Slide 1 The Heavy Ion Fusion Science Virtual National Laboratory Why heavy ions? Target requires: 3.5 – 6 MJ in ~ 10 ns  500 TW Range ~ 0.02 – 0.20 g/cm.

Slides:



Advertisements
Similar presentations
TU Darmstadt Inertial Confinement Fusion Dieter H.H. Hoffmann TU / GSI Darmstadt 300. WE-Heraeus Seminar ENERGIEFORSCHUNG Mai 2003.
Advertisements

Plasma Window Options and Opportunities for Inertial Fusion Applications Leslie Bromberg Ady Herskovitch* MIT Plasma Science and Fusion Center ARIES meeting.
Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation,
Proton / Muon Bunch Numbers, Repetition Rate, RF and Kicker Systems and Inductive Wall Fields for the Rings of a Neutrino Factory G H Rees, RAL.
Particle-Driven Plasma Wakefield Acceleration James Holloway University College London, London, UK PhD Supervisors: Professor Matthew wing University College.
CESR as Light Source David L. Rubin for the CESR Operations Group Cornell University Laboratory for Elementary-Particle Physics.
Ion Accelerator Complex for MEIC January 28, 2010.
Systems Analysis for Modular versus Multi-beam HIF Drivers * Wayne Meier – LLNL Grant Logan – LBNL 15th International Symposium on Heavy Ion Inertial Fusion.
Wayne R. Meier Lawrence Livermore National Lab Heavy Ion Fusion Modeling Update - Spot Size Model Changes* ARIES Meeting April 22-23, 2002 * This work.
Plasma Window Performance Leslie Bromberg Katie Maurer Ady Herskovitch* MIT Plasma Science and Fusion Center ARIES meeting Madison, WI April 23, 2002 *Brookhaven.
Harold G. Kirk Brookhaven National Laboratory Meson Production Efficiencies IDS Target Meeting CERN December 17, 2008.
Wayne R. Meier Lawrence Livermore National Lab Heavy Ion Fusion Modeling Update* ARIES e-Meeting October 17, 2001 * This work was performed under the auspices.
Design Considerations for Beam Port Insulator Rings
The Heavy Ion Fusion Virtual National Laboratory UC Berkeley Christophe S. Debonnel 1,2 (1) Thermal Hydraulics Laboratory Department of Nuclear Engineering.
The Heavy Ion Fusion Virtual National Laboratory UC Berkeley C.S. Debonnel 1,2, S.S. Yu 2, P.F. Peterson 1 (1) Thermal Hydraulics Laboratory Department.
An Update Point Design for Heavy Ion Fusion Wayne Meier LLNL ARIES Meeting Jan. 8-9, 2003 UC San Diego Work performed under the auspices of the U.S. Department.
Simulations of Neutralized Drift Compression D. R. Welch, D. V. Rose Mission Research Corporation Albuquerque, NM S. S. Yu Lawrence Berkeley National.
The Heavy Ion Fusion Virtual National Laboratory Comparison of final focus magnetic systems for the Assisted Pinched Transport and the RPD-2002 J. Barnard,
The Heavy Ion Fusion Virtual National Laboratory ARIES-IFE Meeting Atlanta, Georgia September 4, 2003 “Modular Solenoid with Assisted Pinch” by S. Yu,
Modeling of Assisted and Self- Pinch Transport D. V. Rose and D. R. Welch Mission Research Corporation C. L. Olson Sandia National Laboratories S. S. Yu.
Coupling of APT Transported Ion beam to Hybrid Target D. R. Welch and D. V. Rose Mission Research Corporation C. L. Olson Sandia National Laboratories.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
Wayne R. Meier Lawrence Livermore National Lab Per Peterson UC Berkeley Updated Heavy Ion Driver Parameters for Snowmass Point Design ARIES Meeting July.
Wayne R. Meier Lawrence Livermore National Lab Heavy Ion Driver Model Update* ARIES IFE Meeting LLNL March 8-9, 2001 * This work was performed under the.
Status of Operational Windows for HIF Chamber Transport Modes D. V. Rose, D. R. Welch, C. L. Olson, S. Neff, and S. S. Yu ARIES Project Meeting January.
The Heavy Ion Fusion Virtual National Laboratory UC Berkeley Christophe S. Debonnel 1,2 (1) Thermal Hydraulics Laboratory Department of Nuclear Engineering.
Research Co-ordination Meeting on Elements of Power Plant Design for Inertial Fusion Energy 4-7 November 2003 DESIGN CONCEPT OF FAST-IGNITION HEAVY ION.
Laser accelerated ions and their potential for therapy accelerators I. Hofmann, GSI Accelerator Department HIAT09, Venezia, June 8-12, Introduction.
(ISS) Topics Studied at RAL G H Rees, RAL, UK. ISS Work Areas 1. Bunch train patterns for the acceleration and storage of μ ± beams. 2. A 50Hz, 1.2 MW,
Carbon Injector for FFAG
March 2011Particle and Nuclear Physics,1 Experimental tools accelerators particle interactions with matter detectors.
The Heavy Ion Fusion Virtual National Laboratory Analytical and Numerical Studies of Ion Beam Plasma Interaction for Heavy Ion Driven Inertial Fusion Igor.
The Heavy Ion Fusion Virtual National Laboratory UC Berkeley Christophe S. Debonnel Thermal Hydraulics Laboratory Department of Nuclear Engineering University.
Linac e+ source for ILC, CLIC, SuperB, … Vitaly Yakimenko, Igor Pogorelsky November 17, 2008 BNL.
Compton/Linac based Polarized Positrons Source V. Yakimenko BNL IWLC2010, Geneva, October 18-22, 2010.
Compton based Polarized Positrons Source for ILC V. Yakimenko Brookhaven National Laboratory September 12, 2006 RuPAC 2006, Novosibirsk.
Alex Friedman Fusion Energy Sciences Program, LLNL (for the NDCX-II team) ARPA-E Visit to LBNL, September 4, 2013 * This work was performed under the auspices.
The Heavy Ion Fusion Virtual National Laboratory Pulsed Normal Quadrupoles for a Heavy Ion Fusion Driver Final Focus Section D. Shuman, S. S. Yu, LBNL.
Robust Heavy Ion Fusion Target Shigeo KAWATA Utsunomiya Univ. Japan U.S.-J. Workshop on HIF December 18-19, 2008 at LBNL & LLNL.
January 5, 2004S. A. Pande - CAT-KEK School on SNS MeV Injector Linac for Indian Spallation Neutron Source S. A. PANDE.
Heavy Ion Fusion Sciences Virtual National Laboratory Warp simulations illustrate the novel acceleration strategy Design Studies for NDCX-II W. M. Sharp,
Aerosol Limits for Target Tracking Ronald Petzoldt ARIES IFE Meeting, Madison, WI April 22-23, 2002.
20 April 2009 AAP Review Global Design Effort 1 The Positron Source Jim Clarke STFC Daresbury Laboratory.
Alexander Aleksandrov Oak Ridge National Laboratory
Electron Model for a 3-10 GeV, NFFAG Proton Driver G H Rees, RAL.
Welcome to the eighth HAPL meeting Courtesy, Mark Tillack, UCSD.
PROTON LINAC FOR INDIAN SNS Vinod Bharadwaj, SLAC (reporting for the Indian SNS Design Team)
Progress at BNL Vitaly Yakimenko. Polarized Positrons Source (PPS for ILC) Conventional Non- Polarized Positrons: In our proposal polarized  -ray beam.
1. Fast ignition by hydrodynamic flow
The Heavy Ion Fusion Virtual National Laboratory Neutralized Transport Experiment (NTX) P. K. Roy, S. S. Yu, S. Eylon, E. Henestroza, A. Anders, F. M.
The Heavy Ion Fusion Science Virtual National Laboratory 1 PRoy LINAC06 Neutralized Drift Compression and Related Experiments* P. K. Roy 1, W. L. Waldron.
What I’ve been doing. My Problem: Conceptually LHeC: linear electron collider Basic Design: linac will be connected to a recirculation track (why?) Goal:
The Heavy Ion Fusion Science Virtual National Laboratory Question 1: Assess and document target preheat effects from beams and plasma for the various options.
Target Highlights Scaling (gain curves) and progress on “hybrid “ targets Fast ignition scaling and physics Improved models of fluid instabilities New.
Capture and Transport Simulations of Positrons in a Compton Scheme Positron Source A. VIVOLI*, A. VARIOLA (LAL / IN2P3-CNRS), R. CHEHAB (IPNL & LAL / IN2P3-CNRS)
Future Circular Collider Study Kickoff Meeting CERN ERL TEST FACILITY STAGES AND OPTICS 12–15 February 2014, University of Geneva Alessandra Valloni.
Oct 6, 2009 The Heavy Ion Fusion Science Virtual National Laboratory 1 NDCX-II Project Joe Kwan Project Manager Sept. 7, 2009 San Francisco US-Japan Workshop.
Proton Driver Keith Gollwitzer Accelerator Division Fermilab MAP Collaboration Meeting June 20, 2013.
A. FaccoEURISOL DS Orsay, 3 Feb 2005 Task 7 Proton Accelerator “The objective of the Proton Accelerator Task is the design a 5 mA CW, 1 GeV proton linac.
Project X as a Muon Facility Platform Keith Gollwitzer Fermilab Accelerator Advisory Committee November 7-9, 2011.
UK Neutrino Factory Conceptual Design
V. Bagnoud PHELIX, Plasma Physics department GSI Darmstadt
Vacuum chamber for experiment HIHEX at FAIR
Injection facility for Novosibirsk Super Charm Tau Factory
Meson Production Efficiencies
Heavy Ion Fusion Modeling Update*
Capture and Transmission of polarized positrons from a Compton Scheme
Status of the JLEIC Injector Linac Design
Multi-Ion Injector Linac Design – Progress Summary
Choice of harmonic number with the consideration of ion beam formation
Presentation transcript:

Slide 1 The Heavy Ion Fusion Science Virtual National Laboratory Why heavy ions? Target requires: 3.5 – 6 MJ in ~ 10 ns  500 TW Range ~ 0.02 – 0.20 g/cm 2 Range requirement Power requirement Higher mass  Higher kinetic energy Current ~ 1/Kinetic energy Higher mass requires lower current (easier to focus)

Slide 2 The Heavy Ion Fusion Science Virtual National Laboratory Heavier ions  higher kinetic energy Energy (GeV) Range (g/cm 2 ) Targets require high power (kinetic energy x current) Light ion fusion requires high current, unconventional accelerators (Sandia, 1970's) Heavy Ion Fusion requires lower currents enabling the use of more conventional accelerators (Mashke, ~ 1974)

Slide 3 The Heavy Ion Fusion Science Virtual National Laboratory There are two principle methods of acceleration

Slide 4 The Heavy Ion Fusion Science Virtual National Laboratory A multiple beam induction linac driver

Slide 5 The Heavy Ion Fusion Science Virtual National Laboratory A Robust Point Design study established a baseline for a multiple-beam quadrupole induction linac HIF driver Multiple Ion Source/ Injectors Multiple-beam acceleration Drift compression Bending Final focusing Chamber transport Target Input 7 MJ Yield 400 MJ 1.6 MeV 0.63 A/beam 30  s 120 beams 4 GeV Bi A/beam 200 ns 4 GeV 1.9 kA/beam 9.3 ns Relative beam bunch length at end of: injection acceleration drift compression Common Induction cores 3 km 400 m

Integration of target,chamber, and accelerator requirements led to the self-consistent point design Ion: Bi + (A=209) Main pulse: 4 GeV Foot pulse: 3.3 GeV 120 beams total (72 main, 48 foot) Pulse energy: 7 MJ Final spot radius: 2.2 mm 3 D neutronics calculations Chamber dynamics Mechanical engineering Final beam optics + target physics + chamber propagation Length: 2.7 km; Efficiency 28% Total cost: 2.8 B$

Slide 7 The Heavy Ion Fusion Science Virtual National Laboratory The arrays of flowing FLiNaBe liquid salt jets provide windows through which the beams pass

Slide 8 The Heavy Ion Fusion Science Virtual National Laboratory