Nuclear Weapons Journal PO Box 1663 Mail Stop A142 Los Alamos, NM 87545 WEAPONS Issue 2 • 2009 Journal
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High Energy Density Physics Experiments at Los Alamos
High Energy Density Dante-2 SXI Physics Experiments at Los Alamos FFLEX FABS & Hans Herrmann NBI FABS & 36B NBI 31B Dante-1 Plasma Physics Group (P-24) SXI In this photo, Norris Bradbury, Robert Oppenheimer, Richard Feynman, and Enrico Fermi attend an early Los Alamos weapons colloquium. OMEGA LaserU UserN C L A S SGroup I F I E D Rochester, NY April 29, 2011 Operated by Los Alamos National Security, LLC for NNSA LA-UR 11-02522 Los Alamos has a strong program in High Energy Density Physics aimed at National Applications as well as Basic Science Inertial Confinement Fusion (ICF) Radiation Hydrodynamics Hydrodynamics with Plasmas Material Dynamics Energetic Ion generation Dense Plasma Properties X-ray and Nuclear Diagnostic Development Petaflop performance to Exascale computing Magnetic Reconnection Magnetized Target Fusion High-Explosive Pulsed Power U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA LANL is a multidisciplinary NNSA Lab. overseen by Los Alamos National Security (LANS) LLC. People 11,782 total employees: LANS, LLC 9,665; SOC Los Alamos (Guard Force) 477; Contractors 524; Students 1,116 Place Located 35 miles northwest of Santa Fe, New Mexico, on 36 square miles of DOE-owned property. > 2,000 individual facilities, 47 technical areas with 8 million square feet under roof, $5.9 B replacement value. Operating costs FY 2010: ~ $2 billion 51% NNSA weapons programs 8% Nonproliferation programs 6% Safeguards and Security 11% Environmental Management 4% DOE Office of Science 5% Energy and other programs 15% Work for Others Workforce Demographics (LANS & students only) 42% of employees live in Los Alamos, the rest commute from Santa Fe, Española, Taos, and Albuquerque. -
The National Ignition Facility Diagnostic Set at the Completion of the National Ignition Campaign, September 2012
Fusion Science and Technology ISSN: 1536-1055 (Print) 1943-7641 (Online) Journal homepage: http://www.tandfonline.com/loi/ufst20 The National Ignition Facility Diagnostic Set at the Completion of the National Ignition Campaign, September 2012 J. D. Kilkenny, P. M. Bell, D. K. Bradley, D. L. Bleuel, J. A. Caggiano, E. L. Dewald, W. W. Hsing, D. H. Kalantar, R. L. Kauffman, D. J. Larson, J. D. Moody, D. H. Schneider, M. B. Schneider, D. A. Shaughnessy, R. T. Shelton, W. Stoeffl, K. Widmann, C. B. Yeamans, S. H. Batha, G. P. Grim, H. W. Herrmann, F. E. Merrill, R. J. Leeper, J. A. Oertel, T. C. Sangster, D. H. Edgell, M. Hohenberger, V. Yu. Glebov, S. P. Regan, J. A. Frenje, M. Gatu-Johnson, R. D. Petrasso, H. G. Rinderknecht, A. B. Zylstra, G. W. Cooper & C. Ruizf To cite this article: J. D. Kilkenny, P. M. Bell, D. K. Bradley, D. L. Bleuel, J. A. Caggiano, E. L. Dewald, W. W. Hsing, D. H. Kalantar, R. L. Kauffman, D. J. Larson, J. D. Moody, D. H. Schneider, M. B. Schneider, D. A. Shaughnessy, R. T. Shelton, W. Stoeffl, K. Widmann, C. B. Yeamans, S. H. Batha, G. P. Grim, H. W. Herrmann, F. E. Merrill, R. J. Leeper, J. A. Oertel, T. C. Sangster, D. H. Edgell, M. Hohenberger, V. Yu. Glebov, S. P. Regan, J. A. Frenje, M. Gatu-Johnson, R. D. Petrasso, H. G. Rinderknecht, A. B. Zylstra, G. W. Cooper & C. Ruizf (2016) The National Ignition Facility Diagnostic Set at the Completion of the National Ignition Campaign, September 2012, Fusion Science and Technology, 69:1, 420-451, DOI: 10.13182/FST15-173 To link to this article: http://dx.doi.org/10.13182/FST15-173 Published online: 23 Mar 2017. -
Plasma Interactions
Home Search Collections Journals About Contact us My IOPscience New developments in energy transfer and transport studies in relativistic laser–plasma interactions This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2010 Plasma Phys. Control. Fusion 52 124046 (http://iopscience.iop.org/0741-3335/52/12/124046) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 130.183.90.175 The article was downloaded on 04/01/2011 at 10:43 Please note that terms and conditions apply. IOP PUBLISHING PLASMA PHYSICS AND CONTROLLED FUSION Plasma Phys. Control. Fusion 52 (2010) 124046 (7pp) doi:10.1088/0741-3335/52/12/124046 New developments in energy transfer and transport studies in relativistic laser–plasma interactions P A Norreys1,2,JSGreen1, K L Lancaster1,APLRobinson1, R H H Scott1,2, F Perez3, H-P Schlenvoight3, S Baton3, S Hulin4, B Vauzour4, J J Santos4, D J Adams5, K Markey5, B Ramakrishna5, M Zepf5, M N Quinn6,XHYuan6, P McKenna6, J Schreiber2,7, J R Davies8, D P Higginson9,10, F N Beg9, C Chen10,TMa10 and P Patel10 1 Central Laser Facility, STFC Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0QX, UK 2 Blackett Laboratory, Imperial College London, Prince Consort Road, London SW7 2BZ, UK 3 Laboratoire pour l’Utilisation des Lasers Intenses, Ecole´ Polytechnique, route de Saclay, 91128 Palaiseau Cedex, France 4 Centre Lasers Intenses et Applications, Universite´ Bordeaux 1-CNRS-CEA, Talence, France 5 School of Mathematics and Physics, Queens University Belfast, Belfast BT7 1NN, UK 6 Departmnet of Physics, University of Strathclyde, John Anderson Building, 107 Rottenrow, Glasgow G4 0NG, UK 7 Max-Planck-Institut fur¨ Quantenoptik, Hans-Kopfermann-Str. -
1958 Geneva Conference on the Discontinuation of Nuclear Weapons
1 2 3 4 5 6 7 8 Presidential Decisions on Stockpile Stewardship Test-Based Stewardship and the Cold War Transitioning to Stockpile Stewardship Science: Research, Development, and Technology Deterrence and the Life Extension Program Global Nuclear Security Timeline of U.S. Stockpile Stewardship Innovation The Path Forward Today, I am announcing my “decision to negotiate a true zero-yield comprehensive test ban.” U.S. President Bill Clinton, August 11, 1995 The National Defense Authorization Act for fiscal year 1994 (P.L. 103-160) estab- lished the Stockpile Stewardship Program (SSP) to sustain the nuclear deterrent in the absence of nuclear explosive testing. The SSP supports U.S. national security missions through leading-edge scientific, engineering, and technical tools and expertise – a U.S. response to the end of the Cold War and the need to remake the global nuclear landscape. One year later, on August 11, 1995, Presi- dent Bill Clinton announced that the United States would support a “zero yield” Compre- hensive Nuclear-Test-Ban Treaty (CTBT): “I am assured by the Secretary of Energy and the Directors of our nu- clear weapons labs that we can meet the challenge of maintaining our nuclear deterrent under a Compre- hensive Test-Ban Treaty through a Science-Based Stockpile Stewardship program without nuclear testing.” This year, the Nation and the Department of Energy (DOE) celebrate the 20th anniver- sary of that announcement and the scientific and technical capabilities that have devel- oped to support this policy direction. The national investment in stockpile stewardship has enabled resolution of many stockpile issues and provided more detailed knowledge than what could have been attained through nuclear explosive testing. -
B O O K O F a B Stra C Ts
Book of Abstracts Program Tuesday, June 25 11:00-13:00 Registration 12:00-13:50 Lunch 13:50-14:00 Welcome UHI 1 Chair : L. Yin 14:00-14:30 A. Kemp Kinetic particle-in-cell modeling of Petawatt laser plasma interaction relevant to HEDLP experiments 14:30-14:50 R. Shah Dynamics and Application of Relativistic Transparency 14:50-15:10 C. Ridgers QED effects at UI laser intensities 15:10-15:30 L. Cao Efficient Laser Absorption, Enhanced Electron Yields and Collimated Fast Electrons by the Nanolayered Structured Targets 15:30-16:00 Coffee break Laboratory Astrophysics 1 Chair : P. Drake 16:00-16:30 J. Bailey Laboratory opacity measurements at conditions approaching stellar interiors 16:30-16:50 A. Pak Radiative shock waves produced from implosion experiments at the National Ignition Facility 16:50-17:10 B. Albertazzi Modeling in the Laboratory Magnetized Astrophysical Jets: Simulations and Experiments 17:10-17:30 C. Kuranz Magnetized Plasma Flow Experiments at High-Energy-Density Facilities Wednesday, June 26 ( Joint with WDM ) ICF 1 Chair : A. Casner 09:00-09:40 N. Landen Status of the ignition campaign at the NIF 09:40-10:00 G. Huser Equation of state and mean ionization of Ge-doped CH ablator materials 10:00-10:20 B. Remington Hydrodynamic instabilities and mix in the ignition campaign on NIF: predictions, observations, and a path forward 10:20-10:40 M. Olazabal Laser imprint reduction using underdense foams and its consequences on the hydrodynamic instability growth 10:40-11:10 Coffee break XFEL Chair : B. -
Book of Abstracts
First LMJ-PETAL User Meeting October 4-5, 2018 Le Barp, France Book of Abstracts Program LMJ-PETAL User Meeting Thursday 4 October 2018 Schedule Duration Title Speaker Institution 8:00 AM 0:30 Accueil ILP 8:30 AM 0:30 Welcome Plenary session-1 : LMJ-PETAL performance Chairman : JL. Miquel CEA/DAM CEA/DAM, 9:00 AM 0:25 LMJ Facility: Status and Performance P. Delmas France CEA/DAM, 9:25 AM 0:25 PETAL laser performance N. Blanchot France CEA/DAM, 9:50 AM 0:25 Status on LMJ-PETAL plasma diagnostics R. Wrobel France Preliminary results from the qualification experiments of the PETAL+ 10:15 AM 0:25 D. Batani CELIA, France diagnostics 10:40 AM 0:20 Break Plenary session-2: Next user experiments Chairman : D. Batani CELIA Effect of hot electrons on strong shock generation in the context of shock 11:00 AM 0:25 S. Baton LULI, France ignition 11:25 AM 0:25 Investigating magnetic reconnection in ICF conditions S. Bolanos LULI, France Efficient Creation of High-Energy-Density-State with Laser-Produced Strong S. Fujioka ILE, Osaka U., 11:50 AM 0:25 Magnetic Field or K. Matsuo Japan 12:15 PM 2:00 Lunch / Posters session 2:15 PM 1:30 Round table -1 Targets Chairman: M. Manuel General Atomic CEA/DAM, 0:20 Target laboratory on LMJ Facility O. Henry France Review of General Atomics Target Fabrication : Facilities, Capabilities and General Atomic, 0:20 M. Manuel Notable Recent Developments USA Diagnostics Chairman: W.Theobald LLE Omega ILE, Osaka U., 0:20 Visualization of fast heated plasma by X-ray fresnel phase zone plate K. -
Memorandum to Participants JASON 1994 Summer Study
Hydronnclear Testing and the Comprehensive Test Ban: Memorandum to Participants JASON 1994 Summer Study Natural Resources Defense Council, Inc. 1350 New York Avenue, NW, Suite 300 Washington, D.C. 20005 Tel (main): (202) 783-7800 Cochran (direct dial): (202) 624-9329 Paine (direct dial): (202) 624-9350 Fax: (202) 783-5917 INTERNET: [email protected] Although no commonly accepted defInition exists, a "hydronuclear test" may be generally described as a nuclear weapons test, or high-explosive driven criticality experiment, characterized by a nuclear energy release that is insuffIcient to heat the core material to the plasma temperatures that would cause it to explode "like a bomb." In such a test, the TNT equivalent energy release from fission would therefore not exceed the amount released by the chemical high explosive used to compress the fIssile material, and could be considerably ,less. Nuclear-weapon states, and possibly other states, also perform high-explosive driven implosion experiments using fusjon material, although" these' are not nonnally characterized as "hydronuclear tests". Hydronuclear tests can serve a useful role in the development of the full spectrum of unboosted fIssion weapons, including'first generation nuclear weapons of the implosion type with yields in the 5 to 30 kiloton range, more sophisticated designs with yields up to about a megaton, and advanced micro-nuclear weapons with yields of 5 to 500 tons. For pure fIssion weapons hydronuclear tests can be used to:' * optimize the timing of initiation of the -
Topical Review: Relativistic Laser-Plasma Interactions
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS J. Phys. D: Appl. Phys. 36 (2003) R151–R165 PII: S0022-3727(03)26928-X TOPICAL REVIEW Relativistic laser–plasma interactions Donald Umstadter Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI 48109, USA E-mail: [email protected] Received 19 November 2002 Published 2 April 2003 Online at stacks.iop.org/JPhysD/36/R151 Abstract By focusing petawatt peak power laser light to intensities up to 1021 Wcm−2, highly relativistic plasmas can now be studied. The force exerted by light pulses with this extreme intensity has been used to accelerate beams of electrons and protons to energies of a million volts in distances of only microns. This acceleration gradient is a thousand times greater than in radio-frequency-based accelerators. Such novel compact laser-based radiation sources have been demonstrated to have parameters that are useful for research in medicine, physics and engineering. They might also someday be used to ignite controlled thermonuclear fusion. Ultrashort pulse duration particles and x-rays that are produced can resolve chemical, biological or physical reactions on ultrafast (femtosecond) timescales and on atomic spatial scales. These energetic beams have produced an array of nuclear reactions, resulting in neutrons, positrons and radioactive isotopes. As laser intensities increase further and laser-accelerated protons become relativistic, exotic plasmas, such as dense electron–positron plasmas, which are of astrophysical interest, can be created in the laboratory. This paper reviews many of the recent advances in relativistic laser–plasma interactions. 1. Introduction in this regime on the light intensity, resulting in nonlinear effects analogous to those studied with conventional nonlinear Ever since lasers were invented, their peak power and focus optics—self-focusing, self-modulation, harmonic generation, ability have steadily increased. -
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......... -
With Short Pulse • About 7% Coupling Significantly Less Than the Osaka Experiment
Electron/proton generation from solid targets and applications Farhat Beg University of California, San Diego This work was performed under the auspices of the U.S. DOE under contracts No.DE-FG02-05ER54834, DE-FC0204ER54789 and DE-AC52-07NA27344. We greatly acknowledge support of Institute for Laser Science Applications, LLNL. Committee on Atomic, Molecular and Optical Sciences Meeting The National Academy of Sciences Washington DC, April 5, 2011 1 Summary ü Short pulse high intensity laser solid interactions create matter under extreme conditions and generate a variety of energetic particles. ü There are a number of applications from fusion to low energy nuclear reactions. 10 ns ü Fast Ignition Inertial Confinement Fusion is one application that promises high gain fusion. ü Experiments have been encouraging but point towards complex issues than previously anticipated. ü Recent, short pulse high intensity laser matter experiments show that low coupling could be due to: - prepulse - electron source divergence. ü Experiments on fast ignition show proton focusing spot is adequate for FI. However, conversion efficiency has to be increased. 2 Outline § Short Pulse High Intensity Laser Solid Interaction - New Frontiers § Extreme conditions with a short pulse laser § Applications § Fast Ignition - Progress - Current status § Summary Progress in laser technology 10 9 2000 Relativistic ions 8 Nonlinearity of 10 Vacuum ) Multi-GeV elecs. V 7 1990 Fast Ignition e 10 ( e +e- Production y 6 Weapons Physics g 10 Nuclear reactions r e 5 Relativistic -
Dangerous Thermonuclear Quest: the Potential of Explosive Fusion Research for the Development of Pure Fusion Weapons
Dangerous Thermonuclear Quest: The Potential of Explosive Fusion Research for the Development of Pure Fusion Weapons Arjun Makhijani, Ph.D. Hisham Zerriffi July 1998 Minor editing revisions made in 2003. Table of Contents Preface i Summary and Recommendations v Summary of Findings vi Recommendations vii Chapter 1: Varieties of Nuclear Weapons 1 A. Historical Background 1 B. Converting Matter into Energy 4 C. Fission energy 5 D. Fusion energy 8 E. Fission-fusion weapons 16 Chapter 2: Inertial Confinement Fusion Basics 19 A. Deposition of driver energy 24 B. Driver requirements 25 C. Fuel pellet compression 27 D. Thermonuclear ignition 29 Chapter 3: Various ECF Schemes 31 A. Laser Drivers 32 B. Ion Beam Drivers 34 1. Heavy Ion Beams 35 a. Induction Accelerators 36 b. Radio-Frequency Accelerators 36 2. Light Ion Beams 37 C. Z-pinch 39 D. Chemical Explosives 40 E. Advanced materials manufacturing 42 1. Nanotechnology 42 2. Metallic Hydrogen 45 Chapter 4: The Prospects for Pure Fusion Weapons 47 A. Requirements for pure fusion weapons 47 B. Overall assessment of non-fission-triggered nuclear weapons 48 1. Ignition 48 2. Drivers 53 C. Overall technical prognosis for non-fission triggered nuclear weapons 54 D. Fusion power and fusion weapons - comparative requirements 56 Chapter 5: Nuclear Disarmament and Non-Proliferation Issues Related to Explosive Confinement Fusion 59 A. The Science Based Stockpile Stewardship Program 62 1. Reliability 62 a. Reliability definition 63 b. Future reliability problems 64 c. Relevance of NIF to reliability of the current stockpile 65 2. The US laser fusion program as a weapons development program 65 3. -
A Novel Three-Axis Cylindrical Hohlraum Designed
www.nature.com/scientificreports OPEN A novel three-axis cylindrical hohlraum designed for inertial confinement fusion ignition Received: 19 May 2016 Longyu Kuang1,2,3, Hang Li1,2,3, Longfei Jing1, Zhiwei Lin1, Lu Zhang1, Liling Li1, Accepted: 12 September 2016 Yongkun Ding1,2,3,4, Shaoen Jiang1,2,3,4, Jie Liu3,4,5 & Jian Zheng2,4 Published: 05 October 2016 A novel ignition hohlraum for indirect-drive inertial confinement fusion is proposed, which is named three-axis cylindrical hohlraum (TACH). TACH is a kind of 6 laser entrance holes (LEHs) hohlraum, which is orthogonally jointed of three cylindrical hohlraums. Laser beams are injected through every entrance hole with the same incident angle of 55°. A view-factor simulation result shows that the time-varying drive asymmetry of TACH is less than 1.0% in the whole drive pulse period without any supplementary technology. Coupling efficiency of TACH is close to that of 6 LEHs spherical hohlraum with corresponding size. Its plasma-filling time is close to that of typical cylindrical ignition hohlraum. Its laser plasma interaction has as low backscattering as the outer cone of the cylindrical ignition hohlraum. Therefore, TACH combines most advantages of various hohlraums and has little predictable risk, providing an important competitive candidate for ignition hohlraum. In indirect-drive Inertial Confinement Fusion (ICF), laser beams are injected into a high-Z hohlraum through laser entrance holes (LEHs) and are converted into X-ray radiation, then the radiation irradiates a low-Z capsule in the center of the hohlraum to bring the central fuel in the capsule to ignition conditions1–6.