Abstract

Ionization injection triggered by short wavelength laser pulses inside a nonlinear wakefield driven by a longer wavelength laser is examined via multi-dimensional particle-in-cell simulations. We find that very bright electron beams can be generated through this two-color scheme in either collinear propagating or transverse colliding geometry. For a fixed laser intensity $I$, lasers with longer/shorter wavelength $\lambda$ have larger/smaller ponderomotive potential ($\propto I \lambda^2$). The two color scheme utilizes this property to separate the injection process from the wakefield excitation process. Very strong wakes can be generated at relatively low laser intensities by using a longer wavelength laser driver (e.g. a $10 \micro\meter$ CO$_2$ laser) due to its very large ponderomotive potential. On the other hand, short wavelength laser can produce electrons with very small residual momenta ($p_\perp\sim a_0\sim \sqrt{I}\lambda$) inside the wake, leading to electron beams with very small normalized emittances (tens of $\nano\meter$). Using particle-in-cell simulations we show that a $\sim10 \femto\second$ electron beam with $\sim4 \pico\coulomb$ of charge and a normalized emittance of $\sim 50 \nano\meter$ can be generated by combining a 10 $\micro\meter $ driving laser with a 400 $\nano\meter$ injection laser, which is an improvement of more than one order of magnitude compared to the typical results obtained when a single wavelength laser used for both the wake formation and ionization injection.

Highlights

  • Significant progress has been made in the field of plasma-based acceleration [1]

  • Such low slice energy spread may have significant advantages in applications relevant to future coherent light sources driven by plasma accelerators

  • In this paper we have examined ionization injection into plasma wave wakes, where both the wake and the injection are driven by lasers

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Summary

INTRODUCTION

Significant progress has been made in the field of plasma-based acceleration [1]. Our PIC simulation results show that it is possible to generate electron beams containing ∼4 pC of charge with small normalized emittances (∼50 nm), more than 1 order of magnitude smaller than that obtained in ionization injection using a single 800 nm wavelength laser. This indicates that it is difficult to further reduce the emittance by just fine-tuning the laser parameters of the single laser pulse for ionization injection In this simulation the ðδψÞmin is close to −1, only electrons with large initial transverse positions which lead to large transverse momepntaffiffiffiwffiffiffiffihffiffieffiffinffiffiffiffiffitffihffiffieffiffiyffiffiffiffifficross the z axis are injected (δψ < −1 þ 1 þ p2⊥=m2c2=γφ) [14,34] and form a phase space ring structure in 2D simulations. The injected charge is about 20 pC by assuming a cylindrical distribution around the z axis. (c) The x − px phase spaces at z 1⁄4 1 mm for the laser polarized in (left) and out (right) of the simulation plane

LWFA WITH IONIZATION INJECTION USING TWO LASER PULSES WITH DIFFERENT
CONCLUSION
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