Abstract

Ultra-intense, narrow-bandwidth, electromagnetic pulses have become important tools for exploring the characteristics of matter. Modern tuneable high-power light sources, such as free-electron lasers and vacuum tubes, rely on bunching of relativistic or near-relativistic electrons in vacuum. Here we present a fundamentally different method for producing narrow-bandwidth radiation from a broad spectral bandwidth current source, which takes advantage of the inflated radiation impedance close to cut-off in a medium with a plasma-like permittivity. We find that by embedding a current source in this cut-off region, more than an order of magnitude enhancement of the radiation intensity is obtained compared with emission directly into free space. The method suggests a simple and general way to flexibly use broadband current sources to produce broad or narrow bandwidth pulses. As an example, we demonstrate, using particle-in-cell simulations, enhanced monochromatic emission of terahertz radiation using a two-colour pumped current source enclosed by a tapered waveguide.

Highlights

  • Intense, short-duration pulses of monochromatic electromagnetic radiation are very powerful tools for exploring and controlling the dynamics and structure of matter

  • When the J-source is immersed in a uniform cut-off region [Fig. 1c], the spectrum of the signal determined 10 μm from the J-source is enhanced by factor of 5 from case C, i.e. has an electric field intensity that is 25-fold larger than that obtained for emission in entirely free space and the bandwidth is even lower, 2.5 THz

  • We observe that selectively enhanced emission (SEE) is efficient with current sources

Read more

Summary

Introduction

Short-duration pulses of monochromatic electromagnetic radiation are very powerful tools for exploring and controlling the dynamics and structure of matter. We discover that a monochromatic, continuously oscillating current source in a cut-off region generates a temporally growing and spatially diffusing electric field, which is a solution of the driven-Schrödinger equation[9].

Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call