic Editors: L. R. P. Kassab and Y. S. Kivshar

Copyright © 2013 Marianne Consonni et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


High-power light-emitting diodes (LEDs) for lighting applications require a high-efficient packaging to optimize their performances. Due to its high thermal dissipation potential, the chip-on-board (COB) technology is widely used for developing high-power lighting sources. In order to optimize the optical properties of such sources and to propose high optically efficient encapsulation geometry, ray-tracing simulations have been performed. The impact of the shape and volume of the silicone encapsulation on the light extraction and on the intensity distribution of the module was derived. Then, simulation results were correlated with experimental measurements on blue light-emitting COB sources. It is shown that a nearly hemispherical encapsulation with a minimal volume of 5 to 10 mm3 for a 1 mm2 LED die is the optimal configuration regarding both the light extraction and the intensity distribution.

1. Introduction

High-power light-emitting diodes (LEDs) have attracted a lot of interest in the recent years due to their low-power consumption and long lifetime. However, the integration of these light sources for general lighting applications will require high-efficient packaging with low thermal resistance and compact size [1]. Thus, due to its compactness and its high thermal dissipation potential, the chip-on-board (COB) technology is one of the favourite candidates for developing customized and thermal-efficient LEDs [2].

Beyond the thermal efficiency, one of the key performance criteria of a LED light source is its optical efficiency. This efficiency comprises several components [3]. The first one is the “internal quantum efficiency”. It is defined as the ratio between the number of photons emitted from the active region per second and the number of electrons injected into the LED per second. It describes the LED junction performance.

In this paper, we focus on the second component of this efficiency: the “light extraction efficiency”. It is defined as the ratio between the number of photons emitted into free space per second and the number of photons emitted from the active region per second. At the die level, this efficiency is limited by the total internal reflexions which appear at the interface between the semiconductor material and the air due to their refractive index mismatch. It may be improved either by structuring the die surface [4, 5] and/or by packaging the die with dome-shaped encapsulants with a high refractive index [6]. At the package level, the extraction is limited by the losses which may occur during light propagation within the package. A lot of work has been done to reduce these losses and to optimize the light extraction of a packaged LED. This included adjusting the encapsulation refractive index [7], inserting a reflective part around the light-emitting element [8, 9], or optimizing the exit surface shape of the package [9, 10].

However, in a COB module, an important point is to keep a simple realization process, which allows both cost reduction and performance. In order to reach this target and to optimize the module performances, the parameters which are easier to modify are the encapsulation shape and the volume. Several studies have already been performed to evaluate the impact of the encapsulation on the light extraction [11, 12]. Nevertheless, to our knowledge, these works stayed at the theoretical stage, and they were not demonstrated experimentally.

That is why we propose in this paper to combine both a ray-tracing and an experimental approach for optimizing the light extraction and intensity distribution of a LED COB module. Thanks to the Monte-Carlo ray-tracing simulations, we have determined the encapsulation shape and the volume allowing to maximize light extraction. Then, the originality of this study is that these results have been correlated with experimental measurements done on COB samples, which were made from a 1 mm² LED die encapsulated with silicone. The experimental results are found to be in good agreement with the simulations.

2. Simulations

In order to determine the parameters which are critical for the LED COB encapsulation performance, we have developed a simulation model which calculates the amount of light extracted from a blue light-emitting die depending on the shape and on the size of its encapsulation.

We have used the Zemax software, which is based on the Monte-Carlo ray-tracing. The typical LED COB geometry includes a  mm² GaN LED die (refractive index: for a 450 nm incident wavelength) on a large board. Then, the die emission has been modelled as a lambertian intensity distribution. The light-emitting wavelength has been fixed equal to 450 nm, which is close to the typical wavelength of Royal Blue LEDs. For simplicity reasons, we have also chosen not to take into account the die roughness in these simulations. As will be detailed later, this does not impact the trend of the results, but it implies to carefully analyse them. Then, the board has been considered as a reflective element. In order to reproduce the behaviour of the printed circuit board (PCB) which will be used for the comparative experimental tests and which comprises a white solder mask, we have fixed its reflectivity to 70% with a surface lambertian diffusion. Finally, this module has been covered with a silicone encapsulation ( for a 450 nm incident wavelength), whose shape and size have been modified as depicted in Figure 1. H is the height, and R is the radius of the encapsulation.

Figure 1: Cross-sections of the geometries which have been modelled for evaluating the impact of the encapsulation shape and size on a LED COB performance. (a) Nearly flat encapsulation, with an aspect ratio H/R of 0.3; (b) hemispherical encapsulation; (c) oblong encapsulation, with an aspect ratio H/R = 1.7.

The encapsulation shape has been set as half-ellipsoidal, with an aspect ratio “height above radius” H/R varying from 0.3 (flat encapsulation) to 1.7 (oblong encapsulation). Thus, depending on the shape, the volume of the encapsulation varies accordingly from about 1 mm3 to 70 mm3, which allows observing simultaneously the effect of the shape and of the volume on the module optical characteristics.

Regarding the simulation analysis, this model does not take into account the die roughness as stated above. This does not significantly change the results since both the LED plane surface and a roughened surface have a lambertian distribution. However, it implies that the analysis has to be done by only comparing the results among themselves. Thus, we have normalized the light extraction values which have been obtained through the simulations as follows: where is the light extraction efficiency of the considered geometry and is the light extraction efficiency of a reference case. This reference has been arbitrarily chosen to be a hemispherical encapsulation with a radius R of 1.4 mm.

Then, we have plotted this calculated gain or loss in light extraction depending on the volume and on the aspect ratio of the encapsulation. The corresponding results are given in Figure 2.

Figure 2: Variation of the light extraction of a LED COB module, depending on the volume and on the aspect ratio of the LED die silicone encapsulation (simulation results).

First, the graph clearly evidences that, due to a high amount of total internal reflexions within the encapsulation, a flat encapsulation shape (H/R < 0.7) ever provides a bad light extraction. This is in agreement with previous works [8] which were done for packaged LEDs, where it was shown that a hemispherical dome gave better extraction results than a flat or convex encapsulation shape.

Our simulation results also indicate that, above an aspect ratio H/R of 0.7, the shape of the encapsulation has a small impact on the light extraction and that even an oblong shape may provide an efficient LED COB module. This was also observed in recent works [12] on silicon-based LED packaging. Indeed, above a certain aspect ratio, the ray incident angles at the silicone-air interface are small enough to limit the total internal reflexions. Thus, these rays will always be able to escape from the encapsulation, maintaining the light extraction quite stable.

Then, regarding the impact of the encapsulation volume, previous works have shown that the light extraction stabilized from an encapsulation radius larger than 1.5, where is the die size [10]. In our model configuration, the die size is  mm. Thus, a hemispherical encapsulation such as approximately represents a volume of 7 mm3. Our simulations are also effectively in line with these results. More generally, our computations evidence that, above a silicone volume of 5 to 10 mm3, the light extraction efficiency of the COB module remains quite stable and rather independent of the encapsulation shape. However, for small silicone volumes, the hemispherical encapsulation shape is the most efficient geometry.

Finally, we have studied the impact of the LED COB encapsulation shape on the light intensity distribution. By inserting a far-field intensity detector in the simulation model, we have collected the angular flux emitted by the COB geometry. The light intensity distribution is plotted in Figure 3 for an encapsulation radius of 2.3 mm.

Figure 3: Light intensity distributions provided by a LED COB module depending on the shape of its encapsulation (simulation results). The encapsulation radius is 2.3 mm.

As it is currently done for packaged LED components, the graph evidences that giving a specific shape to the LED COB encapsulation allows beam shaping. Indeed, inserting an oblong-shape encapsulation implies that light rays impacting the silicone-air interface will mainly be extracted along small angles. This will lead to a sharp and narrow intensity distribution, as it is depicted by the simulation curve representing the high aspect ratio H/R = 1.7. On the contrary, making a hemispherical or flat encapsulation favours light angular dispersion at the silicone-air interface, which will provide a rather lambertian distribution.

These theoretical studies indicate that the optimal optical performances for a LED COB module will be obtained with a geometry combining a rather high encapsulation volume (larger than 5 mm3) and a hemispherical shape. An oblong shape may also be considered for applications which require strong narrow beams.

3. Experiments

In order to validate the simulation results which have been presented above and to evaluate the potential of such encapsulation shapes and volumes for improving the performances of LED COB modules, we have mounted several LED dies in a COB configuration. Then, we have performed different tests on these modules to check their optical characteristics. A top view of one of these modules (microscopic imaging) is shown in Figure 4.

Figure 4: Top view of one LED COB module.

The modules include a SemiLEDS LED die of  mm² surface area with a typical dominant wavelength equal to 462.5 nm (reference SL-V-B40AC2, with a typical radiant flux at 350 mA of 350 mW). The LED die has been mounted on a “star” PCB with a silver paste adhesive (Epoxy Technology, reference EPOTEK H20E-HC).

Encapsulation was carried out using a dispensing process with silicone from NuSil, having a refractive index for blue-range incident wavelengths. Volume and shape have been adjusted by varying the dispensing parameters.

Finally, we have used a integrating sphere coupled to a spectrophotometer from LabSphere (SphereOptics) to measure the radiant flux of these encapsulated modules. In order to be able to compare the experimental results with the ray-tracing simulations which were detailed in the previous section, we have followed the same analysis procedure (see (1)). First, we have calculated the light extraction of each module by doing the ratio between the radiant fluxes emitted by the system after and before encapsulation. Then, we have chosen a sample, which presents a hemispherical encapsulation of 2 mm radius, and we have set its light extraction value as reference for the others. Finally, we have normalized all of the sample extraction values to this reference case, and we have plotted the graph which is given in Figure 5. It has to be noted that, due to the different geometries of the two reference samples which have been taken for analysing the experimental and the simulation results (encapsulation radius of 2 mm versus 1.4 mm for the simulations), the maximal gain of light extraction is different between these two graphs.

Figure 5: Gain of light extraction as a function of the encapsulation volume for various H/R ratio (experimental results).

First, the graph confirms the simulation results which stipulated that a flat encapsulation never provides a good light extraction. Whatever the encapsulation volume is, the samples which present an aspect ratio H/R smaller than 0.6 all lead to a poor light extraction. In addition, the absolute values of light extraction measured for these samples (not shown in the graph) also indicate that the radiant flux emitted by some of these modules is even lower than the initial flux of 350 mW emitted by the LED die without silicone encapsulation.

Then, the measurement dispersion is also larger than the simulated one. This is mainly due to the fact that the encapsulation shapes are not always ellipsoidal as it was modelled in the simulations. Indeed, we found that some of them present a ball-shape (diameter at the contact interface of the PCB lower than the encapsulation diameter). Such shapes, which appear to be a consequence of our manual dispense process, may effectively influence the light extraction efficiency of the COB modules. In order to check this phenomenon, we have chosen two of our samples, and we have performed additional simulations by modelling their real encapsulation shapes. The results are summarized in Table 1. The results of the simulations done with ellipsoidal encapsulation shapes of similar volumes are also given. For comparison, the light extraction obtained with these ellipsoidal encapsulations was arbitrarily normalized to 1, and it has been taken as reference for the simulations of the ball-shape encapsulations.

Table 1: Comparative light extraction efficiencies for COB modules, depending on their encapsulation shapes (ellipsoidal or ball-shape).

These simulations evidence that ball shapes improve the light extraction efficiency of several percents compared to an ellipsoidal encapsulation of similar volume. Thus, an encapsulation shape variation may effectively be at the origin of the measurement dispersion compared to simulation results.

Nevertheless, these light extraction measurements generally show the same trend than the one which was observed with the simulations. For instance, when considering the small-volume encapsulations, the light extraction rather increases with the silicone volume.

Finally, among the different modules which were realized, the maximal light extraction is obtained for a rather hemispherical encapsulation, with a volume of about 15 mm3. This is in line with the simulation results, which predicted a stabilization of the light extraction at its optimum with encapsulation volumes larger than 10 mm3. We have measured the radiant flux emitted by this module: we found a light extraction value of about 30% compared to the radiant flux emitted by LED die without silicone, which is of the same order than the light extraction gains which have been measured for silicone packaged LEDs [13]. Thus, this confirms the potential of COB technology for providing high-efficient LED light sources.

In order to check the impact of the encapsulation shape on the module intensity distribution, we have also performed angular measurements with a LED spectrogoniometer to obtain the light intensity distribution of the modules depending on their encapsulation aspect ratio. The results are shown in Figure 6.

Figure 6: Light intensity distributions provided by a LED COB module depending on the shape of its encapsulation (experimental results).

This graph confirms experimentally the phenomena which were observed in simulations. The modules which were encapsulated with an oblong encapsulation shape (H/R > 1) provide a sharper and narrower distribution than the modules covered with a lower aspect ratio encapsulation: this evidences that light extraction at small exit angles is favoured. As theoretically expected, the hemispherical and encapsulation shapes rather provide lambertian distributions.

4. Conclusions

In this paper, we have studied theoretically and experimentally the impact of the encapsulation shape and the volume of a LED COB module on its performances, in terms of both light extraction and intensity distribution. We have shown that flat encapsulation shapes never provide an efficient COB light source, while hemispherical encapsulation shapes lead to lambertian distributions with a light extraction gain which is rather independent of the encapsulation shape above volumes of 10 mm3. Despite providing more dispersed data due to the process parameter variations, the experiments confirmed the simulation results. Presenting up to a 30% encapsulation gain in light extraction, they evidenced that the optimal performances are obtained with a nearly hemispherical encapsulation, with a volume for a 1 mm² LED die larger than 5 to 10 mm3. This work is seen to gain an insight into the potential of LED COB modules for providing high-efficient and custom light sources. Next studies will be devoted to apply these results to white modules and to optimize the insertion of phosphors particles within the encapsulation to obtain efficient white LED COB light sources.


The authors would like to gratefully acknowledge NEOLUX (La Chapelle-Vendômoise, France) and BEST (Gevrey-Chambertin, France) for partially funding this study.


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