Abstract

Strongly self-modulated regime of laser wakefield electron acceleration has been experimentally studied using positively/negatively chirped Ti:sapphire laser pulses with duration $\ensuremath{\ge}45\text{ }\text{ }\mathrm{fs}$, and intensity $\ensuremath{\le}1.2\ifmmode\times\else\texttimes\fi{}{10}^{18}\text{ }\text{ }\mathrm{W}/{\mathrm{cm}}^{2}$ interacting with a plasma having density $>5\ifmmode\times\else\texttimes\fi{}{10}^{19}\text{ }\text{ }{\mathrm{cm}}^{\ensuremath{-}3}$. The total charge of the high energy electrons produced from self-injection and acceleration in the wakefield was found to depend strongly and asymmetrically on the magnitude and sign of the chirp, which was also corroborated by the forward Raman scattering signals. Generation of low divergence ($\ensuremath{\le}10\text{ }\text{ }\mathrm{mrad}$), quasimonoenergetic electron beam was observed with a maximum energy of $\ensuremath{\sim}28\text{ }\text{ }\mathrm{MeV}$ for a positively chirped laser pulse of duration $\ensuremath{\sim}70\text{ }\text{ }\mathrm{fs}$. The observations are explained considering faster rise time associated with a positive chirped laser pulse which generates intense seed for stronger modulation of the laser pulse and consequently stronger wakefield excitation leading to higher electron beam charge and energy.

Highlights

  • The laser wakefield acceleration (LWFA) [1] scheme utilizes large amplitude plasma waves for accelerating electrons to relativistic energies over extremely short distances

  • For a chirped laser pulse, one can define the instantaneous frequency ! as ! 1⁄4 !0 þ bt, where t is the time in the pulse reference frame, b is the chirp parameter given by b 1⁄4 2 ln2=21⁄2ð=oÞ2 À 1Š1=2, where and o are the full width at half maximum (FWHM) duration of the chirped and unchirped pulse, respectively

  • We have studied the effect of positively/negatively chirped Ti:sapphire laser pulses with duration ! 45 fs and intensity 1:2 Â 1018 W=cm2 interacting with high density ( > 5 Â 1019 cmÀ3) under dense plasma in the regime c > d0 * p for generation of relativistic electron beam

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Summary

Introduction

The laser wakefield acceleration (LWFA) [1] scheme utilizes large amplitude plasma waves for accelerating electrons to relativistic energies over extremely short distances. Quasimonoenergetic electron bunches have been produced in the strongly self-modulated LWFA (SM-LWFA) regime by using longer pulses (c ) p) and higher plasma density [16,17,18]. In this regime, a single long laser pulse with duration c ) p breaks up into multiple short pulses through forward Raman scattering (FRS) instability [19], each of which has a width of the order of the plasma wavelength p [16]. The field of this longitudinal wave is sufficiently large to self-trap electrons

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