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研究生: GOPIKA UPPATH
GOPIKA UPPATH
論文名稱: Beam steering of optical phased arrays by thermo-optic phase shifters for LIDAR applications
Beam steering of optical phased arrays by thermo-optic phase shifters for LIDAR applications
指導教授: 李三良
San-Liang Lee
口試委員: 廖顯奎
Shein-Kuei Liaw
徐世祥
Shih-Hsiang Hsu
陳政寰
C.H.Chen
李三良
San-Liang Lee
學位類別: 碩士
Master
系所名稱: 電資學院 - 電子工程系
Department of Electronic and Computer Engineering
論文出版年: 2019
畢業學年度: 107
語文別: 英文
論文頁數: 89
中文關鍵詞: Thermo-optic phase shifterCrosstalkBeam steeringOptical phased arrayTemperature Rise
外文關鍵詞: Thermo-optic phase shifter, Crosstalk, Beam steering, Optical phased array, Temperature Rise
相關次數: 點閱:190下載:2
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Optical phased arrays (OPAs) have been widely used for many applications in the last few years. Optical phased arrays are used in many fields like holographic video displays, free-space optical communication systems and light detection and ranging (LIDAR) systems. Lidar is a remote sensing technique that emits the collimated light beam and measures the time it takes for the reflections to be detected by the signal. This is used to compute the distances to the objects.
Thermal tuning of the optical array with uniform spacing is used to induce a phase shift in waveguides. Heaters of the same length with a linear increase in power will change the refractive index of the waveguides. The change in refractive index will cause a phase shift to the waveguides. Since the waveguides in the optical phased array are placed in uniform spacing, the temperature rise (crosstalk) between the waveguides has been examined in this work. It has been noticed that the temperature rise (crosstalk) between the waveguides will increase in uniform spacing. Therefore, the temperature rise between the waveguides is reduced to 2 K for a fixed area by giving non-uniform spacing between the waveguides.
Then, the far-field analysis of the optical phased array with a single input has been evaluated. The electric field intensity and far-field pattern of the optical phased array are evaluated. The shifting of the beam along the theta direction is given in this work.


Optical phased arrays (OPAs) have been widely used for many applications in the last few years. Optical phased arrays are used in many fields like holographic video displays, free-space optical communication systems and light detection and ranging (LIDAR) systems. Lidar is a remote sensing technique that emits the collimated light beam and measures the time it takes for the reflections to be detected by the signal. This is used to compute the distances to the objects.
Thermal tuning of the optical array with uniform spacing is used to induce a phase shift in waveguides. Heaters of the same length with a linear increase in power will change the refractive index of the waveguides. The change in refractive index will cause a phase shift to the waveguides. Since the waveguides in the optical phased array are placed in uniform spacing, the temperature rise (crosstalk) between the waveguides has been examined in this work. It has been noticed that the temperature rise (crosstalk) between the waveguides will increase in uniform spacing. Therefore, the temperature rise between the waveguides is reduced to 2 K for a fixed area by giving non-uniform spacing between the waveguides.
Then, the far-field analysis of the optical phased array with a single input has been evaluated. The electric field intensity and far-field pattern of the optical phased array are evaluated. The shifting of the beam along the theta direction is given in this work.

ABSTRACT………………………………………………….I ACKNOWLEDGEMENTS……………………………..….II TABLE OF CONTENTS…………………………………..III LIST OF FIGURES………………………………………..VI LIST OF TABLES……………………………………….....XI CHAPTER 1-INTRODUCTION…………………………….....1 1.1 Silicon Photonics…………………………………………1 1.2 Basic introduction of LIDAR technology………………...2 1.3 Motivation of the work…………………………………....3 1.4 Thesis contribution………………………………………..3 CHAPTER 2- LITERATURE REVIEW…………………........4 2.1 Optical phased array…………........……………………...4 2.1.1 Architecture of optical phased array…..…..……....………..…5 2.2 Thermal tuning of optical phased array…………………..7 2.2.1 Different phase shifter by thermo-optic effect..........…….….8 2.3 Beam steering of optical phased array……………….….11 CHAPTER 3-PHASE SHIFT IN OPTICAL WAVEGUIDES……………………………………………….14 3.1 Phase shift in optical waveguides……………………...14 3.1.1 Phase shifter by thermal tuning………………………........14 3.1.2 Refractive index and phase of waveguides……...…….…..19 3.1.2.1 First waveguide……………………………….…….19 3.1.2.2 Change in refractive index (Δneff) and phase (Δφ) of all waveguides……………………………………21 CHAPTER 4- CROSSTALK BETWEEN THE WAVEGUIDES……...………….………………………….…22 4.1 Crosstalk of 10 waveguides placed at uniform spacing of 10 µm in a fixed area of 100 µm…………....….…......23 4.2 Summary of crosstalk method with uniform spacing………………………………………………..…34 4.3 Crosstalk temperature evaluation for the non-uniform spacing of waveguides in a fixed area of 100 µm……………………………………….....…….35 4.4 Summary of crosstalk with non-uniform spacing……….46 CHAPTER 5: BEAM STEERING OF OPTICAL PHASED ARRAY……………………………………………………….49 5.1 Far-field analysis of phased array…………….……...….51 5.1.1 Two-dimensional phased array model………………..……51 5.1.2 One-dimensional phased array model…………………..….53 5.2 Device structure for beam steering……………….……..59 5.3 Component description……………………………….…60 5.3.1 1x8 MMI splitter………………………………………….….60 5.3.2 Different waveguide length………………………………….61 5.3.3 Grating section……………………………………..………...62 5.4 Simulation results of Far-field analysis……………...….64 CHAPTER 6: CONCLUSION AND FUTURE WORK.……..68 REFERENCES………………………………………………..70

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