Abstract

The emittance of high brightness electron sources, particularly field emitters and photocathodes but also thermionic sources, is increased by surface roughness on the emitter. Such structure causes local field enhancement and complicates both the prediction of emittance and the underlying emission models on which such predictions depend. In the present work, a method to find the emission trajectories near regions of high field enhancement is given and applied to emittance predictions for field, photo, and thermal emission for an analytically tractable hemispherical model. The dependence of the emittance on current density, spatial variation, and acceleration close to the emission site is identified and the impact of space charge discussed. The methodology is extensible to field emission from close-spaced wirelike structures, in particular, and extensions to that configuration are discussed. The models have application to electron sources for high frequency vacuum electronics, high power microwave devices, and free-electron lasers.

Highlights

  • For accelerators and electron devices, the usefulness of a high brightness electron beam is constrained by its emittance [1], of which that portion due to the cathode, known as “intrinsic emittance,” is of increasing importance

  • Krasilnikov [38] generalizes the 2D sinusoidal variation of a surface to 3D, as well as examines the Lorenztian model of Lau [39], to conclude that the increased electric field on the surface can lead to an increase in thermal emittance comparable to 30%, and argues that space charge effects increase it; his conclusions are supported by the present work

  • Realistic thermionic and photoemission surfaces have surface features varying in size and randomly placed, and field emitters can be made in triangular arrays rather than on a square lattice, for the analytic model, assume that first, the M2 protrusions are uniformly sized; second, that the protrusions are located on a square array with a pitch of l so that the area of the array is 1⁄2ðM − 1ÞlŠ2 ≡ L2; and third, that l is sufficiently large that to a good approximation, the trajectories of a single boss are unaffected by its neighbors

Read more

Summary

INTRODUCTION

For accelerators and electron devices, the usefulness of a high brightness electron beam is constrained by its emittance [1], of which that portion due to the cathode, known as “intrinsic emittance,” is of increasing importance. For field and photoemission sources, is complicated by emission nonuniformity and geometric effects. For field and photoemission, emittance is strongly coupled to space charge effects. Numerical estimates of a geometrical array of emitters is considered, as is the manner in which the methodology may be extended to wirelike (carbon fiber) field emitters. A discussion of how the methodology may be modified to treat the consequences of space charge forces due to the emitted current, with respect to beam optics codes, is given

EMITTANCE AND APPLICATIONS
Moments and normalized emittance
Potential and field for a hemisphere
Notional and emission parameters
Thermal emission
Photoemission
Single boss emittance
Array of bosses emittance
10-4 Line: Leading Order
Integration of trajectories
Impulse approximation
Performance of impulse approximation
Characteristic array emittances
Variations on characteristic conditions
Extension to wire field emitters
DISCUSSION AND CONCLUSION
Full Text
Paper version not known

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

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.