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transverse-dynamics

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TUPMS048 Measurement and Analysis of Field Emission Electrons in the LCLS Gun gun, cathode, electron, vacuum 1299
 
  • D. Dowell
  • E. N. Jongewaard, C. Limborg-Deprey, J. F. Schmerge, A. E. Vlieks
    SLAC, Menlo Park, California
  Funding: SLAC is operated by Stanford University for the Department of Energy under contract number DE-AC03-76SF00515.

The field emission was measured during the high-power testing of the LCLS photocathode RF gun. A careful study and analysis of the field emission electrons, or dark current is important in assessing the gun's internal surface quality in actual operation, especially those surfaces with high fields. The charge per 2 microsecond long RF pulse (the dark charge) was measured as a function of the peak cathode field for the 1.6 cell, 2.856GHz LCLS RF gun. Faraday cup data was taken for cathode peak RF fields up to 120MV/m producing a maximum of 0.6nC/RF pulse for a diamond-turned polycrystalline copper cathode installed in the gun. The field dependence of the dark charge is analyzed using a temperature-dependent Fowler-Nordheim (FN) theory to obtain the field enhancement factor and other emitter parameters. Digitized images of the dark charge were taken using a 100 micron thick YAG crystal for a range of solenoid fields to determine the location and angular distribution of the field emitters. The FN plots and emitter image analysis will be described in this paper.

 
 
THPAS085 Kinetic Equilibrium and Stability Properties of 3D High-Intensity Charged Particle Bunches simulation, coupling, collective-effects, plasma 3681
 
  • H. Qin
  • R. C. Davidson, E. Startsev
    PPPL, Princeton, New Jersey
  Funding: Research supported by the U. S. Department of Energy.

In 3D high-intensity bunched beams, the collective effects associated with strong coupling between the longitudinal and transverse dynamics are of fundamental importance. A direct consequence of this coupling is that the particle dynamics does not conserve transverse energy and longitudinal energy separately, and there exists no exact kinetic equilibrium which has an anisotropic energy in the transverse and longitudinal directions. The strong coupling also introduces a mechanism for the electrostatic Harris-type instability driven by strong temperature anisotropy, which exists naturally in beams that have been accelerated to large velocities. The self-consistent Vlasov-Maxwell equations are applied to high-intensity bunched beams, and a generalized low-noise delta-f particle simulation algorithm is developed for bunched beams with or without energy anisotropy. Systematic studies are carried out that determine the particle dynamics, the approximate equilibrium, and stability properties under conditions corresponding to strong 3D nonlinear space-charge force. Finite bunch-length effects on collective excitations and anisotropy-driven instabilities are also investigated.