High Energy Density Physics related to Inertial Fusion with Intense Ion and Laser Beams at GSI and FAIR in Darmstadt
|
|
- Nigel Lewis
- 5 years ago
- Views:
Transcription
1 High Energy Density Physics related to Inertial Fusion with Intense Ion and Laser Beams at GSI and FAIR in Darmstadt Dieter H.H. Hoffmann Radiation- and Nuclear Physics Technical University Darmstadt HEDgeHOB Collaboration Currently guest at : Chinese Acad. Science, IMP, Lanzhou IAEA Vienna March 2015 Workshop Physics and Technology of Inertial Fusion
2 Topics: Remarks on Inertial Fusion Properties of Heavy Ion Beams Ion Beam Plasma Interaction Generating WARM DENSE MATTER with Ion Beams Diagnostics: Proton Microscopy 2
3 Physics Technology and Fusion Energy 40 years
4 Indirectly heated Fusion -Target Hohlraumtarget Compression Burn Surface heating by radiation Ignition
5 Fast Ignition Scenario with Heavy Ion Driver M. Roth, TU-Darmstadt
6 Heavy Ion Driven Ignition Facility (HIDIF)
7 Ion- and Laserbeam Interaction with Matter
8 PHASE DIAGRAM OF MATTER Lg N Z 4 HE Γ~ 1 Metals nλ 3 ~ 1 Sparc arc Semicond. Γ~ 1 Flames Γ~10 4 TF Jupiter Γ~ Heavy Ion Beams Ionization Plasma processing Ry MHD Z, Θpinch White Dwarth SUN B. Dwarth Debye Fusion-IC Relativistic T ~ mc 2 Tokamak e + e - pairs Stellar Corona 1 Tb FAIR 1 Gb 1 Mb Big Bang Big Bang Lg T V.E. Fortov
9 Ion Beam Facilities for HEDP (Past) GSI, Darmstadt ИТЭФ, Москва HIFS-VNL, Berkeley IMP, Lanzhou
10 Rare Isotope Science Project M. Chung Korea 10
11 Nazarbayev University at Astana, Kazakhstan is building a facility for HIF/HEDP research
12 The NURA Facility for HIF and HEDP Research Control Room Target Fab and Experiment Prep Clean Room Accelerator Hall NDCX-2 is 14.5m 3MeV Li + Diagnostic Laser The new NURA beam line is ~ 12 m long Drive Laser Compressor From Drive Laser Target Area Clean Room
13 Uniform ion beamheating to create WDM (~ 1 evtemperature) ~mm spot-size ~µm thickness ~30 nc Li at 3 MeV (NDCX-2) ~1 ns high intensity, short pulse ion beam
14 Ion Beam Facilities for HEDP (Future) FAIR, Darmstadt HIAF, China (Lanzhou)
15
16 Beam Parameters SIS-18 FAIR(Ph-I) HIAF (V1) E 0 0.4GeV/u 1 GeV/u 1.1 GeV/u N E total 0.06 kj 15kJ 40 kj S f ~1 mm ~1 mm 1mm-0.5 mm τ 130 ns 50 ns 130ns-33ns E s ~1kJ/g 120 kj/g 300 kj/g-1.2mj/g E ρ J/m J/m J/m J/m 3
17 FAIR Construction Site
18
19
20 Copper target with Au coating C. Maurer, L. Bozyk, P. Spiller
21
22 Yulia Shutko, S. Udrea, P. Forck
23 Yulia Shutko, S. Udrea, P. Forck
24 Yulia Shutko, S. Udrea, P. Forck
25 Yulia Shutko, S. Udrea, P. Forck
26 Intense Beam Diagnostics Said El Moussati, S. Udrea
27
28
29
30
31
32
33
34 HEDgeHOB Experimental Program 34
35 Heating Matter with Intense Ion Beams Ne 10+ beam at E 0 =300MeV/u penetrating into a Kr crystal Intense Pulse of Heavy Ions Bragg Peak
36 Physics of Generating High Energy Density in Matter with Ion Beams P ρ = E τ ρ b de dx = π r 2 N τ b [ g J ] s Eρ: Specific Deposition Energy [J/g] τ b : Beam bunch length [s] Pρ :Specific Deposition Power [W/g]
37 What are the most interesting problems for the next 10 years? What type of experiments can be done at new international facilities HED regions of the phase diagram accessible by intense heavy ion beams
38 Heavy ion beam can be used as an efficient diagnostic tool for HED experiments heavy ion beam solid target Energy Loss Dynamics (ELD) time-resolving energy loss spectrometer SIS-18 heavy ion beam Target collimators fast scintillator target chamber streak camera
39 ELD provides direct quantitative information about the physical state of the interior of the target Verification of EOS model for neon Energy loss [%] U, MeV/u} solid Ne Time [ns] SESAME ChTEOS experiment Energy loss [%] U, MeV/u} solid Ne Time [ns] SESAME ChTEOS experiment For HEDgeHOB experiments: main SIS-100 heating pulse (50 ns) complementary 90º ion beam (200ns-1.4µs) from SIS-18 time-resolved target density along the axis and in the transverse plane, stopping properties of dense non-ideal plasmas D. Varentsov et al.: Europhys. Lett. 64 (2003) 57; Laser and Part. Beams 20 (2002) 485; Nucl. Instr. Meth. B174 (2001) 215.
40 HEDP experiments with intense heavy ion beams HHT: High energy High Temperature: ions up to U, AMeV pulse duration ns focal spot size mm diagnostics for intense, short ion pulses Beams for HEDP experiments: 238 U 73+, 350 AMeV, e-cooled ions in ns bunch 300 µm (FWHM) spot at the target Solid metallic targets: specific energy: ~ kj/g temperature: up to 2 ev pressure: in multi-kbar range
41 N. Tahir
42
43
44
45
46
47
48
49
50
51 P. Lang, M. Endres, D. Varentsov, S. Udrea See also Frank Merrill on Tuesday
52
53 Permanent Magnetic Quadrupoles (PMQ) design High Gradient Split-Pole Quadrupole Extremely High-Level Gradient-Maximal Demagnetization Factor Flexible Choice of the REPM Coercivity on Magnetization Minimal Demagnetization in Median Planes (in Critical Spaces) Gradient Fixed PMQ parameter Inner aperture, 2 Ri Outer dimensions, 2 Ro x L Internal ring magnetization External ring magnetization Pole tip field Value 15 mm 79 x 100 mm 1.16 T 1.19 T 1.7 T
54
55
56 Technical Proposal PRIOR: Proton Microscope at FAIR COSY simulation of magnetic optics
57 PRIOR: Proton Microscope at FAIR QSM quadrupole Magnetic aperture diameter Pole tip field 1.3 T Module length 40 mm 40 mm ITEP proton microscope Four Modules Assembly Axis Gradient Distribution Blue field simulation Red field measurements 1 mm 1 mm
58
59
60
61
62
63
64
65
66
67
68
69
70 The HEDgeHOB collaboration: Studies on high energy density matter with intense heavy ion and laser beams at FAIR (officially inaugurated: June 2005) >200 Scientists 44 Institutes 15 Countries 70
From Inertial Fusion Energy to Accelerator Driven High Energy Density Physics
From Inertial Fusion Energy to Accelerator Driven High Energy Density Physics 霍迪 Dieter HH Hoffmann 1,2 Y. Zhao 1,3, P. Katrick 4 and M. Schanz 4 1)Xi An Jiaotong University, School of Science, Xi An,
More informationPRIOR. Proton Microscope for FAIR
PRIOR Proton Microscope for FAIR Proton Radiography Basics X-rays and protons ranges in matter X-rays 3-10 MeV (Flux attenuation in e times) High Energy Protons ~ GeV cm 1 cm Pb Protons Image Blurring
More informationIon Acceleration from the Interaction of Ultra-Intense Laser Pulse with a Thin Foil
Ion Acceleration from the Interaction of Ultra-Intense Laser Pulse with a Thin Foil Matthew Allen Department of Nuclear Engineering UC Berkeley mallen@nuc.berkeley.edu March 15, 2004 8th Nuclear Energy
More informationHeavy ion fusion energy program in Russia
Nuclear Instruments and Methods in Physics Research A 464 (2001) 1 5 Heavy ion fusion energy program in Russia B.Yu. Sharkov*, N.N. Alexeev, M.D. Churazov, A.A. Golubev, D.G. Koshkarev, P.R. Zenkevich
More informationFigure 1: The current target chamber and beam diagnostic station for the NDCX-I beamline will be used during commissioning of NDCX-II in 2012
Progress in U.S. Heavy Ion Fusion Research* IAEA-10 IFE/P6-06 B G Logan, J J Barnard, F M Bieniosek, R H Cohen, R C Davidson, P C Efthimion, A Friedman, E P Gilson, L R Grisham, D P Grote, E Henestroza,
More informationApplication of Proton Radiography to High Energy Density Research
Application of Proton Radiography to High Energy Density Research S.A. Kolesnikov*, S.V. Dudin, V.B. Mintsev, A.V. Shutov, A.V. Utkin, V.E. Fortov IPCP RAS, Chernogolovka, Russia A.A. Golubev, V.S. Demidov,
More informationHigh-Intensity Ion Beam Neutralization and Drift Compression Experiments
1 / 37 High-Intensity Ion Beam Neutralization and Drift Compression Experiments Prabir K. Roy 1 1 Lawrence Berkeley National Laboratory (LBNL) Berkeley, CA 94720 March 08, 2010 (with S. S. Yu, P.A. Seidl,
More informationFAIR. International Facility for Antiproton and Ion. Research
FAIR International Facility for Antiproton and Ion Research FAIR One of the largest scientific project in the world with a broad spectrum of research programs: - Nuclear physics - Hadron physics - Atomic
More informationa Gesellschaft für Schwerionenforschung, Planckstrasse 1, Darmstadt, Germany
Nuclear Instruments and Methods in Physics Research A 544 (25) 16 26 www.elsevier.com/locate/nima Studies of heavy ion-induced high-energy density states in matter at the GSI Darmstadt SIS-18 and future
More informationIntegrated Modeling of Fast Ignition Experiments
Integrated Modeling of Fast Ignition Experiments Presented to: 9th International Fast Ignition Workshop Cambridge, MA November 3-5, 2006 R. P. J. Town AX-Division Lawrence Livermore National Laboratory
More informationBeam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.
Beam Loss Monitors When energetic beam particles penetrates matter, secondary particles are emitted: this can be e, γ, protons, neutrons, excited nuclei, fragmented nuclei... Spontaneous radiation and
More informationPerspectives in High Intensity Heavy Ion Sources for Future Heavy Ion Accelerators. L. Sun
IMP Perspectives in High Intensity Heavy Ion Sources for Future Heavy Ion Accelerators L. Sun Institute of Modern Physics, CAS, 730000, Lanzhou, China IPAC 18, April 29~May 4, 2018,Vancouver, CA Preface
More informationOptimization of the SIS100 Lattice and a Dedicated Collimation System for Ionisation Losses
Optimization of the SIS100 Lattice and a Dedicated Collimation System for Ionisation Losses P. Spiller, K. Blasche, B. Franczak, J. Stadlmann, and C. Omet GSI Darmstadt, D-64291 Darmstadt, Germany Abstract:
More informationBeam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI)
Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI), 2003, A dedicated proton accelerator for 1p-physics at the future GSI Demands facilities for
More informationThe MEC endstation at LCLS New opportunities for high energy density science
The MEC endstation at LCLS New opportunities for high energy density science Singapore, fttp-5, April 20th, 2011 Bob Nagler BNagler@slac.stanford.edu SLAC national accelerator laboratory 1 Overview Motivation
More informationScaling Hot-Electron Generation to High-Power, Kilojoule-Class Lasers
Scaling Hot-Electron Generation to High-Power, Kilojoule-Class Lasers 75 nm 75 75 5 nm 3 copper target Normalized K b /K a 1.2 1.0 0.8 0.6 0.4 Cold material 1 ps 10 ps 0.2 10 3 10 4 Heating 2.1 kj, 10
More informationSLAC National Accelerator Laboratory FACET & TEST BEAM FACILITIES PROPOSAL
SLAC National Accelerator Laboratory FACET & TEST BEAM FACILITIES PROPOSAL Date: 6/17/13 A. EXPERIMENT TITLE: Development of Electron Radiography for Material Science B. PROPOSERS & REQUESTED FACILITY:
More informationExtreme Light Infrastructure - Nuclear Physics ELI - NP
Extreme Light Infrastructure - Nuclear Physics ELI - NP Nicolae-Victor Zamfir National Institute for Physics and Nuclear Engineering (IFIN-HH) Bucharest-Magurele, Romania www.eli-np.ro Bucharest-Magurele
More informationDevelopments for the FEL user facility
Developments for the FEL user facility J. Feldhaus HASYLAB at DESY, Hamburg, Germany Design and construction has started for the FEL user facility including the radiation transport to the experimental
More informationPoS(EPS-HEP2017)533. First Physics Results of AWAKE, a Plasma Wakefield Acceleration Experiment at CERN. Patric Muggli, Allen Caldwell
First Physics Results of AWAKE, a Plasma Wakefield Acceleration Experiment at CERN Patric Muggli, Max Planck Institute for Physics E-mail: muggli@mpp.mpg.de AWAKE is a plasma wakefield acceleration experiment
More informationActivities on Proton radiography at ITEP
Activities on Proton radiography at ITEP A. Golubev ITEP, Moscow XXIV RuPAC Obninsk, Russia 08.10. 2014 The prad collaboration Institute for Theoretical and Experimental Physics, Moscow, Russia A.Kantsyrev,
More informationNuclear Fusion with Polarized Fuel
Mitglied der Helmholtz-Gemeinschaft Nuclear Fusion with Polarized Fuel -Some thoughts on the PREFER collaboration - Workshop on Nuclear Fusion with Polarized Fuel Ferrara 2/3 October 2017 Markus Büscher
More informationHeavy ion fusion science research for high energy density physics and fusion applications*
Heavy ion fusion science research for high energy density physics and fusion applications* B G Logan 1, J J Barnard 2, F M Bieniosek 1, R H Cohen 2, J E Coleman 1, R C Davidson 3, P C Efthimion 3, A Friedman
More informationPhysics with Exotic Nuclei
Physics with Exotic Nuclei Hans-Jürgen Wollersheim NUclear STructure, Astrophysics and Reaction Outline Projectile Fragmentation A Route to Exotic Nuclei Fragmentation Cross Sections Nuclear Reaction Rates
More informationEnergy loss measurements of swift ions penetrating hot and dense plasma at the UNILAC
Energy loss measurements of swift ions penetrating hot and dense plasma at the UNILAC Abel Blažević A. Frank, T. Hessling, D.H.H. Hoffmann, R. Knobloch-Mass, A. Pelka, M. Roth, G. Schaumann, M. Schollmeier,
More informationBEAM PARAMETERS FROM SIS18 AND SIS100 ON TARGETS
BEAM PARAMETERS FROM SIS18 AND SIS100 ON TARGETS V. Kornilov Primary Beams, Beam Physics GSI Darmstadt, Germany Vladimir Kornilov, HIC4FAIR Workshop, 28-31 July 2015, Hamburg FAIR: BEAM PARAMETERS 2007:
More informationA Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling
A Multi-beamlet Injector for Heavy Ion Fusion: Experiments and Modeling G.A. Westenskow, D.P. Grote; LLNL J.W. Kwan, F. Bieniosek; LBNL PAC07 - FRYAB01 Albuquerque, New Mexico June 29, 2007 This work has
More informationExperimental study of nonlinear laser-beam Thomson scattering
Experimental study of nonlinear laser-beam Thomson scattering T. Kumita, Y. Kamiya, T. Hirose Department of Physics, Tokyo Metropolitan University, 1-1 Minami-Ohsawa, Hachioji, Tokyo 192-0397, Japan I.
More informationUsing a Relativistic Electron Beam to Generate Warm Dense Matter for Equation of State Studies
Using a Relativistic Electron Beam to Generate Warm Dense Matter for Equation of State Studies DOE/NV/25946--1257 M. J. Berninger National Security Technologies, LLC, Los Alamos, NM 87544 T. J. T. Kwan,
More informationLIGHT. ...from laser ion acceleration to future applications. - project overview and lates experimental results -
LIGHT...from laser ion acceleration to future applications - project overview and lates experimental results - 1st European Advanced Accelerator Concepts Workshop La Biodola, Isola d'elba 2nd 7th June
More informationExploration of the Feasibility of Polar Drive on the LMJ. Lindsay M. Mitchel. Spencerport High School. Spencerport, New York
Exploration of the Feasibility of Polar Drive on the LMJ Lindsay M. Mitchel Spencerport High School Spencerport, New York Advisor: Dr. R. S. Craxton Laboratory for Laser Energetics University of Rochester
More informationAn Overview of Laser-Driven Magnetized Liner Inertial Fusion on OMEGA
An Overview of Laser-Driven Magnetized Liner Inertial Fusion on OMEGA 4 compression beams MIFEDS coils B z ~ 1 T Preheat beam from P9 1 mm Ring 3 Rings 4 Ring 3 Target support Fill-tube pressure transducer
More informationFRIB Production Target. Frederique Pellemoine Visiting Associate Professor
FRIB Production Target Frederique Pellemoine Visiting Associate Professor FRIB a DOE-SC National User Facility Enabling Scientists to Make Discoveries Properties of nucleonic matter Classical domain of
More informationFast Ignition Experimental and Theoretical Researches toward Fast Ignition Realization Experiment (FIREX)
1 Fast Ignition Experimental and Theoretical Researches toward Fast Ignition Realization Experiment (FIREX) K. Mima 1), H. Azechi 1), H. Fujita 1), Y. Izawa 1), T. Jitsuno 1), T. Johzaki 1), Y. Kitagawa
More informationTHE SUPER-FRS PROJECT AT GSI
THE SUPER-FRS PROJECT AT GSI M. Winkler 1,2, H. Geissel 2,1,, G. Münzenberg 2, V. Shiskine 2, H. Weick 2, H. Wollnik 1, M. Yavor 3 1 University of Giessen, Germany, 2 GSI, Germany, 3 Institute for Analytical
More informationIn-Kind FAIR. David Urner. FAIR, Darmstadt , D. Urner 1
In-Kind FAIR David Urner FAIR, Darmstadt 4.11.2015, D. Urner 1 Overview Existing Facility HEBT High Energy Beam Transport SIS100 heavy (Schwer) Ion Syncrotron CRYRING HESR High Energy Storage Ring p-bar
More informationAdvanced Ignition Experiments on OMEGA
Advanced Ignition Experiments on OMEGA C. Stoeckl University of Rochester Laboratory for Laser Energetics 5th Annual Meeting of the American Physical Society Division of Plasma Physics Dallas, TX 17 21
More informationInfluence of the equation of state of matter and ion beam characteristics on target heating and compression
PHYSICAL REVIEW SPECIAL TOPICS - ACCELERATORS AND BEAMS, VOLUME 6, 211 (23) Influence of the equation of state of matter and ion beam characteristics on target heating and compression N. A. Tahir, 1 A.
More informationReview of Heavy-Ion Inertial Fusion Physics
Review of Heavy-Ion Inertial Fusion Physics S. Kawata 1, 2, *, T. Karino 1, and A. I. Ogoyski 3 1 Graduate School of Engineering, Utsunomiya University, Yohtoh 7-1-2, Utsunomiya 321-8585, Japan 2 CORE
More informationMarkus Roth TU Darmstadt
Laser-driven Production of Particle Beams and their application to medical treatment Markus Roth TU Darmstadt The Case Laser-driven electrons Potential for Applications in Therapy Use of secondary Radiation
More informationLetter of Intent: Nuclear Fusion Reactions from laser-accelerated fissile ion beams
Letter of Intent: Nuclear Fusion Reactions from laser-accelerated fissile ion beams Peter G. Thirolf, LMU Munich D. Habs, H. Ruhl, J. Schreiber, LMU Munich, MPQ Garching T. Dickel, H. Geissel, W. Plass,
More informationExploring Astrophysical Magnetohydrodynamics Using High-power Laser Facilities
Exploring Astrophysical Magnetohydrodynamics Using High-power Laser Facilities Mario Manuel Einstein Fellows Symposium Harvard-Smithsonian Center for Astrophysics October 28 th, 2014 Ø Collimation and
More informationDetectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014
Detectors in Nuclear and High Energy Physics RHIG summer student meeting June 2014 Physics or Knowledge of Nature Experimental Data Analysis Theory ( application) Experimental Data Initial Conditions /
More informationENERGY DEPOSITION EFFECTS OF THE X PHOTON BEAM ON THE MIRROR OF PLASMON-X EXPERIMENT AT LI2FE. Francesco Broggi, Luca Serafini
SPARC-EBD -10/01 21 Luglio 2010 ENERGY DEPOSITION EFFECTS OF THE X PHOTON BEAM ON THE MIRROR OF PLASMON-X EXPERIMENT AT LI2FE Francesco Broggi, Luca Serafini INFN-LASA-Sezione di Milano, Via F.ll icervi
More informationUltrafast X-Ray-Matter Interaction and Damage of Inorganic Solids October 10, 2008
Ultrafast X-Ray-Matter Interaction and Damage of Inorganic Solids October 10, 2008 Richard London rlondon@llnl.gov Workshop on Interaction of Free Electron Laser Radiation with Matter Hamburg This work
More informationSCIENTIFIC ACTIVITIES AND PERSPECTIVES AT TWAC
SCIENTIFIC ACTIVITIES AND PERSPECTIVES AT TWAC A.A. Golubev, A.A.Drozdovskyi 1, A.D.Fertman 1, V.E.Fortov 2, K.Gubskyi 1,5, D.H.H. Hoffmann 3, A.Hudomjasov, V.S.Demidov 1, E.V.Demidova 1, S.V.Dudin 2,
More informationLaser trigged proton acceleration from ultrathin foil
Laser trigged proton acceleration from ultrathin foil A.V. Brantov 1, V. Yu. Bychenkov 1, D. V. Romanov 2, A. Maksimchuk 3 1 P. N. Lebedev Physics Institute RAS, Moscow 119991, Russia 2 All-Russia Research
More informationDevelopment of a WDM platform for chargedparticle stopping experiments
Journal of Physics: Conference Series PAPER OPEN ACCESS Development of a WDM platform for chargedparticle stopping experiments To cite this article: A B Zylstra et al 216 J. Phys.: Conf. Ser. 717 12118
More informationInvestigations on warm dense plasma with PHELIX facility
2 nd EMMI Workshop on Plasma Physics with Intense Laser and Heavy Ion Beams, May 14-15, Moscow Investigations on warm dense plasma with PHELIX facility S.A. Pikuz Jr., I.Yu. Skobelev, A.Ya. Faenov, T.A.
More informationSTORAGE RINGS FOR RADIO-ISOTOPE BEAMS
STORAGE RINGS FOR RADIO-ISOTOPE BEAMS Takeshi Katayama, Center for Nuclear Study, University of Tokyo, Wako, Japan INTRODUCTION In this decade, new era is opened in nuclear physics with use of radioactive
More informationFAIR AT GSI. P. Spiller, GSI, Darmstadt, Germany
FAIR AT GSI P. Spiller, GSI, Darmstadt, Germany Abstract Based on the experience of the existing GSI facility and with the aim to apply new technical concepts in phase space cooling and fast ramping of
More informationIntegrated simulations of fast ignition of inertial fusion targets
Integrated simulations of fast ignition of inertial fusion targets Javier Honrubia School of Aerospace Engineering Technical University of Madrid, Spain 11 th RES Users Meeting, Santiago de Compostela,
More informationReferences and Figures from: - Basdevant, Fundamentals in Nuclear Physics
Lecture 22 Fusion Experimental Nuclear Physics PHYS 741 heeger@wisc.edu References and Figures from: - Basdevant, Fundamentals in Nuclear Physics 1 Reading for Next Week Phys. Rev. D 57, 3873-3889 (1998)
More informationECR ION SOURCES : A BRIEF HISTORY AND LOOK INTO THE NEXT GENERATION
ECR ION SOURCES : A BRIEF HISTORY AND LOOK INTO THE NEXT GENERATION T. Nakagawa, Nishina center for accelerator based science, RIKEN, Hirosawa 2-1, Wako, Saitama 351-0198, Japan Abstract In the last three
More informationFirst Results from Cryogenic-Target Implosions on OMEGA
First Results from Cryogenic-Target Implosions on OMEGA MIT 1 mm 1 mm 100 µm C. Stoeckl University of Rochester Laboratory for Laser Energetics 43rd Annual Meeting of the American Physical Society Division
More informationMulti-Purpose Accelerator-Accumulator ITEP-TWAC for Nuclear Physics and Practical Applications
Multi-Purpose Accelerator-Accumulator ITEP-TWAC for Nuclear Physics and Practical Applications N.N.Alexeev, D.G.Koshkarev and B.Yu.Sharkov Institute for Theoretical and Experimental Physics, B.Cheremushk.
More informationPIC simulations of laser interactions with solid targets
PIC simulations of laser interactions with solid targets J. Limpouch, O. Klimo Czech Technical University in Prague, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7, Praha 1, Czech Republic
More informationFast proton bunch generation in the interaction of ultraintense laser pulses with high-density plasmas
Fast proton bunch generation in the interaction of ultraintense laser pulses with high-density plasmas T.Okada, Y.Mikado and A.Abudurexiti Tokyo University of Agriculture and Technology, Tokyo -5, Japan
More informationProton-driven plasma wakefield acceleration
Proton-driven plasma wakefield acceleration Konstantin Lotov Budker Institute of Nuclear Physics SB RAS, Novosibirsk, Russia Novosibirsk State University, Novosibirsk, Russia AWAKE Collaboration Motivation
More informationExperimental Initiatives in Nuclear Astrophysics
Experimental Initiatives in Nuclear Astrophysics Carl Brune Astrophysics: H and He burning, S process Facilities: neutron and gamma beams, underground accelerators, ICF plasmas Joint DNP Town Meetings
More informationMeasurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo)
Measurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo) in collaboration with Spencer Gessner (CERN) presented by Erik Adli (University of Oslo) FACET-II Science Workshop
More informationHITRAP Low Energy Diagnostics and Emittance Measurement
HITRAP Low Energy Diagnostics and Emittance Measurement Jochen Pfister 1, Oliver Kester 2, Ulrich Ratzinger 1, Gleb Vorobjev 3 1 Institut für Angewandte Physik, JW Goethe-University Frankfurt, Germany
More informationMagnetized High-Energy-Density Plasma
LLNL PRES 446057 Magnetized High-Energy-Density Plasma D.D. Ryutov Lawrence Livermore National Laboratory, Livermore, CA 94551, USA Presented at the 2010 Science with High-Power Lasers and Pulsed Power
More informationPolar Direct-Drive Simulations for a Laser-Driven HYLIFE-II Fusion Reactor. Katherine Manfred
Polar Direct-Drive Simulations for a Laser-Driven HYLIFE-II Fusion Reactor Katherine Manfred Polar Direct-Drive Simulations for a Laser-Driven HYLIFE-II Fusion Reactor Katherine M. Manfred Fairport High
More informationIntroductory Astrophysics A113. Death of Stars. Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM
Goals: Death of Stars Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM Low Mass Stars (M
More informationDevelopment of a table top TW laser accelerator for medical imaging isotope production
Development of a table top TW laser accelerator for medical imaging isotope production R U I Z, A L E X A N D R O 1 ; L E R A, R O B E R T O 1 ; T O R R E S - P E I R Ó, S A LVA D O R 1 ; B E L L I D O,
More informationEfficient Energy Conversion of the 14MeV Neutrons in DT Inertial Confinement Fusion. By F. Winterberg University of Nevada, Reno
Efficient Energy Conversion of the 14MeV Neutrons in DT Inertial Confinement Fusion By F. Winterberg University of Nevada, Reno Abstract In DT fusion 80% of the energy released goes into 14MeV neutrons,
More informationFLASH overview. Nikola Stojanovic. PIDID collaboration meeting, Hamburg,
FLASH overview Nikola Stojanovic PIDID collaboration meeting, Hamburg, 16.12.2011 Outline Overview of the FLASH facility Examples of research at FLASH Nikola Stojanovic PIDID: FLASH overview Hamburg, December
More informationHigh Resolution Electron Spectrometry at the NESR. Ajay Kumar
High Resolution Electron Spectrometry at the NESR Collaboration Ajay Kumar GSI, Darmstadt Stored Particles Atomic Physics Research Collaboration R. Mann G. Garcia X. Ma B. Sulik J. Ullrich L.C. Tribedi
More informationAccelerator Activities at PITZ
Accelerator Activities at PITZ Plasma acceleration etc. Outline > Motivation / Accelerator Research & Development (ARD) > Plasma acceleration Basic Principles Activities SINBAD > ps-fs electron and photon
More informationSpiraling Beam Illumination Uniformity on Heavy Ion Fusion Target
Spiraling Beam Illumination Uniformity on Heavy Ion Fusion Target T. Kurosaki a, S. Kawata a, K. Noguchi a, S. Koseki a, D. Barada a, Y. Y. Ma a, A. I. Ogoyski b, J. J. Barnard c and B. G. Logan c a Graduate
More informationPHITS calculation of the radiation field in HIMAC BIO
PHITS calculation of the radiation field in HIMAC BIO Ondřej Ploc, Yukio Uchihori, Hisashi Kitamura, Lembit Sihver National Institute of Radiological Sciences, Chiba, Japan Nuclear Physics Institute, Prague,
More informationChapter IX: Nuclear fusion
Chapter IX: Nuclear fusion 1 Summary 1. General remarks 2. Basic processes 3. Characteristics of fusion 4. Solar fusion 5. Controlled fusion 2 General remarks (1) Maximum of binding energy per nucleon
More informationLawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory
Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Title High current density beamlets from RF Argon source for heavy ion fusion applications Permalink https://escholarship.org/uc/item/6zh6c50m
More informationICF ignition and the Lawson criterion
ICF ignition and the Lawson criterion Riccardo Betti Fusion Science Center Laboratory for Laser Energetics, University of Rochester Seminar Massachusetts Institute of Technology, January 0, 010, Cambridge
More informationElectron Spectrometer for FLASHForward Plasma-Wakefield Accelerator
Electron Spectrometer for FLASHForward Plasma-Wakefield Accelerator Artemis Kontogoula Supervisor: Vladyslav Libov September 7, 2017 National & Kapodistrian University of Athens, Greece Deutsches Elektronen-Synchrotron
More informationDiagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site
1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at
More informationThe EDM Polarimeter Development at COSY-Jülich
Noname manuscript No. (will be inserted by the editor) The EDM Polarimeter Development at COSY-Jülich Fabian Müller for the JEDI Collaboration Received: date / Accepted: date Abstract The JEDI (Jülich
More informationTAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University
TAMU-TRAP facility for Weak Interaction Physics P.D. Shidling Cyclotron Institute, Texas A&M University Outline of the talk Low energy test of Standard Model T =2 Superallowed transition Facility T-REX
More informationWhat is. Inertial Confinement Fusion?
What is Inertial Confinement Fusion? Inertial Confinement Fusion: dense & short-lived plasma Fusing D and T requires temperature to overcome Coulomb repulsion density & confinement time to maximize number
More informationThe scanning microbeam PIXE analysis facility at NIRS
Nuclear Instruments and Methods in Physics Research B 210 (2003) 42 47 www.elsevier.com/locate/nimb The scanning microbeam PIXE analysis facility at NIRS Hitoshi Imaseki a, *, Masae Yukawa a, Frank Watt
More informationMinicourse on Experimental techniques at the NSCL Fragment Separators
Minicourse on Experimental techniques at the NSCL Fragment Separators Thomas Baumann National Superconducting Cyclotron Laboratory Michigan State University e-mail: baumann@nscl.msu.edu August 2, 2001
More informationEXTREME ULTRAVIOLET AND SOFT X-RAY LASERS
Chapter 7 EXTREME ULTRAVIOLET AND SOFT X-RAY LASERS Hot dense plasma lasing medium d θ λ λ Visible laser pump Ch07_00VG.ai The Processes of Absorption, Spontaneous Emission, and Stimulated Emission Absorption
More informationExperimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ
Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ Introduction Outline Optimization of Electron Beams Calculations of CTR/CDR Pulse Energy Summary & Outlook Prach Boonpornprasert
More informationLow energy high brilliance beam characterization
Low energy high brilliance beam characterization J. Bähr, DESY, Zeuthen, Germany Abstract Low energy high brilliance beam characterization plays an important role for electron sources and injectors of
More informationNON LINEAR PULSE EVOLUTION IN SEEDED AND CASCADED FELS
NON LINEAR PULSE EVOLUTION IN SEEDED AND CASCADED FELS L. Giannessi, S. Spampinati, ENEA C.R., Frascati, Italy P. Musumeci, INFN & Dipartimento di Fisica, Università di Roma La Sapienza, Roma, Italy Abstract
More informationMøller Polarimetry on Atomic Hydrogen
E.Chudakov June 21, 2011 Møller Polarimetry on Atomic Hydrogen 1 Møller Polarimetry on Atomic Hydrogen E.Chudakov 1 1 JLab Meeting at UVA Outline E.Chudakov June 21, 2011 Møller Polarimetry on Atomic Hydrogen
More informationThe Superconducting SIS100 Synchrotron for High Intensity Proton and Heavy Ion Beams
The Superconducting SIS100 Synchrotron for High Intensity Proton and Heavy Ion Beams Peter Spiller HB2008 26.8.2008 GSI/FAIR Accelerator Facility Primary Beam Intensity x 100-1000 Secondary Beam Intensity
More informationUnpressurized steam reactor. Controlled Fission Reactors. The Moderator. Global energy production 2000
From last time Fission of heavy elements produces energy Only works with 235 U, 239 Pu Fission initiated by neutron absorption. Fission products are two lighter nuclei, plus individual neutrons. These
More informationNUMERICAL MODELING OF LASER-DRIVEN ION ACCELERATION FROM NEAR-CRITICAL GAS TARGETS
NUMERICAL MODELING OF LASER-DRIVEN ION ACCELERATION FROM NEAR-CRITICAL GAS TARGETS Dragos Tatomirescu 1,2, Daniel Vizman 1 and Emmanuel d'humières 2 E-mail: emilian.tatomirescu@e-uvt.ro 1 Faculty of Physics,
More informationAn Overview of Laser-Driven Magnetized Liner Inertial Fusion on OMEGA
An Overview of Laser-Driven Magnetized Liner Inertial Fusion on OMEGA 4 compression beams MIFEDS coils B z ~ 1 T Preheat beam from P9 1 mm Ring 3 Rings 4 Ring 3 Target support Fill-tube pressure transducer
More informationLongitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR. C. Dimopoulou
Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR C. Dimopoulou B. Franzke, T. Katayama, D. Möhl, G. Schreiber, M. Steck DESY Seminar, 20 November 2007
More informationNeutron Sources Fall, 2017 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University
Neutron Sources Fall, 2017 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Neutrons: discovery In 1920, Rutherford postulated that there were neutral, massive particles in
More informationA PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU
IWAA2004, CERN, Geneva, 4-7 October 2004 A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU D. P. Sanderson, NSCL-MSU, 1 Cyclotron Lab, East Lansing, MI 48824, USA 1. INTRODUCTION The Rare Isotope Accelerator
More informationWeak focusing I. mv r. Only on the reference orbit is zero
Weak focusing I y x F x mv r 2 evb y Only on the reference orbit is zero r R x R(1 x/ R) B y R By x By B0y x B0y 1 x B0 y x R Weak focusing (II) Field index F x mv R 2 x R 1 n Betatron frequency 2 Fx mx
More informationTHE GSI FUTURE PROJECT: AN INTERNATIONAL ACCELERATOR FACILITY FOR BEAMS OF IONS AND ANTIPROTONS
THE GSI FUTURE PROJECT: AN INTERNATIONAL ACCELERATOR FACILITY FOR BEAMS OF IONS AND ANTIPROTONS Ina Pschorn Gesellschaft für Schwerionenforschung mbh, D-64291 Darmstadt, Germany 1. INTRODUCTION The GSI
More informationHED Physics. 1) By means of laser-driven shock waves (LMJ as driver, PETAL as a backlighter)
HED Physics High-energy lasers allow reaching HED states: 1) By means of laser-driven shock waves (LMJ as driver, PETAL as a backlighter) 2) By using short laser pulses to heat matter using lasergenerated
More informationLaser Induced Shock Pressure Multiplication in Multi Layer Thin Foil Targets
1 Laser Induced Shock Pressure Multiplication in Multi Layer Thin Foil Targets Mayank Shukla 1), Yogesh Kashyap 1), P. S. Sarkar 1), A. Sinha 1), H. C. Pant 2), R.S.Rao 1), N.K.Gupta 1), B.K.Godwal 1)
More informationStatus and Prospect of Laser Fusion Research at ILE Osaka University
Fusion Power Associates 39th Annual Meeting and Symposium Fusion Energy: Strategies and Expectations through the 2020s Status and Prospect of Laser Fusion Research at ILE Osaka University Introduction
More informationHigh-Performance Inertial Confinement Fusion Target Implosions on OMEGA
High-Performance Inertial Confinement Fusion Target Implosions on OMEGA D.D. Meyerhofer 1), R.L. McCrory 1), R. Betti 1), T.R. Boehly 1), D.T. Casey, 2), T.J.B. Collins 1), R.S. Craxton 1), J.A. Delettrez
More information