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Simulation of the Wisconsin-Argonne Plasma Wakefield Experiment
The plasma wakefield accelerator (PWFA) is an advanced accelerator concept that uses the large electric fields that can be generated in a plasma to accelerate charged particles. We present the results of a self-consistent two-dimensional simulation of the first experiment designed to test this conce...
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Published in: | IEEE transactions on plasma science 1987-04, Vol.15 (2), p.199-202, Article 199 |
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container_end_page | 202 |
container_issue | 2 |
container_start_page | 199 |
container_title | IEEE transactions on plasma science |
container_volume | 15 |
creator | Keinigs, Rhon Jones, Michael E. Su, J. J. |
description | The plasma wakefield accelerator (PWFA) is an advanced accelerator concept that uses the large electric fields that can be generated in a plasma to accelerate charged particles. We present the results of a self-consistent two-dimensional simulation of the first experiment designed to test this concept. Linear theory predicts for this experiment an accelerating gradient of approximately 95 MV/m. However, the simulations indicate that a much larger accelerating field is achieved in the plasma. This enhancement is due to strong beam pinching, which is not treated self-consistently by a linear theory. Wave steepening due to a nonlinear modulation of the background plasma is also observed. This steepening results in a phase shift that degrades the acceleration. |
doi_str_mv | 10.1109/TPS.1987.4316685 |
format | article |
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J.</creator><creatorcontrib>Keinigs, Rhon ; Jones, Michael E. ; Su, J. J.</creatorcontrib><description>The plasma wakefield accelerator (PWFA) is an advanced accelerator concept that uses the large electric fields that can be generated in a plasma to accelerate charged particles. We present the results of a self-consistent two-dimensional simulation of the first experiment designed to test this concept. Linear theory predicts for this experiment an accelerating gradient of approximately 95 MV/m. However, the simulations indicate that a much larger accelerating field is achieved in the plasma. This enhancement is due to strong beam pinching, which is not treated self-consistently by a linear theory. Wave steepening due to a nonlinear modulation of the background plasma is also observed. 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This steepening results in a phase shift that degrades the acceleration.</description><subject>Acceleration</subject><subject>Electron beams</subject><subject>Exact sciences and technology</subject><subject>Particle accelerators</subject><subject>Particle beams</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma accelerators</subject><subject>Plasma density</subject><subject>Plasma interactions (nonlaser)</subject><subject>Plasma measurements</subject><subject>Plasma simulation</subject><subject>Plasma waves</subject><issn>0093-3813</issn><issn>1939-9375</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1987</creationdate><recordtype>article</recordtype><recordid>eNp9kM1LwzAYxoMoOKd3wUsP4q0zaT6anGSM-QEDB5vsGNL0rUbTdDYd6H9v56YHD57ew_s8Px5-CJ0TPCIEq-vlfDEiSuYjRokQkh-gAVFUpYrm_BANMFY0pZLQY3QS4yvGhHGcDdDNwtUbbzrXhKSpku4FkpWLtgnRhXTcPjchQDL3JtYmWZk3qBz4Mpl-rKF1NYTuFB1Vxkc4298herqdLif36ezx7mEynqWWMtmlUBSMS45ziZksc6FIYYViVAnCjSozwCoHXpWlLYpCWmJobpkwIGkpuKWUDtHVjrtum_cNxE7X_Uzw3gRoNlFnTEisMtwH8S5o2ybGFiq97pea9lMTrLemdG9Kb03pvam-crlnm2iNr1oTrIu_PZkpIrHoY-IP2bru21zXGuf_41_sig4AfrE_3y_QyoK4</recordid><startdate>19870401</startdate><enddate>19870401</enddate><creator>Keinigs, Rhon</creator><creator>Jones, Michael E.</creator><creator>Su, J. 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J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c348t-ebb4585078048d7691bc69439615a9d2e097e5fddcbbb8c1a37c46ae83d65c333</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1987</creationdate><topic>Acceleration</topic><topic>Electron beams</topic><topic>Exact sciences and technology</topic><topic>Particle accelerators</topic><topic>Particle beams</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>Plasma accelerators</topic><topic>Plasma density</topic><topic>Plasma interactions (nonlaser)</topic><topic>Plasma measurements</topic><topic>Plasma simulation</topic><topic>Plasma waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Keinigs, Rhon</creatorcontrib><creatorcontrib>Jones, Michael E.</creatorcontrib><creatorcontrib>Su, J. 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J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Simulation of the Wisconsin-Argonne Plasma Wakefield Experiment</atitle><jtitle>IEEE transactions on plasma science</jtitle><stitle>TPS</stitle><date>1987-04-01</date><risdate>1987</risdate><volume>15</volume><issue>2</issue><spage>199</spage><epage>202</epage><pages>199-202</pages><artnum>199</artnum><issn>0093-3813</issn><eissn>1939-9375</eissn><coden>ITPSBD</coden><abstract>The plasma wakefield accelerator (PWFA) is an advanced accelerator concept that uses the large electric fields that can be generated in a plasma to accelerate charged particles. We present the results of a self-consistent two-dimensional simulation of the first experiment designed to test this concept. Linear theory predicts for this experiment an accelerating gradient of approximately 95 MV/m. However, the simulations indicate that a much larger accelerating field is achieved in the plasma. 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language | eng |
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source | IEEE Electronic Library (IEL) Journals |
subjects | Acceleration Electron beams Exact sciences and technology Particle accelerators Particle beams Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma accelerators Plasma density Plasma interactions (nonlaser) Plasma measurements Plasma simulation Plasma waves |
title | Simulation of the Wisconsin-Argonne Plasma Wakefield Experiment |
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