Longitudinal compression and transverse matching of electron bunch for external injection LPWA at ESCULAP

TL;DR

This paper presents theoretical and numerical methods for compressing and matching electron bunches for laser-plasma acceleration, achieving significant bunch length reduction and optimized beam parameters at ESCULAP.

Contribution

It introduces a combined theoretical and simulation approach for longitudinal compression and transverse matching of electron bunches in LWFA injection.

Findings

Electron bunch compressed from 0.9ps to 70fs RMS

Peak current of 152A achieved after compression

Optimized quadrupole settings match beam to plasma entrance

Abstract

We present theoretical and numerical studies of longitudinal compression and transverse matching of electron bunch before injecting into the Laser-plasma Wake Field Accelerator (LWFA) foreseen at the ESCULAP project in ORSAY. Longitudinal compression is performed with a dogleg chicane, the chicane is designed based on theory of beam optics, beam dynamics in dogleg is studied with ImpactT and cross checked with CSRtrack, both 3D space charge (SC) and coherent synchrotron radiation (CSR) effects are included. Simulation results show that the energy chirp at the dogleg entrance should be smaller than the nominal optic design value, in order to compensate the negative energy chirp increase caused by longitudinal SC, while CSR can be ignored in our case. With an optimized configuration, the electron bunch ($\sim$10MeV, 10pC) is compressed from 0.9ps RMS to 70fs RMS (53fs FWHM), with a peak current of 152A. Transverse matching is realized with a doublet and a triplet, they are matched with Madx and the electron bunch is tracked with ImpactT, simulation results show little difference with the nominal design values, that is due to the SC effect. Finally, by simply adjusting the quadrupole strength, a preliminary optimized configuration has been achieved, that matches the Courant-Snyder (C-S) parameters to $\alpha_{x}=0.01$,$\alpha_{y}=-0.02$, $\beta_{x}=0.014$m,$\beta_{y}=0.012$m at the plasma entrance.