Pulse Shaping and Ultrashort Laser Pulse Filamentation for Applications in Extreme Nonlinear Optics Antonio Lotti
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Near-Infrared Optical Modulation for Ultrashort Pulse Generation Employing Indium Monosulfide (Ins) Two-Dimensional Semiconductor Nanocrystals
nanomaterials Article Near-Infrared Optical Modulation for Ultrashort Pulse Generation Employing Indium Monosulfide (InS) Two-Dimensional Semiconductor Nanocrystals Tao Wang, Jin Wang, Jian Wu *, Pengfei Ma, Rongtao Su, Yanxing Ma and Pu Zhou * College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China; [email protected] (T.W.); [email protected] (J.W.); [email protected] (P.M.); [email protected] (R.S.); [email protected] (Y.M.) * Correspondence: [email protected] (J.W.); [email protected] (P.Z.) Received: 14 May 2019; Accepted: 3 June 2019; Published: 7 June 2019 Abstract: In recent years, metal chalcogenide nanomaterials have received much attention in the field of ultrafast lasers due to their unique band-gap characteristic and excellent optical properties. In this work, two-dimensional (2D) indium monosulfide (InS) nanosheets were synthesized through a modified liquid-phase exfoliation method. In addition, a film-type InS-polyvinyl alcohol (PVA) saturable absorber (SA) was prepared as an optical modulator to generate ultrashort pulses. The nonlinear properties of the InS-PVA SA were systematically investigated. The modulation depth and saturation intensity of the InS-SA were 5.7% and 6.79 MW/cm2, respectively. By employing this InS-PVA SA, a stable, passively mode-locked Yb-doped fiber laser was demonstrated. At the fundamental frequency, the laser operated at 1.02 MHz, with a pulse width of 486.7 ps, and the maximum output power was 1.91 mW. By adjusting the polarization states in the cavity, harmonic mode-locked phenomena were also observed. To our knowledge, this is the first time an ultrashort pulse output based on InS has been achieved. -
Modern Quantum Kinetic Theory and Spectral Line Shapes
LOUIS MONCHICK MODERN QUANTUM KINETIC THEORY AND SPECTRAL LINE SHAPES The modern quantum kinetic theory of spectral line hapes i outlined and a typical calculation of a Ra man scattered line hape described. The distingui hing feature of thi calculation i that it was completely ab initio and therefore con tituted a test of modern quantum kinetic theor ,the tate of the art in computing molecular-scattering cross sections, and novel method of olving kinetic equation. The computation em ployed a large assortment of tools: group theory finite-element method. cIa ic method of solving cou pled sets of ordinary differential equations, graph method of combining angular momenta, and matrix methods of solving integral equations. Agreement with experimental re ult wa excellent. THE PROBLEM Almo t with the inception of quantum mechanics, parison. 1 the a ailability of an extremely good model of theorists-mostly nuclear and atomic physici t -had the interaction of helium ith two deuterium atoms, and developed the general scattering equations neces ary to the feasibilit of carrying out the calculation in a finite describe collision between fundamental particles. With time and at a rea onable co t. The goal which we did not almost no exception, however, only a few angular quite reach. a an entirely ab initio computation con momentum and spin states were invol ed; as a re ult, taining a umption only about the rate of convergence these calculations were not computationally intensive. In of the numerical procedure u ed, ith no e peri mental principle, the general methodology was applicable to the quantitie except Planck' and Boltzmann' con tant calculation of molecular inela tic and reactive colli ion, and the electronic charg and mas of the electron, deuter which are important ingredients of reaction rates. -
Autocorrelation and Frequency-Resolved Optical Gating Measurements Based on the Third Harmonic Generation in a Gaseous Medium
Appl. Sci. 2015, 5, 136-144; doi:10.3390/app5020136 OPEN ACCESS applied sciences ISSN 2076-3417 www.mdpi.com/journal/applsci Article Autocorrelation and Frequency-Resolved Optical Gating Measurements Based on the Third Harmonic Generation in a Gaseous Medium Yoshinari Takao 1,†, Tomoko Imasaka 2,†, Yuichiro Kida 1,† and Totaro Imasaka 1,3,* 1 Department of Applied Chemistry, Graduate School of Engineering, Kyushu University, 744, Motooka, Nishi-ku, Fukuoka 819-0395, Japan; E-Mails: [email protected] (Y.T.); [email protected] (Y.K.) 2 Laboratory of Chemistry, Graduate School of Design, Kyushu University, 4-9-1, Shiobaru, Minami-ku, Fukuoka 815-8540, Japan; E-Mail: [email protected] 3 Division of Optoelectronics and Photonics, Center for Future Chemistry, Kyushu University, 744, Motooka, Nishi-ku, Fukuoka 819-0395, Japan † These authors contributed equally to this work. * Author to whom correspondence should be addressed; E-Mail: [email protected]; Tel.: +81-92-802-2883; Fax: +81-92-802-2888. Academic Editor: Takayoshi Kobayashi Received: 7 April 2015 / Accepted: 3 June 2015 / Published: 9 June 2015 Abstract: A gas was utilized in producing the third harmonic emission as a nonlinear optical medium for autocorrelation and frequency-resolved optical gating measurements to evaluate the pulse width and chirp of a Ti:sapphire laser. Due to a wide frequency domain available for a gas, this approach has potential for use in measuring the pulse width in the optical (ultraviolet/visible) region beyond one octave and thus for measuring an optical pulse width less than 1 fs. -
Stark Broadening Measurements in Plasmas Produced by Laser Ablation of Hydrogen Containing Compounds Miloš Burger, Jorg Hermann
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Archive Ouverte en Sciences de l'Information et de la Communication Stark broadening measurements in plasmas produced by laser ablation of hydrogen containing compounds Miloš Burger, Jorg Hermann To cite this version: Miloš Burger, Jorg Hermann. Stark broadening measurements in plasmas produced by laser ablation of hydrogen containing compounds. Spectrochimica Acta Part B: Atomic Spectroscopy, Elsevier, 2016, 122, pp.118-126. 10.1016/j.sab.2016.06.005. hal-02348424 HAL Id: hal-02348424 https://hal.archives-ouvertes.fr/hal-02348424 Submitted on 5 Nov 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Stark broadening measurements in plasmas produced by laser ablation of hydrogen containing compounds Milosˇ Burgera,∗,Jorg¨ Hermannb aUniversity of Belgrade, Faculty of Physics, POB 44, 11000 Belgrade, Serbia bLP3, CNRS - Aix-Marseille University, 13008 Marseille, France Abstract We present a method for the measurement of Stark broadening parameters of atomic and ionic spectral lines based on laser ablation of hydrogen containing compounds. Therefore, plume emission spectra, recorded with an echelle spectrometer coupled to a gated detector, were compared to the spectral radiance of a plasma in local thermal equi- librium. -
The Science and Applications of Ultrafast, Ultraintense Lasers
THE SCIENCE AND APPLICATIONS OF ULTRAFAST, ULTRAINTENSE LASERS: Opportunities in science and technology using the brightest light known to man A report on the SAUUL workshop held, June 17-19, 2002 THE SCIENCE AND APPLICATIONS OF ULTRAFAST, ULTRAINTENSE LASERS (SAUUL) A report on the SAUUL workshop, held in Washington DC, June 17-19, 2002 Workshop steering committee: Philip Bucksbaum (University of Michigan) Todd Ditmire (University of Texas) Louis DiMauro (Brookhaven National Laboratory) Joseph Eberly (University of Rochester) Richard Freeman (University of California, Davis) Michael Key (Lawrence Livermore National Laboratory) Wim Leemans (Lawrence Berkeley National Laboratory) David Meyerhofer (LLE, University of Rochester) Gerard Mourou (CUOS, University of Michigan) Martin Richardson (CREOL, University of Central Florida) 2 Table of Contents Table of Contents . 3 Executive Summary . 5 1. Introduction . 7 1.1 Overview . 7 1.2 Summary . 8 1.3 Scientific Impact Areas . 9 1.4 The Technology of UULs and its impact. .13 1.5 Grand Challenges. .15 2. Scientific Opportunities Presented by Research with Ultrafast, Ultraintense Lasers . .17 2.1 Basic High-Field Science . .18 2.2 Ultrafast X-ray Generation and Applications . .23 2.3 High Energy Density Science and Lab Astrophysics . .29 2.4 Fusion Energy and Fast Ignition. .34 2.5 Advanced Particle Acceleration and Ultrafast Nuclear Science . .40 3. Advanced UUL Technology . .47 3.1 Overview . .47 3.2 Important Research Areas in UUL Development. .48 3.3 New Architectures for Short Pulse Laser Amplification . .51 4. Present State of UUL Research Worldwide . .53 5. Conclusions and Findings . .61 Appendix A: A Plan for Organizing the UUL Community in the United States . -
14. Measuring Ultrashort Laser Pulses I: Autocorrelation the Dilemma the Goal: Measuring the Intensity and Phase Vs
14. Measuring Ultrashort Laser Pulses I: Autocorrelation The dilemma The goal: measuring the intensity and phase vs. time (or frequency) Why? The Spectrometer and Michelson Interferometer 1D Phase Retrieval Autocorrelation 1D Phase Retrieval E(t) Single-shot autocorrelation E(t–) The Autocorrelation and Spectrum Ambiguities Third-order Autocorrelation Interferometric Autocorrelation 1 The Dilemma In order to measure an event in time, you need a shorter one. To study this event, you need a strobe light pulse that’s shorter. Photograph taken by Harold Edgerton, MIT But then, to measure the strobe light pulse, you need a detector whose response time is even shorter. And so on… So, now, how do you measure the shortest event? 2 Ultrashort laser pulses are the shortest technological events ever created by humans. It’s routine to generate pulses shorter than 10-13 seconds in duration, and researchers have generated pulses only a few fs (10-15 s) long. Such a pulse is to one second as 5 cents is to the US national debt. Such pulses have many applications in physics, chemistry, biology, and engineering. You can measure any event—as long as you’ve got a pulse that’s shorter. So how do you measure the pulse itself? You must use the pulse to measure itself. But that isn’t good enough. It’s only as short as the pulse. It’s not shorter. Techniques based on using the pulse to measure itself are subtle. 3 Why measure an ultrashort laser pulse? To determine the temporal resolution of an experiment using it. To determine whether it can be made even shorter. -
Femtosecond Pulse Generation
Femto-UP 2020-21 School Femtosecond Pulse Generation Adeline Bonvalet Laboratoire d’Optique et Biosciences CNRS, INSERM, Ecole Polytechnique, Institut Polytechnique de Paris, 91128, Palaiseau, France 1 Definitions Electric field of a 10-fs 800-nm pulse nano 10-9 sec pico 10-12 femto 10-15 2,7 fs atto 10-18 10 fs time 2 Many properties Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Ultrashorti Duration Spectral Properties i (Frequency Comb) time 3 Time-resolved spectroscopy Electric field of a 10-fs 800-nm pulse Ultrashorti Duration Time-resolved spectroscopy Direct observation of ultrafast motions time Ahmed Zewail, Nobel Prize in chemistry 1999, femtochemistry 4 Imaging Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Nonlinear microscopy time 5 Material processing Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Laser matter interaction Drilling, cutting, etching,… time Areas of applications : aeronautics, electronics, medical,6 optics… Light matter interaction Electric field of a 10-fs 800-nm pulse High peaki power (Energy /Duration) Ability to reach extreme conditions (amplified system) Applications : Sources of intense particles beams, X-rays, high energy density science, laboratory astroprophysics … time 7 Metrology Electric field of a 10-fs 800-nm pulse Spectral Properties i (Frequency Comb) Nobel Prize 2005 "for their contributions to the development of laser-based time precision spectroscopy, including the optical frequency comb technique." 8 Outline -
Frequency Generation (HD 2D SFG) Spectroscopy
Adding a dimension to the infrared spectra of interfaces using heterodyne detected 2D sum- frequency generation (HD 2D SFG) spectroscopy Wei Xiong, Jennifer E. Laaser, Randy D. Mehlenbacher , and Martin T. Zanni1 Department of Chemistry, University of Wisconsin-Madison, Madison, WI 53706 Edited by Michael L. Klein, Temple University, Philadelphia, PA, and approved October 13, 2011 (received for review September 13, 2011) In the last ten years, two-dimensional infrared spectroscopy has of carbon monoxide on polycrystalline platinum. Pt-CO is studied become an important technique for studying molecular structures extensively to better understand electrochemical catalysis (13– and dynamics. We report the implementation of heterodyne de- 16). The linear SFG spectrum of Pt-CO has been measured many tected two-dimensional sum-frequency generation (HD 2D SFG) times previously. The spectrum is almost always fit to a Lorent- spectroscopy, which is the analog of 2D infrared (2D IR) spectro- zian line shape (14–16), from which one concludes that Pt-CO is scopy, but is selective to noncentrosymmetric systems such as vibrationally narrowed, meaning that the structural dynamics interfaces. We implement the technique using mid-IR pulse shap- of the CO and its surrounding environment are so fast that the ing, which enables rapid scanning, phase cycling, and automatic system is homogeneous. By resolving the 2D line shape of Pt-CO, phasing. Absorptive spectra are obtained, that have the highest we find that there is a significant inhomogeneous contribution, frequency resolution possible, from which we extract the rephas- which indicates that there is a slow component to the vibrational ing and nonrephasing signals that are sometimes preferred. -
Development of an Ultrasensitive Cavity Ring Down Spectrometer in the 2.10-2.35 Μm Region : Application to Water Vapor and Carbon Dioxide Semen Vasilchenko
Development of an ultrasensitive cavity ring down spectrometer in the 2.10-2.35 µm region : application to water vapor and carbon dioxide Semen Vasilchenko To cite this version: Semen Vasilchenko. Development of an ultrasensitive cavity ring down spectrometer in the 2.10- 2.35 µm region : application to water vapor and carbon dioxide. Instrumentation and Detectors [physics.ins-det]. Université Grenoble Alpes, 2017. English. NNT : 2017GREAY037. tel-01704680 HAL Id: tel-01704680 https://tel.archives-ouvertes.fr/tel-01704680 Submitted on 8 Feb 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THÈSE Pour obtenir le grade de DOCTEUR DE LA COMMUNAUTE UNIVERSITE GRENOBLE ALPES Spécialité : Physique de la Matière Condensée et du Rayonnement Arrêté ministériel : 25 mai 2016 Présentée par Semen VASILCHENKO Thèse dirigée par Didier MONDELAIN codirigée par Alain CAMPARGUE préparée au sein du Laboratoire Interdisciplinaire de Physique dans l'École Doctorale Physique Development of an ultrasensitive cavity ring down spectrometer in the 2.10-2.35 µm region. -
Ultrashort Laser Pulses I
Ultrashort Laser Pulses I Description of pulses Intensity and phase The instantaneous frequency and group delay Zero th and first-order phase Prof. Rick Trebino Georgia Tech The linearly chirped Gaussian pulse www.frog.gatech.edu An ultrashort laser ) t I( t ) ( pulse has an intensity X and phase vs. time. Neglecting the spatial dependence for field Electric now, the pulse electric field is given by: Time [fs] X ∝1 ω −φ + (t )2 I( t ) exp{ it [0 (t) ]} cc. Intensity Carrier Phase frequency A sharply peaked function for the intensity yields an ultrashort pulse. The phase tells us the color evolution of the pulse in time. The real and complex ) t I( t ) pulse amplitudes ( X X Removing the 1/2, the c.c., and the exponential factor with the carrier frequency yields the complex amplitude, E(t), of the pulse: field Electric E(t )∝I( t ) exp{ − i φ(t ) } Time [fs] This removes the rapidly varying part of the pulse electric field and yields a complex quantity, which is actually easier to calculate with. I( t ) is often called the real amplitude, A(t), of the pulse. The Gaussian pulse For almost all calculations, a good first approximation for any ultrashort pulse is the Gaussian pulse (with zero phase). = − τ 2 EtE( )0 exp ( t /HW 1/ e ) = − τ 2 E0 exp 2ln 2( t /FWHM ) = − τ 2 E0 exp 1.38( t /FWHM ) τ τ where HW1/e is the field half-width-half-maximum, and FWHM is the intensity full-width-half-maximum. 2 The intensity is: ∝ − τ 2 ItE()0 exp 4ln2(/ t FWHM ) ∝2 − τ 2 E0 exp 2.76( t /FWHM ) Intensity vs. -
Ultrashort Pulse Generation in the Mid-IR
Ultrashort pulse generation in the mid-IR H. Pires1, M. Baudisch1, D. Sanchez1,M. Hemmer 1,J. Biegert 2;1 1ICFO - The Institute of Photonics Sciences Mediterranean Technology Park 08860 Castelldefels (Barcelona), Spain 2ICREA - Institucio Catalana de Recerca i Estudis Avan¸cats,08010 Barcelona, Spain Abstract Recent developments in laser sources operating in the mid-IR (3 - 8 µm), have been motivated by the numerous possibilities for both fundamental and applied research. One example is the ability to unambiguously detect pollutants and car- cinogens due to the much larger oscillator strengths of their absorption features in the mid-IR spectral region compared with the visible. Broadband sources are of particular interest for spectroscopic applications since they remove the need for arduous scanning or several lasers and allow simultaneous use of multiple ab- sorption features thus increasing the confidence level of detection. In addition, sources capable of producing ultrashort and intense mid-IR radiation are gain- ing relevance in attoscience and strong-field physics due to wavelength scaling of re-collision based processes. In this paper we review the state-of-the-art in sources of coherent, pulsed mid-IR radiation. First we discuss semi-conductor based sources which are compact and turnkey, but typically do not yield short pulse duration. Mid-IR laser gain material based approaches will be discussed, either for direct broadband mid-IR lasers or as narrowband pump lasers for parametric amplification in nonlinear crystals. The main part will focus on mid-IR generation and amplification based on parametric frequency conversion, enabling highest mid-IR peak power pulses. -
Ultrashort Pulse Laser Technology for Processing of Advanced Electronics Materials
Proceedings of LPM2017 - the 18th International Symposium on Laser Precision Microfabrication Ultrashort Pulse Laser Technology for Processing of Advanced Electronics Materials Jim BOVAT SEK *1, Rajesh PATEL*1 *1 Spectra-Physics, MKS Instruments, Inc., 3635 Peterson Way, Santa Clara, CA., 95054, USA E-mail: [email protected] Laser technology is increasingly being employed for an ever expanding range of applications in a variety of industries. The success of laser processing is due in large part to manufacturers under- standing the benefits of non-contact, precise processing and a growing need for machining smaller and more precise features. In a broader view, it is also the continual evolution of laser technolo- gy—with related improvements in the cost, capability, and reliability of product offerings—that fur- ther drives its adoption. Indeed, the laser product marketplace has seen product offerings expand in nearly every conceivable way: higher power and pulse energy, higher pulse repetition rate, shorter wavelengths, better beam quality, shorter pulse widths, pulse shape tailoring and burst-mode opera- tion—and all of these with lower costs and improved reliability. In this work, we present processing results achieved using Spectra-Physics’ state-of-the-art ultrashort pulse laser technology. This laser provides both high pulse energy and high average power, both of which are attractive to industry. We have processed materials commonly used in advanced electronics and semiconductor manufac- turing industries. The high energy pulses are shown to effectively ablate hard to machine materi- als—such as alumina ceramic–with good quality. For lower-threshold materials such as silicon and copper, we demonstrate that certain pulse parameters result in more fully optimized volumetric abla- tion efficiencies.