1 brookhaven science associates considerations for nonlinear beam dynamics in nsls-ii lattice design...
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1 BROOKHAVEN SCIENCE ASSOCIATES
Considerations for Nonlinear Beam Dynamics in NSLS-II lattice design
Weiming Guo
05/26/08
Acknowledgement:
J. Bengtsson S. Kramer S. Krinsky B. Nash
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Outline
Method:
Simulation using Elegant
1. Introduction to the linear lattice
2. Nonlinear requirements: injection and Toschek scattering
3. Minimum needed sextupole families
4. Required physical aperture
5. Effects of the multipole field errors
Subjects will not be covered:
On-going optimization of the nonlinear lattice;
Misalignment errors; choice of the working point;
and effects of the damping wigglers and IDs
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Main Design Parameters
Beam Energy 3 GeV
Circumference 792 m
Circulating current 500 mA
Total number of buckets 1320
Lifetime 3 hours
Electron beam stability 10% beam size
Top-off injection current stability <1%
ID straights for undulators >21
Straight length 9.3/6.6 m
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Magnets and lattice
Quad. Family: 8, 10 magnets per cell
Sext. Family: 9, 10 magnets per cell
Chromaticity per cell: -3.4/-1.4
0
0.5
1
1.5
2
2.5
200 400 600 800 1000 1200 1400
Total Radiated Energy [KeV]
Em
itta
nc
e [
nm
]
Natural emittance with 0, 1, 2, 3, 5 and 8 DWs added
Courtesy of S. Kramer
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Linear Lattice design approaches
1. Large bending radius enhances the effect of the damping wigglers
2. Strict double-bend-acromat
sin'
)cos1(,25,4.0
x
x
D
DmTB
Two reasons NSLS-II is sensitive to the residual dispersion:
• 1nm emittance. For βx =2 m, ηx=4.5 cm, βxεx~(ηxσδ)2
• Damping wiggler has quantumn excitation effect
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Nonlinear Design Goal
1. Sufficient dynamic aperture (>11mm) for injection
On momentum particle
Sep
tum
Bum
ped
stor
ed b
eam
Inje
cted
bea
m
(σx=
0.39
mm
, σ´ x
=77
μra
d)
3+1
mm
3.5
mm
1+1.
2 m
m
(σx=
0.15
mm
)
2. Sufficient dynamic aperture to keep Touschek scattered particles with δ= ±2.5%
Off momentum particle
Minimum required dynamic aperture
δ
Courtesy of I. Pinayev
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Source of the nonlinearity
yx
yx
J ,
,
d
dh
d
dh
Dh
h
h
y
x
y
x
00201
20001
)2(10002
)1(00111
)1(11001
Frist order chromatic terms (5)
yx
yx
x
x
x
h
h
h
h
h
2
2
3
10200
10020
10110
30000
21000
Frist order geometric terms (5)
Amplitude tune dependence
Second order chromaticity
}][{8
1
2
1
}][{8
1
2
1
)1(21
)2(2
)1()2(
)1(21
)2(2
)1()2(
d
dDKKDKds
d
dDKKDKds
yyyy
xxxx
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Number of chromatic sextupole families
)2||2cos()()2sin(2
)2||2cos()()2sin(2
)|cos(|)sin(2
)|cos(|)2
()sin(2
)1(21
)1(21
)1()1(1
)1(
)1()1(21
)1()2(
yyy
xxx
x
DKKdsd
d
DKKdsd
d
cDdsKD
DDK
KdsDD
yxyx DdsK ,)1(
2,)1(
Conclusion:
Because the betatron phase advance in the dispersive region is small (x: ~ 10o, y~ 20o),
the five chromatic terms have only two degree of freedom. 7~8 sextupole families
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Stay-clear aperture
38x12.5 mm
)()()()(
00.... s
ssxsx ococ
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Dynamic Aperture with Multipole Error
Magnet Type
Magnet Aperture(mm)
Multipole Order
Relative Strength (x10-4)
Quad 66 6 1
Quad 66 10 3
Sext 68 9 1
Sext 68 15 2
DA collapse at negative momentum
The Feb.-08 multipole components at 25 mm
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Effects of Multipoles
Conclusion:
introducing systematic
multipole errors doesn’t add
resonance lines.
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Amplitude Tune Dependence
Conclusion: Multipole terms changes the tunes at large
amplitude dramatically, and makes the stable area smaller.
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Why Negative Momentum?
nnxx
n
noc
n
n
n
noc
noc
oc
yM
JxC
xxCxxx
xxx
yxxx
B
BH
cos)2(
)(
...)45(!10
11
2/10
0
10..10
10
0
10..10
10..
10
..
28109
9
,cos)2(!10
11 15
1
2210..
2109
9
1010
kx
k
kkkoc
ky
x
JxkCx
B
B
HJ
,cos)2(
!10
11
15
1
2210..
210
9
9
1010
kx
k
kkkoc
k
y
x
JxkC
x
B
B
HJ
xxx
yxxx
B
BH
oc
y
..
28109
9
10 ...),45(!10
11
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Minimizing 2nd Order Dispersion
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Tune Scan
Conclusion: moving the tune doesn’t solve
this problem.
Delta = -3.0%
Delta = 3.0%
Delta = 0.0% Delta = -3.0%
Area of DA
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Squeeze the Tune Excursion
Tunes moved, sextupoles reoptimized
CDR lattice with multipole errorsRed: Jan4th lattice
Black: re-tuned lattice
The re-tuned lattice
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New Specifications
Magnet Type Magnet Aperture (mm)
Multipole Order Relative Strength (x10-4)
Quad 90 6 1
Quad 90 10 0.5
Quad 90 14 0.1
Sext 76 9 0.5
Sext 76 15 0.5
Sext 76 21 0.5
Multipole components of high precision magnets (25 mm)
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Summary
•Nonlinear design goal to provide sufficient dynamic aperture for injection and Touschek scattered particles up to δ=2.5%
•There are 8 sextupole families in the lattice, one more might be added.
•The physical aperture is conservatively retained.
•The reduction of the dynamic aperture due to multipole errors is show to be the momentum related tune shift with amplitude.
•Identified the multipole errors in the high dispersion region, and required increasing the pole radius.
•Further optimization of the dynamic aperture is proceeding.