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Thin Film Compression Toward the Single-Cycle Regime for the Advancement of High Field Science
UC Irvine UC Irvine Electronic Theses and Dissertations Title Thin film compression toward the single-cycle regime for the advancement of high field science Permalink https://escholarship.org/uc/item/7bc837xn Author Farinella, Deano Michael-Angelo Publication Date 2018 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA, IRVINE Thin film compression toward the single-cycle regime for the advancement of high field science DISSERTATION submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in Physics by Deano Michael-Angelo Farinella Dissertation Committee: Professor Franklin Dollar, Chair Professor Toshiki Tajima Professor Roger McWilliams 2018 Chapter 6 c 2016 American Physical Society Chapter 7 c 2016 American Institute of Physics All other materials c 2018 Deano Michael-Angelo Farinella DEDICATION To my family ii TABLE OF CONTENTS Page LIST OF FIGURES vi LIST OF TABLES xiii ACKNOWLEDGMENTS xiv CURRICULUM VITAE xvi ABSTRACT OF THE DISSERTATION xix 1 Introduction 1 1.1 Pulsed laser technology . .2 1.1.1 Chirped pulse amplification . .3 1.2 Compression of ultrashort laser pulses . .5 1.2.1 Fiber and bulk compression . .6 1.2.2 Thin film compression . .8 1.3 Applications of compressed ultrashort laser pulses . .9 1.3.1 Single-cycle ion acceleration . .9 1.3.2 X-ray generation . 11 1.4 Structure of thesis . 13 2 Laser pulses in matter 14 2.1 Linear response . 14 2.1.1 The electric susceptibility χ(1) ..................... 17 2.1.2 Dispersive effects . 19 2.2 Nonlinear response . 22 2.2.1 The nonlinear electric susceptibility χ(3) .............. -
Laboratoire Pour L'utilisation Des Lasers Intenses
LULI - Laboratoire pour l’utilisation des lasers intenses Rapport Hcéres To cite this version: Rapport d’évaluation d’une entité de recherche. LULI - Laboratoire pour l’utilisation des lasers intenses. 2014, École polytechnique - X, Commissariat à l’énergie atomique et aux énergies alternatives - CEA, Centre national de la recherche scientifique - CNRS, Université Pierre et Marie Curie - UPMC. hceres-02033272 HAL Id: hceres-02033272 https://hal-hceres.archives-ouvertes.fr/hceres-02033272 Submitted on 20 Feb 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. Department for the evaluation of resea Department for the evaluation of research units AERES report on unit: Laboratoire d’Utilisation des Lasers Intenses LULI Under the supervision of the following institutions and research bodies: École Polytechnique Université Pierre et Marie Curie - UPMC Centre National de la Recherche Scientifique - CNRS Commissariat à l’Énergie Atomique et aux Énergies Alternatives - CEA December 2013 Department for the evaluation of research units On behalf of AERES, pursuant to the Decree On behalf of the expert committee, of 3 november 20061, Mr. Didier HOUSSIN, president Mr. Marc SENTIS, chair of the committee Mr. Pierre GLAUDES, head of the evaluation of research units department 1 The AERES President “signs [...], the evaluation reports, [...] countersigned for each department by the director concerned” (Article 9, paragraph 3 of the Decree n ° 2006-1334 of 3 November 2006, as amended). -
Solid-State Lasers: a Graduate Text
Solid-State Lasers: A Graduate Text Walter Koechner Michael Bass Springer Solid-State Lasers Springer New York Berlin Heidelberg Hong Kong London Milan Paris Tokyo Advanced Texts in Physics This program of advanced texts covers a broad spectrum of topics that are of current and emerging interest in physics. Each book provides a comprehensive and yet accessible introduction to a field at the forefront of modern research. As such, these texts are intended for senior undergraduate and graduate students at the M.S. and Ph.D. levels; however, research scientists seeking an introduction to particular areas of physics will also benefit from the titles in this collection. Walter Koechner Michael Bass Solid-State Lasers A Graduate Text With 252 Figures 1 Springer Walter Koechner Michael Bass Fibertek, Inc. School of Optics/CREOL 510 Herndon Parkway University of Central Florida Herndon, VA 20170 Orlando, FL 32816 USA USA Cover illustration: Diode-pumped ND: YAG slab laser with positive branch unstable resonator and variable reflectivity output coupler (adapted from Figure 5.24, page 182). Library of Congress Cataloging-in-Publication Data Koechner, Walter, 1937– Solid state lasers : a graduate text / Walter Koechner, Michael Bass. p. cm.—(Advanced texts in physics) Includes bibliographical references and index. ISBN 0-387-95590-9 (alk. paper) 1. Solid-state lasers. I. Bass, Michael, 1939–. II. Title III. Series. TA1705 .K633 2003 621.36 61—dc21 2002030568 ISBN 0-387-95590-9 Printed on acid-free paper. c 2003 Springer-Verlag New York, Inc. All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer-Verlag New York, Inc., 175 Fifth Avenue, New York, NY 10010, USA), except for brief excerpts in connection with reviews or scholarly analysis. -
Lasers As Weapons Y 9 Fictional Predictions Y 10 See Also Y 11 Notes and References Y 12 Further Reading Y 13 External Links
Laser From Wikipedia, the free encyclopedia Jump to: navigation, search For other uses, see Laser (disambiguation). Laser United States Air Force laser experiment Inventor Charles Hard Townes Launch year 1960 Available? Worldwide Laser beams in fog, reflected on a car windshield Light Amplification by Stimulated Emission of Radiation (LASER or laser) is a mechanism for emitting electromagnetic radiation, often visible light, via the process of stimulated emission. The emitted laser light is (usually) a spatially coherent, narrow low-divergence beam, that can be manipulated with lenses. In laser technology, "coherent light" denotes a light source that produces (emits) light of in-step waves of identical frequency, phase,[1] and polarization. The laser's beam of coherent light differentiates it from light sources that emit incoherent light beams, of random phase varying with time and position. Laser light is generally a narrow-wavelengthelectromagnetic spectrum monochromatic light; yet, there are lasers that emit a broad spectrum of light, or emit different wavelengths of light simultaneously. Contents [hide] y 1 Terminology y 2 Design y 3 Laser physics o 3.1 Modes of operation 3.1.1 Continuous wave operation 3.1.2 Pulsed operation 3.1.2.1 Q-switching 3.1.2.2Modelocking 3.1.2.3 Pulsed pumping y 4 History o 4.1 Foundations o 4.2 Maser o 4.3 Laser o 4.4 Recent innovations y 5 Types and operating principles o 5.1 Gas lasers 5.1.1 Chemical lasers 5.1.2Excimer lasers o 5.2 Solid-state lasers 5.2.1Fiber-hosted lasers 5.2.2 Photonic crystal lasers 5.2.3 Semiconductor lasers o 5.3 Dye lasers o 5.4 Free electron lasers o 5.5 Exotic laser media y 6 Uses o 6.1 Examples by power o 6.2 Hobby uses y 7 Laser safety y 8 Lasers as weapons y 9 Fictional predictions y 10 See also y 11 Notes and references y 12 Further reading y 13 External links Terminology From left to right: gamma rays, X-rays, ultraviolet rays, visible spectrum, infrared, microwaves, radio waves. -
Appendix B Acronyms and Abbreviations
Appendix B Acronyms and Abbreviations Units of Measure and some Physical Constants A . ampere --- unit of electric current [named after André M. Ampère (1775---1836), French physicist]. 1 A represents a flow of one coulomb of electricity per second (or: 1A = 1C/s) Ah ............ amperehour Å . angstrom --- unit of length (used in particular for the short wavelength spectrum); 1Å= 10---10 m [named after Anders Jonas Ängström (1814--- 1874), Swedish physicist and astronomer] amu. atomic mass unit (1.6605402 10---27 kg) are............) unit of area (1 are = 100 m2 arcmin......... arcminute [1’ = (1/60)º or 1 arcmin = 2.908882 x 10---4 radian] arcsec.......... arcsecond [1” = (1/60)’ or 1 arcsec = 4.848137 x 10---6 radian= 0.000278º] au . astronomical unit --- unit of length, namely the mean Earth/sun distance [=1.495978706 1013 cm, which is the semimajor axis of the Earth’s orbit around the sun (or about 150 million km)] bar............) pressure, (1 bar = 105 Nm---2 Bq . Becquerel [named after Alexandre Edmond Becquerel, a French physi- cist (1820---1891)]. The Bq is a SI unit used to measure a radioactivity. One Becquerel is that quantity of a radioactive material that will have 1 transformations in one second. c . velocity of light in vacuum (299,792,458 m/s) cd . candela (unit of luminous intensity). The candela is the luminous inten- sity, in a given direction, of a source that emits monochromatic radi- ation of frequency 540 × 1012 Hz and that has a radiant intensity in that direction of 1/683 watt per steradian. cm........... -
Laser Technology Applications
International Journal of Applied Research 2015; 1(7): 476-486 ISSN Print: 2394-7500 ISSN Online: 2394-5869 Laser Technology Applications: A gift to Humanity Impact Factor: 5.2 IJAR 2015; 1(7): 476-486 www.allresearchjournal.com Received: 28-04-2015 Devaryan Gupta Accepted: 30-05-2015 Abstract Devaryan Gupta LASER technology is something that we use almost every day in our lives, but don’t even think about Delhi Public School, Faridabad, Haryana, India it. It has been used to make huge scientific findings and can help us in many ways. A LASER is a coherent and focused beam of photons. LASER stands for Light Amplification by Stimulated Emission of Radiations. This paper describes the LASER technology in details. This paper describes the history and extensibility of LASER. It also explains the concept of principles of LASER technology and how a LASER works? This paper also describes the different types of LASER and the application areas of LASER. Different types of LASER have different operation wavelengths and pump source. This paper also gives the knowledge on how the LASER beam is made and what components are required to make a LASER. The output of a LASER is a coherent electromagnetic field. Keywords: Technology, Applications, electromagnetic Introduction A LASER is a device that emits light through a process of optical amplification based on the stimulated emission of electromagnetic radiation. A LASER is a coherent and focused beam of photons; coherent means that it is all one wavelength, unlike ordinary light which showers on us in many wavelengths. The acronym LASER stands for "Light Amplification by Stimulated Emission of Radiation”. -
Laser Technology and Applications in Assorted Domains
ISSN (Online) : 2348 - 2001 International Refereed Journal of Reviews and Research Volume 5 Issue 6 November 2017 International Manuscript ID : 23482001V5I6112017-11 (Approved and Registered with Govt. of India) Laser Technology and Applications in Assorted Domains Rashmi Research Scholar Department of Physics Sri Venkateshwara University, Uttar Pradesh, India Dr. Nempal Singh Associate Professor Department of Physics Sri Venkateshwara University Uttar Pradesh, India Abstract The word laser started as an acronym for "light amplification by stimulated emission of radiation". In this usage, the term "light" includes electromagnetic radiation of any frequency, not only visible light, hence the terms infrared laser, ultraviolet laser, X-ray laser and gamma- ray laser. Because the microwave predecessor of the laser, the maser, was developed first, devices of this sort operating at microwave and radio frequencies are referred to as "masers" rather than "microwave lasers" or "radio lasers". In the early technical literature, especially at Bell Telephone Laboratories, the laser was called an optical maser; this term is now obsolete. A laser that produces light by itself is technically an optical oscillator rather than an optical amplifier as suggested by the acronym. It has been humorously noted that the acronym LOSER, for "light oscillation by stimulated emission of radiation", would have been more correct. With the widespread use of the original acronym as a common noun, optical amplifiers have come to be referred to as "laser amplifiers". Keywords: Laser Technology, Applications of Laser, Laser in Engineering Registered with Council of Scientific and Industrial Research, Govt. of India URL: irjrr.com ISSN (Online) : 2348 - 2001 International Refereed Journal of Reviews and Research Volume 5 Issue 6 November 2017 International Manuscript ID : 23482001V5I6112017-11 (Approved and Registered with Govt. -
Thin Film Compression Toward the Single-Cycle Regime for The
UNIVERSITY OF CALIFORNIA, IRVINE Thin film compression toward the single-cycle regime for the advancement of high field science DISSERTATION submitted in partial satisfaction of the requirements for the degree of DOCTOR OF PHILOSOPHY in Physics by Deano Michael-Angelo Farinella Dissertation Committee: Professor Franklin Dollar, Chair Professor Toshiki Tajima Professor Roger McWilliams 2018 Chapter 6 c 2016 American Physical Society Chapter 7 c 2016 American Institute of Physics All other materials c 2018 Deano Michael-Angelo Farinella DEDICATION To my family ii TABLE OF CONTENTS Page LIST OF FIGURES vi LIST OF TABLES xiii ACKNOWLEDGMENTS xiv CURRICULUM VITAE xvi ABSTRACT OF THE DISSERTATION xix 1 Introduction 1 1.1 Pulsed laser technology . .2 1.1.1 Chirped pulse amplification . .3 1.2 Compression of ultrashort laser pulses . .5 1.2.1 Fiber and bulk compression . .6 1.2.2 Thin film compression . .8 1.3 Applications of compressed ultrashort laser pulses . .9 1.3.1 Single-cycle ion acceleration . .9 1.3.2 X-ray generation . 11 1.4 Structure of thesis . 13 2 Laser pulses in matter 14 2.1 Linear response . 14 2.1.1 The electric susceptibility χ(1) ..................... 17 2.1.2 Dispersive effects . 19 2.2 Nonlinear response . 22 2.2.1 The nonlinear electric susceptibility χ(3) ............... 22 2.3 Intensity dependent refractive index . 26 2.3.1 Self-phase modulation . 29 2.3.2 Self-focusing . 31 3 Methods/laser diagnostics 34 3.1 Second harmonic generation FROG . 34 3.2 Compressor calibration . 38 iii 4 Demonstration of thin film compression 43 4.1 Introduction . -
LASER FUSION DIAGNOSTICS .Ft*-" Lamar W
PREPRINT UCRL- 81099 do /OP- VJ05TI---3 Lawrence Liver more Laboratory 1 LASER FUSION DIAGNOSTICS .ft*-" Lamar W. Coleman May 9, 1978 Prepared for presentation at IEEE Modern Plasma Diaqnostics Course, Monterey, California, May 17, 1978 This is a preprint of a paper intended for publication in a journal or proceedings. Since changes may be made before publication, this preprint is made available with the understanding that it will not be cited or reproduced without the permission of the author. MASTER pBTBUXmbK OF THIS DOCUMENT 18 UNUHtTKD -NOTICE- •nu «po^ MI m»«d . «, KCOU„, „, „rt riT/ " ' """' S""><=""«™"C. r*lft<, ft. Untad Sun, BO, ft, u^,M s„,„ ^„,„„, 0, &«'0. TO iny of ih,i, rapioy,,,, „o, m of dm, smncio,.. .obcooinno,,. „, ft,t ,„,„)*,., ral„ tohBy o, mp.„M,^ fo, ft. .,„,„„, ^..S 01 «full,m of my ii.fom.lta, .ppmoa. p,odu<i or INTRODUCTION PI0«I. d«|o«d, 01 rep««„tt ft,, ,„ „ „u„ In'ruiy pnwitly owned rljhu. Detailed diagnosis of laser target interaction experiments requires a variety of diagnostics techniques and systems capable of measurements over a broad range of physical parameters with high spatial and temporal resolutions and which also conform to some system design and operational constraints. These requirements, goals and constraints are summarized in Fig. 1. There is a broad range of physical parameters to be covered and our ultimate goal, in being able to accurately diagnose laser target interaction e, eriments, is to be able to make broad variety of measurements of physical parameters with a spatial resolution of 1 ym and a temporal resolution of 1 ps ar d yet be able to cover the range of variables as indicated in Fig. -
Laser Driven Nuclear Physics at ELI–NP
Laser Driven Nuclear Physics at ELI–NP Negoita, F., Roth, M., Thirlof, P. G., Tudisco, S., Mirfayzi, S., Kar, S., Hannachi, F., Moustaizis, S., Pomerantz, I., McKenna, P., Fuchs, J., Sphor, K., Acbas, G., Anzalone, A., Audebert, P., & Balascuta, S. (2016). Laser Driven Nuclear Physics at ELI–NP. Romanian Reports in Physics, 68(Supplement), S37-S144. http://www.rrp.infim.ro/2016_68_S.html Published in: Romanian Reports in Physics Document Version: Peer reviewed version Queen's University Belfast - Research Portal: Link to publication record in Queen's University Belfast Research Portal Publisher rights © 2016 Editura Academiei Romane General rights Copyright for the publications made accessible via the Queen's University Belfast Research Portal is retained by the author(s) and / or other copyright owners and it is a condition of accessing these publications that users recognise and abide by the legal requirements associated with these rights. Take down policy The Research Portal is Queen's institutional repository that provides access to Queen's research output. Every effort has been made to ensure that content in the Research Portal does not infringe any person's rights, or applicable UK laws. If you discover content in the Research Portal that you believe breaches copyright or violates any law, please contact [email protected]. Download date:01. Oct. 2021 LASER DRIVEN NUCLEAR PHYSICS AT ELI–NP F.NEGOITA1*, M.ROTH2, P.G.THIROLF3, S.TUDISCO4, F.HANNACHI5, S.MOUSTAIZIS6, I.POMERANTZ7 , P.MCKENNA8, J.FUCHS9, K.SPHOR10, G.ACBAS1, A.ANZALONE4, P.AUDEBERT9, S.BALASCUTA1, F.CAPPUZZELLO4,11, M.O.CERNAIANU1, S.CHEN9, I.DANCUS1, R.FREEMAN12, H.GEISSEL13, P.GENUCHE1, L.GIZZI14, F.GOBET5, G.GOSSELIN15, M.GUGIU1, D.HIGGINSON9, E.D’HUMIÈRES16, C. -
Interim Report of the National Ignition Facility Laser System Task Force
Interim Report of the National Ignition Facility Laser System Task Force National Ignition Facility Laser System Task Force Secretary of Energy Advisory Board U.S. Department of Energy Washington, D.C. January 10, 2000 1 INTERIM REPORT OF THE NATIONAL IGNITION FACILITY LASER SYSTEM TASK FORCE January 10, 2000 2 MEMBERS OF THE NATIONAL IGNITION FACILITY LASER SYSTEM TASK FORCE Dr. John McTague Former Vice President, Technical Affairs Ford Motor Company Mr. Andrew Athy Partner O’Neill, Athy & Casey, PC Dr. Robert Byer Director Hansen Experimental Physics Laboratory Stanford University Dr. Gail Kendall Director for Strategic Science and Technology Electric Power Research Institute (EPRI) Dr. Lawrence Papay Sector Vice President, Integrated Solutions Sector Science Applications International Corp. (SAIC) Dr. Burton Richter Director Emeritus Stanford Linear Accelerator Center Dr. Rochus Vogt R. Stanton Avery Distinguished Service Professor and Professor of Physics California Institute of Technology (CALTECH) Dr. John M. Warlaumont Director IBM/Silicon Technology and Advance Semiconductor Technology Laboratory 3 INTERIM REPORT OF THE NATIONAL IGNITION FACILITY (NIF) LASER SYSTEM TASK FORCE EXECUTIVE SUMMARY In the late summer of 1999 it was revealed that, contrary to earlier reports, the National Ignition Facility (NIF) Laser System at the Lawrence Livermore National Laboratory would require more funds and time for completion than had been previously planned. In response to these revelations, Secretary Richardson announced a series of initiatives to get the project back on track, including the creation of an independent Task Force to review the project and provide recommendations for how to best tackle NIF’s remaining technical and managerial challenges. On October 6, 1999, Secretary Richardson requested that the Secretary of Energy Advisory Board (SEAB) form a subcommittee to conduct an independent review of the engineering and management aspects of the assembly and installation of the NIF laser system. -
Laser Produced Electromagnetic Pulses: Generation, Detection and Mitigation
High Power Laser Science and Engineering, (2020), Vol. 8, e22, 59 pages. doi:10.1017/hpl.2020.13 REVIEW Laser produced electromagnetic pulses: generation, detection and mitigation Fabrizio Consoli 1, Vladimir T. Tikhonchuk 2;3, Matthieu Bardon4, Philip Bradford 5, David C. Carroll 6, Jakub Cikhardt 7;8, Mattia Cipriani 1, Robert J. Clarke 6, Thomas E. Cowan 9, Colin N. Danson 10;11;12, Riccardo De Angelis 1, Massimo De Marco13, Jean-Luc Dubois 2, Bertrand Etchessahar4, Alejandro Laso Garcia 9, David I. Hillier10;12, Ales Honsa 3, Weiman Jiang14, Viliam Kmetik3, Josef Krasa´ 15, Yutong Li 14;16, Fred´ eric´ Lubrano4, Paul McKenna 17, Josefine Metzkes-Ng 9, Alexandre Poye´ 18, Irene Prencipe9, Piotr Ra¸czka 19, Roland A. Smith 20, Roman Vrana3, Nigel C. Woolsey 5, Egle Zemaityte17, Yihang Zhang14;16, Zhe Zhang 14, Bernhard Zielbauer21, and David Neely 6;10;17 1ENEA, Fusion and Technologies for Nuclear Safety Department, C.R. Frascati, 00044 Frascati, Italy 2CELIA, University of Bordeaux, CNRS, CEA, 33405 Talence, France 3ELI Beamlines, Institute of Physics, Czech Academy of Sciences, 25241 Doln´ı Breˇ zany,ˇ Czech Republic 4CEA, DAM, CESTA, 33116 Le Barp, France 5Department of Physics, York Plasma Institute, University of York, Heslington, York YO10 5DD, UK 6Central Laser Facility, Rutherford Appleton Laboratory, STFC, UKRI, Chilton, Didcot, Oxfordshire OX11 0QX, UK 7Czech Technical University in Prague, Faculty of Electrical Engineering, 166 27 Prague 6, Czech Republic 8Institute of Plasma Physics of the Czech Academy of Sciences, Za Slovankou