Abstract

Incoherent effects of space charge and sum resonances on particle beams in a storage ring

Highlights

  • Collective effects in a non-neutral plasma as a beam in a partiqcleffiffiffiffiffiaffifficffifficffi elerator are related to the Debye length λ ∝ v2th=n, where v2th is the rms square “thermal” component of the velocity of the particles and n the particle density [1,2]

  • We have proposed to use the parameter Iχ;l, based on a plasma physics argument, to define the incoherent space charge regime and to anticipate the goodness of space charge frozen models

  • We have presented the theory of the sum resonances with the frozen space charge

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Summary

Franchetti

GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, 64291 Darmstadt, Germany and Goethe Universität Frankfurt, Max-von-Laue-Straße 7, 60438 Frankfurt am Main, Germany (Received 4 August 2018; published 25 November 2019). Several studies, numerical and experimental, have been carried out for enlightening the effect of space charge and resonances on particle beams stored in accelerators. The last effort of this quest focused on the third-order coupled resonances, emphasizing the existence of the periodic crossing of fixed lines induced by space charge. The theory of nonlinear sum resonances in coasting beams in the presence of space charge is presented and applied to unravel the key features of the four-dimensional coupled dynamics in high-intensity bunched beams

THE INCOHERENT SPACE CHARGE REGIME
FRANCHETTI
SUM RESONANCES AND INCOHERENT SPACE CHARGE
Hamiltonian and space charge potential
Full solution
Slowly varying Hamiltonian
Time-independent slowly varying Hamiltonian
Incoherent amplitude-dependent detuning
Reduced system
Stationary solutions
EFFECT OF THE INCOHERENT SPACE CHARGE ON FIXED LINES
AN EXAMPLE OF APPLICATION
A CHARACTERIZATION OF THE PERIODIC CROSSING OF FIXED LINES
SUMMARY
Space charge coefficients
Nonlinear magnet coefficients
Nonresonant slowly varying potential from space charge
Nonresonant slowly varying potential from nonlinear magnet components
Secondary tunes
Full Text
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