beam observation and introduction to collective beam instabilities observation of collective beam...
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Beam observation and
Introduction to Collective Beam Instabilities
Observation of collective beam instability
Collective modes
Wake fields and coupling impedances
Head-tail instability
Microwave instability
Beyond
T. Toyama KEK
Observation of collective beam instability
Example: KEK-PS 12 GeV Main Ring
At 500 MeV injection plat bottom
a beam loss occurs (red curve).
Amount and timing of the loss => random.
Proton number NB
(Feedback CT)
Magnetic field
Example: KEK-PS 12 GeV Main Ring
At phase transition energy~5.4 GeV (in kinetic energy)
a large beam loss occurs (red curve).
Amount of the loss is at random.
Proton number NB
(Feedback CT)
Magnetic field
Observation
NB
Multi-trace of horizontal betatron oscillation
NB
Amplitude of betatron oscillationMagnetic field
Observation horizontal betatron tune during acceleration
t
f
frev 2frev
frev-ffrev-f
2frev-f 2frevf
Without external kick, coherent oscillation emerged
Measurement by a wall current monitor
Real signals may be attenuatedby the loss in the cable > 100 mand limited band width of the WCM.
Beam loss: collective instabilities --- at random, a kind of
positive feedback starting from a random seed direct space charge effects --- regular
some mistake in parameterrs --- regular(B, fRF, tune, …)
Collective modes
Coasting beam / longitudinal
n=3
Beam
Coasting beam / transverse
Collective modes
n=3
Beam
betattonoscillation
x or y
Bunched beam / logitudinal
Collective modes
l=1 l=2 l=3dipole quadrupole sextupole
zz z
charge density
Phase space
…..
no momopole mode
Bunched beam / transverse
Collective modes
dipole mode density zx
zzz
l=0 l=1 l=2monopole dipole quadrupole …..
superimposed
Wake fields and coupling impedance
Electromagnetic fields is produced by the beam passed by.
+ + +++++++ + +
− − − − − − −
− − − − − − −
IB
Wall Current −IB
−
−
v
Wall Current
++e qF//
s
F⊥
€
Wake functions (W//, W⊥) : "Green function"
Force acting on a test particle (charge e)
produced by the delta-function beam (charge q, dipole moment qy)
Longitudinal component:
F // = F//ds−L /2
L /2
∫ =−eqW//(s)
Transverse component:
F ⊥ = F⊥ds−L /2
L /2
∫ =−eqyW⊥(s)
[W//]=[V /C]
[W⊥]=[V /Cm]
Wake fields and coupling impedance
€
Wake functions (W//, W⊥) of a resistive wall
Force acting on a test particle (charge e)
Wake fields and coupling impedance
€
Longitudinal impedance Z// :
Sinusoidal current J 0(s,t)= ˆ J 0ei(ks−ωt) produces
longitudinal wake potential across the section:
V(s,t) =−1v
d ′ s J 0(s,t−′ s −sc
) s∞∫ W//(s− ′ s )
=−J 0(s,t) Z//(ω)
longitudinal impedance:
Z// =dzc
e−iωz/c −∞∞∫ W//(s)
[Z//]=[Ω]
Wake fields and coupling impedance
€
Transverse impedance Z⊥ :
Sinusoidal dipole moment J1(s,t) =
Current J 0(s,t)× dipole displacement y(s,t)
J1(s,t)=y(s,t) J 0(s,t) = ˆ J 1ei(ks−ωt) produces
transverse wake potential across the section:
V⊥ =i J1(s,t) Z⊥(ω)
transverse impedance:
Z⊥ =iβ
dzc
e−iωz/c −∞∞∫ W⊥(s)
[Z⊥]=[Ω/m]
Wake fields and coupling impedance
Wake fields due to a Gaussian beam in a resistive pipe
Longitudinal wake potential Transverse wake potential
Acc
eler
atio
nD
ecce
lera
tion
Dam
pen
defl
ecti
onF
urth
er
defl
ecti
on
Wake fields and coupling impedance
Impedance of a resistive pipe
Wake fields and coupling impedance
Wake fields by cavities
Q=1 Q=10
Wake fields and coupling impedance
Impedance of cavities
Q=1 Q=10
Head-Tail InstabilityTransverse bunched beam instability
Time domain picture
Head-Tail InstabilityChromaticity = 0
Red full line: (z)x(z)Red dushed line: (z)x’(z)Blue: kick due to resistive wall
x
x’
Growth
Damp No effect
~Totally no effect
(1)
(1)
(2)
(2)
(3)
(3)
(4)
(4)
headtail
Head-Tail Instability
Head-tail phase
z
p/p
€
ˆ z
€
−̂ z 0
€
χ =ξωβˆ z
cη
€
Δνβ
νβ=ξ
Δpp
phase of betatron oscillation
phase space of synchrotron oscillation
Head-Tail Instability
x
x’
Damp
~ 1
Red full line: (z)x(z)Red dushed line: (z)x’(z)Blue: kick due to resistive wall
(1)
(2)
(1)
(2)
~Totally damping
headtail
Head-Tail Instability
x
x’
Growth
~Totally growing
(1)
(2)
~
Red full line: (z)x(z)Red dushed line: (z)x’(z)Blue: kick due to resistive wall
(1)
(2)
headtail
Head-Tail Instability
Summary of Growth rate vs. Chromaticity
Head-tail phase
Gro
wth
rat
e
Chao’s text book
mode = 0
mode = 1mode =2
mode =3
€
χ =ξωβˆ z
cη
Stab
le
Un
stable
Head-Tail InstabilityKEK-PS 12 GeV Main Ring
T. Toyama et al., PAC97, APAC98, PAC99
mode=0
mode=1 mode=2
NB
amplitude of dipole oscillation
Head-Tail InstabilityCERN PS higher order head-tail mode
R. Cappi, NIM
Head-Tail Instability
KEK-PS12GeV MR
Frequencydomainanalysis
growth rate∝Re[Z()] F()
Re[
ZT]
For
m f
a ct o
r F
(f
req.
spe
ctru
m
o f t h
e b e
a m)
m=0
m=1
m=2
€
ωξ =ξωβ
η
Head-Tail Instability
ObservationGrowth ratemode=0
Head-Tail Instability
Cure
Chromaticity control
Landau damping by octupole magnets …
Beam response and Landau dampingCoasting beamTransverse motion
€
Single particle oscillating at ω.
External driving force is on at t=0.
˙ ̇ x +ωx=AcosΩt
x(t >0) =−A
Ω2−ω2(cosΩt−cosωt), ω≠Ω
x(t >0) =−AtΩ
(cosΩt−cosωt), ω=Ω
Beam response and Landau damping
€
Magenta: x(t)=−A
Ω2 −ω2(cosΩt−cosωt),
Ω =1.1ω
Driving force
Response
€
Blue: x(t)=−AtΩ
SinΩt,
Ω =ω
€
Red: f(t)=AcosΩt
Driving force
Response of the beam
Absorbed power by the beam
The beam: ensemble of the particlesFrequency distribution:
The beam motionapproaches steady oscillation.
Velocity d<x>/dt: in phase with the forceWork is done on the beam
Absorbed power by the beam: constantStored energy in the beam:
Macroscopic aspect: a beam driven by a force approaches steady oscillation.
Microscopic aspect: Small amount of resonant particles grows infinitely large.
€
∝ tResponse of particles
Longitudinal instabilityMicrowave Instability uniform distribution
Wake: V=Z (z)The seed of density modulation is produced
V1= Z (z), slippage,
Landau damping by the spread of rev =p/p phase slippage factor = 1/t
21/2
t phase transition energy
p/p
p/p
p/p
p/p
Density modulation reduced! Larger p/p more stable
Microwave Instability
Observation & simulation
K. Takayama et al., Phys. Rev. Lett. 78 (1997) 871
Microwave Instability
Sources: Narrow-band resonances
res ~ 1GHz
Cures
Reducing Impedance
Landau dampingReducing local beam chaege line density
Artificial increasing momentum spread
p/p > rev
MethodsHigher harmonic rf cavity
Voltage modulation of foundamental rf cavity
…
Cures
Reducing Impedance Exchange ~ 2/3 BPMs new ESM BPM
~2/3 Pump port new one with slits
Growth rate reduction
Reducing local beam chaege line density
Increasing momentum spread > rev
Voltage modulation of foundamental rf cavity
T. Toyama, NIM A447 (2000) 317
BeyondImpedance calculationImpedance measurements
Beam transfer function
Vlasov equationCoupled bunch instability
Mode-coupling instability
Electron-cloud instabilityfeedback system
feedback in RF control system
feedback damper = pick-up & kicker
“… every increase in machine performance has accompanied by the discovery of new types of instabilities.” - J. Gareyte (CERN)
References
Schools:CAS, USPAS, and OHO (Japanese)
Conferences proceedings:APAC, EPAC, and PAC
Textbook etc.:• A. W. Chao, PHYSICS OF COLLECTIVE BEAM
INSTABILITIES IN HIGH ENERGY ACCELERATORS• Editors: A. Chao and M. Tigner, Handbook OF
ACCELERATOR PHISICS AND ENGINEERING
Good Luck!