Abstract

High-charge electron beams produced by laser-wakefield accelerators are potentially novel, scalable sources of high-power terahertz radiation suitable for applications requiring high-intensity fields. When an intense laser pulse propagates in underdense plasma, it can generate femtosecond duration, self-injected picocoulomb electron bunches that accelerate on-axis to energies from 10s of MeV to several GeV, depending on laser intensity and plasma density. The process leading to the formation of the accelerating structure also generates non-injected, sub-picosecond duration, 1–2 MeV nanocoulomb electron beams emitted obliquely into a hollow cone around the laser propagation axis. These wide-angle beams are stable and depend weakly on laser and plasma parameters. Here we perform simulations to characterise the coherent transition radiation emitted by these beams if passed through a thin metal foil, or directly at the plasma–vacuum interface, showing that coherent terahertz radiation with 10s μJ to mJ-level energy can be produced with an optical to terahertz conversion efficiency up to 10−4–10−3.

Highlights

  • Terahertz (THz) radiation, which lies between mid-infrared and microwaves, is of great interest to researchers and industrialists because of the wide range of applications [1,2,3,4,5,6,7]

  • This paper investigates the production of THz radiation from very high-charge, wide-angle electron beams from a laser-wakefield accelerator (LWFA) that are not injected into the wake [36, 37]

  • We have shown, using numerical simulations, that wide-angle electron beams produced by LWFAs can deliver 10s μJ to mJ-level, single-cycle radiation in the 0.1–5 THz spectral region, depending on the radiator size and location

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Summary

20 April 2018

Attribution to the author(s) and the title of When an intense laser pulse propagates in underdense plasma, it can generate femtosecond duration, the work, journal citation and DOI. Self-injected picocoulomb electron bunches that accelerate on-axis to energies from 10s of MeV to several GeV, depending on laser intensity and plasma density. The process leading to the formation of the accelerating structure generates non-injected, sub-picosecond duration, 1–2 MeV nanocoulomb electron beams emitted obliquely into a hollow cone around the laser propagation axis. These wide-angle beams are stable and depend weakly on laser and plasma parameters.

Introduction
Theoretical model
Simulation results
Conclusions
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