Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session TO8: Plasma Acceleration: Computation, Beam Driven, Mid-IR lasers
9:30 AM–12:30 PM,
Thursday, November 8, 2018
OCC
Room: C120-122
Chair: Jessica Shaw, Laboratory for Laser Energetics, Rochester, NY
Abstract ID: BAPS.2018.DPP.TO8.8
Abstract: TO8.00008 : FACET Beam Ionization Injection Technique Advantages and Challenges*
10:54 AM–11:06 AM
Presenter:
Ligia Diana Pinto de Almeida Amorim
(State Univ of NY - Stony Brook)
Authors:
Ligia Diana Pinto de Almeida Amorim
(State Univ of NY - Stony Brook)
Navid Vafaei-Najafabadi
(State Univ of NY - Stony Brook)
Kenneth A Marsh
(Univ of California - Los Angeles)
Christopher E Clayton
(Univ of California - Los Angeles)
Weiming An
(Univ of California - Los Angeles)
Frank Shih-Yu Tsung
(Univ of California - Los Angeles)
Warren B Mori
(Univ of California - Los Angeles)
Chandrashekhar Joshi
(Univ of California - Los Angeles)
Wei Lu
(Tsinghua Univ)
Carl A. Lindstrom
(University of Oslo)
Erik Adli
(University of Oslo)
James Allen
(SLAC - Natl Accelerator Lab)
Christine I Clarke
(SLAC - Natl Accelerator Lab)
Sebastien Corde
(Ecole Polytechnique)
Spencer J Gessner
(CERN)
Michael Dennis Litos
(Univ of Colorado - Boulder)
Brendan O'Shea
(SLAC - Natl Accelerator Lab)
Joel T Frederico
(HRL Laboratories, LLC)
Selina Z. Green
(SLAC - Natl Accelerator Lab)
Nate Lipkowitz
(SLAC - Natl Accelerator Lab)
Gerald Yocky
(SLAC - Natl Accelerator Lab)
Mark J Hogan
(SLAC - Natl Accelerator Lab)
Vitaly Yakimenko
(SLAC - Natl Accelerator Lab)
Beam-driven Plasma Wakefield Accelerators (PWFAs) can sustain accelerating gradients that surpass those of standard accelerators. In the PWFA technique called “Beam Induced Ionization Injection” (BIII) a mismatched beam excites the wakefields while performing betatron oscillations. During each betatron cycle, the beam space charge fields exceed the high ionization thresholds of gas impurities and inject their electrons into the wake’s accelerating phase. By correctly positioning the impurity gas, it is possible to produce a single, high-quality accelerated beam. Moreover, if the impurity section encompasses several cycles, a multi-colored beam of electrons with narrow energy spread can be generated. Although BIII can produce low energy spread beams through beam-loading, the required charge ionizes and injects an additional low quality “inception beam”. Here we will discuss different BIII scenarios modeled with Particle in Cell code OSIRIS [R.A.Fonseca et al., LNCS (2331) 342, 2002]. We will show the BIII formation of single accelerated beams, multi-colored beams and the impact of “inception beams” on beam quality.
*We acknowledge resources of the NERSC facility, operated under Contract No. DE-AC02-05CH11231, and of SEAWULF at Stony Brook University.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.TO8.8
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2024 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700