2 August 2012 Design and fabrication of an imprinted wavelength-independent coupler
Author Affiliations +
Optical Engineering, 51(8), 085003 (2012). doi:10.1117/1.OE.51.8.085003
An imprinted polymeric wavelength-independent coupler (WINC), which is one of the core components used in optical fiber communications and fiber-to-the-home systems, was designed with a beam propagation method. Its designed structure has the form of the Mach-Zehnder interferometer. The polymer core size of the WINC was optimized at 8×8  μm using an imprinting technique, the hot embossing process. Optical properties of the polymeric WINC were evaluated by measuring its insertion loss and transmission spectrum. The insertion loss values for channels 1 and 2 were 3.5 and 4.2 dB, respectively, and the transmission spectrum was flat over a range of 1260 to 1640 nm.
Jang, Kim, Kim, and Jeong: Design and fabrication of an imprinted wavelength-independent coupler



Multimedia data, such as that used for voice, text, images, and video, has become essential in our information-oriented society. Recently, the increased demand for these data has called for broadband convergence networks. To construct a high-speed information network, optical communication technology advances into the Tbps domain after the 2010s. This increased demand for high-speed information and communication networks require massive transmission capabilities and super-high-speed switching technologies for optical communications. Fiber-to-the-home (FTTH) systems are gaining strength all over the world and used for an access network for massive multimedia service.1 To use FTTH more efficiently, the wavelength division multiplexing (WDM) method is required, which transmits different wavelengths at constant intervals. Therefore, the FTTH system needs not only optical fibers for data transmission but also photonic components for data distribution, switching, and routing between optical network terminals (ONT).

The photonic components can be generally divided into optical fiber components and planar waveguide components. The optical fiber components have to fuse optical fibers, so relatively large ones are too hard to integrate. So it has limited functions and other demerits. On the contrary, planar waveguide components not requiring the fusion process can carry out multiple functions, such as switching, routing, mux/demux, splitting, and filtering. Moreover, they can perform more than one function because they are easy to integrate with each other.2

Currently, planar waveguide devices are mainly fabricated using semiconductor process technology, i.e., photolithography and etching. However, the cost of waveguide components produced by these methods is relatively high and thus not suitable for low-cost application to FTTH systems.3 Therefore imprinting technology has become more popular and is considered a better patterning technology to fabricate polymeric waveguide devices because it is much simpler and easier to replicate than the semiconductor process technology. It produces planar components with polymer materials by duplicating a pattern formed on a mask. Among imprinting technologies, the hot embossing method is a cheap processing technology available for massive production.4,5 Many researchers have been studying and developing it to use not only for an optical waveguide devices but also for biocomponents, micro-electromechanical systems (MEMS), and so on. Since the polarization characteristics of polymer such as absorption loss and birefringence have been improved greatly, it does not show a notable difference from the silica commonly used for waveguide materials.4,6

In the present study, we designed a wavelength-independent coupler (WINC), one of the planar waveguide components, with a hot embossing imprint technique and tried to optimize the size of the polymer core in the WINC. It can be located at the front end of optical communication multiplexers and used over the 1310- and 1550-nm range, and it influences wavelength characteristics of the multiplexer. Even though WINC can be fabricated using a fusion splicing method with optical fibers, that method is much more difficult than the hot embossing method.7,8 The polymeric WINC, which has a flat transmission 5050 branching fraction from 1260 to 1640 nm, was designed and then fabricated with the hot embossing method. The optical properties of the polymeric WINC were measured and compared to values from a simulation.


Design of WINC

Two common designing methods are used for the planar WINC: one uses the Mach–Zehnder interferometer, and the other is the taper method for the waveguide of the coupling zone. It has been discovered that when using the Mach–Zehnder interferometer, the optical characteristics of the coupler are especially well matched with the designed values. Thus, we designed the WINC with Mach–Zehnder interferometer using the beam propagation method for accurate simulation of a curved structure. The structure of the WINC, shown in Fig. 1, consists of two directional couplers and two different optical paths designed in a Mach–Zehnder type. The operational principle is based on the suppression of the monotonic increase of the coupling ratio along the wavelength by creating a phase difference between the two directional couplers. In addition, we designed the 3dB coupler by computing the transfer matrix of a couple of straight waveguides based on the coupled mode theory. The transfer matrix can be expressed as Eq. (1), representing the multiplication of the 3dB coupler and transfer matrix of the optical channel difference:9


TWINC is the total transfer matrix of the WINC, where T3dB1 and T3dB2 are the transfer matrix of the 3dB couplers for the front and the back ends, respectively, and TΔL is the transfer matrix of the Mach–Zehnder interference. Equation (1) for TWINC can be expressed in detail as in Eq. (2), with the transfer matrix of an ideal 3dB coupler and the transmission constant, where β is the propagation constant and ΔL is the optical path difference:


If the optical power is incident to a port, the output intensity will be calculated with Eq. (3):


If Eq. (3) is expressed as an optical power equation, it will be RR*=sin2(0.5ϕ) or SS*=cos2(0.5ϕ), where ϕ is the phase difference caused by the optical path difference. The optical path difference ΔL can be expressed by Eq. (4):


where λ is optical wavelength and neff is the effective refractive index of the polymer waveguide.

Fig. 1

The wavelength-independent coupler based on the Mach–Zehnder interferometer.


The important factors with regard to this structure are the coupling ratio of the two directional couplers and the phase difference created by the optical path difference. Thus, the coupling ratio of the directional coupler was determined by the coupling length and the distance between two separated waveguides. The optical path difference was determined by the height of the Mach–Zehnder interferometer, as shown in Fig. 1. In addition, the core size of the waveguide WINC was 8×8μm, because the core of the waveguide needed to have a mode diameter identical to that of the optical fiber in the single mode used for the connection. Polymethyl methacrylate (PMMA) was used as a cladding material, and the refractive index was 1.4816. The resin (WIR30-490) of ChemOptics was used as the core material; its refractive index was 1.4862 (at 1310 nm). A 0.3% difference existed between the refractive indexes of the two substances. S-bends were mainly used for the curves.

Figure 2 shows the simulation results with varying the curvature radius, coupling length (L1, L2), arm height (h), and waveguide gap (g1, g2) in terms of the coupling losses. As shown in Fig. 2(a), the power of channels 1 and 2 were almost the same when the curvature radius was more than 40,000 μm. We set the radius of curvature at 50,000 μm because we considered the tolerances of curvature manufacturing process. We also set 4 μm for the waveguide gap (g1, g2), 1420 μm for the coupling length L1, 200 μm for L2, and 36 μm for the arm height (h). The optical powers of channels 1 and 2 simulated in regard to the wavelengths from 1260 to 1640 nm are presented in Fig. 3. After normalizing, the power in results was suitable for a 3dB broadband coupler, because the power values for channels 1 and 2 were almost same at 12601640nm wavelength.

Fig. 2

Simulation results according to radius of curvature (a), coupling length (b), arm height (c), and gap of two waveguides (d).


Fig. 3

Optical power according to wavelength.


When the polymer waveguide is fabricated with the hot embossing method, the core size is usually changed. Thus, we performed a power simulation for that changed core size of the waveguide from 7.9 to 8.1 μm. As shown in Fig. 4, the allowable structure size tolerance was up to ±0.3μm, which might be acceptable for insertion losses occurring in the WINC.

Fig. 4

Simulation results according to waveguide size.



Fabrication and Experimental Results

We fabricated a WINC with the hot embossing method with polymer. For the hot embossing process, which is one of the most flexible and appropriate methods for fabrication of polymer optical devices,5 a molding master is necessary. To make a master, generally processes such as the lithography, electroplating, and molding (lithographie galvanoformung abformung) process, the Bosch process, and the deep reactive ion etching (DRIE) method are applied.1011.12 In this study, we used the DRIE to make a silicon molding master. Figure 5 illustrates in detail the hot embossing process flow for the fabrication of the WINC. The hot embossing method consisted of several processing steps of imprinting by pressing a silicon master into the PMMA sheet. First, a cleaned silicon master was prepared as shown in Fig. 5(a). Second, the master was impressed onto the PMMA sheet using a hot embossing method with three steps as shown in Fig. 5(b). The three steps of the hot embossing are as follows. The temperature, pressure, and time were 140°C, 16 bar, and 60 s for the first step; 140°C, 25 bar, and 80 s for the second step; and 140°C, 16 bar, and 60 s for the third step. After these steps, the master was removed as shown in Fig. 5(c).

Fig. 5

Fabrication process of the polymeric WINC device: silicon master (a), hot embossing process (b), demolding master (c), core filling (d), UV curing (e), and final structure (f).


At that time, the temperature was set to 70°C. Figure 5(d) shows the core resin filled over the formed pattern. Figure 5(e) describes the solidification process; the core resin was solidified with 15-bar nitrogen pressure and exposed for 10 min to UV light after being covered with an upper clad sheet. Figure 5(f) shows the fabricated WINC device. To evaluate the size of optical waveguides of the fabricated WINC, we took a scanning electron microscope (SEM) image of the surface of the WINC. The size of the optical waveguide of the WINC was 8×8μm, as shown in Fig. 6.

Fig. 6

(a), SEM images for several parts of the WINC device. (b), Cross-sectional view of the optical waveguide.


The optical characteristics of the fabricated WINC, such as propagation loss, insertion loss, and power uniformity in a broadband range, were evaluated. Figure 7 illustrates the schematics of the measurement. A tunable light source producing 1310- to 1550-nm wavelengths was used; the single-mode fiber was aligned with the input port of the polymeric WINC to evaluate the characteristics of the fabricated device. A multimode fiber was connected to the output port of the device; the output power was measured by a power meter (Newport, 1835-C). The broadband characteristics of the WINC were observed by an optical spectrum analyzer (OSA, ANDO, AQ6417B). The displayed characteristics of each broadband wavelength ranged from 1260 to 1640 nm. To evaluate the propagation loss of the WINC, we constructed the straight waveguide with the same polymer using the hot embossing method. The optical power of the light source from the input fiber was 6.76 dBm (at 1310 nm), and the power of the light from the out fiber was 6.31 dBm after running the 2-cm straight waveguide and 6.53 dBm after running the 1-cm straight waveguide. Therefore, the propagation loss of the WINC was about 0.23dB/cm.

Fig. 7

Schematics of test setup.


The insertion loss can be defined as 10log(P2/P1) and 10log(P3/P1), where P1 is the optical power of the incident light of the WINC and P2 and P3 are the optical power at the output ports after the light passes through the coupler. The output power at the output ports is presented in Table 1. To ensure the accuracy of the measurement of the insertion loss, two kinds of light sources (1310 and 1550 nm) were used. The results were average values of five measurements. The evaluated bandwidth of the WINC is shown in Fig. 8. The result was the 5050 split ratio at 12601640nm. Therefore, the basic characteristics of the WINC were confirmed. The insertion losses of channel 2 were slightly bigger than those of channel 1 and also different from the simulation results. However, such differences could be ignored because of process tolerance and measurement errors. All optical characteristics of the fabricated WINC did satisfy the requirements of Telcoria–GR1209 core. We measured the devices for 5 h and confirmed the excellent stability of the device, as shown in Fig. 9. Therefore, we think that it is suitable for the optical communication system.

Table 1

Optical power (dB) at the output ports.

Input wavelengthOptical power at channel 1Optical power at channel 2
1310 nm3.64.2
1550 nm3.44.1

Fig. 8

Splitting characteristics according to wavelength.


Fig. 9

Insertion loss changes after 5 h at port 1 (a) and port 2 (b).




We designed a WINC, usable for broadband wavelengths from 1260 to 1640 nm, using a beam propagation method based on the coupled mode theory. The coupling length, waveguide gap, and waveguide interval conditions were optimized through simulations. We fabricated the designed device using the hot embossing method that employs a nanoimprint lithography, and we evaluated its optical characteristics through the experiment. The measured propagation loss of the fabricated device was about 0.2dB/cm. The insertion loss was measured to be 3.6 dB on channel 1 and 4.2 dB on channel 2. The output characteristics of the fabricated device were almost identical in the range from 1260 to 1640 nm, which proves its usefulness for FTTH. We expect that the proposed design and fabrication method will be applied for the development of optical switches, optical modulators, WDM optical components, and electro-optic circuit boards and make those better than other methods.


This research was supported by the World Class University program through the National Research Foundation of Korea funded by the Ministry of Education, Science and Technology, South Korea (Grant No. R31-20004).



Y. Xu, “Polymer planar waveguide device using inverted channel structure with upper liquid crystal cladding,” Opt. Express 17(10), 7837–7843 (2009).OPEXFF1094-4087http://dx.doi.org/10.1364/OE.17.007837Google Scholar


K.-J. Kimet al., “Flexible polymer waveguide tunable lasers,” Opt. Express 18(8), 8392–8399 (2010).OPEXFF1094-4087http://dx.doi.org/10.1364/OE.18.008392Google Scholar


J. Halldorssonet al., “High index contrast polymer waveguide platform for integrated biophotonics,” Opt. Express 18(15), 16217–16226 (2010).OPEXFF1094-4087http://dx.doi.org/10.1364/OE.18.016217Google Scholar


D.-H. Kimet al., “Polymeric microring resonator using nanoimprint technique based in a stamp incorporating a smoothing buffer Layer,” IEEE Photon. Technol. Lett. 17(11), 2352–2354 (2005).IPTLEL1041-1135http://dx.doi.org/10.1109/LPT.2005.857598Google Scholar


T. BallaS. M. SpearingA. Monk, “An assessment of the process capabilities of nanoimprint lithography,” J. Phys. D Appl. Phys. 41(17), 17401–17411 (2008).0022-3727http://dx.doi.org/10.1088/0022-3727/41/17/174001Google Scholar


M.-C. Ohet al., “Integrated photonic devices incorporating low-loss fluorinated polymer materials,” Polymers 3(3), 975–997 (2011).0032-2725http://dx.doi.org/10.3390/polym3030975Google Scholar


J. Van Campenhoutet al., “Low-power, 2×2 silicon electro-optic switch with 110-nm bandwidth for broadband reconfigurable optical networks,” Opt. Express 17(26), 24020–24029 (2009).OPEXFF1094-4087http://dx.doi.org/10.1364/OE.17.024020Google Scholar


N.-S. Sonet al., “Near-infrared tunable lasers with polymer waveguide Bragg gratings,” Opt. Express 20(2), 827–834 (2012).OPEXFF1094-4087http://dx.doi.org/10.1364/OE.20.000827Google Scholar


S. Garcia-BlancoJ. S. Aitchison, “Direct electron beam writing of optical devices on Ge-doped flame hydrolysis deposited silica,” IEEE J. Sel. Top. Quantum Electron. 11(2), 528–538 (2005).IJSQEN1077-260Xhttp://dx.doi.org/10.1109/JSTQE.2005.845617Google Scholar


D. Weilandet al., “Optical fibre array manufacture using electrostatic actuation,” in IEEE Advanced Packaging Materials: Microtech, 2010 International symposium, pp. 92–97 (2010).Google Scholar


S. W. Younet al., “Prototype development of a roller imprint system and its application to large area polymer replication for a microstructured optical device,” J. Mater. Proc. Technol. 202(1–3), 76–85 (2008).JMPTEF0924-0136http://dx.doi.org/10.1016/j.jmatprotec.2007.08.069Google Scholar


S. W. Ahnet al., “Polymeric wavelength filter based on a Bragg grating using nanoimprint technique,” IEEE Photon. Technol. Lett. 17(10), 2122–2124 (2005).IPTLEL1041-1135http://dx.doi.org/10.1109/LPT.2005.854404Google Scholar



Kyung Su Jang received his BS degree from Pusan University of Foreign Studies and MS degrees from Pusan University, Busan, Korea, in 2007 and 2010, respectively. He is currently working toward the PhD degree in Pusan National University, Busan, Korea. His research interests are passive optical devices and optical interconnection.


Eung Soo Kim received his BS and MS in electronics engineering from Kyungpook National University, Korea, in 1990 and 1992. He received the PhD degree in material science from Faculty of Science and Technology, Keio University, in Japan in 1996. He has been a visiting professor in Department of Electronics Engineering at Keio University in Japan as a JSPS fellowship in 2003. He has been the head of the Institute of Information & Communication in Pusan University of Foreign Studies from 2008 to 2010. He is currently a professor in Division of Digital Media Engineering, Pusan University of Foreign Studies. His research interests are optical sensors, nonlinear optics, optical waveguide devices, polymer optical fibers, and optical integrated circuits.


Chang Seok Kim received his BS degree from Korea Advanced Institute of Science and Technology, Daejeon, Korea, in 1996, the MS degree from Gwangju Institute of Science and Technology, Gwangju, in 1999, and the PhD degree from Johns Hopkins University, Baltimore, MD, in 2004. From 1999 to 2000, he was a research engineer with the Wavelength Division Multiplexing Optical Communication Team of Korea Telecom, Daejeon. His work was supported by the Korean Government Overseas Study Scholarship. In 2004 and 2005, he was a postdoctoral researcher with Beckman Laser Institute and Medical Clinic, University of California, Irvine. He joined Pusan National University, Busan, in 2005 as an assistant professor. Since 2009, he has been an associate professor in the Department of Cogno-Mechatronics Engineering, Pusan National University. His research interests include development of novel fiber laser systems and their application into biomedical, telecommunication, and sensor areas.


Myung Yung Jeong received BS and MS degrees from Pusan National University, Pusan, Korea, in 1982 and 1984, and the PhD degree from the Korea Advanced Institute of Science and Technology, Daejeon, Korea, in 2000. Since September 1983, he has worked for the Electronics and Telecommunications Research Institute, Daejeon, Korea. He is currently a professor in the Department of Cogno-Mechatronics Engineering, Pusan National University. His present research interests include imprinted optical devices, nanophotonics, optical interconnection, and optical components for in-vehicle networks.

Kyung-Su Jang, Chang-Seok Kim, Myung-Yong Jeong, Eung-Soo Kim, "Design and fabrication of an imprinted wavelength-independent coupler," Optical Engineering 51(8), 085003 (2 August 2012). http://dx.doi.org/10.1117/1.OE.51.8.085003
Submission: Received ; Accepted



Polymer multimode waveguides

Fiber to the x

Optical fibers

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Mach-Zehnder interferometer

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