brookhaven science associates nsls-ii injection system t. shaftan nsls-ii accelerator systems...
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BROOKHAVEN SCIENCE ASSOCIATES
NSLS-II Injection System
T. ShaftanNSLS-II Accelerator Systems
Advisory Committee
October 11, 2006
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Contributors
• I. Pinayev, • J. Rose, • J. Skaritka,• R. Heese,• C. Stelmach,• S. Pjerov• S. Sharma,• L.H. Yu• T. Shaftan
• G. Ganetis,
• D. Hseuh,
• N. Tsoupas,
• W. Meng,
• J. Beebe-Wang,
• A. Luccio,
• D. Raparia
• D. Wang
• J. Safranek,• L. Emery,• W. Joho
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Outline
• NSLS-II injection requirements• Considerations for injection system• Injection straight arrangement and
simulations• Low energy accelerator• Booster• Transport lines• Concluding remarks
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Requirements for NSLS-II Injection
• High reliability• Reasonable fill speed• Low losses• Low power consumption
• Lifetime 3 hours (with 3rd HC)• Top-up
Stability of current <1 % Time between top-up injections
>1 min Bunch-to-bunch variations of
charge <20%
Ī
t
Īt
QI
t
Ib
bunch #
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Ring parameters related to injectionParameter Value
Energy, GeV 3
Circulating current, A 0.5
Circumference, m 780
Revolution period, s 2.6
RF frequency, MHz (wavelength, m) 500(0.6)
Circulating charge, C 1.3
Total number of buckets 1300
Number of filled buckets 13004/51040
Charge per bucket, nC 1.25
Lifetime, hours 3
Interval between top-up cycles, min 1
Current variation between top-up cycles, % 0.55%
Charge variation between top-up cycles, nC 7.15
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Injection ScenarioNM=20-100
Injected bunch train
#
Ring bunch pattern
t
t1st turn 2nd turn 3rd turn
Ib
kicker
• Many (~1000) bunches in the ring multi-bunch injection NM bunches in injected train Filling NM consecutive buckets in
the ring Sequentially shift injection timing
• 1 Hz repetition rate suffices with pulse train injection
• 1 minute between top-up cycles
• Kickers duration can be 2 turns long (5 sec) or even longer
• Considered in ALS top-up (10 bunches)
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Injection straight design8 m
Fla
g
Fla
g
Fin
al
Septu
m
Kic
ker
1
Kic
ker
2
Kic
ker
3
Kic
ker
4
Quad
Quad
Stripline for transversefeedback
Stripline for transversefeedback
Ring Injection Kickers (4)
Field, T 0.193
Length, m 0.75
Angle, mrad 14.4
Current Amplitude, kA 5.34
Voltage, V 4500
Temporal shape 5 μsec ½ sine wave
Pre-septum magnet
Field, T 1.1
Length / Angle, m / mrad 0.75 / 83
Peak current/voltage, kA/kV 12/0.6
Pulse shape 100 μsec ½ sine wave
Final Injection Septum
Field, T 0.9
Length / Angle, m / mrad 0.5 / 45
Peak current/voltage, kA/kV 10/0.6
Pulse shape 60 μsec full sine waveI. Pinayev and R. Heese
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Requirements on Ring Stay-Clear• Tracking is done with TRACY-2
• Tracking a set of particles corresponding to injected beam
• • Tracking for 500 turns
• Beam envelope is recorded at every ring turn on every element
• Tracking for 10, 50, 100 nm• • Black envelope: scaled septum
aperture for horizontal
• Scaled undulator gap for vertical
• Conclusion: stay-clear required for injection can be easily met
J. Rose, I. Pinayev and J. Bengtsson
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NSLS-II injector
Linac200 MeV
Th. Gun100 keV
3 GeV
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Low-energy accelerator• Specifications for NSLS-II linac:
• Energy 200 MeV, energy spread <0.5% RMS,
emittance ~100 nm at 200 MeV
• Defined by small vacuum chamber in the booster
• Soleil linac:
10 nC in 300 ns at 100 MeV Energy spread <0.5% RMS Emittance ~40 mm mrad Beam loading compensation
• Fits NSLS-II requirements• Turn-key system
Soleil linac
Measured bunch train along the linac
from: A. Setty et al., Commissioning of the 100 MEV …
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Layout of 200 MeV linac
• 5 linac sections• 3 klystrons• With loss of one klystron: 177 MeV
J. Rose
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Linac-to-booster Transport Line
• Length: 19 meters 2 dipoles, 8 quadrupoles, 4 correctors Energy spectrometer Safety shutter Flags, BPMs Loss monitors• Diagnostics set-up sufficient
for commissioning of the linac
fromlinac BQ
BQ
kicker
QD
1
QD
2
QD
3
QD
4QF
1
QF
2
QF
3
QF
4B1
trim
s
trim
s
trim
s
B2
trim
fromlinac BQ
BQ
kicker
QD
1
QD
2
QD
3
QD
4QF
1
QF
2
QF
3
QF
4B1
trim
s
trim
s
trim
s
B2
trim
I. Pinayev
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Booster: design considerations
“Compact” booster “Same tunnel” boosterBuilding and shielding are very expensive
Higher cost for vacuum, diagnostics
Ability to commission booster in advance
OK, based on the SLS experience
Ability to service and troubleshoot without beam interruption
Lifetime is 3 hours Average hardware failure leads to stop anyway
“Conventional” design Higher beam quality, relaxed tolerances
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Booster location
• Mounting on the ceiling
No expanding tunnel
No transport lines blocking tunnel pathway
No magnets above ring straights
No water-cooling for magnets
Cross-talks?
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Booster parametersParameter NSLS-II SLS
Energy range [GeV] 0.2 – 3.0 0.1 – 2.4
Circumference,[ m] 780 270
Emittance [nm] 11.5 9
Repetition rate [Hz] 1 3
Radiation loss per turn [keV] 500 233
RF frequency [MHz] 500 500
Magnet power [kW] 75.3 150
RF voltage [MV] 1.0 0.5
RF acceptance [%] 1 0.43
Beam current [mA] 3 1
Momentum compaction 5.7·10-4 5·10-3
Tunes [x / y] 19.19 / 10.73 12.41 / 8.38
Chromaticity [x/y] –21.7 / –21.7 –15 / –12
Damping times [ms] (x / y / E) 22 / 31 / 19 11 / 19 / 14
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Booster lattice
Dynamic Aperture
• Modified NSLS booster lattice
• 60 combined function dipoles
• 90+6 quadrupoles
• 15+15 sextupoles
• 60 X-Y correctors
• 75 BMPs for orbit correction, rms orbit < 1mm
• Dipole field 0.7 T at 3 GeV
• Large dynamic aperture
• Negligible eddy current effect at 1Hz
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Booster magnets• Magnets are located above
storage ring
• Use of air-cooled coils
• Small size of vacuum chamber small magnet size and weight
• Small power consumption
• Relaxed tolerances on magnet alignment and field errors
• Simple design of support hangers
• Quadrupoles and sextupoles: standard and compact design
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Booster Magnet Power Supplies and RF• In series circuits:
B-PS – 60 dipoles Q1-PS – 60 quadrupoles Q2-PS – 30 quadrupoles SF-PS – 15 sextupoles SD-PS – 15 sextupoles
• Separate circuits:
60 horizontal trims 60 vertical trims 3 x 2 quadrupole trims
• All power supplies can operate at 1 Hz
• Programmable ramping profiles
• Synchronization from line voltage
G. Ganetis
J. Rose• RF voltage ramps to 1 MV • Energy acceptance 1% at 3 GeV• Total RF power 37 kW• Single 5-cell PETRA cavity• Capable of delivering 1.5 MV• IOT transmitter 80 kW at 500 MHz
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1.E-09
1.E-08
1.E-07
1.E-06
0 2 4 6 8 10 12 14 16 18 20 22 24 26
Longitudinal Distance (m)
Pre
ssur
e (T
orr)
q(t) = 1e-10 Torr.l/ sec.cm̂ 2
η = 1e-3 mol/ photon
I e = 3 mA
P
S (P) = 30 l/ s
Pavg = 1.5e-7 Torr
S (P) = 100 l/ s
Pavg = 1.3e-7 Torr
P PP
DD
D
P
Booster vacuum• Target average value 1E-7
• Gas-scattering losses throughout energy ramp 0.5%
• Vacuum chamber provides with > 10xRMS beam sizes in both planes
• 2 sizes of vacuum chamber: 20x30mm2 in dipoles 25x40mm2 in dispersive
straights
• 5 pumps per superperiod = 150 pumps total
• Pumps in RF and injection/extraction straights
D. Hseuh
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Booster-to-Storage ring Transport Line• Consists of 3 parts
– Horizontal achromat– Vertical dogleg– Horizontal achromat
• Doublets for optimizing -functions without disturbing -functions
• Maintain small beam size along the transport line
• Magnets / diagnostics: 4 dipoles, 17 quadrupoles, 6 trims, 6 BPMs, 6 flags, 2 ICTs
C. Stelmach, S. Pjerov
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Concluding Remarks• We designed reliable and robust NSLS-II injection
system
• Conceptual design of NSLS-II injector Linac will be purchased, turn-key + some R&D? “Same tunnel” booster Transport lines: sufficient diagnostics for step-by step
commissioning• Storage ring:
Sufficient dynamic aperture for injection Sufficient stay-clear for injection Injection kicker system will be purchased, turn-key
• Future work: Optimization of injector design/cost tracking in realistic scenario, injection tolerances Consider Lambertson septum