Visible Wavelength Photonic Insulator for Enhancing LED Light Emission
Visible Wavelength Photonic Insulator for Enhancing LED Light Emission
Journal of information and communication convergence engineering. 2015. Mar, 13(1): 50-55
Copyright © 2015, The Korean Institute of Information and Commucation Engineering
This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License ( which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
  • Received : October 20, 2014
  • Accepted : December 08, 2014
  • Published : March 31, 2015
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About the Authors
Kwangki, Ryoo
Department of Information & Communication Engineering, Hanbat National University, Daejeon 305-729, Korea
Jeong Bong, Lee
Department of Electrical Engineering, University of Texas at Dallas, Richardson, TX 75083, USA

We report design and simulation of a two-dimensional (2D) silicon-based nanophotonic crystal as an optical insulator to enhance the light emission efficiency of light-emitting diodes (LEDs). The device was designed in a manner that a triangular array silicon photonic crystal light insulator has a square trench in the middle where LED can be placed. By varying the normalized radius in the range of 0.3–0.5 using plane wave expansion method (PWEM), we found that the normalized radius of 0.45 creates a large band gap for transverse electric (TE) polarization. Subsequently a series of light propagation simulation were carried out using 2D and three-dimensional (3D) finite-difference time-domain (FDTD). The designed silicon-based light insulator device shows optical characteristics of a region in which light propagation was forbidden in the horizontal plane for TE light with most of the visible light spectrum in the wavelength range of 450 nm to 600 nm.
Since the seminal work reported by Yablonovitch [1] in 1987, photonic crystals [2 , 3] have attracted considerable research interest in various fields of study. Photonic crystals are artificial structures in which different dielectric materials are arranged to form periodically varying dielectric constants throughout the structures. It has been demonstrated that photonic crystals are capable of generating, manipulating, and detecting electromagnetic waves [3] . Such artificially created periodically arranged photonic crystals show many unique phenomena that cannot be seen in conventional natural materials. Some of these unique phenomena include negative refraction [4 , 5] , super-lensing [6 , 7] , super-prism [8 , 9] , sharply bent waveguide [10] , and slow light [11] . Many theoretical and experimental works have been carried out by numerous investigators to study these unique phenomena and apply these phenomena to a variety of unique applications.
In the past two decades or so, light-emitting diodes have become an essential technology for a variety of display applications, and their application has been extended to general indoor and outdoor lighting as well [12 , 13] due to their small size, long life, and high efficiency. However, high light extraction efficiency is desirable as the light emitted from LEDs has a tendency to propagate in any direction. An appropriately designed photonic crystal can function as a photonic insulator for a designated polarization and wavelength range of light. This characteristic of photonic crystals can be applied to enhance the light intensity in certain directions. There have been several investigations to enhance the light extraction of LEDs by using photonic crystals. In order to increase light extraction efficiency and achieve fabrication simplicity, photonic crystals have been typically directly fabricated on III-nitride LEDs [14] .
In this paper, we report the design of a silicon-based photonic crystal that can be independently fabricated in silicon by utilizing a well-established silicon-based technology. An LED die irrespective of the material can be placed in the fabricated silicon-based photonic crystal to enhance the light extraction efficiency.
As the light wave propagates inside the photonic crystal, due to the periodic arrangement of the dielectric materials (periodic potential), the light wave experiences multiple scatterings and interferences from various periodic layers. Due to the constructive and destructive interferences in the light traveling path, the amplitude of the propagating light can be increased or decreased depending upon the wavelength and propagation direction of the light. According to the Bloch wave theory, only light modes with a certain eigenfrequency are allowed in the photonic crystal with a certain wave vector. By plotting all of the allowed eigenmodes in the format of eigenfrequency versus wave vector, we can create a photonic band diagram. A photonic band gap can be formed when none of the allowed eigenmodes exist in a certain frequency range. This photonic band gap can be used to appropriately design a photonic insulator in a certain wavelength range.
Theoretically, on the basis of Maxwell’s equation, we can describe the photon behavior in a periodically arranged photonic crystal device with a time-varying magnetic field as follows [3] :
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where ε ( r ) denotes the relative permittivity; H ( r ), the timevarying magnetic field; ω , the radial frequency; and c, the speed of light. By correlating the dielectric constant ε ( r ) information and solving for the eigenvalue, we can obtain the eigenvalue for ( ω / c ) 2 . This eigenvalue along with the wave vector forms the photonic band diagram.
The plane-wave expansion method (PWEM) solves eigenvalue problems for electromagnetic waves with a periodical potential. PWEM is aneffective method for generating photonic band dispersion diagrams and equifrequency contours for periodic structures. The method expands the unit cell of the periodic dielectric constant function ε ( r ) and the periodic part of the Bloch wave function by the Fourier series and reassembles them in the wave equation of the electromagnetic wave. By solving the expanded wave equation numerically, the photonic band dispersion diagram and the equifrequency surface/contour can be obtained. Since photonic crystals are periodic structures, the relative dielectric constant ε ( r ) is also periodic. The periodicity of ε ( r ) can be expressed as ε ( r ) = ε ( r + A ), where A denotes the lattice vector of the photonic crystal. Lattice vector A can be expressed in terms of the elementary lattice vectors of the photonic crystal. Since ε ( r ) is a periodic function, ε ( r ) -1 can be expanded by the Fourier series as follows:
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where T denotes the reciprocal lattice vector and β ( T ), the expansion coefficient for ε ( r ) -1 , which could be calculated by an inverse Fourier transform. By applying the Bloch wave theorem to magnetic field H ( r ) and plugging into Eq. (1), we can obtain a single eigenvalue equation as follows [15] :
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where k denotes the wave vector in the first Brillouin zone and n represents the band number. By numerically solving Eq. (3), we can obtain the eigenvalues for specific k and n . The photonic band diagram can be obtained using all the calculated eigenvalues.
In photonic crystal design, refractive index is a critical factor since the origin of the photonic crystal is a periodically varying refractive index/dielectric constant. Therefore, obtaining the accurate refractive index value is of utmost importance. Typically for the sake of simplicity and fast calculation, the effective index method is applied to simplify the three-dimensional (3D) modeling of twodimensional (2D) slab photonic crystals into 2D modeling. In other words, the 3D modeling problems of finite-height slab photonic crystals can be converted into 2D photonic crystal problems with infinite thickness. The greatest advantage of this modification is the dramatic reduction of the number of involved elements and the calculation time.
The effective refractive index ( neff ) can be expressed as follows:
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where β denotes the propagation constant of the wave and k represents the wave vector in free space ( / λ ). By solving the electromagnetic wave equation and combining the solution with boundary conditions at the interfaces of different refractive index media, we can obtain the wave propagation constant. Thus, we can calculate the effective refractive index. There is an increasing chance for multimode existence, as the thickness of the core layer increases. The multimode case is an unwanted scenario in photonic crystal design. As a result, to control the mode number in the optical waveguide, typically, the thickness of the 2D photonic crystal slab is controlled to be under half the wavelength ( λ/2 ) of the propagating electromagnetic wave of interest.
The photonic crystal device was designed to have periodically arranged air-hole structures inside a 2D silicon slab with the thickness of 1 μm and arranged in a triangular lattice. It was designed to be similar to a silicon-on-insulator in that the silicon slab sat on top of a thick SiO 2 layer. The effective refractive indices used for silicon, air, and glass in this design were 3.46, 1.0, and 1.5, respectively. To design the device effectively, we blocked the visible light wavelengths in the range of 400 to 700 nm and used both theoretical calculations and commercially available software PBGLab (EM Photonics, Newark, DE, USA) to calculate the photonic band diagrams and equifrequency surfaces. MATLAB (The MathWorks Inc., Natick, MA, USA) was used as the computation engine for the software.
Several normalized radii ( r / a ) in the range of 0 to 0.5 were tested to find the largest band gap, where r denotes the air-hole radius and a represents the lattice constant for the triangular lattice structure ( Fig. 1 (a)). The reason to search for the largest band gap was that light with its normalized frequency ( a / λ ) lying in the band gap cannot propagate in a photonic crystal structure. At a normalized radius of 0.45, a large band gap was generated by PWEM in the cases of transverse electric (TE) polarization; the band gap was found to be wide enough to design a photonic crystal-based light insulator to cover almost the entire visible light wavelength range. As the photonic band diagram shows an eigenfrequency as a function of the Bloch wave vectors in the first Brillouin zone, Fig. 1 (b) shows the photonic band diagram for the designed 2D air-hole triangular lattice photonic crystal generated by PWEM with the normalized radius of 0.45. In the figure, the band gap lies in the normalized frequency ( a / λ ) range of around 0.3 to 0.47. In order to let the entire visible light wavelength range lie inside the band gap, we selected a triangular lattice constant of 200 nm. Consequently, the air-hole diameter was set to be 180 nm.
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(a) A schematic showing a triangular lattice photonic crystal structure (r denotes the radius of the air-hole and a represents the lattice constant), (b) dispersion diagram for the 2D slab silicon photonic crystal for a visible-wavelength LED application.
Fig. 2 shows a 3D view of the silicon-based photonic crystal light insulator structure. The silicon slab with airhole arrays sits on top of the glass substrate. The LED is placed in the center of the square trench in the 2D silicon photonic crystal slab and the light emitted from the LED needs to be guided to emit in the perpendicular direction as the silicon photonic crystal structure functions as a light insulator in the horizontal direction.
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3D view of the designed silicon-based triangular lattice light insulator for visible light wavelengths.
Based on the design parameter achieved by using the PWEM, the 2D and 3D finite-difference time-domain (FDTD) methods were used to find the light propagation characteristics of the device. The simulations were carried out using commercially available software EMPLab (EM Photonics). In the 2D FDTD simulation, a light source with the wavelength of 400, 450, 500, 550, 600, or 650 nm was placed at the center of the square trench where the LED would be placed.
Fig. 3 (a) shows the top view of the light propagation characteristic of the device with 400-nm-wavelength light, which clearly shows that some portion of the light leaks in the horizontal direction. However, as the wavelength increases (450–600 nm), as shown in Figs. 3 (b)–(e), light propagation in the horizontal direction at these wavelengths was nearly completely blocked and there was no sign of light leakage in the photonic crystal structure. This result clearly shows that the designed photonic crystal device functions as a light insulator for most of the visible light wavelengths in the range of 450–600 nm in the horizontal direction. When the wavelength was increased to 650 nm ( Fig. 3 (f)), light leakage resumed.
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2D finite-difference time-domain simulation results for various visible light wavelengths: (a) 400 nm, (b) 450 nm, (c) 500 nm, (d) 550 nm, (e) 600 nm, and (f) 650 nm.
To verify the 2D FDTD simulation results, a 3D FDTD simulation was also carried out. Fig. 4 shows the 3D FDTD simulation result with the point light source wavelength of 500 nm. The result clearly shows the strict confinement of the light only in the square trench in the middle of the device, confirming that there was no light leakage in the horizontal direction. This result agrees well with the 2D FDTD simulation result for 500 nm ( Fig. 3 (c)).
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3D finite-difference time-domain simulation result for the 500-nmwavelength point light source placed at the center of the square trench.
In order to quantitatively understand the light leakage characteristics in the horizontal direction, subsequent simulations were carried out with four detectors placed in the four primary directions of light propagation, as shown in Fig. 5 . Again, the light source was placed at the center of the square trench of the device.
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Top view of the device with four detectors (green ‘+’ mark) placed in the primary directions of light propagation. A point light source (red ‘+’ mark) was placed at the center of the device.
Light intensities at the four light detectors were recorded as the wavelength of the light source changed from 400 to 650 nm. Fig. 6 shows the light intensities as a function of the wavelengths. The four different colors represent the light intensity detection results obtained using four different detectors. It was found that the light intensities at all four detectors are very low in the wavelength range of 440 to 590 nm. This ensures that the designed photonic crystal device works properly to block light propagation in the horizontal direction for most of the visible light wavelengths.
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Light intensities as a function of wavelengths in the visible light wavelength range. Four different colors represent the four different light detectors shown in Fig. 5.
A 2D silicon-based photonic crystal device was designed and simulated as a visible wavelength optical insulator package for an LED light enhancement application. Theoretical modeling as well as PWEM computer modeling was carried out to design the photonic crystal to have a broad range of light insulating properties for visible light wavelengths. Both 2D and 3D FDTD computer simulations were carried out to verify the light blocking properties of the designed silicon-based device. Effective light insulation in the horizontal direction all around the device was demonstrated. The simple assembly of an LED die (irrespective of the material used) into an appropriately designed 2D slab silicon photonic crystal will be beneficial for the enhancement of the light emissionefficiency of LEDs. Such a mix-and-match concept will streamline the manufacturing process of LEDs and can be utilized for the fabrication of photonic crystal-based light insulators required for obtaining high light extraction efficiency.
This research was supported in part by The Ministry of Science, ICT and Future Planning, Korea, under the Brain Scouting Program (HB606-12-2001) supervised by the National IT Promotion Agency (NIPA).
Kwangki Ryoo
was born in Kongju, Chungnam Province, Korea. He received his B.S., M.S., and Ph.D. in Electronics Engineering from Hanyang University, Seoul, Korea, in 1986, 1988, and 2000, respectively. He is currently a full professor with the Department of Information and Communication Engineering, Hanbat National University, Daejeon, Korea. From 1991 to 1994, he was a full-time lecturer in the Department of Electronics Engineering at the Korea Military Academy (KMA) and worked as part of the System IC Design team at Electronics and Telecommunications Research Institute (ETRI) from 2000 to 2002. From 2010 to 2011, he was a visiting scholar at the University of Texas at Dallas. His research interests include engineering education, SoC platform design and verification, hardware/software co-design, and multimedia codec design.
Jeong Bong Lee
was born in Seoul, Korea. He received his B.S. in Electronics Engineering from Hanyang University, Seoul, Korea, in 1986, and his M.S. and Ph.D. in Electrical Engineering from Georgia Institute of Technology, Atlanta, Georgia in 1993 and 1997, respectively. He is currently a full professor with the Department of Electrical Engineering, The University of Texas at Dallas, Richardson, Texas. His current research interests include MEMS and nanophotonics. Dr. Lee received the US National Science Foundation CAREER Award in 2001. He served as an executive program subcommittee member for the Transducers 2011 Conference and a program committee member for the Transducers 2013 and IEEE Sensors Conferences. Dr. Lee also serves as an editorial board member for Micromachines Journal, The Scientific World Journal, and Journal of Nanotechnology and Smart Materials.
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