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研究生: 李傳巽
Li, Chuan-Hsun
論文名稱: Pulsed Sodium-Yellow Intracavity Raman Laser
脈衝式腔內拉曼鈉黃光雷射
指導教授: 黃衍介
Huang, Yen-Chieh
口試委員:
學位類別: 碩士
Master
系所名稱: 電機資訊學院 - 光電工程研究所
Institute of Photonics Technologies
論文出版年: 2009
畢業學年度: 97
語文別: 英文
論文頁數: 77
中文關鍵詞: 脈衝式腔內拉曼鈉黃光雷射
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  • Recently, high-power and narrow-linewidth sodium-yellow laser generation has been attractive, since it may excite a laser-guide star for the application in adaptive optics, and laboratory spectroscopy. The main purpose of my project is to demonstrate and study the properties of a compact pulsed sodium-yellow intra-cavity Raman laser. Besides, we have proposed some cavity configurations for further narrowing down the linewidth of the output laser. The feasibility and effectiveness of the proposed ideas will be discussed and investigated in the dissertation.
    The laser system was fabricated based on a diode-end-pumped Q-switched Nd:YVO4 laser and stimulated Raman scattering in a Raman crystal CaWO4. We used a fiber-coupled diode laser at 808nm to pump a Nd:YVO4 crystal. The wave at 1064nm radiated from Nd:YVO4 could be well confined in a specially designed cavity. By Q-switched operation, a pulse train at 1064 nm with a tunable pulse repetition rate up to 79.4 kHz could be generated to pump an intra-cavity Raman crystal CaWO4. The Raman crystal is used as a wavelength shifter to provide a Raman shift around 910cm-1. Through the stimulated Raman scattering (SRS) in CaWO4, which is a 3rd order nonlinear optical process, a photon of the wave at 1064nm can be transformed into a Stokes photon at 1178nm and an excited optical phonon. Therefore a Raman laser operated at 1178nm is generated. Due to many significant thermal effects in the laser system, the resulted dynamic cavity was modeled and simulated with reference to the actual experiment. The properties and performance of the Raman laser were investigated and studied.
    Furthermore, cavities with a grating feedback and an etalon coupler were proposed to narrow down the linewidth of 589nm. Linewidth of around 0.1nm at 1178nm was achieved in a linear cavity configuration with an etalon coupler. Through the intracavity second harmonic generation (SHG) based on type I noncritical phase matching in a LBO crystal at temperature around 40 degree C, we successfully generated 589nm sodium yellow laser in another linear cavity with yellow-laser power around 360mW, corresponding to a diode-to-yellow-laser conversion efficiency of 2%. On another hand, a folded cavity configuration was proposed for using the grating feedback. The experiment about this part is still under way.


    Chapter 1 Introduction 1 1.1 Motivation 1 1.2 Diode-End-Pumped Solid State Laser Systems 2 1.3 Raman Scattering Process 5 1.4 Possible Configurations of Raman Lasers 9 1.5 Overview of the Dissertation 13 Chapter 2 Physical Mechanisms in Our Raman Laser 14 2.1 Diode-End-Pumped Q-Switched Nd:YVO4 Laser Generation 14 2.2 Stimulated Raman Scattering (SRS) in Calcium Tungstate (CaWO4) 15 2.3 Intracavity and Extracavity Second Harmonic Generation (SHG) in Lithium Triborate (LBO, LiB3O5) 22 2.4 Energy Flow and the Efficiency at Each Transfer 26 2.5 Methods of Narrowing Down the Laser Bandwidth 28 2.5.1 Intracavity Etalon 28 2.5.2 Grating Feedback at Grazing-Incidence 29 2.6 Thermal Lensing in Nd:YVO4 and CaWO4 and Cavity Simulation 30 Chapter 3 Experimental Results and Discussions 39 3.1 Introduction 39 3.2 Configurations of the Raman Laser 39 3.2.1 Raman Laser with an Etalon Coupler 39 3.2.2 Raman Laser with a Grating Feedback 46 3.3 Cooling and Temperature-Controllable Systems 50 3.3.1 Water Tank Cooling System 50 3.3.2 Thermal Electric Cooler with a Temperature Controller 50 3.4 Investigation of the Mode-Matching Lens 51 3.5 Experimental Results 53 3.5.1 Raman Laser with an Etalon Coupler 53 3.5.2 Raman Laser with a Grating Feedback 71 Chapter 4 Conclusions and Future Works 72 References 73

    [1] Craig A. Denman et al, “20 W CW 589 nm sodium beacon excitation source for adaptive optical telescope applications”, Optical Materials, 26 (2004) 507–513
    [2] Joseph D. Vance et al, “Continuous-wave, all-solid-state, single-frequency 400-mW source at 589 nm based on doubly resonant sum-frequency mixing in a monolithic lithium niobate resonator”, Applied Optics, Vol. 37, No. 21, 20 July 1998
    [3] Yan Feng et al, “589nm Light Source Based on Raman Fiber Laser”, Japanese Journal of Applied Physics, Vol. 43, No. 6A, 2004
    [4] Jirí Janousek et al, “Efficient all solid-state continuous-wave yellow orange light source”, Optics Express, Vol. 13, No. 4, 21 February 2005
    [5] Peter Dekker et al, “All-solid-state 704mW continuous-wave yellow source based on an intracavity, frequency-doubled crystalline Raman laser”, Optics Letters, Vol. 32, No. 9 / May 1, 2007
    [6] P. H. Chiu et al, “All-solid-state single-mode sum-frequency generation of sodium resonance radiation”, Optics Letters, Vol. 19, No. 24 / December 15, 1994
    [7] Peter Dekker et al, “Continuous-wave, intracavity doubled, self-Raman laser operation in Nd:GdVO4 at 586.5nm”, Optics Express, Vol. 15, No. 11, 28 May 2007
    [8] Shutao Li et al, “Diode-side-pumped intracavity frequency-doubled Nd:YAG/BaWO4 Raman laser generating average output power of 3.14 W at 590 nm”, Optics Letters, Vol. 32, No. 20, October 15, 2007
    [9] Richard P. Mildren et al, “Discretely tunable, all-solid-state laser in the green, yellow, and red”, Optics Letters, Vol. 30, No. 12 / June 15, 2005
    [10] H. M. Pask and J. A. Piper, “Efficient all-solid-state yellow laser source producing 1.2-W average power”, Optics Letters, Vol. 24, No. 21 / November 1, 1999

    [11] Malte Duering et al, “Generation of tunable 589nm radiation as a Na guide star source using an optical parametric amplifier”, Optics Express, Vol. 17, No. 2, 19 January 2009
    [12] Yan Feng et al, “Multiple-color cw visible lasers by frequency sum-mixing in a cascading Raman fiber laser”, Optics Express, Vol. 12 No. 93, May 2004
    [13] A. B. Rulkov1 et al, “Narrow-line, 1178nm CW bismuth-doped fiber laser with 6.4W output for direct frequency doubling”, Optics Express, Vol. 15, No. 9, 30 Apr 2007
    [14] D. Georgiev et al, “Watts-level frequency doubling of a narrow line linearly polarized Raman fiber laser to 589 nm,” Optics Express, Vol. 13, No. 18, September 2005
    [15] James T. Murray et al, “End-pumped intracavity solid state Raman lasers”, Advanced Solid State Lasers, OSA TOPS Vol. 19, 1998
    [16] T. H. Jeys et al. in Conference on Lasers and Electro-Optics (Optical Society of America, Washington, D.C., 1987), paper WE6.
    [17] Robert L. Byer, “Diode laser-pumped Solid-State Lasers”, Science, Vol.239, 12 February 1998
    [18] W. Koechner, “Solid-State Laser Engineering”, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [19] W. Koechner, “Solid-State Laser Engineering”, page 54, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [20] W. Koechner, “Solid-State Laser Engineering”, page 72,73, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [21] H. M. Pask, “The design and operation of solid-state Raman lasers”, Progress in Quantum Electronics, 27 (2003) 3-56
    [22] http://en.wikipedia.org/wiki/Raman_scattering
    [23] Singh, Rajinder, "C.V. Raman and the Discovery of the Raman Effect", Physics in Perspective (PIP) 4: 399. (2002)
    [24] Yen-Chieh Huang, “Principles of Nonlinear Optics”, course reader in the course “Nonlinear Optics” in National Tsing Hua University
    [25] http://www.rp-photonics.com/raman_scattering.html
    [26] Charles Kittel, “Introduction to Solid State Physics”, Eighth Edition, Wiley
    [27] H. M. Pask, “Continuous-wave, all-solid-state, intracavity Raman laser”, Optics Letters, Vol. 30, No. 18, September 15, 2005
    [28] L. Fan et al, “Continuous-wave intracavity Raman laser at 1179.5nm with SrWO4 Raman crystal in diode-end-pumped Nd:YVO4 laser”, Applied Physics B, 2009
    [29] Saleh and Teich, “Fundamentals of Photonics”, chapter 19, First Edition, Wiley
    [30] YC. Huang and R.L. Byer, report on “Raman gain measurement for Calcium Tungstate”, September 8, 1995
    [31] Alexander A. Kaminskii et al, “Properties of Nd3+-doped and undoped tetragonal PbWO4, NaY(WO4)2, CaWO4, and undoped monoclinic ZnWO4 and CdWO4 as laser-active and stimulated Raman scattering-active crystals”, Applied Optics, Vol. 38, No. 21, 20 July 1999
    [32] M. Bass, Handbook of Optics, McGraw-Hill, New York, 1995
    [33] T.T. Basiev et al, Optical Materials 11 (4) (1999) 307–314
    [34] T.T. Basiev et al, Applied Optics 38 (3) (1999) 594–598
    [35] Datasheet of the vendor, EXCEL OPTRONICS
    [36] Datasheet of the vendor, EKSMA OPTICS
    [37] Y.P. Lan, Y.F.Chen, S.C.Wang, “Repetition-rate dependence of thermal loading in diode-end-pumped Q-switched lasers: influence of energy-transfer upconversion”, Applied Physics B, 71, 27–31 (2000)
    [38] T. Hänsch, Applied Optics, 11, 895, 1972
    [39] I. Shoshan et al, “Narrowband operation of a pulsed dye laser without intracavity beam expansion”, Journal of Applied Physics, Vol.48, No.11, November 1977
    [40] Michael G. Littman and Harold J. Metcalf, “Spectrally narrow pulsed dye laser without beam expander”, Applied Optics, Vol. 17, No. 14, 15 July 1978
    [41] K. C. Harvey and C. J. Myatt, “External-cavity diode laser using a grazing-incidence diffraction grating”, Optics Letters, Vol. 16, No. 12, June 15, 1991
    [42] J. E. Bernard et al, “Grating-tuned, single-longitudinal-mode, diode-pumped Nd:YVO4 laser”, Optics Letters , Vol. 18, No. 23, December 1, 1993
    [43] Chi-Sheng Yu and A. H. Kung, “Grazing-incidence periodically poled LiNbO3 optical parametric oscillator”, J. Opt. Soc. Am. B, Vol. 16, No. 12, December 1999
    [44] Y. Y. Lin et al, “Single-longitudinal-mode, tunable dual-wavelength, CW Nd:YVO4 laser”, Optics Express, Vol.14, No.12, 12 June 2006
    [45] H. Kogelnik: Bell Syst. Tech. J. 44, 455 (1965)
    [46] W. Koechner, “Solid-State Laser Engineering”, page 232, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [47] W. Koechner, “Solid-State Laser Engineering”, page 233, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [48] W. Koechner, “Solid-State Laser Engineering”, page 477, 478, Sixth Revised and Updated Edition, Springer Series in OPTICAL SCIENCES
    [49] Yi-Ying Lai, “High efficiency diode pumped Nd:YAG laser using a needle-thin gain medium”, Master thesis, National Tsing Hua University
    [50] Y. F. Chen, “Efficient 1521-nm Nd:GdVO4 Raman laser”, Optics Letters , Vol. 29, No. 22, November 15, 2004
    [51] Y. F. Chen et al, “Efficient diode-pumped actively Q-switched Nd:YAG/BaWO4 intracavity Raman laser”, Optics Letters , Vol. 30, No. 24, December 15, 2005
    [52] K. W. SU et al, “Power scale-up of the diode-pumped actively Q-switched Nd:YVO4 Raman laser with an undoped YVO4 crystal as a Raman shifter”, Applied Physics B , 88, 47-50 (2007)
    [53] Kuan-Wei Su et al, “Efficient high-peak-power diode-pumped actively Q-switched Nd:YAG/YVO4 intracavity Raman laser”, Applied Optics, Vol. 47, No. 35, December 10, 2008

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