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研究生:徐瑜聰
研究生(外文):Hsu, Yu-Cong
論文名稱:單光子測距儀之設計與製作
論文名稱(外文):Design and implementation of a single-photon rangefinder
指導教授:蔡嘉明
指導教授(外文):Tsai, Chia-Ming
口試委員:林聖迪、桑梓賢、郭明清
口試委員(外文):Lin, Sheng-Di、Sang,Tzu-Hsien、Kuo, Ming-Ching
口試日期:2016-01-28
學位類別:碩士
校院名稱:國立交通大學
系所名稱:電子工程學系 電子研究所
學門:工程學門
學類:電資工程學類
論文種類:學術論文
論文出版年:2016
畢業學年度:104
語文別:中文
論文頁數:59
中文關鍵詞:測距、單光子崩潰二極體、飛時測距法、時間延遲元件、FPGA、蓋格模式、累增崩潰
外文關鍵詞:rangerfinder、SPAD、TOF、PDL、FPGA、Geiger mode、avalanche
相關次數:
  • 被引用被引用:2
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本論文以單光子崩潰二極體(Single-Photon Avalanche Diode)為感測器,其後端電路為被動抑制、主動回復電路,實現一個用return-center法為測量距離的架構。模擬時,將光波形以弦波、三角波和方波做為所接收之光波形模擬,在此方法下,系統皆可以鎖定完成,故此方法較不受光調變波形所影響。在此測距系統中,加入一個可程式延遲元件(Programmable Delay Line,PDL),目的是要使波形產生器輸出之訊號延遲,再與因距離產生延遲之光訊號作比較,兩訊號進入以FPGA建立之鎖定電路達到鎖定後,FPGA會以Chipscope為傳輸介面,我們便可取得8位元之距離資訊。
This thesis present a range finder base on return-center method with a single photon avalanche diode (SPAD) by applying the passive quenching-active reset circuit. In the simulation, we use sine wave, triangular wave and square wave as waveform of light to test the locking circuit is locking or not. The result shows that the range finder will not be affected by the waveform of light. In the range finder system, there is a programmable delay line (PDL) will make a delay to the signal which is generated from the pulse generation. And then we can compare the delay signal with the other signal which the light pass through the distance we want to know and detect by SPAD. After comparing the signals in FPGA, the locking circuit will lock. And then we can use chipscope as interface to get the distance information in 8-bit format form FPGA.

內容
摘 要 II
Abstract III
目錄 IV
圖目錄 VI
第一章 簡介 1
1.1. 研究背景 1
1.2. 論文架構 2
第二章 測距方法之相關研究 3
2.1 直接飛時測距法(D-TOF) 4
2.1.1 D-TOF 4
2.2 間接飛時測距法(I-TOF) 4
2.2.1 I-TOF調變波形為方波 5
2.2.2 I-TOF調變波形為弦波 5
2.3 測距相關研究介紹 6
2.3.1 I-TOF調變波形為方波 6
2.3.2 I-TOF調變波形為弦波 7
第三章 單光子崩潰二極體 9
3.1 單光子崩潰二極體(SPAD)操作原理 9
3.1.1 累增崩潰模式(Geiger mode)操作 9
3.1.2 SPAD抑制電路 11
3.2 元件物理 14
第四章 模擬與分析 18
4.1 模擬架構 18
4.2 模擬結果 20
第五章 Return-center測距架構 26
5.1 距離量測與傳輸流程簡介 26
5.2 距離量測 28
5.2.1 FPGA板介紹 28
5.2.2 PDL介紹 37
5.2.3 SPAD電路架構 40
5.2.4 光源介紹 41
第六章 量測結果與分析 45
6.1 背景光影響 45
6.2 光強度影響 47
6.3 手動距離量測 48
第七章 總結與未來展望 56
參考文獻 57


[1] C. Niclass, M. Soga, H. Matsubara, M.Ogawa, and M.Kagami, “A 0.18_m CMOS SoC for a 100 m-range 10-frame/s 200×96-pixel time-of flight depth sensor,” in IEEE ISSCC Dig. Tech. Papers, Feb. 2013, pp. 488-489.

[2] R.J. Walker, J.A. Richardson, and R.K. Henderson, “A 128×96 pixel event-driven phase-domain ΔΣ-based fully digital 3D camera in 0.13 um CMOS imaging technology,”in IEEE ISSCC Dig. Tech. Papers, Feb. 2011, pp.410-412.

[3] C. Veerappan, C. Bruschini, and E. Charbon, “Sensor network architecture for a fully digital and scalable SPAD based PET system,” in IEEE Nucl. Sci. Symp. Conf. Rec. (NSS/MIC), 2012, pp. 1115-1118.

[4] R.H. Hadfield, “Single-photon detectors for optical quantum information applications”, Nature Photonics, VOL. 3, 2009, P.696~705

[5] Y. Maruyama, J. Blacksberg, and E. Charbon, “A 1024×8 700ps time-gated SPAD line sensor for laser Raman spectroscopy and libs in space and rover-based planetary exploration,” in IEEE ISSCC Dig. Tech. Papers, Feb. 2013, pp. 110-111.

[6]C. Niclass, C. Favi, T. Kluter, M. Gersbach, and E. Charbon, “A 128×128 single- photon imager with on-chip column-level 10b time-to-digital converter array capable of 97ps resolution,” in IEEE Int. Solid-State Circuits Conf. Dig., 2008, pp. 44–45.

[7] ] C. Veerappan, J. Richardson, R. Walker, D. Li, M. W. Fishburn, Y. Maruyama, D. Stoppa, F. Borghetti, M. Gersbach, R. K. Henderson, and E. Charbon, B “A 160×128 single-photon image sensor with on-pixel 55ps 10b time-to-digital converter”, in Proc. IEEE Int. Solid-State Circuits Conf. Dig. Tech. Papers, 2011, pp. 312–314.

[8] C. Niclass, M. Soga, H. Matsubara, M. Ogawa, and M. Kagami, “A 0.18um CMOS SoC for a 100 -range 10ps 200×96-pixel time-of- flight depth sensor,” in IEEE Int. Solid-State Circuits Conf. Dig. Tech. Papers, Jan. 2013, pp. 488–489.
[9] C. Niclass, A. Rochas, P. A. Besse, and E. Charbon, “Design and characterization of a CMOS 3-D image sensor based on single photon avalanche diodes,” IEEE J. Solid-State Circuits, vol. 40, no. 9, pp. 1847–1854, Sep. 2005.

[10] C. Niclass, K. Ito, M. Soga, H. Matsubara, I. Aoyagi, S. Kato, and M. Kagami, “Design and characterization of a 256 × 64-pixel singlephoton imager in CMOS for a MEMS-based laser scanning time-of-flight sensor,” Opt. Exp., vol. 20, no. 11, pp. 118 63–118 81, May 2012.

[11] C. Niclass, C. Favi, T. Kluter, F. Monnier, and E. Charbon, “Single photon synchronous detection,” IEEE J. Solid-State Circuits, vol. 44, no. 7, pp. 1977–1989, Jul. 2009.

[12] D. Stoppa and A. Simoni, “Single-photon detectors for time-of-flight range imaging,” in Single-Photon Imaging, P. Seitz and A. J. P. Theuwissen Eds., Berlin Heidelberg, Springer-Verlag, 2011, pp. 275-300.

[13] D. Stoppa, L. Pancheri, M. Scandiuzzo, L. Gonzo, G.F. Dalla Betta, A. Simoni, “A CMOS 3-D Imager Based on Single Photon Avalanche Diode,” IEEE Trans. Circuits Syst. I, Reg. Papers, vol.54, no.1, pp. 4-12, Jan. 2007.

[14] S. Bellisai, D. Bronzi, F. Villa, S. Tisa, A. Tosi, and F. Zappa, “Single-photon pulsed light indirect time-of-flight 3D ranging,” Opt. Exp., vol.21, no.4, pp. 5086-5098, Feb. 2013.

[15] F. Zappa, S. Tisa, A. Tosi, and S. Cova, “Principles and features of single-photon avalanche diode arrays,” Sensors and Actuators A: Physical, vol.140, no.1, pp. 103-112, Oct. 2007.

[16] A. Gallivanoni, I. Rech, and M. Ghioni, “Progress in Quenching Circuits for Single Photon Avalanche Diodes,” IEEE Trans. Nucl. Sci., vol.57, no.6, pp. 3815-3826, Dec. 2010.

[17] S. Tisa, F. Zappa, A. Tosi, and S. Cova, “Electronics for single photon avalanche diode arrays,” Sensors and Actuators A: Physical, vol.140, no.1, pp. 113-122, Oct. 2007.


[18] 黃來得, “標準CMOS高壓技術製作之單光子累崩二極體”, 碩士論文, 交通大學電子工程研究所, 2015.

[19] D. Piatti, F. Remondino and D. Stoppa, “State-of-the-art of TOF range-imaging
sensors,” in TOF Range-Imaging Cameras, F. Remondino and D. Stoppa Eds., Berlin Heidelberg, Springer-Verlag, 2013, pp. 1-9.

[20] Xilinx, Inc., ML605 Hardware User Guide (UG534, v1.7), 2012.

[21] C. Niclass and M. Soga, “A miniature actively recharged single-photon detector free of after-pulsing effects with 6 ns dead time in a 0.18um CMOS technology,” in Proc. of IEEE Int. Electron Devices Meeting (IEDM), 2010, pp. 14.3.1–14.3.4

[22] D. Stoppa, N. Massari, L. Pancheri, M. Malfatti, M. Perenzoni, and L. Gonzo, “A range image sensor based on 10 m lock-in pixels in 0.18 um CMOS imaging technology,” IEEE J. Solid-State Circuits, vol. 46, no. 1, pp. 248–258, Jan. 2011.

[23] C. Niclass,M. Soga, H. Matsubara, S. Kato, and M. Kagami, “A 100 m-range 10-frame/s 340×96-pixel time-of-flight depth sensor in 0.18 um CMOS,” IEEE J. Solid-State Circuits, vol. 48, no. 2, pp. 559–572, Feb. 2013.

[24] S.-J. Kim, B. Kang, J. D. K. Kim, K. Lee;, C.-Y. Kim, and K. Kim, “A 1920× 1080 3.65 m-pixel 2D/3D image sensor with split and binning pixel structure in 0.11 m standard CMOS,” in ISSCC Dig. Tech. Papers, Feb. 2012, pp. 396–397.

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