UCLA and USC AARD PROGRAMS C.Joshi, W.Mori, C.Clayton(UCLA), T.Katsouleas, P.Muggli(USC) “Putting the Physics of Beams at the Forefront of Science” 50+

Slides:



Advertisements
Similar presentations
Chengkun Huang UCLA Quasi-static modeling of beam/laser plasma interactions for particle acceleration Zhejiang University 07/14/2009.
Advertisements

Plasma Wakefield Accelerator
Erdem Oz* USC E-164X,E167 Collaboration Plasma Dark Current in Self-Ionized Plasma Wake Field Accelerators
The scaling of LWFA in the ultra-relativistic blowout regime: Generation of Gev to TeV monoenergetic electron beams W.Lu, M.Tzoufras, F.S.Tsung, C. Joshi,
Physics of a 10 GeV laser-plasma accelerator stage Eric Esarey HBEB Workshop, Nov , C. Schroeder, C. Geddes, E. Cormier-Michel,
Beam characteristics UCLA What is a “perfect” beam? It comes from the Injector. It is affected by many factors A few highlights from contributed talks…
A Resonant, THz Slab- Symmetric Dielectric-Based Accelerator R. B. Yoder and J. B. Rosenzweig Neptune Lab, UCLA ICFA Advanced Accelerator Workshop Sardinia,
Plasma wakefields in the quasi- nonlinear regime J.B. Rosenzweig a, G. Andonian a, S. Barber a, M. Ferrario b, P. Muggli c, B. O’Shea a, Y. Sakai a, A.
Historical Review on the Plasma Based Particle Accelerators Congratulation for opening “Plasma and Space Science Center” Yasushi Nishida Lunghwa University.
Particle-Driven Plasma Wakefield Acceleration James Holloway University College London, London, UK PhD Supervisors: Professor Matthew wing University College.
UCLA Experiments with short single e-bunch using preformed and beam ionized plasma Retain ability to run short single bunch with pre-ionized plasma Ken.
Hollow Channel Plasma Wakefield Acceleration Spencer Gessner 5 th SAREC Review September 15 th, 2014.
Modeling narrow trailing beams and ion motion in PWFA Chengkun Huang (UCLA/LANL) and members of FACET collaboration SciDAC COMPASS all hands meeting 2009.
Chengkun Huang | Compass meeting 2008 Chengkun Huang, I. Blumenfeld, C. E. Clayton, F.-J. Decker, M. J. Hogan, R. Ischebeck, R. Iverson, C. Joshi, T. Katsouleas,
Erik Adli CLIC Workshop 2015, CERN, CH 1 Erik Adli Department of Physics, University of Oslo, Norway Input from: Steffen Doebert, Wilfried Farabolini,
Doe FACET Review February 19, 2008 A Plasma Wakefield Accelerator-Based Linear Collider Vision for Plasma Wakefield R&D at FACET and Beyond e-e+Colliding.
New Technologies for Accelerators - Advanced Accelerator Research - Bob Siemann March 19, 2003 Introduction An Incomplete Survey Plasma Waves and The Afterburner.
An overview of the advanced accelerator research at SLAC. Experiments are being conducted with the goal of exploring high gradient acceleration mechanisms.
Lecture 3: Laser Wake Field Acceleration (LWFA)
Full-scale particle simulations of high- energy density science experiments W.B.Mori, W.Lu, M.Tzoufras, B.Winjum, J.Fahlen,F.S.Tsung, C.Huang,J.Tonge M.Zhou,
UCLA Evidence for beam loading by distributed injection of electrons in a Plasma Wakefield Accelerator. Presented by Navid Vafaei-Najafabadi Advisor: Chan.
2 Lasers: Centimeters instead of Kilometers ? If we take a Petawatt laser pulse, I=10 21 W/cm 2 then the electric field is as high as E=10 14 eV/m=100.
Chan Joshi University of California Los Angeles Fermi national Accelerator Lab May The Future of Plasma Wakefield Acceleration.
25-26 June, 2009 CesrTA Workshop CTA09 Electron Cloud Single-Bunch Instability Modeling using CMAD M. Pivi CesrTA CTA09 Workshop June 2009.
FACET and beam-driven e-/e+ collider concepts Chengkun Huang (UCLA/LANL) and members of FACET collaboration SciDAC COMPASS all hands meeting 2009 LA-UR.
W.B.Mori UCLA Orion Center: Computer Simulation. Simulation component of the ORION Center Just as the ORION facility is a resource for the ORION Center,
All-optical accelerators
High Energy Density Physics with Ultra- Relativistic Beams T. Katsouleas University of Southern California Ron Davidson Symposium June 12, 2007 Celebrating.
Particle acceleration by circularly polarized lasers W-M Wang 1,2, Z-M Sheng 1,3, S Kawata 2, Y-T Li 1, L-M Chen 1, J Zhang 1,3 1 Institute of Physics,
Beam dynamics on damping rings and beam-beam interaction Dec 포항 가속기 연구소 김 은 산.
Recent Results on the Plasma Wakefield Acceleration at FACET E 200 Collaboration 1)Beam loading due to distributed injection of charge in the wake reduces.
Beam Plasma Physics Experiments at ORION Mark Hogan SLAC 2 nd ORION Workshop February 18-20, 2003.
Nonlinear Optics in Plasmas. What is relativistic self-guiding? Ponderomotive self-channeling resulting from expulsion of electrons on axis Relativistic.
LASER-PLASMA ACCELERATORS: PRODUCTION OF HIGH-CURRENT ULTRA-SHORT e - -BEAMS, BEAM CONTROL AND RADIATION GENERATION I.Yu. Kostyukov, E.N. Nerush (IAP RAS,
W.Lu, M.Tzoufras, F.S.Tsung, C.Joshi, W.B.Mori
SIMULATIONS FOR THE ELUCIDATION OF ELECTRON BEAM PROPERTIES IN LASER-WAKEFIELD ACCELERATION EXPERIMENTS VIA BETATRON AND SYNCHROTRON-LIKE RADIATION P.
Beam Driven Plasma-Wakefield Linear Collider: PWFA-LC J.P Delahaye / SLAC On behalf of J.P. E. Adli, S.J. Gessner, M.J. Hogan, T.O. Raubenheimer (SLAC),
Consideration for a plasma stage in a PWFA linear collider Erik Adli University of Oslo, Norway FACET-II Science Workshop, SLAC Oct 14,
Max Cornacchia, SLAC LCLS Project Overview BESAC, Feb , 2001 LCLS Project Overview What is the LCLS ? Transition from 3 rd generation light sources.
E-cloud studies at LNF T. Demma INFN-LNF. Plan of talk Introduction New feedback system to suppress horizontal coupled-bunch instability. Preliminary.
UCLA Positron Production Experiments at SABER Presented by Devon Johnson 3/15/06.
SABER, “maybe” a new facility in the South Arc (South Arc Beam Experimental Region) End Station A (ESA) in 2007 ILC Test Beams in 2008 Test Beams beyond.
1 1 Office of Science C. Schroeder, E. Esarey, C. Benedetti, C. Geddes, W. Leemans Lawrence Berkeley National Laboratory FACET-II Science Opportunities.
GWENAEL FUBIANI L’OASIS GROUP, LBNL 6D Space charge estimates for dense electron bunches in vacuum W.P. LEEMANS, E. ESAREY, B.A. SHADWICK, J. QIANG, G.
Beam-Plasma Working Group Summary Barnes, Bruhwiler, DavidTech-X Clayton,
Erik Adli CLIC Project Meeting, CERN, CH 1 Erik Adli Department of Physics, University of Oslo, Norway Input from: Steffen Doebert, Wilfried Farabolini,
Non Double-Layer Regime: a new laser driven ion acceleration mechanism toward TeV 1.
Tuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory Chris Melton SLAC Accelerator Operations.
Prospects for generating high brightness and low energy spread electron beams through self-injection schemes Xinlu Xu*, Fei Li, Peicheng Yu, Wei Lu, Warren.
Ultra-short electron bunches by Velocity Bunching as required for Plasma Wave Acceleration Alberto Bacci (Sparc Group, infn Milano) EAAC2013, 3-7 June,
Beam quality preservation and power considerations Sergei Nagaitsev Fermilab/UChicago 14 October 2015.
Ionization Injection E. Öz Max Planck Institute Für Physik.
V.N. Litvinenko (SBU) C. Joshi, W. Mori (UCLA)
of High-Energy, High-Density Electron and Positron Beams
Proton-driven plasma wakefield acceleration in hollow plasma
Electron acceleration behind self-modulating proton beam in plasma with a density gradient Alexey Petrenko.
The 2nd European Advanced Accelerator Concepts Workshop
Stefano Romeo on behalf of SPARC_LAB collaboration
Electron cloud and collective effects in the FCC-ee Interaction Region
Test of Notch Collimator - December 2005
Proton driven plasma accelertion
Wakefield Accelerator
E-164 E-162 Collaboration: and E-164+X:
Proton Driven Plasma Wakefield Acceleration
Key Physics Topics for Plasma Wakefield Accelerator Research
Requests of Future HEP e+/e-Facilities
M. Pivi PAC09 Vancouver, Canada 4-8 May 2009
Explanation of the Basic Principles and Goals
2. Crosschecking computer codes for AWAKE
Optimization of JLEIC Integrated Luminosity Without On-Energy Cooling*
Presentation transcript:

UCLA and USC AARD PROGRAMS C.Joshi, W.Mori, C.Clayton(UCLA), T.Katsouleas, P.Muggli(USC) “Putting the Physics of Beams at the Forefront of Science” 50+ PRL 5 Nature 1Science 2Physics Today 25 PhDs

� Double the energy of Collider w/ short plasma sections before IP � 1 st half of beam excites wake --decelerates to 0 � 2 nd half of beams rides wake--accelerates to 2 x E o � Make up for Luminosity decrease  N 2 /  z 2 by halving  in a final plasma lens 50 GeV e - 50 GeV e + e - WFA e + WFA IP LENSES 5m PLASMA AFTERBURNER S. Lee et al., PRST-AB (2001) GRAND CHALLENGE in AARD OO

Betatron Radiation Positron Source Collimators e - Extraction e-e- z x Plasma 40 m 10 cm Bending Magnet hνhν Target 8mm  One meter long plasma of density 1e17 could produce 20 positrons/e The energy spectrum is in the 5-30 MeV range. Possibility of generating polarized positrons? D.Johnson et.al.To be submitted to PRL

Electron Cloud Formation Cloud build-up due to acceleration in beam potential and secondary emission Clouds form in positron rings via synchrotron radiation Clouds form in proton rings via halo or residual gas ionization Predicted Electron cloud density is cm -3 A head-tail type instability results in beam blow up

 Advanced Computational Modeling Program All AARD Schemes will eventually need access to a 10 GeV class electron/positron beam line.  Beam Research Facilities : SABER  Strong University-Based Research Program AARD Needs

OUR VISION  To address critical issues for realizing the promise of a plasma-based accelerator at the energy frontier in the next decade.  To Design a Hi-fidelity virtual accelerator at full scale and end-to-end.  To address critical issues for realizing the promise of a plasma-based accelerator at the energy frontier in the next decade.  To Design a Hi-fidelity virtual accelerator at full scale and end-to-end.

PLASMA WAKEFIELD ACCELERATOR Blowout regime flattens wake, reduces energy spread Unloaded wake E157,162,164(X), 167 EzEz Beam load Loaded wake N load ~30% N max 1% energy spread

MASSIVELY PARALLEL COMPUTATIONS IN AID OF PLASMA ACCELERATION RESEARCH afterburner hosing E164X OSIRIS: (Full PIC) Moving window, parallel Dynamic load balancing Field and Impact Ionization Successfully applied to full 3D modeling of LWFA and PWFA experiments QuickPIC: Highly efficient quasi-static model for beam- driven plasma accelerators Fully parallel with dynamic load balancing Ponderomotive guiding center + envelope models for laser driven ADK model for field ionization At least100x faster than full PIC.

Accelerating field 24GeV/m at the load 500 GeV Energy Gain in 20 meters! N=3x10 10 electrons N=1x10 10 electrons

E164X August Run 12GeV Energy Gain in less than 30cm !

Latest Results from E164X  First attempt at crafting two distinct bunches First bunch drives the wake while the second gains energy.  Positrons created from betatron X-rays and positron spectra measured.  Multi GeV trapped particles observed whenever the gradient exceeded 40 GeV/m.

Clear threshold Self Trapping of Plasma Electrons Trapping above a threshold accelerating field of 40 GeV/m Dark current ~ beam current (loads the wake) Trapping above a threshold accelerating field of 40 GeV/m Dark current ~ beam current (loads the wake) Trapped particle energy scales with plasma length: 30cm

What’s Next?:E167 Energy Doubling of the SLAC 28.5 GeV Beam in 60 cm Possible Plasma Length(cm) Energy Gain (GeV) If successful E167 will try doubling the 50 GeV Beam 3D OSIRIS SIMULATIONS

RAL LBL Osaka UCLA E164X ILC Current Energy Frontier ANL Plasma Accelerator Progress “Accelerator Moore’s Law” E167 O E167 O

CRITICAL R&D PATH TO PLASMA AFTERBURNER High Gradient Electron and Positron Acceleration Transverse Beam Quality (emittance preservation) –jitter and pointing,head erosion –hose instability,ion motion,scattering “Crafting” Two Bunches Nanometer Focusing,Asymmetric Beams All these issues can be addressed with SABER One-to-One PIC Simulations Capability of a Virtual One-to-One PIC Simulations Capability of a Virtual Plasma Afterburner Plasma Afterburner

Short e + pulses from SABER will give gradients of 5 GeV/m 5.7GeV in 39cm N=1.5e10 Spot Size=10 micron Bunch length=100fs Simulations:M.Zhou UCLA

Plasma Focusing to Nanometer Spot Sizes FFTB experiments have shown focusing Strengths of giga- Gauss/cm Can we focus e +,e - SABER beams to submicron dimension using plasma lenses? Can we design layered structures as lenses for obtaining nanometer spot sizes? M.Hogan et.al. PRL 03 J.Ng et al. PRL E162: Positron Focusing

PH.D STUDENTS TRAINED IN PAST FIVE YEARS Brian Duda, 2000 Mori Shuoqin Wang, 2002 Joshi Brent Blue, 2003 Joshi Catalin Filip, 2003 Joshi Ritesh Narang, 2003 Joshi Chengkun Huang, 2005Mori Advisor: Over 25 Ph.Ds granted since group ’ s inception. Faculty placed at USC, UCLA, U. Michigan/Nebraska, Florida A&M, CalState, U. Osaka 5 Student Awards including two Best Ph.D. Thesis Awards Suzhi Deng Ali Ghalam Jerry Hoffman Seung Lee Peter Lai Chiou

Statistical Data $1 million/yr average since 1987 SciDAC ~ $170 K /year Theory and Simulations NSF ~ $150 K/year UCLA, present SLAC, present SLAC, as soon as it is built 3.Users at Neptune: Joshi, Rosenzweig, Pellegrini, Muggli, Katsouleas Annual Funding: DoE HEP$490k NSF (ORION)$50k DoESciDAC$40k

CONCLUSIONS Acknowledgements:E157,162,164,164Xand167 collaborators DOE HEP,NSF,SCIDAC,USC,UCLA Exciting time for AARD DOE’s investment in AARD is beginning to pay off. The AARD community is putting the Physics of Beams at the forefront of Physics and science. Continuing access to a high energy electron and positron beams is a must for the health of the field. (Need SABER at SLAC) Plasmas are leading to well behaved optical elements of incredible power for incorporation into future HEP machines. table-top GeV class accelerators for applications other than HEP.

Conclusions AARD program is doing an excellent job in training students. Retention would be significantly improved if the National Labs were more aggressive in assisting with Permanant Residence ( Green Card)in the US. Industry is very successful with this strategy.