Title: Collective Effects and Beam Measurements in Particle Accelerators
1Collective Effects and Beam Measurements in
Particle Accelerators
- beam diagnostics and fundamental limitations to
the performance of high-intensity accelerators
http//ab-abp-rlc.web.cern.ch/ab-abp-rlc/
See also slides on Measurements, ideas,
curiosities
2Wakefield for a pill-box cavity
- Animation showing a bunch of charged particles
moving on the cavity axis and the corresponding
electric field lines computed by the program ABCI - Courtesy Andreas Wagner http//awagner.home.cern.c
h/awagner/
3TRISIM3D simulation of a LEP bunch E 22 GeV,
Qs 0.092, I 0.3 mA
- 3-dimensional computer simulation of single bunch
collective effects in particle accelerators - top and side view of the particle distribution
turn by turn, over 60 turns - Courtesy Andreas Wagner http//awagner.home.cern.c
h/awagner/
4CERN Linac4layout and parameters
160MeV
3MeV
40MeV
90MeV
3MeV
95keV
DTL
CCDTL
SCL
CHOPPER
RFQ
H-
Drift Tube Linac 352 MHz 13.4 m 3 tanks 5
klystrons 4 MW
Side Coupled Linac 704 MHz 28 m 20 tanks 4
klystrons 12 MW
Cell-Coupled Drift Tube Linac 352 MHz 25.3 m 24
tanks 8 klystrons 6.5 MW
Chopper 352 MHz 3.6 m
Radio Frequency Quadrupole 352 MHz 6 m 1
Klystron 1 MW
Duty cycle 0.1 phase 1 (Linac4) 3-4 phase 2
(SPL) (RF design 15)
4 different structures, (RFQ, DTL, CCDTL, SCL) 2
frequencies
Total Linac4 80 m, 18 klystrons
current 40 mA (avg. in pulse), 65 mA (bunch)
Courtesy A. Lombardi
5Instabilities in a Linac
Transverse tune depression
Longitudinal to transverse phase advance
6Intra-Beam Scattering (simplified formulae by K.
Bane, EPAC 2002)
- For the LHC, the average dispersion invariant is
ltHxgt0.03 m, bav100 m, and the Coulomb logarithm
(log)24 - Note that the transverse IBS growth rate is about
proportional to the particle density in the 6D
phase space Nb/(e2szsd)
IBS growth times for long super-bunches
in the LHC as a function of the rms momentum
spread sd