Abstract

This paper presents a study of coherent and superradiant Smith-Purcell (SP) radiation with the help of a two-dimensional particle-in-cell (PIC) simulation. The simulation model supposes a rectangular grating with period length of $173\text{ }\ensuremath{\mu}\mathrm{m}$ to be driven by a single electron bunch, a train of periodic bunches and a continuous beam, respectively. We chose 40 keV as the initial energy of electrons and therefore the SP radiation frequency falls in the THz regime. From our single bunch simulation we distinguish the true SP radiation separated in time from the emission of the evanescent wave. The evanescent wave radiates from both ends of the grating and is characterized by an angle independent frequency lower than the minimum allowed SP frequency. In order to avoid the buildup of beam bunching from an initially continuous beam, we use a train of periodic bunches to excite the grating and observe the superradiant phenomenon. The repetition frequency of the spatially periodic bunches is assumed to be 300 GHz. We find that the superradiant radiation is only emitted at higher harmonics of this frequency and at the corresponding SP angles. This result conforms to the viewpoint of Andrews and co-workers. The simulation with a continuous beam shows the dependence of the output power on the beam current. The power curve shows two regimes, one for the incoherent SP radiation and the other for the superradiance, which resembles the Dartmouth experimental result. And furthermore, the frequency spectrum shows an apparent difference for the two regimes, which is in contrast to the observations of Urata and co-workers.

Highlights

  • A renewed interest in SP radiation has been raised in recent years, since Urata and co-workers observed the superradiance in the THz regime from the experiment at Dartmouth college [1,2]

  • The superradiant radiation of the Dartmouth experiment is regarded as the result of electron beam bunching, induced by the strong interaction of the continuous beam with the evanescent wave propagating along the grating surface

  • We have studied the coherent and superradiant SP radiation through simulation of an open grating system driven by different modes of electron beam

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Summary

INTRODUCTION

A renewed interest in SP radiation has been raised in recent years, since Urata and co-workers observed the superradiance in the THz regime from the experiment at Dartmouth college [1,2]. The superradiant radiation of the Dartmouth experiment is regarded as the result of electron beam bunching, induced by the strong interaction of the continuous beam with the evanescent wave propagating along the grating surface. Donohue and Gardelle employed a PIC code and performed the simulation in the few GHz regime with a continuous electron beam [18]. They carefully studied the electron-wave interaction and demonstrated the beam bunching and the superradiant radiation. They addressed the relation of growth rate and beam current. We find the relation between output power and the beam current, which is not given in Ref. [18]

SIMULATION DESCRIPTION
A single bunch
Train of bunches
Continuous beam
CONCLUSION
Methods

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