UBC Faculty Research and Publications

Y-branch optical modulator. Jaeger, Nicolas A. F.; Lai, Winnie C. 1991

Your browser doesn't seem to have a PDF viewer, please download the PDF to view this item.

Item Metadata


52383-Jaeger_SPIE_1583_202.pdf [ 498.12kB ]
JSON: 52383-1.0107534.json
JSON-LD: 52383-1.0107534-ld.json
RDF/XML (Pretty): 52383-1.0107534-rdf.xml
RDF/JSON: 52383-1.0107534-rdf.json
Turtle: 52383-1.0107534-turtle.txt
N-Triples: 52383-1.0107534-rdf-ntriples.txt
Original Record: 52383-1.0107534-source.json
Full Text

Full Text

Y-Branch optical modulator  Nicolas A.F. Jaeger and Winnie C. Lai University of British Columbia, Department of Electrical Engineering Vancouver, British Columbia, Canada V6T 1Z4  ABSTRACT  To characterize z-cut Ti:LiNbO3 Y-branch optical modulators, numerical simulations were performed showing that high on/off ratios are attainable without special Y-junction asymmetries or long electrodes. The effective index and 2-D finite difference beam propagation methods were used for the simulations. A modulator with a 2° Y-branch was fabricated. The measured on/off ratios were 5 : 1 at 25 V, 12: 1 at 50 V, and 60: 1 at 75 V, corresponding to 4: 1 , 12: 1 , and 62: 1 for the = 632.8 nm. simulations for 1. iNTRODUCTION Increasing research is being done in the area of electro-optic modulators in part due to their potential use in time division multiplexers' as well as in digital switches2 for high bit rate optical communications. Y-branch optical modulators are more suitable for such use than Mach-Zehnder type modulators because they are easier to fabricate and to control. Y-branch optical modulators are non-interferometric by nature and are tolerant of variations in parameters such as applied voltage, branch angle, and wavelength. The Y-branch optical modulator operates by the electro-optic effect. In its neutral state, without any voltage application, each branch arm guides an equal amount of light. Application of voltage  to its electrodes channels light into one of the arms of the Y-branch while at the same time channelling light out of the other arm. The arm to which the light is channelled or not channelled depends on the polarity of the applied voltage. We examine, both numerically and experimentally, a Y-branch optical modulator fabricated in z-cut lithium niobate (LiMbO3), where the waveguides are formed by titanium (Ti) indiffusion. Previous devices with high on/off ratios have had very small branch angles3 (i.e., less than 0.2°) and/or asymmetric branch arms4. Small branch angles give rise to long devices and long electrodes resulting in wasted real estate on the LiNbO3 substrate and increased capacitance. Furthermore, asymetric branches are more difficult to fabricate. Here, we show that devices with high on/off ratios can be obtained without long horn lengths or any special Y-junction asymmetries.  202 / SPIE Vol. 1583 Integrated Optical Circuits (1991) Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  O-8194-0714-3/91/$4.OO  2. NUMERICAL SIMULATIONS Although there are 3-D numerical methods which can simulate a propagating optical field within  a waveguide, a 2-D beam propagation method (BPM) is chosen due to its increased speed and comparable accuracy5. The effective index method6 (ElM) is first applied to reduce the refractive index profile from 3-D to 2-D. The refractive index n(x,z) for metal indiffused strip waveguides (here, we use z instead of y to indicate the z-axis of the LiNbO3) is defined as follows6: 2  2 7z (x,z) =  22Z  2x  D  W  (la)  where = exp(-z2/D2)  (ib) and  g(4) =  +  ii{eit[(i+4)} e,t[(i_.)]}  (ic)  where D is the diffusion depth, W is the width of the Ti strip prior to diffusion, nb is the bulk refractive index for z-cut LiNbO3 at ) = 632.8 nm, and n is the maximum refractive index at the surface due to the Ti indiffusion. The device configuration and fabrication parameters of the Ybranch optical modulator are given in Figure 1 and Table I respectively. After using the ElM to reduce the refractive index profile, giving the effective index ne(x) from n(x,z), the finite difference beam propagation method7 (FDBPM) is used to calculate the optical field distribution. The FDBPM is based on the Fresnel approximation to the scalar Helmholtz equation. The evolution of the electric field for a single polarization of a monochromatic optical wave in our case is7:  = De  - n) dy'  b  e 'ohbY'(xy) + O(Ly)3  (2a)  where  -  DX -  1÷  i iy  8kOnb aX a2  (2b)  8kOnb aX2  SPIE Vol. 1583 Integrated Optical Circuits (1991) / 203  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  I-  228Un- (2 horn lengths) -  —  1 1 4Ufl  A ,n5-2.204  A  1  I  A'  I  diffusion at 1050°C  for  6hr  diffused Ti  LINbO3  Figure 1 Dimensions and fabrication parameters of the Y-branch optical modulator. 1 50  60  on/off ratio  125  — — % guided power  0 -I-) a  100  /  75 44-  0  0  /  50  /  //  a)  0  0 -a a) :3  25  10  20 30 40 50 60  applied voltage (V) Figure 2 On/off ratios and percent guided power vs. applied voltage for the 2° V-branch optical modulator for = 632.8 nm.  204 I SPIE Vol. 1583 Integrated Optical Cfrcuits (1991)  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  The FDBPM is chosen over the BPM because it remains accurate for larger longitudinal step lengths8 and therefore it is considerably faster.  To simulate the effect of voltage application to the electrodes of the Y-branch optical modulator, conformal mapping9 is used to calculate the electric field components in the x and z directions in the  electro-optic substrate, E, and E. These fields are used, in turn, to determine the 3-D modulated refractive index profile, which is subsequently used in computing the modulated effective index for use with the 2-D FDBPM. The optical field that is input to the modulator is the fundamental TM-like mode with unit power, here called the eigenfunction U0(x). This function can be determined by using the method described in Reference 10. The power of the fundamental mode guided by the modulator at any distance y can be calculated using the orthogonality principle from 2  P(y) = fE(x,y) u:(x) t  (3)  In our simulations, we use a 100 jm wide window with a transverse grid of 1000 points. An absorber is placed 15 jm from either side of the window edge to dampen the field preventing high frequency numerical instabilities11. The Y-branch spreads out in 0. 1 m steps and the power output is computed when the two arms are 40 m apart so that the optical fields in the two arms no longer interact with each other.  Table I Fabrication parameters for a Y-branch optical modulator Ti thickness bulk refractive index nb maximum refractive index n diffusion depth D diffusion temperature diffusion time waveguide pattern width W electrode gap at input electrode gap at output branch angle 0 electrode length  500 A 2.2 2.204  3m 1050 °C  6 hrs  4 jm 4 jm  8m  20 228 /Lm  SPIE Vol. 1583 Integrated Optical Circuits (1991) / 205  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  3. SIMULATION RESULTS The goal of this numerical simulation is to study a Y-branch modulator combining short electrode  lengths with high on/off ratios at intermediate voltages, i.e. about 50 V. We have found that generally, on/off ratios at any given applied voltage increase with increasing branch angle'2. However, the amount of guided power also decreases with increasing branch angle. A 2° branch angle is chosen for this particular study because it exhibits high on/off ratios while retaining about 50% of the input power as well as having short electrode lengths. We have simulated the modulator using various electrode lengths, and found that a two-hornlength electrode provides better performance than a one-horn-length or three-horn-length electrode. A one-horn-length electrode is too short to cause substantial modulation, while a three-horn-length electrode shows no notable improvement in the on/off ratio but obviously increases the electrodes' capacitance.  The simulations show that both the on/off ratio and the percent guided power increase with applied voltage. For example, the on/off ratio is predicted to be 2.4: 1 at 20 V with 37% guided power and 85: 1 at 80 V with 51 % guided power, as shown in Figure 2. The on/off ratio's increase with applied voltage is to be expected because the greater the electric field the greater the change in  the refractive index and the more light directed into one of the arms. The relationship between applied voltage and guided power shows that guiding efficiency increases with voltage, this is because light which is originally radiated at low voltages is increasingly captured and channelled into one of  the arms as the voltage is increased. Figures 3 and 4 show the optical field in the Y-branch with 0 V and 50 V applied respectively.  4. FABRICATION  A Y-branch optical modulator, having the parameters shown in Figure 1 and Table I, was fabricated on z-cut y-propagating LiNbO3. The Y-branch pattern was formed in the 500 A thick Ti using photo-lithography and plasma-etching. The Ti was diffused into the crystal at 1050°C for 6 hours in flowing wet oxygen. The wet oxygen was used to prevent surface waveguiding due to Li02 out-diffusion'3. The estimated maximum refractive index change due to the Ti-indiffusion is 0.004 at A0 = 632.8 nm. Before putting on the electrodes, a thin Si02 optical buffer layer was sputtered onto the sample. Then a 4000A thick layer of aluminum was deposited and patterned into the electrodes using photolithography and chemical wet-etching. The samples were subsequently cut to the approriate sizes, and the input and output ends of the waveguides were polished.  206 / SPIE Vol. 1583 Integrated Optical Circuits (1991)  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  Figure 3 Optical field distribution of the Y-branch optical modulator with 0 V applied.  (Jo,)  0  S  'I  C S.—  At  S  S  I  I  ?e  So  -S e '3  Y-branch optical modulator with 50 V applied.  Figure 4 Optical field distribution of the  (do,)  0  S  C  At  'I  4  S  I  5. MEASURED RESULTS  Polarized light from a Helium-Neon laser (A0 = 632.8 nm) was coupled into a single mode polarization-maintaining monomode fibre through a microscope objective. Next the light from the fibre was endfire coupled into the TM-like mode of the input waveguide of the Y-branch optical modulator. The output from the modulator was projected through a microscope objective and a polarizer onto a pinhole in front of the detector which was connected to a storage oscilloscope. The output power from the two branches of the modulator was equalized prior to voltage application. Using a waveform generator a slowly-varying triangular wave was applied to the electrodes of the optical modulator. The measured on/off ratios were 5: 1 at 25 V, 12: 1 at 50 V, and 60: 1 at 75 V. Here we have accounted for the effects of the radiation modes since, in our case, the detector picked up both the guided TM-like mode as well as a portion of the radiation modes. Using our simulation results, the amount of radiation was calculated and used to adjust the measured data accordingly. The percentage guided power can be obtained by maximizing the power at the output of the modulator and then maximizing the power at the output of a 4 j.m straight waveguide, fabricated on the same substrate adjacent to the modulator, and comparing the two. Since the straight waveguide is adjacent to the Y-branch modulator, we assume that both waveguides have nearly identical guiding characteristics. The amount of guided power measured using the above method was 36% with 0 V  and 43% with 75 V applied, again we accounted for the effects of the radiation modes. These measured on/off ratios and percent guided powers compare reasonably well with the theoretical values, see Table II.  Table II  Performance comparison of the Y-branch optical modulator theoretical  on/off ratio:  % guided power:  experimental  25 V  4  5  50V 75V  12  12  62  60  35% 50%  36% 43%  0V  75V  6. CONCLUSION A Y-branch optical modulator was modelled and its behavior simulated numerically using the 2-D  FDBPM with the ElM. A device was then fabricated on z-cut LiNbO3, having a 2° branch angle and an electrode length of 228 m. On/off ratios of 5: 1 at 25 V, 12: 1 at 50 V, and 60: 1 at 75V were measured for light at a wavelength of 632.8 nm. The measured results are in good agreement with the theoretical performance predictions.  208 / SPIE Vol. 1583 Integrated Optical Circuits (1991) Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  7. ACKNOWLEGEMENT This work was supported by an NSERC operating grant and an NSERC post-graduate scholarship.  8. REFERENCES 1 . A. Djupsjöbacka, "Time Division Multiplexing Using Optical Switches, " IEEEJ. Select. Areas Commun. , vol. 6, No. 7, pp. 1227- 123 1 , August 1988. 2. R. L. Jungerman et al. , "High-Speed Optical Modulator for Application in Instrumentation,"  IEEE J. Light. Tech. , vol. 8, No. 9, pp. 1363-1370, September 1990. 3. P. Granestrand et al. , "Integrated Optics 4x4 Switch Matrix with Digital Optical Switches," Electron. Lett. , vol. 26, No. 1 , pp.4-5, January 1990. 4. Y. Silberberg, P. Perlmutter, and J. E. Baran, "Digital Optical Switch, " Appl. Phys. Lett., vol. 51, No. 16, pp.1230-1232, October 1987. 5.  Working Group I, COST 216, "Comparison of Different Modelling Techniques for  Longitudinally Invariant Integrated Optical Waveguides," lEE Proc. , vol. 136, No. 5, pp. 273-280, October 1989. 6. G. B. Hocker and W. K. Bums, "Mode Dispersion in Diffused Channel Waveguides by the Effective Index Method, " Appl. Opt. , vol. 16, No. 1 , pp. 1 13-118 January 1977. 7. D. Yevick and B. Hermansson, "Split-Step Finite Difference Analysis of Rib Waveguides," Electron. Lett. , vol. 25, No. 7, pp. 461-462, March 1989. 8. D. Yevick and B. Hermansson, "Efficient Beam Propagation Techniques, " IEEE J. Quantum Electron. , vol. 26, No. 1 , pp. 109- 1 12, January 1990. 9. N. A. F. Jaeger and L. Young, "Voltage-Induced Optical Waveguide Modulator in Lithium Niobate, " IEEE J. Quantum Electron. , vol. 25 , No. 4, pp. 720-728, April 1989. 10. D. Yevick and P. Danielsen, "Numerical Investigation of Mode Coupling in Sinusoidally Modulated GRIN Planar Waveguides, " Appl. Opt. , vol. 21 , No. 15 , pp. 2727-2733, August 1982. 1 1 . J. Saijonmaa and D. Yevick, "Beam-propagation Analaysis of Loss in Bent Optical Waveguides and Fibers, " .1. Opt. Soc. Am. , vol. 73, No. 12, pp. 1785-1791 , December 1983. 12. W. C. Lai, "The Effects of Branch Angle on a Y-branch Optical Modulator," The First Graduate Student Conference on Opto-Electronics Materials, Devices, and Systems, pp.30,McMaster University, Hamilton, Ontario, June 24-26, 1991. 13. J. L. Jackel, "Suppression of Outdiffusion in  Titanium Diffused LiNbO3: A Review," J. Opt.  Commun., vol. 3, pp. 82-85, 1982.  SPIE Vol. 1583 Integrated Optical Circuits (1991)1 209  Downloaded from SPIE Digital Library on 07 Jun 2011 to Terms of Use: http://spiedl.org/terms  


Citation Scheme:


Citations by CSL (citeproc-js)

Usage Statistics



Customize your widget with the following options, then copy and paste the code below into the HTML of your page to embed this item in your website.
                            <div id="ubcOpenCollectionsWidgetDisplay">
                            <script id="ubcOpenCollectionsWidget"
                            async >
IIIF logo Our image viewer uses the IIIF 2.0 standard. To load this item in other compatible viewers, use this url:


Related Items