C Zhang, D Storey, P San Miguel Claveria, Z Nie, K A Marsh, M Hogan, W B Mori, E Adli, W An, R Ariniello, G J Cao, C Clarke, S Corde, T Dalichaouch, C E Doss, C Emma, H Ekerfelt, E Gerstmayr, S Gessner, C Hansel, A Knetsch, V Lee, F Li, M Litos, B O’Shea, G White, G Yocky, V Zakharova, C Joshi
{"title":"Generation of meter-scale hydrogen plasmas and efficient, pump-depletion-limited wakefield excitation using 10 GeV electron bunches","authors":"C Zhang, D Storey, P San Miguel Claveria, Z Nie, K A Marsh, M Hogan, W B Mori, E Adli, W An, R Ariniello, G J Cao, C Clarke, S Corde, T Dalichaouch, C E Doss, C Emma, H Ekerfelt, E Gerstmayr, S Gessner, C Hansel, A Knetsch, V Lee, F Li, M Litos, B O’Shea, G White, G Yocky, V Zakharova, C Joshi","doi":"10.1088/1361-6587/ad1ae4","DOIUrl":null,"url":null,"abstract":"High repetition rates and efficient energy transfer to the accelerating beam are important for a future linear collider based on the beam-driven plasma wakefield acceleration scheme (PWFA-LC). This paper reports the first results from the Plasma Wakefield Acceleration Collaboration (E300) that are beginning to address both of these issues using the recently commissioned FACET-II facility at SLAC national accelerator laboratory. We have generated meter-scale hydrogen plasmas using time-structured 10 GeV electron bunches from FACET-II, which hold the promise of dramatically increasing the repetition rate of PWFA by rapidly replenishing the gas between each shot compared to the hitherto used lithium plasmas that operate at 1–10 Hz. Furthermore, we have excited wakes in such plasmas that are suitable for high gradient particle acceleration with high drive-bunch to wake energy transfer efficiency- a first step in achieving a high overall energy transfer efficiency. We have done this by using time-structured electron drive bunches that typically have one or more ultra-high current (<inline-formula>\n<tex-math><?CDATA $\\gt$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mo>></mml:mo></mml:math>\n<inline-graphic xlink:href=\"ppcfad1ae4ieqn1.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>30 kA) femtosecond spike(s) superimposed on a longer (∼0.4 ps) lower current (<inline-formula>\n<tex-math><?CDATA $\\lt$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mo><</mml:mo></mml:math>\n<inline-graphic xlink:href=\"ppcfad1ae4ieqn2.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>10 kA) bunch structure. The first spike effectively field-ionizes the gas and produces a meter-scale (30–160 cm) plasma, whereas the subsequent beam charge creates a wake. The length and amplitude of the wake depends on the longitudinal current profile of the bunch and plasma density. We find that the onset of pump depletion, when some of the drive beam electrons are nearly fully depleted of their energy, occurs for hydrogen pressure <inline-formula>\n<tex-math><?CDATA $\\unicode{x2A7E}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:mtext>⩾</mml:mtext></mml:math>\n<inline-graphic xlink:href=\"ppcfad1ae4ieqn3.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>1.5 Torr. We also show that some electrons in the rear of the bunch can gain several GeV energies from the wake. These results are reproduced by particle-in-cell simulations using the QPAD code. At a pressure of ∼2 Torr, simulation results and experimental data show that the beam transfers about 60% of its energy to the wake.","PeriodicalId":20239,"journal":{"name":"Plasma Physics and Controlled Fusion","volume":"251 1","pages":""},"PeriodicalIF":2.1000,"publicationDate":"2024-01-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Physics and Controlled Fusion","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-6587/ad1ae4","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0
Abstract
High repetition rates and efficient energy transfer to the accelerating beam are important for a future linear collider based on the beam-driven plasma wakefield acceleration scheme (PWFA-LC). This paper reports the first results from the Plasma Wakefield Acceleration Collaboration (E300) that are beginning to address both of these issues using the recently commissioned FACET-II facility at SLAC national accelerator laboratory. We have generated meter-scale hydrogen plasmas using time-structured 10 GeV electron bunches from FACET-II, which hold the promise of dramatically increasing the repetition rate of PWFA by rapidly replenishing the gas between each shot compared to the hitherto used lithium plasmas that operate at 1–10 Hz. Furthermore, we have excited wakes in such plasmas that are suitable for high gradient particle acceleration with high drive-bunch to wake energy transfer efficiency- a first step in achieving a high overall energy transfer efficiency. We have done this by using time-structured electron drive bunches that typically have one or more ultra-high current (>30 kA) femtosecond spike(s) superimposed on a longer (∼0.4 ps) lower current (<10 kA) bunch structure. The first spike effectively field-ionizes the gas and produces a meter-scale (30–160 cm) plasma, whereas the subsequent beam charge creates a wake. The length and amplitude of the wake depends on the longitudinal current profile of the bunch and plasma density. We find that the onset of pump depletion, when some of the drive beam electrons are nearly fully depleted of their energy, occurs for hydrogen pressure ⩾1.5 Torr. We also show that some electrons in the rear of the bunch can gain several GeV energies from the wake. These results are reproduced by particle-in-cell simulations using the QPAD code. At a pressure of ∼2 Torr, simulation results and experimental data show that the beam transfers about 60% of its energy to the wake.
期刊介绍:
Plasma Physics and Controlled Fusion covers all aspects of the physics of hot, highly ionised plasmas. This includes results of current experimental and theoretical research on all aspects of the physics of high-temperature plasmas and of controlled nuclear fusion, including the basic phenomena in highly-ionised gases in the laboratory, in the ionosphere and in space, in magnetic-confinement and inertial-confinement fusion as well as related diagnostic methods.
Papers with a technological emphasis, for example in such topics as plasma control, fusion technology and diagnostics, are welcomed when the plasma physics is an integral part of the paper or when the technology is unique to plasma applications or new to the field of plasma physics. Papers on dusty plasma physics are welcome when there is a clear relevance to fusion.