The Central Laser Facility Steve Blake Mechanical Section Leader
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Laboratory Astrophysics with Lasers Chantal Stehlé
Laboratory Astrophysics with lasers Chantal Stehlé LERMA (Laboratoire d’Etudes de la Ma4ère et du Rayonnement en Astrophysique et Atmosphères) This work is partly supported by French state funds managed by the ANR within the InvesBssements d'Avenir programme under reference ANR-11-IDEX-0004-02. Plasma astrophysics see for instance Savin et al. « Lab astro white paper », 2010 Perimeter Methods • Microscopic physical • Experiments processes (opacity, EOS) • Theory, databases • • MulBscale, mulphysics Numerical simulaons • Links to observaons processes (e.g. magne4c reconnecon, shock waves, instabili4es …) Tools • Study of large scale scaled • Medium size lab. processes, (e.g. stellar jets) experiments • Large scale faciliBes (lasers and pinches ) • Super-compung ressources OUTLINE • IntroducBon • Stellar Opacity • EOS for gazeous planets • Scaling • Accreon & Ejecon processes in Young Stars • Conclusion Opacity for stellar interiors From Turck Chièze et al. ApSS 2010 4 Opacity An example of opacity : For a optically thick medium, Hydrogen( Stehlé et al 1993) • LTE is ~ valid -> near blackbody radiaon κν/ρ • The monochromac radiave flux Fν ! is proporBonal to the gradient of rad. Energy and to 1/κν (The radia4on tends to escape from regions where κν is low, ie between lines) hν • The frequency averaged flux <F> is linked to the Rosseland opacity κR. 1 3 dν dB (T) / dT 16 σ T dT 1 ∫ κ ν < F > = and = ν d dB (T) / dT 3 κ R dz κ R ∫ ν ν 5 CEPHEIDS: the enigma Strong periodic (P~ 1 – 50 days) Rela4on P-L : variaons of luminosity L, Teff, and distance calibrator radius. Enveloppe 2 The pulsaon (κ mechanism) log(κR in g/cm ) 2 • in the external part of the stellar envelope 1.5 • linked to an increase of the opacity 1 4 6 -7 -2 3 0.5 10 < T < 10 K (10 < ρ < 10 g/cm ) 0 Hence radiaon is blocked in the internal layers, -> heang -> expansion and beang Core 34 32 30 28 log(External Mass in g ) 2 In the 90’, no code was able Temperature in K, κ in cm /g for M* = 5 M8, Y=0.25, Z=0.08, to reproduce the pulsa6on. -
7 Upgrade to the Vulcan Laser System to Support the TAW Upgrade
LASER SCIENCE AND DEVELOPMENT I Vulcan 7 Upgrade to the Vulcan laser system to support the TAW upgrade Contact [email protected] B. T. Parry, T. B. Winstone, P. N. Anderson, A. J. Frackiewicz, M. Galimberti, S. Hancock, C. Hernandez-Gomez, A. K. Kidd, M. M. Notley, M. Read and C. Wise Central Laser Facility, STFC, Rutherford Appleton Laboratory, HSIC, Didcot, Oxon OX11 0QX, UK Introduction chains. One of the rod amplifier beam lines is split The Vulcan laser facility has recently been upgraded to into two to form beams 7 and 8, the other is split into deliver an additional short pulse beam to Target Area beams 1-6. Beams 7 and 8 are normally used as short West (TAW) [1]. This new beamline is capable of pulse (CPA) beamlines. operating in the same mode as the previously existing Modelling showed that the extra amplification needed one, at energies up to 100 J in 1 ps. It also allows the to deliver the increased energy could be carried out at laser to reach new, previously inaccessible regimes, smaller beam diameter while still keeping the B-integral with the capability to deliver up to 500 J in pulses of below three, the limit for what was acceptable for a 10 ps or longer (100ps max). 10 ps pulse. This meant that rod amplifiers, rather than The increase in the delivered energy was made possible large, costly disk amplifiers, could be used. An by the use of dielectric gratings for this new 10 ps additional 45 mm diameter rod amplifier was installed beamline. -
Inertial Fusion Power Development:Path for Global Warming Suppression
Inertial Fusion Power Development:Path for Global Warming Suppression EU:France, UK,etc. US: LLNL, SNL, U. Rochester East Asia: Japan, China,etc. Kunioki Mima Institute of Laser Engineering, Osaka University IAEA- FC 2008, 50 years’ Ann. of Fusion Res. , Oct.15, 2008, Geneva, SW Outline • Brief introduction and history of IFE research • Frontier of IFE researches Indirect driven ignition by NIF/LMJ Ignition equivalent experiments for fast ignition • IF reactor concept and road map toward power plant IFE concepts Several concepts have been explored in IFE. Driver Irradiation Ignition Laser Direct Central hot spark Ignition HIB Indirect Fast ignition Impact ignition Pulse power Shock ignition The key issue of IFE is implosion physics which has progressed for more than 30 years Producing 1000times solid density and 108 degree temperature plasmas Plasma instabilities R Irradiation non-uniformities Thermal transport and ablation surface of fuel pellet ΔR R-M Instability ΔR0 R-T instability R0 R Feed through R-M and R-T Instabilities in deceleration phase Turbulent Mixing Canter of fuel pellet t Major Laser Fusion Facilities in the World NIF, LLNL, US. LMJ, CESTA, Bordeaux, France SG-III, Menyang,CAEP, China GXII-FIREX, ILE, Osaka, Japan OMEGA-EP, LLE, Rochester, US HiPER, RAL, UK Heavy Ion Beam Fusion: The advanced T-lean fusion fuel reactor Test Stand at LBNL NDCX-I US HIF Science Virtual National Lab.(LBNL, LLNL,PPPL) has been established in 1990. (Directed by G Logan) • Implosion physics by HIB • HIB accelerator technology for 1kA, 1GeV, 1mm2 beam: Beam brightness, Neutralization, NDCX II Collective effects of high current beam, Stripping.(R.Davidson etal) • Reactor concept with Flibe liquid jet wall (R.Moir: HYLIF for HIF Reactor) History of IFE Research 1960: Laser innovation (Maiman) 1972: Implosion concept (J. -
Nova Laser Technology
Nova Laser Technology In building the Nova laser, we have significantly advanced many technologies, including the generation and propagation of laser beams. We have also developed innovations in the fields of alignment, diagnostics, computer control, and image processIng.• For further information contact Nova is the world's most powerful at least 10 to 30 times more energetic John F. Holzrichter (415) 423-7454. laser system. It is designed to heat and than Shiva would be needed to compress small targets, typically 0.1 cm investigate ignition conditions and in size, to conditions otherwise produced possibly to reach gains near unity. only in nuclear weapons or in the Because of the importance of such a interior of stars. Its beams can facility to the progress of inertial fusion concentrate 80 to 120 kJ of energy (in research and because of the construction 3 ns) or 80 to 120 TW of power (in time entailed (at least five to seven 100 ps) on such targets. To couple energy years), the Nova project was proposed to more favorably with the target, Nova's the Energy Research and Development laser light will be harmonically converted Administration and to Congress. It was with greater than 50% efficiency from its decided to base this system on the near-infrared fundamental wavelength proven master-oscillator, linear-amplifier (1.05-,um wavelength) to green (0.525- chain laser system used on the Argus ,um) or blue (0.35-,um) wavelengths. The and Shiva systems. We had great goals of our experiments with Nova are confidence in extending this to make accurate measurements of high neodymium-glass laser technology to the temperature and high-pressure states of 200- to 300-kJ level. -
ENGINEERING DESIGN of the NOVA LASER FACILITY for By
ENGINEERING DESIGN OF THE NOVA LASER FACILITY FOR INERTIAL-CONFINEMENT FUSION* by W. W. Simmons, R. 0. Godwin, C. A. Hurley, E. P. Wallerstein, K. Whitham, J. E. Murray, E. S. Bliss, R. G. Ozarski. M. A. Summers, F. Rienecker, D. G. Gritton, F. W. Holloway, G. J. Suski, J. R. Severyn, and the Nova Engineering Team. Abstract The design of the Nova Laser Facility for inertia! confinement fusion experiments at Lawrence Livermore National Laboratory is presented from an engineering perspective. Emphasis is placed upon design-to- performance requirements as they impact the various subsystems that comprise this complex experimental facility. - DISCLAIMER - CO;.T-CI104n--17D DEf;2 013.375 *Research performed under the auspices of the U.S. Department of Energy by the Lawrence Livermore National Laboratory under contract number W-7405-ENG-48. Foreword The Nova Laser System for Inertial Confinement Fusion studies at Lawrence Livermore National Laboratories represents a sophisticated engineering challenge to the national scientific and industrial community, embodying many disciplines - optical, mechanical, power and controls engineering for examples - employing state-of-the-art components and techniques. The papers collected here form a systematic, comprehensive presentation of the system engineering involved in the design, construction and operation of the Nova Facility, presently under construction at LLNL and scheduled for first operations in 1985. The 1st and 2nd Chapters present laser design and performance, as well as an introductory overview of the entire system; Chapters 3, 4 and 5 describe the major engineering subsystems; Chapters 6, 7, 8 and 9 document laser and target systems technology, including optical harmonic frequency conversion, its ramifications, and its impact upon other subsystems; and Chapters 10, 11, and 12 present an extensive discussion of our integrated approach to command, control and communications for the entire system. -
Nd Lu Caf2 for High-Energy Lasers Simone Normani
Nd Lu CaF2 for high-energy lasers Simone Normani To cite this version: Simone Normani. Nd Lu CaF2 for high-energy lasers. Physics [physics]. Normandie Université, 2017. English. NNT : 2017NORMC230. tel-01689866 HAL Id: tel-01689866 https://tel.archives-ouvertes.fr/tel-01689866 Submitted on 22 Jan 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. THESE Pour obtenir le diplôme de doctorat Physique Préparée au sein de l’Université de Caen Normandie Nd:Lu:CaF2 for High-Energy Lasers Étude de Cristaux de CaF2:Nd:Lu pour Lasers de Haute Énergie Présentée et soutenue par Simone NORMANI Thèse soutenue publiquement le 19 octobre 2017 devant le jury composé de M. Patrice CAMY Professeur, Université de Caen Normandie Directeur de thèse M. Alain BRAUD MCF HDR, Université de Caen Normandie Codirecteur de thèse M. Jean-Luc ADAM Directeur de Recherche, CNRS Rapporteur Mme. Patricia SEGONDS Professeur, Université de Grenoble Rapporteur M. Jean-Paul GOOSSENS Ingénieur, CEA Examinateur M. Maurizio FERRARI Directeur de Recherche, CNR-IFN Examinateur Thèse dirigée par Patrice CAMY et Alain BRAUD, laboratoire CIMAP Université de Caen Normandie Nd:Lu:CaF2 for High-Energy Lasers Thesis for the Ph.D. -
Advanced Approaches to High Intensity Laser-Driven Ion Acceleration
Advanced Approaches to High Intensity Laser-Driven Ion Acceleration Andreas Henig M¨unchen2010 Advanced Approaches to High Intensity Laser-Driven Ion Acceleration Andreas Henig Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Andreas Henig aus W¨urzburg M¨unchen, den 18. M¨arz2010 Erstgutachter: Prof. Dr. Dietrich Habs Zweitgutachter: Prof. Dr. Toshiki Tajima Tag der m¨undlichen Pr¨ufung:26. April 2010 Contents Contentsv List of Figures ix Abstract xiii Zusammenfassung xv 1 Introduction1 1.1 History and Previous Achievements...................1 1.2 Envisioned Applications.........................3 1.3 Thesis Outline...............................5 2 Theoretical Background9 2.1 Ionization.................................9 2.2 Relativistic Single Electron Dynamics.................. 14 2.2.1 Electron Trajectory in a Linearly Polarized Plane Wave.... 15 2.2.2 Electron Trajectory in a Circularly Polarized Plane Wave... 17 2.2.3 Electron Ejection from a Focussed Laser Beam......... 18 2.3 Laser Propagation in a Plasma..................... 18 2.4 Laser Absorption in Overdense Plasmas................. 20 2.4.1 Collisional Absorption...................... 20 2.4.2 Collisionless Absorption..................... 21 2.5 Ion Acceleration.............................. 22 2.5.1 Target Normal Sheath Acceleration (TNSA).......... 22 2.5.2 Shock Acceleration........................ 26 2.5.3 Radiation Pressure Acceleration / Light Sail / Laser Piston. 27 3 Experimental Methods I - High Intensity Laser Systems 33 3.1 Fundamentals of Ultrashort High Intensity Pulse Generation..... 33 vi CONTENTS 3.1.1 The Concept of Mode-Locking.................. 33 3.1.2 Time-Bandwidth Product.................... 37 3.1.3 Chirped Pulse Amplification................... 39 3.1.4 Optical Parametric Amplification (OPA)............ 40 3.2 Laser Systems Utilized for Ion Acceleration Studies......... -
Proton Beams Generated by Ultrashort-Pulse Lasers Will Help
S&TR December 2003 Proton-Beam Experiments 11 Proton beams ROTONS, the positively charged, Psubatomic particles discovered by Lord Rutherford nearly 100 years ago, are still surprising scientists. Lawrence generated by Livermore researchers are discovering that proton beams created by powerful, ultrashort pulses of laser light can be used to create and even diagnose plasmas, the ultrashort-pulse superhot state of matter that exists in the cores of stars and in detonating nuclear weapons. The proton-beam experiments promise new techniques for maintaining lasers will help the nationʼs nuclear arsenal and for better understanding how stars function. The proton beams used in the Laboratoryʼs experiments are produced advance our by pulses of laser light lasting only about 100 femtoseconds (a femtosecond is 10–15 seconds, or one-quadrillionth of a second) and having a brightness, or understanding of irradiance, up to 5 × 1020 watts per square centimeter. When such fleeting pulses are focused onto thin foil targets, as many as 100 billion protons are emitted, with plasmas. energies up to 25 megaelectronvolts. The protons come from a spot on the foil about 200 micrometers in diameter, and the beamʼs duration is a few times longer than the laser pulse. The highest-energy protons diverge 1 to 2 degrees from the perpendicular, while the lowest-energy protons form a cone about 20 degrees from perpendicular. Funded by the Laboratory Directed Research and Development Program, the Livermore experiments are led by physicists Pravesh Patel and Andrew Mackinnon. Patel, who works in the Laboratoryʼs Physics and Advanced Lawrence Livermore National Laboratory 12 Proton-Beam Experiments S&TR December 2003 Technologies Directorate, is researching per gram) that exist in stars. -
The Vulcan 10 PW Project 7
LASER SCIENCE AND DEVELOPMENT I Vulcan The Vulcan 10 PW project 7 Contact [email protected] C. Hernandez-Gomez, S. P. Blake, O. Chekhlov, R. J. Clarke, A. M. Dunne, M. Galimberti, S. Hancock, P. Holligan, A. Lyachev, P. Matousek, I. O. Musgrave, D. Neely, P. A. Norreys, I. Ross, Y. Tang, T. B. Winstone, B. E. Wyborn and J. Collier Central Laser Facility, STFC, Rutherford Appleton Laboratory, HSIC, Didcot, Oxfordshire, OX11 0QX, UK Introduction This projects aim is to upgrade the Vulcan high power laser located at the Central Laser Facility (CLF), to beyond the 10 PW power level (1016 W) and provide focused intensities of greater than 1023 Wcm-2 to its international user community [1]. The project was divided in two phases. Phase 1 of 2 year duration, started in December 2006. A proposal for phase 2 has been submitted and reviewed. The start date of phase 2 is still under discussions. We report here on the overall progress made during the first phase. There were essentially three key areas to address as part of phase 1: • A novel “front end” system has been developed for Figure 1. Area photograph of the 10 PW Front End. the overall project and its performance has been verified with respect to key indicators such as wavelength, energy, bandwidth, pulselength, develop this high (150 nm) bandwidth version and the contrast etc. overall design is now based on this approach. • There has been a significant reduction in the risk associated with several key technical elements of the The 910 nm seed currently generated with the chirped project, particularly the large aperture diffraction scheme has a bandwidth of 165 nm and energy of gratings and laser amplifiers Several outstanding 40 µJ per pulse. -
A New Interlock System for the Vulcan Laser
Laser Science and Development – Instrumentation A new interlock system for the Vulcan laser C J Reason, W J Lester, P Holligan, D A Pepler, R W W Wyatt Central Laser Facility, CCLRC Rutherford Appleton Laboratory, Chilton, Didcot, Oxon., OX11 0QX, UK Main contact email address: [email protected] Introduction architecture allows the rest of the system to continue providing safety functionality even when a room is ‘turned The provision of safety interlocks in the CLF has developed off’ (e.g. lost power). through stages, starting with a hardwired system, through to a computer system, ‘Cerberus’1) using Arcnet and written in Cerberus Borland Turbo Pascal V 3 running under DOS, to Layout display Door / room displays ‘Cerberus’2) – rewritten as a computer system using Ethernet and written in Borland Turbo Pascal V 7 running under DOS. This has had to be replaced for a number of reasons including Cerberus Computer Video splitter • Much of the hardware is no longer available (e.g. Ethernet network door displays, Amplicon IO cards etc). PLC system Digital signals • The computers with ISA slots are no longer easily available. Safety PLC system • DOS and Borland Turbo Pascal are no longer Laser or target area Next room supported. Argus • The limits on code and data of 64 Kbytes were preventing necessary changes to the system. Figure 1. The system architecture. Also a new international standard IEC 61508 - Functional Safety for E, E, EP (Electrical / Electronic / Electronic The Argus PLC system 3) Programmable) systems has been published. It is This was designed from the lifecycle developed from IEC recommended (but not mandatory) that safety systems should 61508. -
Review of Laser Diagnostics at the Vulcan Laser Facility
High Power Laser Science and Engineering, (2015), Vol. 3, e26, 10 pages. © The Author(s) 2015. The online version of this article is published within an Open Access environment subject to the conditions of the Creative Commons Attribution licence <http://creativecommons.org/licenses/by/3.0/>. doi:10.1017/hpl.2015.27 Review of laser diagnostics at the Vulcan laser facility Ian Musgrave, Marco Galimberti, Alexis Boyle, Cristina Hernandez-Gomez, Andrew Kidd, Bryn Parry, Dave Pepler, Trevor Winstone, and John Collier Central Laser Facility, Science and Technology Facilities Council, RAL, Didcot, Oxfordshire OX 11 0QX, UK (Received 1 May 2015; revised 6 July 2015; accepted 31 July 2015) Abstract In this paper we review the provision of the laser diagnostics that are installed on the Vulcan laser facility. We will present strategies for dealing with the energy of high energy systems and with ways of handling the beam sizes of the lasers. We present data captured during typical experimental campaigns to demonstrate their reliability and variation in shot to shot values. Keywords: calorimeter; high power laser; laser diagnostics; pulse energy 1. Introduction Offner¨ stretcher. Following this are three further stages of OPCPA to achieve >60 mJ of energy. These pulses are The Vulcan laser facility of the Central Laser Facility is then amplified in a mixed silicate and phosphate glass rod located in the UK. It is an open access laser facility operated amplifier chain before final amplification in a phosphate ostensibly for the UK academic community for the purposes disc chain. The pulses are finally compressed before being of studying laser–matter interactions[1–3]. -
Radiation Safety Plan
RADIATION SAFETY PLAN ENVIRONMENTAL NOVA SOUTHEASTERN HEALTH AND SAFETY UNIVERSITY POLICY/PROCEDURE POLICY/PROCEDURE TITLE: Radiation Safety Plan NUMBER: 9 DOCUMENT HISTORY OWNER: Facilities Management/AHIS Date: 1 Sept 2011 APPROVED: NSU Radiation Safety Committee Date: 1 Sept 2011 IMPLEMENTED: Date: 1 Oct 2010 RETIRED: Date: Date: Revision No. Review / Changes Reviewer 1/2017 1 Remove Gamma Irradiator reference RSO-5 form RSC 1/2017 2 Change EHS Committee to Radiation Safety RSC Committee (RSC) 1/2017 3 Change references from EHS to RSO RSC 4/2019 4 Edit section 5.4 to remove shipping building RSO RADIATION SAFETY PLAN RADIATION SAFETY PLAN Table of Contents Section 1: Introduction ........................................................................................................ 4 Section 2: Biological Effects and Exposure Protection ......................................................... 9 Section 3: Responsibilities ................................................................................................. 12 Section 4: License Requirements ....................................................................................... 15 Section 5: Authorization and Procurement of Radioactive Materials ................................ 16 Section 6: Training ............................................................................................................. 19 Section 7: Personnel Monitoring and Occupational Dose Limits ....................................... 22 Section 8: Signs and Labels ...............................................................................................