TY - JOUR
T1 - Generation of meter-scale hydrogen plasmas and efficient, pump-depletion-limited wakefield excitation using 10 GeV electron bunches
AU - Zhang, C.
AU - Storey, D.
AU - San Miguel Claveria, P.
AU - Nie, Z.
AU - Marsh, K. A.
AU - Hogan, M.
AU - Mori, W. B.
AU - Adli, E.
AU - An, W.
AU - Ariniello, R.
AU - Cao, G. J.
AU - Clarke, C.
AU - Corde, S.
AU - Dalichaouch, T.
AU - Doss, C. E.
AU - Emma, C.
AU - Ekerfelt, H.
AU - Gerstmayr, E.
AU - Gessner, S.
AU - Hansel, C.
AU - Knetsch, A.
AU - Lee, V.
AU - Li, F.
AU - Litos, M.
AU - O’Shea, B.
AU - White, G.
AU - Yocky, G.
AU - Zakharova, V.
AU - Joshi, C.
N1 - Publisher Copyright:
© 2024 IOP Publishing Ltd.
PY - 2024/2/1
Y1 - 2024/2/1
N2 - 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.
AB - 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.
KW - beam-ionized wake excitation
KW - high beam-to-wake energy transfer efficiency
KW - high-gradient electron acceleration
KW - meter-scale hydrogen plasmas
KW - particle-in-cell simulations
KW - plasma wakefield acceleration
KW - time-structured electron bunches
UR - https://www.scopus.com/pages/publications/85182526397
U2 - 10.1088/1361-6587/ad1ae4
DO - 10.1088/1361-6587/ad1ae4
M3 - Article
AN - SCOPUS:85182526397
SN - 0741-3335
VL - 66
JO - Plasma Physics and Controlled Fusion
JF - Plasma Physics and Controlled Fusion
IS - 2
M1 - 025013
ER -