HIGH-REPETITION-RATE RELATIVISTIC ELECTRON ACCELERATION IN PLASMA WAKEFIELDS DRIVEN BY SINGLE-CYCLE LASER PULSES

Dominykas Gustas1, Aline Vernier1, Diego Guénot1, Marie Ouillé1, Frederik Böhle1, Stefan Hässler1, Rodrigo Lopez-Martens1, Agustin Lifschitz1, Jérôme Faure1

1 Laboratoire d'Optique Appliquée, Ecole Polytechnique, Université Paris-Saclay Palaiseau, France

[email protected]

Continuing progress in laser technology has enabled dramatic advances in laser wakefield acceleration (LWFA), an electron acceleration technique that permits accelerating gradients three orders of magnitude higher than conventional radio-frequency methods. Due to significantly reduced space charge and velocity dispersion effects, relativistic electron bunches accelerated by laser wakefields have also been identified as a candidate tool to achieve unprecedented sub-10 fs temporal resolution in ultrafast electron diffraction (UED) experiments [1], [2]. High repetition rate operation is desirable to improve data collection statistics and wash out shot-to-shot charge fluctuations inherent to plasma accelerators. It is well known that high-quality electron beams with narrow energy spreads and small divergences can be achieved in the blowout, or "bubble" regime [3], which is at present regularly accessed with ~30 fs Joule-class lasers that can perform up to few shots per second. Our group on the contrary employed a cutting edge laser system producing few-mJ pulses compressed nearly to a single optical cycle (3.4 fs) [4] to demonstrate for the first time that, consistently with the scaling laws [5], relativistic electron beams with properties characteristic to the blowout regime and peaked at 4-6 MeV energy can also be achieved at kilohertz repetition rate [6]. We further investigate the plasma density profile effects on the accelerated charge and electron energy and show that using certain structured gas jets several tens of pC/shot can be achieved [7]. We expect this technique to lead to a highly accessible and robust instrument for the scientific community to conduct UED experiments or use it for other applications.

Figure 1

[1] J. Faure et al., Phys. Rev. Accel. Beams 19, 021302 (2016)

[2] Z.-H. He et al., Sci. Rep. 6, 36224 (2016)

[3] A. Pukhov and J. Meyer-ter-Vehn, Appl. Phys. B 74, 355-361 (2002)

[4] F. Böhle et al., Laser Phys. Lett. 11, 095401 (2014)

[5] W. Lu et al., Phys. Rev. Accel. Beams 10, 061301 (2007)

[6] D. Guénot et al., Nat. Photon. 11, 293-296 (2017)

[7] D. Gustas et al., Phys. Rev. Accel. Beams 21, 013401 (2018)