Optofluidic Dye Lasers
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An Application of the Theory of Laser to Nitrogen Laser Pumped Dye Laser
SD9900039 AN APPLICATION OF THE THEORY OF LASER TO NITROGEN LASER PUMPED DYE LASER FATIMA AHMED OSMAN A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Physics. UNIVERSITY OF KHARTOUM FACULTY OF SCIENCE DEPARTMENT OF PHYSICS MARCH 1998 \ 3 0-44 In this thesis we gave a general discussion on lasers, reviewing some of are properties, types and applications. We also conducted an experiment where we obtained a dye laser pumped by nitrogen laser with a wave length of 337.1 nm and a power of 5 Mw. It was noticed that the produced radiation possesses ^ characteristic^ different from those of other types of laser. This' characteristics determine^ the tunability i.e. the possibility of choosing the appropriately required wave-length of radiation for various applications. DEDICATION TO MY BELOVED PARENTS AND MY SISTER NADI A ACKNOWLEDGEMENTS I would like to express my deep gratitude to my supervisor Dr. AH El Tahir Sharaf El-Din, for his continuous support and guidance. I am also grateful to Dr. Maui Hammed Shaded, for encouragement, and advice in using the computer. Thanks also go to Ustaz Akram Yousif Ibrahim for helping me while conducting the experimental part of the thesis, and to Ustaz Abaker Ali Abdalla, for advising me in several respects. I also thank my teachers in the Physics Department, of the Faculty of Science, University of Khartoum and my colleagues and co- workers at laser laboratory whose support and encouragement me created the right atmosphere of research for me. Finally I would like to thank my brother Salah Ahmed Osman, Mr. -
Laser Linewidth, Frequency Noise and Measurement
Laser Linewidth, Frequency Noise and Measurement WHITEPAPER | MARCH 2021 OPTICAL SENSING Yihong Chen, Hank Blauvelt EMCORE Corporation, Alhambra, CA, USA LASER LINEWIDTH AND FREQUENCY NOISE Frequency Noise Power Spectrum Density SPECTRUM DENSITY Frequency noise power spectrum density reveals detailed information about phase noise of a laser, which is the root Single Frequency Laser and Frequency (phase) cause of laser spectral broadening. In principle, laser line Noise shape can be constructed from frequency noise power Ideally, a single frequency laser operates at single spectrum density although in most cases it can only be frequency with zero linewidth. In a real world, however, a done numerically. Laser linewidth can be extracted. laser has a finite linewidth because of phase fluctuation, Correlation between laser line shape and which causes instantaneous frequency shifted away from frequency noise power spectrum density (ref the central frequency: δν(t) = (1/2π) dφ/dt. [1]) Linewidth Laser linewidth is an important parameter for characterizing the purity of wavelength (frequency) and coherence of a Graphic (Heading 4-Subhead Black) light source. Typically, laser linewidth is defined as Full Width at Half-Maximum (FWHM), or 3 dB bandwidth (SEE FIGURE 1) Direct optical spectrum measurements using a grating Equation (1) is difficult to calculate, but a based optical spectrum analyzer can only measure the simpler expression gives a good approximation laser line shape with resolution down to ~pm range, which (ref [2]) corresponds to GHz level. Indirect linewidth measurement An effective integrated linewidth ∆_ can be found by can be done through self-heterodyne/homodyne technique solving the equation: or measuring frequency noise using frequency discriminator. -
Self Amplified Lock of a Ultra-Narrow Linewidth Optical Cavity
Self Amplified Lock of a Ultra-narrow Linewidth Optical Cavity Kiwamu Izumi,1, ∗ Daniel Sigg,1 and Lisa Barsotti2 1LIGO Hanford Observatory, PO Box 159 Richland, Washington 99354, USA 2LIGO laboratory, Massachusetts Institute of Technology, Cambridge, Massachussetts 02139, USA compiled: January 8, 2016 High finesse optical cavities are an essential tool in modern precision laser interferometry. The incident laser field is often controlled and stabilized with an active feedback system such that the field resonates in the cavity. The Pound-Drever-Hall reflection locking technique is a convenient way to derive a suitable error signal. However, it only gives a strong signal within the cavity linewidth. This poses a problem for locking a ultra-narrow linewidth cavity. We present a novel technique for acquiring lock by utilizing an additional weak control signal, but with a much larger capture range. We numerically show that this technique can be applied to the laser frequency stabilization system used in the Laser Interferometric Gravitational-wave Observatory (LIGO) which has a linewidth of 0.8 Hz. This new technique will allow us to robustly and repeatedly lock the LIGO laser frequency to the common mode of the interferometer. OCIS codes: (140.3425), (140.3410) http://dx.doi.org/10.1364/XX.99.099999 High finesse optical cavities have been an indispens- nonlinear response [8, 9] dominant and thus hinder the able tool for precision interferometry to conduct rela- linear controller. tivistic experiments such as gravitational wave detection Gravitational wave observatories deploy kilometer [1{3] and optical clocks [4]. The use of a high finesse cav- scale interferometers with extremely narrow linewidth. -
PG0308 Pulsed Dye Laser Therapy for Cutaneous Vascular Lesions
Pulsed Dye Laser Therapy for Cutaneous Vascular Lesions Policy Number: PG0308 ADVANTAGE | ELITE | HMO Last Review: 09/22/2017 INDIVIDUAL MARKETPLACE | PROMEDICA MEDICARE PLAN | PPO GUIDELINES This policy does not certify benefits or authorization of benefits, which is designated by each individual policyholder contract. Paramount applies coding edits to all medical claims through coding logic software to evaluate the accuracy and adherence to accepted national standards. This guideline is solely for explaining correct procedure reporting and does not imply coverage and reimbursement. SCOPE X Professional _ Facility DESCRIPTION Port-wine stains (PWS) are a type of vascular lesion involving the superficial capillaries of the skin. At birth, the lesions typically appear as flat, faint, pink macules. With increasing age, they darken and become raised, red-to- purple nodules and papules in adults. Congenital hemangiomas are benign tumors of the vascular endothelium that appear at or shortly after birth. Hemangiomas are characterized by rapid proliferation in infancy and a period of slow involution that can last for several years. Complete regression occurs in approximately 50% of children by 5 years of age and 90% of children by 9 years of age. The goals of pulsed dye laser (PDL) therapy for cutaneous vascular lesions, specifically PWS lesions and hemangiomas, are to remove, lighten, reduce in size, or cause regression of the lesions to relieve symptoms, to alleviate or prevent medical or psychological complications, and to improve cosmetic appearance. This is accomplished by the preferential absorption of PDL energy by the hemoglobin within these vascular lesions, which causes their thermal destruction while sparing the surrounding normal tissues. -
Power Build-Up Cavity Coupled to a Laser Diode
I POWER BUILD-UP CAVITY COUPLED I TO A LASER DIODE Daniel J. Evans I Center of Excellence for Raman Technology University of Utah I Abstract combination of these elements will emit photons at different frequencies. The ends of these semiconductor In many Raman applications there is a need to devices are cleaved to form mirrors that bounce the I detect gases in the low ppb range. The desired photons back and forth within the cavity. The photons sensitivity can be achieved by using a high power laser excite more electrons, which form more photons source in the range of tens of watts. A system (referred to as optical pumping). 2 A certain portion of I combining a build-up cavity to enhance the power and the photons emit through the front and back cleaved an external cavity laser diode setup to narrow the surfaces of the laser diode. The amount of photons that bandwidth can give the needed power to the Raman get through the cleaved surfaces can be adjusted by I spectroscopy system. coating the surface or installing other mirrors. Introduction to Laser Diodes The planar cleaved surfaces of the laser diode form a Fabry-Perot cavity with set resonance frequencies I An important characteristic of all lasers is the (vp).3 The typical laser diode has a spacing of 150 f.1I11 mode structure. The mode structure refers to both the with an index of refraction of 3.5, yielding a resonance lasing frequency and the spatial characteristics of the frequency of 285 GHz. The wavelength spacing (~A.) I laser. -
Quantum Illumination at the Microwave Wavelengths
Quantum Illumination at the Microwave Wavelengths 1 2 3 4 5 6, Shabir Barzanjeh, Saikat Guha, Christian Weedbrook, David Vitali, Jeffrey H. Shapiro, and Stefano Pirandola ∗ 1Institute for Quantum Information, RWTH Aachen University, 52056 Aachen, Germany 2Quantum Information Processing Group, Raytheon BBN Technologies, Cambridge, Massachusetts 02138, USA 3QKD Corp., 60 St. George St., Toronto, M5S 3G4, Canada 4School of Science and Technology, University of Camerino, Camerino, Macerata 62032, Italy 5Research Laboratory of Electronics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 6Department of Computer Science & York Centre for Quantum Technologies, University of York, York YO10 5GH, United Kingdom Quantum illumination is a quantum-optical sensing technique in which an entangled source is exploited to improve the detection of a low-reflectivity object that is immersed in a bright thermal background. Here we describe and analyze a system for applying this technique at microwave frequencies, a more appropriate spectral region for target detection than the optical, due to the naturally-occurring bright thermal background in the microwave regime. We use an electro-opto- mechanical converter to entangle microwave signal and optical idler fields, with the former being sent to probe the target region and the latter being retained at the source. The microwave radiation collected from the target region is then phase conjugated and upconverted into an optical field that is combined with the retained idler in a joint-detection -
Amplified Spontaneous Emission and Lasing in Lead Halide
applied sciences Review Amplified Spontaneous Emission and Lasing in Lead Halide Perovskites: State of the Art and Perspectives Maria Luisa De Giorgi and Marco Anni * Dipartimento di Matematica e Fisica “Ennio De Giorgi”, Università del Salento, Via per Arnesano, 73100 Lecce, Italy; [email protected] * Correspondence: [email protected]; Tel.: +39-0832-297540 Received: 9 October 2019; Accepted: 24 October 2019; Published: 29 October 2019 Abstract: Lead halide perovskites are currently receiving increasing attention due to their potential to combine easy active layers fabrication, tunable electronic and optical properties with promising performance of optoelectronic and photonic device prototypes. In this paper, we review the main development steps and the current state of the art of the research on lead halide perovskites amplified spontaneous emission and on optically pumped lasers exploiting them as active materials. Keywords: lead halide perovskite; thin film; nanocrystal; optical gain; amplified spontaneous emission; laser 1. Introduction In the frame of developing novel active materials for electronic, optoelectronic and photonic devices, lead halide perovskites are currently receiving great attention due to their capability to combine an easy realization procedure, widely tunable electronic properties and promising performance as active materials for a wide range of devices. In particular, perovskite-based solar cells demonstrated an impressively fast power conversion efficiency increase, from 3.8% in TiO2 sensitized photoelectrochemical cells [1], to the recent record value of 25.2% [2] in thin film solar cells. Lead halide perovskites also showed interesting photoluminescence (PL) and electroluminescence properties, which stimulated the research in light emitting devices, such as light emitting diodes (LEDs) [3]. -
Narrow Line Width Frequency Comb Source Based on an Injection-Locked III-V-On-Silicon Mode-Locked Laser
Narrow line width frequency comb source based on an injection-locked III-V-on-silicon mode-locked laser Sarah Uvin,1;2;∗ Shahram Keyvaninia,3 Francois Lelarge,4 Guang-Hua Duan,4 Bart Kuyken1;2 and Gunther Roelkens1;2 1Photonics Research Group, Department of Information Technology, Ghent University - imec, Sint-Pietersnieuwstraat 41, 9000 Ghent, Belgium 2Center for Nano- and Biophotonics (NB-Photonics), Ghent University, Ghent, Belgium 3Fraunhofer Heinrich-Hertz-Institut Einsteinufer 37 10587, Berlin, Germany 4III-V lab, a joint lab of Alcatel-Lucent Bell Labs France, Thales Research and Technology and CEA Leti, France ∗[email protected] Abstract: In this paper, we report the optical injection locking of an L-band (∼1580 nm) 4.7 GHz III-V-on-silicon mode-locked laser with a narrow line width continuous wave (CW) source. This technique allows us to reduce the MHz optical line width of the mode-locked laser longitudinal modes down to the line width of the source used for injection locking, 50 kHz. We show that more than 50 laser lines generated by the mode-locked laser are coherent with the narrow line width CW source. Two locking techniques are explored. In a first approach a hybrid mode-locked laser is injection-locked with a CW source. In a second approach, light from a modulated CW source is injected in a passively mode-locked laser cavity. The realization of such a frequency comb on a chip enables transceivers for high spectral efficiency optical communication. © 2016 Optical Society of America OCIS codes: (250.5300) Photonic integrated circuits; (140.4050) Mode-locked lasers. -
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 . -
Arxiv:2106.00060V1 [Physics.Optics] 31 May 2021
Self-injection locking of the gain-switched laser diode Artem E. Shitikov1,∗ Valery E. Lobanov1, Nikita M. Kondratiev1, Andrey S. Voloshin2, Evgeny A. Lonshakov1, and Igor A. Bilenko1,3 1Russian Quantum Center, 143026 Skolkovo, Russia 2Institute of Physics, Swiss Federal Institute of Technology Lausanne (EPFL), CH-1015 Lausanne, Switzerland and 3Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia (Dated: April 2021) We experimentally observed self-injection locking regime of the gain-switched laser to high-Q optical microresonator. We revealed that comb generated by the gain-switched laser experiences a dramatic reduce of comb teeth linewidths in this regime. We demonstrated the Lorentzian linewidth of the comb teeth of sub-kHz scale as narrow as for non-switched self-injection locked laser. Such setup allows generation of high-contrast electrically-tunable optical frequency combs with tunable comb line spacing in a wide range from 10 kHz up to 10 GHz. The characteristics of the generated combs were studied for various modulation parameters - modulation frequency and amplitude, and for parameters, defining the efficiency of the self-injection locking - locking phase, coupling efficiency, pump frequency detuning. I. INTRODUCTION In this work, we developed the first microresonator stabilized gain-switched laser operating in the SIL Narrow-linewidth lasers are in increasing demand in regime. We demonstrated experimentally high-contrast science and bleeding edge technologies as they give a electrically tuned optical frequency combs with line competitive advantage in such areas as coherent com- spacing from 10 kHz to 10 GHz. It was revealed that munications [1], high-precision spectroscopy [2, 3], op- SIL leads to a frequency distillation of each comb teeth tical clocks [4, 5], ultrafast optical ranging [6–8] and and consequently increase the comb contrast. -
2.6 Q-Switched Erbium-Doped Fiber Laser
COPYRIGHT AND CITATION CONSIDERATIONS FOR THIS THESIS/ DISSERTATION o Attribution — You must give appropriate credit, provide a link to the license, and indicate if changes were made. You may do so in any reasonable manner, but not in any way that suggests the licensor endorses you or your use. o NonCommercial — You may not use the material for commercial purposes. o ShareAlike — If you remix, transform, or build upon the material, you must distribute your contributions under the same license as the original. How to cite this thesis Surname, Initial(s). (2012) Title of the thesis or dissertation. PhD. (Chemistry)/ M.Sc. (Physics)/ M.A. (Philosophy)/M.Com. (Finance) etc. [Unpublished]: University of Johannesburg. Retrieved from: https://ujcontent.uj.ac.za/vital/access/manager/Index?site_name=Research%20Output (Accessed: Date). Development, characterisation and analysis of an active Q-switched fiber laser based on the modulation of a fiber Fabry-Perot tunable filter By KABOKO JEAN-JACQUES MONGA DISSERTATION Submitted for partial fulfillment of the requirements for the degree DOCTOR OF PHILOSOPHY in ELECTRICAL AND ELECTRONIC ENGINEERING SCIENCES in the FACULTY OF ENGINEERING at the UNIVERSITY OF JOHANNESBURG STUDY LEADERS: Dr. Rodolfo Martinez Manuel Pr. Johan Meyer April 2018 Abstract The field of fiber lasers and fiber optic devices has experienced a sustained rapid growth. In particular, all-fiber Q-switched lasers offer inherent advantages of relatively low cost, compact design, light weight, low maintenance, and increased robustness and simplicity over other fiber laser systems. In this thesis, a design of a new Q-switching approach in all-fiber based laser is proposed. -
Development of the LDS698 Solid Dye Laser for High Durability
Transactions of the Korean Nuclear Society Spring Meeting Chuncheon, Korea, May 25-26 2006 Development of the LDS698 Solid Dye Laser for High Durability Ji-Hun Kim, Chan-Ju Lim, Sang-Beom Joa and Heon-Ju Lee Faculty of Mechanical & Energy System Engineering, Cheju National Univ., 1 Ara-1 Dong, Jeju-Do, Korea [email protected] 1. Introduction grazing incidence configuration with an incident angle of 11.4°. The reflectivity of the rear mirror is 99% and It is essential to use a tunable laser in atomic its dimension are 50 × 50mm. The reflectivity of the spectroscopy and environmental analysis. LDS 698 dye partial reflector is 10% at 650nm. The solid dye cell is laser can be used for hydrogen plasma spectroscopy. located between the total reflector and the diffraction Solid dye laser has the advantages that are cheap, grating. The partial reflector is in the direction of 1st compact and simple to operate. Recently, compact solid order diffracted light from the grating. The length of the dye lasers have been developed by many researchers resonator is 80 nm. The solid dye cell is pumped by the with various solid-host materials by the sol-gel and 2nd harmonics of the Nd-YAG laser (532nm). When a polymerization methods. However, the durability is the narrower spectrum or a scanning of the spectrum is main problem in the solid dye laser because of the dye needed, it can be achieved by adding a turning mirror at bleaching. To fabricate the reliable diagnostic system of the position of the 0th order diffraction beam.