3 research outputs found
High-charge 10 GeV electron acceleration in a 10 cm nanoparticle-assisted hybrid wakefield accelerator
In an electron wakefield accelerator, an intense laser pulse or charged
particle beam excites plasma waves. Under proper conditions, electrons from the
background plasma are trapped in the plasma wave and accelerated to
ultra-relativistic velocities. We present recent results from a
proof-of-principle wakefield acceleration experiment that reveal a unique
synergy between a laser-driven and particle-driven accelerator: a high-charge
laser-wakefield accelerated electron bunch can drive its own wakefield while
simultaneously drawing energy from the laser pulse via direct laser
acceleration. This process continues to accelerate electrons beyond the usual
decelerating phase of the wakefield, thus reaching much higher energies. We
find that the 10-centimeter-long nanoparticle-assisted wakefield accelerator
can generate 340 pC, 10.4+-0.6 GeV electron bunches with 3.4 GeV RMS convolved
energy spread and 0.9 mrad RMS divergence. It can also produce bunches with
lower energy, a few percent energy spread, and a higher charge. This
synergistic mechanism and the simplicity of the experimental setup represent a
step closer to compact tabletop particle accelerators suitable for applications
requiring high charge at high energies, such as free electron lasers or
radiation sources producing muon beams
The acceleration of a high-charge electron bunch to 10 GeV in a 10-cm nanoparticle-assisted wakefield accelerator
An intense laser pulse focused onto a plasma can excite nonlinear plasma waves. Under appropriate conditions, electrons from the background plasma are trapped in the plasma wave and accelerated to ultra-relativistic velocities. This scheme is called a laser wakefield accelerator. In this work, we present results from a laser wakefield acceleration experiment using a petawatt-class laser to excite the wakefields as well as nanoparticles to assist the injection of electrons into the accelerating phase of the wakefields. We find that a 10-cm-long, nanoparticle-assisted laser wakefield accelerator can generate 340 pC, 10 ± 1.86 GeV electron bunches with a 3.4 GeV rms convolved energy spread and a 0.9 mrad rms divergence. It can also produce bunches with lower energies in the 4–6 GeV range
The acceleration of a high-charge electron bunch to 10 GeV in a 10-cm nanoparticle-assisted wakefield accelerator
An intense laser pulse focused onto a plasma can excite nonlinear plasma waves. Under appropriate conditions, electrons from the background plasma are trapped in the plasma wave and accelerated to ultra-relativistic velocities. This scheme is called a laser wakefield accelerator. In this work, we present results from a laser wakefield acceleration experiment using a petawatt-class laser to excite the wakefields as well as nanoparticles to assist the injection of electrons into the accelerating phase of the wakefields. We find that a 10-cm-long, nanoparticle-assisted laser wakefield accelerator can generate 340 pC, 10 ± 1.86 GeV electron bunches with a 3.4 GeV rms convolved energy spread and a 0.9 mrad rms divergence. It can also produce bunches with lower energies in the 4–6 GeV range