'Beam radius' presentation slideshows

Alex Friedman, LLNL & LBNL OFES Remote Theory Seminar July 13, 2004

Simulation of space-charge-dominated ion beams plays a major role in developing the answers. Key question in Heavy Ion Fusion beam science: How do intense ion beams behave as they are accelerated and compressed into a small volume in space and time?. Alex Friedman, LLNL & LBNL

648 views • 59 slides

Igor D. Kaganovich, Edward A. Startsev Ronald C. Davidson Plasma Physics Laboratory

Analytical and Numerical Studies of Ion Beam Plasma Interaction for Heavy Ion Driven Inertial Fusion. Igor D. Kaganovich, Edward A. Startsev Ronald C. Davidson Plasma Physics Laboratory Princeton University. Talk Outline. Basics Why do Heavy Ion Fusion? What do we have to do?

601 views • 53 slides

R.6.2 Lasery Optoelektronika 2014

R.6.2 Lasery Optoelektronika 2014. Dr hab. in?. B. B. Kosmowski. 1. Active material : Ions in crystals (eg. Fe 2+ , Dy 2+ , Cr 3+ , Ti 3+ , Nd 3+ , Pr 3+ , Dy 3+ , Ho 3+ , Er 3+ , Tm 3+ , Yb 3+ ), Atoms ( e.g . Cu, Ne, I), Ions ( e.g . Cd + , Ar + ),

486 views • 38 slides

Robust Heavy Ion Fusion Target

Robust Heavy Ion Fusion Target. Shigeo KAWATA Utsunomiya Univ. Japan U.S.-J. Workshop on HIF December 18-19, 2008 at LBNL & LLNL. Acknowledgments Thanks for Collaborations with Grant, John & Friends in VNL for WDM/HEDM physics + HIF with wobblers! Colleagues in HIF Japan, Sasho, Jacob

450 views • 33 slides

Steigerwald results reported in SPIN 2000 JLab measurements in June 2012

Steigerwald results reported in SPIN 2000 JLab measurements in June 2012 after 12 years good agreement Results depend on (energy=same, targets=same, TOF cut=same) Do we agree at a precision level? similar at few percent, but what about <1% ??? => motivates experiment.

370 views • 29 slides

Pukhov, Meyer-ter-Vehn, PRL 76, 3975 (1996)

plasma box ( n e /n c =0.6). Laser pulse 10 19 W/cm 2. B ~ mc w p /e ~ 10 8 Gauss. Relativistic electron beam j ~ en c c ~ 10 12 A/cm 2 10 kA of 1-20 MeV electrons. Lecture 2: Basic plasma equations , self-focusing, direct laser acceleration.

472 views • 29 slides

X. Ding, UCLA AAG June 27, 2012

Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update). X. Ding, UCLA AAG June 27, 2012. Focused Incident Proton Beam at 8 GeV (Beam radius is fixed at 0.12 cm at z=-37.5 cm).

398 views • 28 slides

X. Ding, UCLA AAG June 27, 2012

Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update). X. Ding, UCLA AAG June 27, 2012. Focused Incident Proton Beam at 8 GeV (Beam radius is fixed at 0.12 cm at z=-37.5 cm).

402 views • 28 slides

X. Ding, UCLA Target Studies June 20, 2012

Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance. X. Ding, UCLA Target Studies June 20, 2012. Focused Incident Proton Beam at 8 GeV. Relative normalized meson production is 0.84 of max at ?* of 0.3 m for ? x = ? y = 5 ?m.

225 views • 22 slides

Transverse Coherent Transition Radiation (TCTR) Experiment First Ideas for a Measurement Setup

Transverse Coherent Transition Radiation (TCTR) Experiment First Ideas for a Measurement Setup. Max-Planck-Institute for Physics Munich Olaf Reimann , Scott Mandry Geneva, October 19, 2012. Outline. Short introduction Why TCTR in frequency domain? Principle of the measurement First results

353 views • 20 slides

Luminosity variations with pellet targets

Luminosity variations with pellet targets. Anatoly Sidorin, Alexander Smirnov , Dmitry Krestnikov Joint Institute for Nuclear Research (JINR) Dubna, Russia http://lepta.jinr.ru/betacool. BETACOOL application over the world (since 1995). TSL, Uppsala MSL, Stockholm. JINR, Dubna

305 views • 19 slides

X. Ding, UCLA AAG Meeting

256 views • 17 slides

Setting of Focused Beam in MARS for Meson Production Optimization

271 views • 11 slides

X. Ding, UCLA Target Studies Sept 20, 2012

Optimized Target Parameters and Meson Production by IDS120h with Focused Gaussian Beam and Fixed Emittance (Update). X. Ding, UCLA Target Studies Sept 20, 2012. Focused Incident Proton Beam at 8 GeV (Beam radius is fixed at 0.12 cm at z=-37.5 cm).

113 views • 11 slides

Particle Production with Carbon Target and IDS120j Configuration at 3 GeV

113 views • 10 slides

Particle Production with Carbon Target and IDS120j Configuration at 3 GeV

105 views • 10 slides

Polarized Electrons Using the PWT RF Gun

202 views • 9 slides

Beam sizes and mirror curvatures for Advanced Virgo

Beam sizes and mirror curvatures for Advanced Virgo. Stefan Hild and Andreas Freise University of Birmingham Advanced Virgo telecon, June 2008. Introduction. Advanced Virgo conceptual shows an inconsisten-cy regarding the beam size: The optics section uses 3.5cm radius

99 views • 9 slides

LS-DYNA

Target: repetition rate = 50 Hz; beam energy = 6 GeV; beam radius = target radius; beam offset = 0.5*target radius; 3 x 2 ns long bunches; pulse length = 20 ? s (2cm x 17cm), 25 ? s (3cm x 20cm); energy deposition = MARS. Wire: 0.5 mm diameter, 3 cm long;

264 views • 4 slides

LS-DYNA

Power = 4 MW, repetition rate = 50 Hz, Beam energy = 6 GeV ( parabolic distribution ) 2 ns long bunches. 3 cm x 20 cm Beam radius = Rod radius. 3 bunches. 5 bunches. Peak Von Mises Stress [ MPa ]. Pulse length [ ? s]. Results. TUNGSTEN target operating at 2000 K.

174 views • 4 slides