Title: Presentazione di PowerPoint
1INTENSITY LIMITATIONS (Space Charge and Impedance)
M. Zobov
2Is it important?
J.Bosser et al., NIM 441 (2000) 1-8
3SELF FIELDS AND WAKE FIELDS
In a real accelerator, there is another important
source of e.m. fields to be considered, the beam
itself, which circulating inside the pipe,
produces additional e.m. fields called
"self-fields
4These fields depend on the current and on the
charges velocity. They are responsible of many
phenomena of beam dynamics
-
- energy loss
- shift of the synchronous phase and frequency
(tune) -
- shift of the betatron frequencies (tunes)
- energy spread and emittance degradation
-
- instabilities.
5- What do we mean with space charge?
- It is net effect of the Coulomb interactions in
a multi-particle system - Space Charge Regime gt dominated by the self
field produced by the particle distribution,
which varies appreciably only over large
distances compared to the average separation of
the particles gt Collective Effects
6Example 1. Relativistic Continuous Uniform
Cylindrical
Gausss law
Linear with r
Amperes law
L. Palumbo, JUAS
7Lorentz Force
- has only radial component
- is a linear function of the transverse coordinate
The attractive magnetic force, which becomes
significant at high velocities, tends to
compensate for the repulsive electric force.
8Transverse Incoherent Effects
We take the linear term of the transverse force
in the betatron equation
The betatron shift is negative since the space
charge forces are defocusing on both planes.
Notice that the tune shift is in general function
of z, therefore there is a tune spread inside
the beam.
9Incoherent Tune Shift
The tune shift for unbunched beams in a perfectly
conducting vacuum chamber of half-height h,
between perfect magnetic pole pieces at a
distance g from the axis
For bunched beams we have to take into account a
bunching factor B defined as the ratio of average
to peak current
10Estimates for EDM Machine
P 0.7 GeV/c g 1.0674
P 1.5 GeV/c g 1.2804
! To be compared with
111.
2. Optics functions change by changing the tune.
This leads to the size changes, i.e. collective
effects
12Wake Potentials
there can be two effects on the test charge
1) a longitudinal force which changes its
energy, 2) a transverse force which deflects
its trajectory.
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15Impedance of a Step (S. Kheifets and S. Heifets)
16Limits on Impedances
The wake fields can act as a positive feedback
leading to instabilities. Nonlinearities damp
them (Landau damping)
Longitudinal
Transverse
Similar to DAFNE ?
17REFERENCES
- L. Palumbo, Space Charge Effects and
Instabilities, JUAS, 2003. - M. Zobov and A. Gallo, Instabilities,
http//www.lnf.infn.it/acceleratori/dafne/seminary
/dafne_zobov.pdf - L. Palumbo, V. Vaccaro and M. Zobov, Wake Fields
and Impedance, CAS CERN 95-06, 1995