Abstract

Flat beams -- beams with asymmetric transverse emittances -- have important applications in novel light-source concepts, advanced-acceleration schemes and could possibly alleviate the need for damping rings in lepton colliders. Over the last decade, a flat-beam-generation technique based on the conversion of an angular-momentum-dominated beam was proposed and experimentally tested. In this paper we explore the production of compressed flat beams. We especially investigate and optimize the flat-beam transformation for beams with substantial fractional energy spread. We use as a simulation example the photoinjector of the Fermilab's Advanced Superconducting Test Accelerator (ASTA). The optimizations of the flat beam generation and compression at ASTA were done via start-to-end numerical simulations for bunch charges of 3.2 nC, 1.0 nC and 20 pC at ~37 MeV. The optimized emittances of flat beams with different bunch charges were found to be 0.25 {\mu}m (emittance ratio is ~400), 0.13 {\mu}m, 15 nm before compression, and 0.41 {\mu}m, 0.20 {\mu}m, 16 nm after full compression, respectively with peak currents as high as 5.5 kA for a 3.2-nC flat beam. These parameters are consistent with requirements needed to excite wakefields in asymmetric dielectric-lined waveguides or produce significant photon flux using small-gap micro-undulators.

Highlights

  • Flat beams with high-emittance ratio directly generated in a photoinjector via linear transformation of angularmomentum-dominated round beams have many attractive applications

  • We investigated the formation of compressed flat beams

  • We presented start-to-end simulations of flat beam generation and compression using as an example the 50-MeV photoinjector of the Advanced Superconducting Test Accelerator (ASTA) facility currently in commissioning phase at Fermilab

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Summary

INTRODUCTION

Flat beams with high-emittance ratio directly generated in a photoinjector via linear transformation of angularmomentum-dominated round beams ( referred to as “magnetized beams”) have many attractive applications. Compressed low-energy (

THEORY OF FLAT BEAM GENERATION
ASTA INJECTOR SETUP
FLAT BEAM GENERATION
Optimization procedure description
Emittance growth mitigation for RFBT
FLAT BEAM COMPRESSION
Bunch length evolution in the chicane
Emittance growth in the flat beam compression
Phase-space dilution during compression
Compression of the flat beam with lower charges
SUMMARY
Findings
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