Advances in Materials Science and Engineering

Advances in Materials Science and Engineering / 2018 / Article

Research Article | Open Access

Volume 2018 |Article ID 8097841 | 11 pages |

Design and Modeling of the Photonic Crystal Waveguide Structure for Heat-Assisted Magnetic Recording

Academic Editor: Andres Sotelo
Received07 Dec 2017
Accepted10 Jan 2018
Published28 Feb 2018


The application of the photonic crystal (PC) waveguide (WG) as the light delivery system in the heat-assisted magnetic recording (HAMR) system is demonstrated. The structure consists of a 90° bending PC waveguide and a ridge dielectric waveguide taper coupler. Three-dimensional (3D) models of structures are built and simulated in order to determine light coupling and transmission efficiencies. Geometric parameters including the taper length (LTP), coupler inlet width (WFW), and PC waveguide width (WWG) are investigated. The initial simulation shows that the transmission efficiency of over 90% can be achieved with the coupler integrated with the straight PC waveguide. However, the overall transmission efficiency is substantially reduced to 53.8% when the coupler is attached to the 90° bending PC waveguide. Our analysis shows that the wave mode matching and light decay rate in the waveguide cavity are significant contributing factors. The transmission efficiency increases to around 60.8% after some modification of the bending region.

1. Introduction

Photonic crystals (PCs) are periodical optical micro- and nanostructures that receive increasing attention due to their ability to manipulate light propagation while maintaining high transmission efficiency. They are typically designed based on their energy band gap to prohibit certain wavelengths. They can be arranged in one dimension (1D) [1, 2], two dimensions (2D) [35], and three dimensions (3D) depending on guiding requirements. The 2D PC structure is the most popular choice for optical devices and has found various applications such as integrated circuits (ICs), wave filters or multiplexers, and waveguides [613]. The PC’s excellent transmission properties [1416] and physical flexibility are attractive to minuscule WG fabrication. It can be bent to fit in a limited space and still achieve desirable performance [14, 15, 1719]. A significant enhancement in operating bandwidth [18, 19] has also been reported.

Coupling is an important issue when it comes to the WG integration with other components of an optical communication device. Several taper PC coupling structures were investigated [2023]. These studies agree on one common fact that the light propagation depends largely on the geometries of the coupler and guiding structure.

The capability of the PC to manipulate light as described above suggests the use of the PC structure as a potential candidate for light delivery in the heat-assisted magnetic recording (HAMR) system [24]. Several HAMR light delivery systems have been proposed, for example, the structure consisting of grating, slab waveguide, and near-field transducer (NFT) [24], the fiber optic connected with a spot-size converter (SSC) [25], and the butt-grating structure associated with multilayer core and cladding [26]. These proposed light deliveries, however, suffer from power losses at different locations and produce less than 50% transmission efficiency.

In this paper, the photonic crystal waveguide for the light delivery in HAMR is demonstrated. The proposed structure shown in Figure 1 replaces the conventional structure [24] by combining grating, slab waveguide, and fixed curve mirror into a single piece through utilizing of coupling and bending sections. Note that the NFT is not included in the proposed design. The PC waveguide is attached at the front of the slider. The light path can be guided directly to the waveguide via the coupler at the inlet, and the fixed curve mirror is thus not required [24, 27, 28]. The light is then guided via a 90° bend and propagates in the straight guiding section to the output.

The 3-dimensional (3D) design of the 2D PC waveguide is carried out using the basic Photonic Band Gap (PBG) software [29]. The modeling is performed with the widely used finite element method (FEM) simulator COMSOL Multiphysics [30]. The performances of the waveguide including transmission and coupling efficiencies through bending and coupling sections are investigated.

2. Photonic Band Gap (PBG)

The 2D photonic crystal structure is the dielectric constant periodically modulated in two dimensions. In this paper, our PC waveguide is operated at 1,550 nm [31], and our PC waveguide is constructed using a 2D triangular lattice array of air holes embedded in polysilicon (p-Si). At this wavelength, the frequency-dependent refractive index of p-Si is 3.476 [9]. This structure is preferred since its band gap contains a larger overlapping area than other PC lattices and can be associated with both transverse electric (TE) and transverse magnetic (TM) modes. A simple laser source can thus be utilized without the need for a mode selector. Moreover, silicon has high refractive index and exhibits low loss at the wavelength of interest [32]. Note that if the NFT is included in the design, the waveguide must possess a certain polarization as most NFTs are polarization specific.

The PBG diagram is created by calculating each PBG, the forbidden wavelength range for propagation, associated with a specified ratio of air hole radius (r) and lattice constant (a). The consolidation of band gaps can be depicted by the gap map shown in Figure 2(a). The selected ratio of radius and lattice space constant (r/a) is 0.43, a relatively low value in the overlapping area known as the complete band [6]. A lower r/a ratio is desirable in order to prevent structure collapse during fabrication. The calculated photonic band diagram of the lattice with r/a = 0.43 is shown in Figure 2(b). In this figure, the normalized frequency is plotted versus the wave vector into the lattice (Γ, M, and K). The calculations show that the band gap width is about 49.45% (from 0.276 to 0.458) for the TE mode and 5.12% (from 0.385 to 0.406) for the TM mode, respectively. An overlapping area with the center normalized frequency (ωa/2πc) is chosen at 0.395.

The radius of the air hole (r) and lattice space constant (a) are determined by the following relation:where ω is the angular frequency (rad/s), c is the light velocity (m/s), and λ is the wavelength (m).

Therefore, the air hole radius (r) and the lattice space constant (a) are 263 and 612 nm, respectively.

3. Design and Modeling of the PC Waveguide for HAMR

The PC waveguide is designed as a slab waveguide with coupling and bending sections. The 3D model and light path are shown in Figures 3 and 4, respectively. The coupling efficiencies associated with different coupling structures will be determined first. After the integration of the bending section, they will be reevaluated along with the transmission efficiencies.

The length of the PC waveguide is about 24.48 (40a) µm, and there are 21 rows in the air hole array. The PC guiding path is created by removing a center row. The slab thickness (t) of the PC waveguide is chosen at 0.4a or around 245 nm. This thickness value is determined following the relation between the gap size and the PC thickness described in [33]. The taper section is formed by a conventional ridge dielectric slab waveguide whose thickness can be expressed as follows [34, 35]:where h is the dielectric taper slab thickness (m) and n1 is the core material (silicon) refractive index.

At the operating wavelength of 1,550 nm, the thickness of the taper slab is around 245 nm (t/a = 0.4), similar to the thickness of the PC slab.

3.1. Ridge Dielectric Taper Coupler Integrated with the Straight PC Waveguide Structure

We perform an initial simulation to observe light coupling into the straight PC waveguide from a ridge dielectric taper coupler shown in Figure 5. The taper coupler is an inlet width converter that is employed to convert the large inlet to the smaller one. The ridge dielectric waveguide taper structure, in particular, is simple and easy to fabricate [36].

The coupler inlet width (WFW) and the taper length (LTP) are varied from 5 to 30 µm. Note that the initial coupler inlet width of 5 µm is selected based on the actual size of a typical fiber optic outlet. A parametric study is performed to observe the dependence of the coupling efficiency on the coupler inlet width (WFW) and taper length (LTP). Two sizes of the PC waveguide inlet width (WWG) are considered which are 0.8a√3 and 1.0a√3 (about 0.848 and 1.060 µm). The former is selected to demonstrate the extreme case of coupling. The PC waveguide length (LWG) is 24.48 µm (40a), and the waveguide slab thickness is 0.245 µm (0.4a). However, the computed power distribution is displayed as the net power. In order to accurately determine the coupling efficiency or the transmission efficiency over the coupler, values of incoming and reflected powers are needed. The coupling efficiency can be calculated from power density integration over the cross-sectional plane at the input (Pin = Psource + Preflection) and output (Pout = Ptransmission) ports of the coupler. The transmission T is determined by T = 2Pout/(Pin + Pout) = Ptransmission/Psource, whereby we assume Psource = Preflection + Ptransmission [37]. Pout is the surface integration of power densities over the cross-sectional plane at the output port (point B in Figure 5), and Pin is the surface integration of power densities over the cross-sectional plane at the input port (point A in Figure 5). The input power is set at 1 mW for convenience. Note that these formulas can be applied to any kind of waveguiding structures.

Figure 6 shows the coupling efficiency profiles with WWG equal to 0.8a√3 and 1.0a√3, respectively. It can be seen that the coupling efficiency decreases as the taper length increases. At WWG = 0.8a√3, the maximum efficiency of 95.3% is achieved with WFW = 10 µm and LTP = 5 µm, as shown in Figure 6(a). The power density distribution associated with peak coupling efficiency is depicted on the right. The coupling efficiencies obtained from other structures are much lower and stay between 30 and 45%.

The results are however different for WWG = 1.0a√3 as shown in Figure 6(b). It is observed that there are 3 structures that can achieve over 90% coupling efficiency, that is, WFW = 15 µm and LTP = 5 µm, WFW = 25 µm and LTP = 5 µm, and WFW = 30 µm and LTP = 5 µm, respectively. The smaller the LTP, the better the coupler efficiency. At higher taper lengths, the bell-shaped profiles are observed. In our case, the good matching condition appears at smaller taper lengths. The power density distribution of the WFW = 25 µm and LTP = 5 µm structure is shown on the right of Figure 6(b). Compared to the WWG = 0.8a√3 PC structure, the WWG = 1.0a√3 structure provides better overall coupling efficiency. It is believed that a certain amount of power loss occurs from a reflection at the inlet of the PC waveguide. From the PC design standpoint, a bending section with a narrow inlet is difficult to construct. Therefore, the WWG = 1.0a√3 structure is selected for further study.

3.2. Ridge Dielectric Taper Coupler Integrated with the Bending PC Waveguide Structure

The ridge dielectric taper coupler is integrated with the 90° bending PC slab waveguide to form the light delivery structure of HAMR as shown in Figure 7. The dimension of the 90° bending PC slab waveguide includes 50 µm of width (w) and 55 µm of length (l). Unfortunately, we cannot enlarge the waveguide dimension due to processing limitations. A number of periodic structures in the horizontal and vertical planes are 40 and 80 periods, respectively.

The transmission efficiencies are determined at 3 locations, shown as points B, C, and D in Figure 7. These efficiencies are defined by ratios of power flows at the locations of interest and powers at the inputs. The coupling efficiency, transmission efficiency after the bending section, and the overall waveguide transmission efficiency are expressed by

Referring to Figure 7, PA is the power over the cross-sectional surface at point A (Watt), PB is the power over the cross-sectional surface at point B (Watt), PC is the power over the cross-sectional surface at point C (Watt), and PD is the power over the cross-sectional surface at point D (Watt).

Figure 8(a) shows the plot of the taper coupling efficiency (CT) where WFW is varied from 5 to 30 µm and LTP is varied from 2 to 30 µm. All structures exhibit bell-shaped efficiency profiles as a result of reflection and scattering in the guiding bodies at certain geometries. These findings indicate the strong dependence of the light transmission on the geometry. The highest CT of 97.2% is achieved with the WFW = 15 µm and LTP = 5 µm structure. However, the highest overall efficiency is achieved with the WFW = 5 µm and LTP = 10 µm structure. Figures 8(b) and 8(c) show the plots of the bending transmission efficiency (CB) and overall transmission efficiency (CO), respectively. We observe that, for every case, the efficiency decreases along the waveguide; moreover, it drops substantially after the bending section. The maximum overall efficiency is achieved at around 53.8% with the WFW = 5 µm and LTP = 10 µm structure.

The coupling behavior of the proposed structure is analyzed as follows. According to the coupled-mode theory [38], the wave mode profiles of the ridge dielectric taper waveguide and PC waveguide must be matched in order to optimize the transmission. Some researchers have reported applications of the taper waveguide as a wave mode converter [3941]. We then calculate the wave mode profiles displayed in terms of electric field distributions of a single piece of the ridge dielectric taper waveguide with WFW and LTP both varying from 5 to 30 µm, with a 5 µm increment, followed by those of a single-piece PC waveguide. Note that the wave mode profiles are determined at the outlet of the ridge taper waveguide and at the input of the PC waveguide.

Our results show that the number of wave mode profiles increases when WFW increases. The second-order wave mode profile of the WFW = 5 µm structure is observed. In particular, we found that the wave mode at the output of the ridge taper waveguide with the WFW = 5 µm and LTP = 10 µm structure exhibits a strong match with that at the input of the PC waveguide, as shown in Figure 9. This result supports the highest value of coupling efficiency achieved for this particular structure.

For comparison, an example of mismatched wave mode profiles is illustrated in Figure 10. This structure has WFW = 10 µm and LTP = 10 µm. The wave mode profile at the output of the ridge taper waveguide is in the third order, while that at the input of the PC waveguide is in the second order. This could explain a nearly 0% efficiency obtained in the coupling section.

Although the matching wave modes between the ridge taper waveguide and PC waveguide can be obtained, power loss in the waveguide is still realized. The well-known concept of temporal coupled-mode theory [33, 42] is then applied to analyze the optical phenomena inside the light delivery structure. We construct the equivalent diagram of the light delivery structure as shown in Figure 11.

The light delivery structure can be separated into two regions. Region one is the ridge dielectric taper coupler waveguide (WG1) connected with PC waveguide (WG2). Region two is the horizontal PC waveguide (WG2) connected with vertical PC waveguide (WG3) to form a 90° bending. Region one is considered first. When the light I1 reaches WG2, some part will be reflected and some will be radiated away due to the difference between WG1 and WG2. The reflected and transmitted waves in WG1 are denoted as R1 and T1, respectively.

According to the temporal coupled-mode theory, the cavity that connects WG1 and WG2 is considered as the resonator. Ideally, if the cavity resonates with a frequency (ω0) equal to the operating frequency (ω) and light decays into WG1 and WG2 with equal lifetimes τ1 = τ2, 100% transmission can be achieved. Note that the resonant frequency and decay rate of the cavity-resonant mode strongly depend on geometry [33, 43, 44]. Therefore, the geometry of the cavity should be modified to increase the coupling between WG1 and WG2. For region two, another cavity is formed between WG2 and WG3. Again, to achieve 100% transmission efficiency over this section, the abovementioned conditions must be applied.

The improvement of cavity matching is then demonstrated here. Several modifying patterns of the WFW = 5 µm and LTP = 10 µm structure are created by randomly removing some air holes near the joint and corner. Figure 12(a) shows the location of air hole removal, where hij is the coordinate of removed hole position at the joint between the taper and PC waveguide for i = j = {1, 2, 3, 4}. The location of removed air holes around the corner is depicted in Figure 12(b). More than 30 cases are run, and the six best cases are selected and shown in Figure 13. The coupling and bending transmission efficiencies are displayed in the figure.

It can be seen that the coupling and bending transmission efficiencies of the PC waveguide structure can actually be improved when joints and corners are modified. In our 6 best cases, MOD#5 provides the highest efficiency. Specifically, CT, CB, and CO increase from 88.6% to 97.2%, 59.8% to 72.2%, and 53.8% to 60.8%, respectively. Note that the obtained overall transmission efficiency from the MOD#5 case is better than those reported previously [2426]. To further improve the transmission efficiency, a systematic approach should be implemented. In addition, deformation of some air holes might be necessary [13].

Finally, the hotspot size at the output facet of the WFW = 5 µm and LTP = 10 µm structure is determined. The power distribution at the output facet of the structure is shown in Figure 14. By considering the full width half maximum (FWHM) of the power distribution profile, we obtain a spot size of about 103 nm × 413 nm. This spot size is still too large for high areal density recording. More alteration of air holes near the output or NFT integration is recommended for further confinement of the spot size.

4. Conclusions

This paper investigates a PC waveguide-based light delivery system for HAMR. We examined taper coupling and bending structures. The PC waveguide model is created by removing a single row of photonic crystals in a triangular lattice array of air holes in the silicon substrate. The PC waveguide operates at 1,550 nm and can accommodate both TM- and TE-polarized sources. The lattice space (a) and air hole radius (r) are 612 and 263 nm, respectively. The dielectric coupler model is designed by varying the inlet waveguide width (WFW) and the taper length (LTP) from 5 to 30 μm. The PC waveguide widths of interest are 0.8a√3 or 0.848 µm and 1.0a√3 or 1.060 μm. The dielectric taper coupler integrated with the straight PC waveguide structure shows the highest coupling efficiency of 95.3% with the WFW = 10 µm, LTP = 5 µm, and WWG = 0.8a√3 µm structure. For WWG = 1.0a√3 µm, there are 3 structures with LTP = 5 µm that achieve over 90% coupling efficiency, that is, 94.6% for WFW = 15 µm, 97.4% for WFW = 25 µm, and 90.8% for WFW = 30 µm. The 1.0a√3 µm width is chosen for integration with the 90° bending structure to form the proposed light delivery structure since it provides larger guiding area at the bending section.

The coupling efficiencies of most structures drop slightly after attaching the bending structures. The overall highest CT is achieved at LTP = 5 µm. The bell-shaped profiles are observed in every case of WFW. These results indicate that the effects of light reflection and scattering are altered in different guiding geometries, and the optimization of waveguide geometry is necessary. The transmission efficiency apparently decreases along the waveguide. The maximum overall efficiency of around CO = 53.8% is achieved with the WFW = 5 µm and LTP = 10 µm structure.

Different dimensions of the ridge dielectric coupler taper waveguides produce varied output wave modes that affect the matching to the PC waveguide. Modification of air holes at the joint and corner of the PC waveguide of the WFW = 5 µm and LTP = 10 µm structure appears to improve the efficiencies at the taper coupler section and the overall structure. The optimal coupling and overall transmission efficiencies increase to 97.2% and 60.8%, respectively. These efficiency levels are definitely sufficient, considering our simple design and fabrication [36]. In addition, the value of the overall transmission efficiency is better than those reported previously. The PC waveguide is therefore a promising candidate for the HAMR light delivery system. However, more alteration of air holes near the output or NFT integration is recommended to further confine the spot size.

Conflicts of Interest

The authors declare that they have no conflicts of interest.


The authors would like to thank King Mongkut’s University of Technology Thonburi and Seagate Technology (Thailand) Co., Ltd., for supporting this work. In addition, the authors would like to acknowledge the financial support to this work received from the NSTDA University Industrial Research Collaboration (NUI-RC) and National Science and Technology Development Agency.


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Copyright © 2018 Orrathai Watcharakitchakorn and Rardchawadee Silapunt. 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.

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