Laser – Light Amplification by Stimulated Emission of Radiation
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FABRICATION of TRANSPARENT CERAMIC LASER MEDIA for HIGH ENERGY LASER APPLICATIONS Karn Serivalsatit Clemson University, [email protected]
Clemson University TigerPrints All Dissertations Dissertations 5-2010 FABRICATION OF TRANSPARENT CERAMIC LASER MEDIA FOR HIGH ENERGY LASER APPLICATIONS Karn Serivalsatit Clemson University, [email protected] Follow this and additional works at: https://tigerprints.clemson.edu/all_dissertations Part of the Materials Science and Engineering Commons Recommended Citation Serivalsatit, Karn, "FABRICATION OF TRANSPARENT CERAMIC LASER MEDIA FOR HIGH ENERGY LASER APPLICATIONS" (2010). All Dissertations. 525. https://tigerprints.clemson.edu/all_dissertations/525 This Dissertation is brought to you for free and open access by the Dissertations at TigerPrints. It has been accepted for inclusion in All Dissertations by an authorized administrator of TigerPrints. For more information, please contact [email protected]. FABRICATION OF TRANSPARENT CERAMIC LASER MEDIA FOR HIGH ENERGY LASER APPLICATIONS A Dissertation Presented to the Graduate School of Clemson University In Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Materials Science and Engineering by Karn Serivalsatit May 2010 Accepted by: Dr. John Ballato, Committee Chair Dr. Stephen Foulger Dr. Jian Luo Dr. Eric Skaar i ABSTRACT Sesquioxides of yttrium, scandium, and lutetium, i.e., Y2O3, Sc 2O3, and Lu 2O3, have received a great deal of recent attention as potential high power solid state laser hosts. These oxides are receptive to lanthanide doping, including trivalent Er, Ho and Tm which have well known emissions at eye-safe wavelengths that can be excited using commercial diode lasers. These sesquioxides are considered superior to the more conventional yttrium aluminum garnet (YAG) due to their higher thermal conductivity, which is critical for high power laser system. Unfortunately, these oxides possess high melting temperatures, which make the growth of high purity and quality crystals using melt techniques difficult. -
Construction of a Flashlamp-Pumped Dye Laser and an Acousto-Optic
; UNITED STATES APARTMENT OF COMMERCE oUBLICATION NBS TECHNICAL NOTE 603 / v \ f ''ttis oi Construction of a Flashlamp-Pumped Dye Laser U.S. EPARTMENT OF COMMERCE and an Acousto-Optic Modulator National Bureau of for Mode-Locking Iandards — NATIONAL BUREAU OF STANDARDS 1 The National Bureau of Standards was established by an act of Congress March 3, 1901. The Bureau's overall goal is to strengthen and advance the Nation's science and technology and facilitate their effective application for public benefit. To this end, the Bureau conducts research and provides: (1) a basis for the Nation's physical measure- ment system, (2) scientific and technological services for industry and government, (3) a technical basis for equity in trade, and (4) technical services to promote public safety. The Bureau consists of the Institute for Basic Standards, the Institute for Materials Research, the Institute for Applied Technology, the Center for Computer Sciences and Technology, and the Office for Information Programs. THE INSTITUTE FOR BASIC STANDARDS provides the central basis within the United States of a complete and consistent system of physical measurement; coordinates that system with measurement systems of other nations; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scien- tific community, industry, and commerce. The Institute consists of a Center for Radia- tion Research, an Office of Measurement Services and the following divisions: Applied Mathematics—Electricity—Heat—Mechanics—Optical Physics—Linac Radiation 2—Nuclear Radiation 2—Applied Radiation 2—Quantum Electronics 3— Electromagnetics 3—Time and Frequency 3 —Laboratory Astrophysics3—Cryo- 3 genics . -
Tunable, Low-Repetition-Rate, Cost-Efficient Femtosecond Ti:Sapphire Laser for Nonlinear Microscopy
Appl Phys B (2012) 107:17–22 DOI 10.1007/s00340-011-4830-7 Tunable, low-repetition-rate, cost-efficient femtosecond Ti:sapphire laser for nonlinear microscopy P.G. Antal · R. Szipocs˝ Received: 29 July 2011 / Revised version: 26 September 2011 / Published online: 25 November 2011 © Springer-Verlag 2011 Abstract We report on a broadly tunable, long-cavity light intensity sufficient for nonlinearities, ultrashort (fs or Ti:sapphire laser oscillator being mode-locked in the net ps) pulse mode-locked lasers are used as light sources, most negative intracavity dispersion regime by Kerr-lens mode- often femtosecond pulse, tunable Ti:sapphire lasers having locking, delivering τFWHM < 300 fs pulses at 22 MHz rep- a repetition rate at around 80 MHz. etition rate. The wavelength of the laser can be tuned over Multiphoton transitions of intracellular fluorophores used a 170 nm wide range between 712 nm and 882 nm. Hav- in microscopy can be efficiently excited in the 700–1200 nm ing a typical pump power of 2.6 W, the maximum pulse spectral region, which wavelengths penetrate deeper in tis- peak power is 60 kW. Comparison of the reported laser sues and are much less harmful for living specimen than with a standard, 76 MHz Ti:sapphire oscillator regarding direct UV illumination in single-photon fluorescent mi- two-photon excitation efficiency in a laser scanning micro- croscopy. Photochemical damage mechanisms, which can scope shows that the 22 MHz laser generates the same flu- cause oxidative stress or direct DNA damage, only occur orescence signal at considerably, 1.82 times lower average in the focus of the objective lens, where multiphoton ab- power, which is expected to result in a reduced photothermal sorption takes place. -
Fibre Lasers – Conditioning Constructional and Technological
BULLETIN OF THE POLISH ACADEMY OF SCIENCES OPTOELECTRONICS TECHNICAL SCIENCES, Vol. 58, No. 4, 2010 DOI: 10.2478/v10175-010-0048-9 Fibre lasers – conditioning constructional and technological A. ZAJĄC1,2∗, D. DOROSZ2, M. KOCHANOWICZ2, M. SKÓRCZAKOWSKI1, and J. ŚWIDERSKI1 1, Institute of Optoelectronics, Military University of Technology, 2 Kaliskiego St., 00-908 Warszawa, Poland 2 Faculty of Electrical Engineering, Bialystok University of Technology, 45d Wiejska St., 15-351 Białystok, Poland Abstract. In this paper the actual level of fiber lasers’ development is presented. There is also presented the analysis of technological and constructional conditions that limit energy parameters of those sources. Authors also show a construction and a technological work, conducted in Poland, which led to improving energy and exploit parameters of fiber lasers. Key words: fibre lasers, conditioning constructional, conditioning technological. 1. Introduction Typical, basically known the 1964’s configuration of a fiber laser set-up fulfils two basic conditions: an active cen- The year of 1960 was a breakthrough in the optical science – tre is a core of an optical fiber with addition of rare earth ions on 16th May the first laser was built. (it is likely to use a single-mode fiber but in many applica- The properties of laser beam – monochromatic, coherent tions also a multi-mode fiber is used), an active addition is and collimated beam – had not been possible to get in exist- optically stimulated – for lasers of medium and high power ing sources of optical radiation in visible spectrum until that it is effective in the configuration of lateral pumping (dis- moment. -
Laser Tutorial
36ch_LaserGuide_f_v3.qxd 6/8/2005 11:16 AM Page 36.2 Basic Laser Principles www.mellesgriot.com Lasers are devices that produce intense beams of light which For an electron to jump to a higher quantum state, the atom are monochromatic, coherent, and highly collimated. The wavelength must receive energy from the outside world. This can happen through (color) of laser light is extremely pure (monochromatic) when com- a variety of mechanisms such as inelastic or semielastic collisions pared to other sources of light, and all of the photons (energy) that with other atoms and absorption of energy in the form of electro- make up the laser beam have a fixed phase relationship (coherence) magnetic radiation (e.g., light). Likewise, when an electron drops with respect to one another. Light from a laser typically has very from a higher state to a lower state, the atom must give off energy, low divergence. It can travel over great distances or can be focused either as kinetic activity (nonradiative transitions) or as electro- to a very small spot with a brightness which exceeds that of the magnetic radiation (radiative transitions). For the remainder of sun. Because of these properties, lasers are used in a wide variety this discussion we will consider only radiative transitions. of applications in all walks of life. The basic operating principles of the laser were put forth PHOTONS AND ENERGY by Charles Townes and Arthur Schalow from the Bell Telephone In the 1600s and 1700s, early in the modern study of light, there Laboratories in 1958, and the first actual laser, based on a pink was a great controversy about light’s nature. -
1 LASERS LASER Is the Acronym for Light Amplification by Stimulated
1 LASERS LASER is the acronym for Light Amplification by Stimulated Emission of Radiation. Laser is a light source but quite different from conventional light sources. In conventional light sources different atoms emit radiations at different times and in different directions and there is no phase relationship between them Light from an incandescent lamp is an example of incoherent radiation and it is spread over a continuous range of wavelengths The characteristics of laser light : i) The light is coherent which means that waves all exactly in phase with one another It is possible to observe interference effects from two independent lasers ii) The light is monochromatic ( same frequency ) in the visible region of the electromagnetic spectrum. The spread in wavelength () is extremely small. Ordinary incandescent light is spread over a continuous range iii) The beam is very narrow, highly directional and does not diverge . The directionality of the laser beam is expressed in terms of divergence = ( r2 --r1)/ ( D2 --D1) where r2 and r1 are the radii of laser beam spots at distances D2 and D1, respectively. iv)The laser beam is extremely intense. The intensity of laser beam is expressed by number of photons coming out from the laser per second per unit area. It is about 1022 to 1034 photons /sec/sq cm Lasers are based on the concept of amplification of light by stimulated emission of radiation by matter. Einstein predicted this possibility of stimulated emission in 1917 but the first laser was built bt T.A.Maiman in 1960. To explain the working principle of a laser, let us consider the interaction of photons with atoms. -
Infrared Laser Catheter Apparatus
~" ' MM II II II Ml II I II III II II II I II J European Patent Office © Publication number: 0 214 712 B1 Office_„. europeen- desj brevets^ » © EUROPEAN PATENT SPECIFICATION © Date of publication of patent specification: 02.09.92 © Int. CI.5: A61 B 17/00, A61B 17/36 © Application number: 86303982.2 @ Date of filing: 27.05.86 © Infrared laser catheter apparatus. ® Priority: 31.07.85 US 761188 © Proprietor: C.R. BARD, INC. 731 Central Avenue @ Date of publication of application: Murray Hill New Jersey 07974(US) 18.03.87 Bulletin 87/12 @ Inventor: Slnofsky, Edward © Publication of the grant of the patent: Apartment 8 South Washington Street 02.09.92 Bulletin 92/36 Reading Massachusetts(US) © Designated Contracting States: DE FR GB IT NL © Representative: Woodward, John Calvin et al VENNER SHIPLEY & CO. 368 City Road © References cited: London EC1V 2QA(GB) EP-A- 0 153 847 GB-A- 2 017 506 GB-A- 2 125 986 US-A- 3 327 712 US-A- 4 383 729 US-A- 4 458 683 ELECTRONIC DESIGN, vol. 17, no. 13, June 21, 1969, pp 36, 38, 40 D.N. KAYE: "The happy merger of fiber optics and lasers" 00 CM s O Note: Within nine months from the publication of the mention of the grant of the European patent, any person ^ may give notice to the European Patent Office of opposition to the European patent granted. Notice of opposition qj shall be filed in a written reasoned statement. It shall not be deemed to have been filed until the opposition fee has been paid (Art. -
Chapter 4 the Quantum Theory of Light
Chapter 4 The quantum theory of light In this chapter we study the quantum theory of interactions between light and matter. Historically the understanding how light is created and absorbed by atoms was central for development of quantum theory, starting with Planck’s revolutionary idea of energy quanta in the description of black body radiation. Today a more complete description is given by the theory of quantum electrodynamics (QED), which is a part of a more general relativistic quantum field theory (the standard model) that describe the physics of the elementary particles. Even so the the non- relativistic theory of photons and atoms has continued to be important, and has been developed further, in directions that are referred to as quantum optics. We will study here the basics of the non-relativistic description of interactions between photons and atoms, in particular with respect to the processes of spontaneous and stimulated emission. As a particular application we study a simple model of a laser as a source of coherent light. 4.1 Classical electromagnetism The Maxwell theory of electromagnetism is the basis for the classical as well as the quantum description of radiation. With some modifications due to gauge invariance and to the fact that this is a field theory (with an infinite number of degrees of freedom) the quantum theory can be derived from classical theory by the standard route of canonical quantization. In this approach the natural choice of generalized coordinates correspond to the field amplitudes. In this section we make a summary of the classical theory and show how a Lagrangian and Hamiltonian formulation of electromagnetic fields interacting with point charges can be given. -
Numerical Study of the Dynamics of Laser Lineshape and Linewidth M
Vol. 130 (2016) ACTA PHYSICA POLONICA A No. 3 Numerical Study of the Dynamics of Laser Lineshape and Linewidth M. Eskef∗ Department of Physics, Atomic Energy Commission of Syria, P.O. Box 6091, Damascus, Syria (Received January 28, 2015; revised version May 31, 2016; in final form July 27, 2016) A rate equations model for lasers with homogeneously broadened gain is written and solved in both time and frequency domains. The model is applied to study the dynamics of laser lineshape and linewidth using the example of He–Ne laser oscillating at λ = 632:8 nm. Saturation of the frequency spectrum is found to take much longer time compared to the saturation time of the overall power. The saturated lineshape proves to be Lorentzian, whereas the unsaturated line profile is found to have a Gaussian peak and a Lorentzian tail. Above threshold, our numerical results for the linewidth are in good agreement with the Schawlow–Townes formula. Below threshold, however, the linewidth is found to have an upper limit defined by the spectral width of the pure cavity. Our model provides a unique and powerful tool for studying the dynamics of the frequency spectrum for different kinds of laser systems, and is also applicable for investigating lineshape and linewidth of pulsed lasers. DOI: 10.12693/APhysPolA.130.710 PACS/topics: 42.55.Ah, 42.55.Lt 1. Introduction give no information about the dynamics of lineshape and Laser lineshape and linewidth play a key role in the- linewidth. Second, their way of calculating lineshape and oretical studies related to the fields of resonance ion- linewidth leads through the implicit assumption that the ization spectroscopy (RIS) [1, 2], laser isotope separa- laser field can be represented by a complex amplitude tion [3], as well as resonance ionization mass spectrome- oscillating at the resonance frequency of the pure cav- try (RIMS) [4]. -
Construction and Measurement of an Actively Mode-Locked Sigma Laser
Calhoun: The NPS Institutional Archive Theses and Dissertations Thesis Collection 1998-06 Construction and measurement of an actively mode-locked sigma laser Butler, James M. Monterey, California. Naval Postgraduate School http://hdl.handle.net/10945/8146 DUOU=\ c SCHOOL <> NPS-EC-98-011 NAVAL POSTGRADUATE SCHOOL MONTEREY, CALIFORNIA THESIS CONSTRUCTION AND MEASUREMENT OF AN ACTIVELY MODE-LOCKED SIGMA LASER by James M. Butler June, 1998 Thesis Co-Advisors: Phillip E. Pace John P. Powers Approved for public release; distribution is unlimited. Prepared for: Center for Reconnaissance Research Naval Postgraduate School Monterey, CA NAVAL POSTGRADUATE SCHOOL Monterey, California 93943 Rear Admiral Chaplain Superintendent This thesis was prepared in conjunction with research sponsored in part by the Center for Reconnaissance Research at the Naval Postgraduate School. Reproduction of all or part of this report is authorized. 1 REPORT DOCUMENTATION PAGE Form Approved OMB N'o 0704-0188 Public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instruction, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing the collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite 1204, Arlington, VA 22202-4302, and to the Office of Management and Budget, Paperwork Reduction Project (0704-0188) Washington DC 20503. 1 . AGENCY USE ONLY (Leave blank) REPORT DATE 3. REPORT TYPE AND DATES COVERED June 1998 Master's Thesis TITLE AND SUBTITLE TITLE. -
Stimulated Emission from a Single Excited Atom in a Waveguide
week ending PRL 108, 143602 (2012) PHYSICAL REVIEW LETTERS 6 APRIL 2012 Stimulated Emission from a Single Excited Atom in a Waveguide Eden Rephaeli1,* and Shanhui Fan2,† 1Department of Applied Physics, Stanford University, Stanford, California 94305, USA 2Department of Electrical Engineering, Stanford University, Stanford, California 94305, USA (Received 6 September 2011; published 3 April 2012) We study stimulated emission from an excited two-level atom coupled to a waveguide containing an incident single-photon pulse. We show that the strong photon correlation, as induced by the atom, plays a very important role in stimulated emission. Additionally, the temporal duration of the incident photon pulse is shown to have a marked effect on stimulated emission and atomic lifetime. DOI: 10.1103/PhysRevLett.108.143602 PACS numbers: 42.50.Ct, 42.50.Gy, 78.45.+h Introduction.—Stimulated emission, first formulated by In recent years, there has been much advancement in Einstein in 1917 [1], is the fundamental physical mecha- the capacity to deterministically generate single photons nism underlying the operation of lasers [2] and optical [25,26] and to control the shape of the single-photon pulse amplifiers [3,4], both of which are of paramount impor- [27,28]. In both waveguide and free space, a single photon, tance in modern technology. In recent years, stimulated by necessity, must exist as a pulse [29]. Therefore, our emission has been studied in a variety of novel systems, study of stimulated emission at the single-photon level including a surface plasmon nanosystem [5], a single mole- reveals important dynamic characteristics of stimulated cule transistor [6], and superconducting transmission lines emission. -
Construction of an Interference-Filter-Stabilized Diode
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