Author: Bishofberger, K.
Paper Title Page
PLT004
Three-Dimensional Coherent Synchrotron Radiation Calculations  
 
  • B.E. Carlsten, K. Bishofberger, C. Huang, T.J. Kwan, N.A. Yampolsky
    LANL, Los Alamos, New Mexico, USA
  • P. Piot, C.R. Prokop
    Northern Illinois University, DeKalb, Illinois, USA
  • R.D. Ryne
    LBNL, Berkeley, California, USA
 
  Funding: Los Alamos National Laboratory LDRD Program
We report on ab initio three-dimensional coherent synchrotron radiation (CSR) calculations using realistic numbers of simulation particles (~ 6 billion for bunch charges of 1 nC), for different electron bunch aspect ratios. These calculations use the exact Lienard-Weichert fields and are done for electron beam energies of both 100 MeV and 1 GeV. These results confirm many features of the standard one-dimensional CSR model, but also provide some surprises, particularly in regards to noise present in the fields which increases at higher beam energies. These results are compared to those from three-dimensional simulations using CSRtrack and using finite-difference time-domain particle-in-cell techniques.
 
slides icon Slides PLT004 [0.982 MB]  
 
WG2021
Emittance Partitioning Through Controlling Eigen-Emittances  
 
  • B.E. Carlsten, K. Bishofberger, L.D. Duffy, Q.R. Marksteiner, N.A. Yampolsky
    LANL, Los Alamos, New Mexico, USA
  • R.D. Ryne
    LBNL, Berkeley, California, USA
 
  Funding: Los Alamos National Laboratory LDRD Program
High-brightness photoinjectors tend to produce electron beams with equipartitioned emittances, where the transverse normalized emittances are roughly the same as the normalized longitudinal emittance. However, the needs of future free-electron lasers will require transverse emittances up to three orders of magnitude smaller than the longitudinal emittances. Recent work on exotic optics schemes has pointed to significant new opportunities for providing arbitrary control of the beam emittance partitioning, based on the conservation of eigen-emittances which results from the symplectic behavior of electrodynamics. Specifically, we can use initial correlations imposed on the beam as it is formed to control the beam's eigen-emittances, which can then be recovered later at high energy as the actual beam emittances, in a linear sense. Here we discuss different schemes to provide arbitrary control of the eigen-emittances, including the addition of nonsymplectic beamline elements after the beam has been accelerated.
 
slides icon Slides WG2021 [0.659 MB]