details of space charge calculations for j-parc rings
DESCRIPTION
Details of space charge calculations for J-PARC rings. KEK Portion. JAERI Portion. J-PARC accelerator complex. Phase 1 + Phase 2 = 1,890 Oku Yen (= $1.89 billions if $1 = 100 Yen). Phase 1 = 1,527 Oku Yen (= $1.5 billions) for 7 years. JAERI: 860 Oku Yen (56%), KEK: 667 Oku Yen (44%). - PowerPoint PPT PresentationTRANSCRIPT
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Details of space charge calculations for J-PARC rings
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J-PARC accelerator complex
– Phase 1 + Phase 2 = 1,890 Oku Yen (= $1.89 billions if $1 = 100 Yen).
– Phase 1 = 1,527 Oku Yen (= $1.5 billions) for 7 years.– JAERI: 860 Oku Yen (56%), KEK: 667 Oku Yen (44%).
JAERI Portion
KEK Portion
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Repetition of 3GeV Synchrotron
• injection 500μs• injection turns ~350• particles per pulse 8.3e13
• acceleration 20 ms
• extraction <1μs
injection
extraction
acceleration
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Repetition of 50 GeV Synchrotron
• injection 0.17s• particles per pulse 3.3e14
• acceleration 1.96 s
• extraction (slow) 0.7sinjection
extraction
acceleration
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Two approaches
• A whole cycle of 3 GeV synchrotron takes 20 ms.– Full simulation with self-consistent model is possible.– Tracking parameters (# of macro particles, grid size, etc)
have to be optimized.
• Only injection period of 50 GeV synchrotron takes 0.6 s (or a bit less).– Not realistic to make self-consistent simulation.– Frozen space charge model might be justified because of well defi
ned particle distribution.
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Examples of full tracking for 3GeV Syn.
Different colors shows results of differentnumber of macro particles.
Things are included.• Injection painting• Multipole errors• Misalignment• Acceleration• Aperture of all elements• Image in a circular pipe
3 months (100,000)
5 weeks (50,000)
2 weeks (20,000)
Results within 3 months (1,000,000~200,000)
Things are not included.• Scattering at foil.• RF jitter• Impedance
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Other tracking parameters
Number of azimuthal mode
Number of z grids
Max. mode= 4, 8, 16
z grids= 10, 20, 30, 40, 50
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Detailed study results
• Correlated and anti-correlated painting• COD and beam loss
– Coupled with strong chromaticity correction sextupole, COD introduces nonlinearity of all harmonics.
• Beam intensity dependence
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Correlated and anti-correlated painting
There is particle loss even during injection period.
correlatedanti-correlated
0.5 s for injection
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Phase space density right after injection and at 3 ms later
horizontal vertical
at 0.5 ms
at 3 msat 3 ms
at 0.5 ms
correlatedanti-correlated
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COD and beam loss
rms COD 0 mm 0.2 mm 0.5 mm 1.0 mm
Coupled with strong chromaticity correction sextupole, COD introduces nonlinearity of all harmonics.
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Phase space density for different COD
• No difference in core density.• Tails are developed with COD.
rms COD 0 mm 0.2 mm 0.5 mm 1.0 mm
rms COD 0 mm 0.2 mm 0.5 mm 1.0 mm
Hor. Ver.
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Beam intensity dependence
30mA
20mA
cf. 30mA is design value which deliver 0.6 MW beam from RCS with tune spread of ~0,25.
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Intensity dependence
• Core density is reduce with 30 mA. (lower order resonance is involved?)• Tails are also developed.
20mA30mA
20mA30mA
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Summary of self-consistent simulation
• A whole cycle of 3 GeV Syn can be simulated even though it takes a few months.
• Horizontal and vertical coupling is the source which makes anti-correlated painting worse.
• Increase of particle loss due to larger COD is attributed to tail development. Higher order effects are involved.
• Intensity limitation may be explained with lower order resonance. That is a regime where coherence picture is applicable.
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Example of beam loss during injection with frozen space charge model
Model assumes• Particle distribution is Gaussian.• Emittance is constant.• dp/p is finite and there are synchrotron oscillations.• Transverse space charge force depends on longitudinal position.
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Tracking model
• “Frozen model” of space charge is adopted.– Space charge potential is fixed throughout a tracking.– No self-consistency.– No coherent oscillations.– Gaussian charge distribution in 3D is assumed.
• Lattice nonlinearities and misalignment errors are included.• Aperture of magnets and collimator are included so that we can
estimate beam loss.• Macro particles (1,000) of 3D Gaussian distribution with 2 sigma
cut are tracked for 0.12s (original design value for accumulation) or more.
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Some numbers
• Emittance(2sigma) 54 pi mm-mrad (36pi, 45pi, 64pi)
• Acceptance at collimator 71 pi mm-mrad for H and V• Acceptance at magnets > 81 pi mm-mrad• Circulating current 10 A (3.3E14 ppp)• Incoherent tune shift -0.16• Bare tune (22.42, 20.80)
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COD
• Chromaticity sextupoles coupled
with COD introduce beta modulation
and higher harmonics of nonlinearity.
• Survival at 0.12s after injection.
• COD shows a rms value.
Maximum is about 3 times.
• Collimator aperture is adjusted
taking a local COD into account.
• We expect COD(rms) is less than
0.5mm after correction.
• The loss is not linear as COD.
sur
viva
l at 0
.12s
(%)
80
85
90
9
5
10
0
0 0.5 1.0 1.5 2.0 COD (rms) (mm)
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Different lattices
• Although rms COD is almost same,
different lattices (seeds) give
different results.• Previous example is the worst
case among three.
sur
viva
l (%
)96
97
9
8
99
10
0
0 0.05 0.1 time (s)
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Beam current
• The pattern of COD is the
same for both. Magnitude is
different.
• The design current is 10A.
Blue: COD=0.5mm
Red: COD=1.0mm
sur
viva
l at 0
.12s
(%)
80
85
90
9
5
10
0
0 5.0 10 15 beam current (A)
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Initial emittance
• Acceptance at collimator is fixed at
71 pi mm-mrad.
• Space charge force is fixed according
to the initial emittance.
• We expect 54 pi mm-mrad emittance
shaped at the 3-50BT collimator.
• Collimator acceptance should be
optimized to have the maximum
survival.
sur
viva
l at 0
.12s
(%)
80
85
90
9
5
10
0
30 40 50 60 70 80 initial emittance (pi mm-mrad)
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Location of loss
COD Magnet acceptance
Collimator acceptance
Initial emittance
Loss at collimator
Loss at magnet
Total number
0mm > 81 pi
mm-mrad
71 pi
mm-mrad
54 pi
mm-mrad
3 (100%) 0 (0%) 3/1000
0.2 > 81 pi 71 pi 54 pi 4 (100%) 0 (0%) 4/1000
0.5 > 81 pi 71 pi 54 pi 11 (92%) 1 (0%) 12/1000
1 > 81 pi 71 pi 36 pi 33 (97%) 1 (3%) 34/1000
1 > 81 pi 71 pi 45 pi 33 (92%) 3 (8%) 36/1000
1 > 81 pi 71 pi 54 pi 21 (88%) 3 (12%) 24/1000
1 > 81 pi 71 pi 64 pi 59 (88%) 8 (12%) 67/1000
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Beam loss at collimator (h=18)total 0.72 MW
COD 0 mm 0.2 mm 0.5 mm
Loss 670 W 800 W 1370W
COD (rms) = Red: 0mm Yellow: 0.2mm Green: 0.5mm
1000
980
960
940
920
900
survival
0.60.50.40.30.20.10.0
time [s]
All the particles hit collimator first.
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Beam loss at collimator (h=18)total 0.58 MW
COD 0 mm 0.2 mm 0.5 mm
Loss 350 W N/A 690 W
COD (rms) = Red: 0mm Yellow: 0.2mm Green: 0.5mm
1000
980
960
940
920
900
survival
0.60.50.40.30.20.10.0
time [s]
All the particles hit collimator first.
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Frozen model with acceleration
phis
bunch length dp/p
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300
280
260
240
220
200
2.52.01.51.00.50.0-0.5
horizontal vertical
300
280
260
240
220
200
2.52.01.51.00.50.0-0.5
horizontal vertical
1000
990
980
970
960
950
940
1.51.00.50.0-0.5
1000
990
980
970
960
950
940
1.51.00.50.0-0.5
99% emittance and beam loss
Acceleration starts right after injection.
Acceleration starts at 0.16 s after injection.
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300
280
260
240
220
200
2.52.01.51.00.50.0-0.5
horizontal vertical
1000
990
980
970
960
950
940
1.51.00.50.0-0.5
Acceleration starts at 0.6 s after injection and h=18.
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Single particle behavior
• Tracking without aperture limit
to see single particle behavior.
• Slow growth of amplitude.• Not obvious correlation with
synchrotron oscillations. Trapping?
Timing ofhitting collimator
0 0.01 0.02 0.03 0.04 0.05 time (s)
hori
zont
al p
osit
ion
(m)
-0.1
-0.0
5
0
0.5
0
0
.1
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Single particle behavior
• Track a single particle which is lost in 0.6 s.• Look at betatron oscillation amplitude and transverse tune as a f
unction of turn until a particle is lost.
• For example, there are– 38 lost particles (out of 1000) when rms COD is 0mm.– 40 lost particles (out of 1000) when rms COD is 0.2 mm.– 52 lost particles (out of 1000) when rms COD is 0.5 mm.
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#1 #2 #3
#5 #6#4
H
V
H
V
turn number (~ 10,000 turns)
ampl
itud
e
rms COD is 0.5 mm
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H
V
H
V
#7 #8 #9
#11 #12#10
turn number (~ 10,000 turns)
ampl
itud
e
rms COD is 0.5 mm
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H
V
• Horizontal amplitude always increases and gets to the aperture limit.• Vertical amplitude always decreases. Coupling between H and V is manifest.
#16
#15#14#13
H
V
turn number (~ 10,000 turns)
ampl
itud
e
rms COD is 0.5 mm
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In tune space
Blue points are intermediatetune of lost particles.Red points are tune just beforeparticles are lost.
Tune before particle loss aresame with and without COD.
2x-y=24
x-2y=-19
bare tune
x-22 x-22
y-2
0
y-2
0
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Coupling between H and V is manifest, but
• Tune space plot does not show resonance driving term.– 2x-y=24 is skew and cannot be excited even with finite dp/
p and dispersion in a lattice.• If there is any way to reduce a driving term.
– Since the source is not identified, it is difficult.
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Summary of frozen space charge simulation
• Particle loss occurs because horizontal amplitude increases and hits the collimator aperture. The source of the increase is a coupling between H and V.
• With finite COD, particle loss occurs with less turns. However, transverse tune when a particle loss occurs does not depend on COD magnitude.
• Loss is very slow process: the order of 104 turns. Time scale of horizontal and vertical coupling is also same order.
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Basic loop of calculation
Advance particle coordinatesdo ip=1,np (200,000)
Calculate space chargepotential based onparticle positions.
do imode=1,nmode (16)
Apply space charge kicksto all particles
do ip=1,np (200,000)
Simpsons uses Fourierexpansion in azimuthaldirection.
Make parallel processingof Fourier modes.
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Distribution of workload (4 CPUs) with MPI
imode=3,4,5,6
imode=0,1,2
imode=7~11
imode=12~16
Add up all E-fields4 CPU worksin the same way