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High-Power Proton Drivers
Alessandro G. RuggieroBrookhaven National Laboratory
FFAG 03 KEK International Center
Japan, July 7 - 11, 2003
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 2
There are several Applications that require High-Power Proton Drivers
Nuclear Physics FacilitiesSpallation Neutron SourcesProduction of TritiumNuclear Waste TransmutationEnergy ProductionLong-Baseline Neutrino OscillationNeutrino FactoriesMuon Colliders…
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 3
Accelerator Technology
Rapid Cycling Accelerators
Accumulator Rings
Cyclotrons
Fixed-Field Alternating Gradient
Linear Accelerators (Room Temp.)
Linear Accelerators (SuperCond.)
Induction Linear Accelerators
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 4
Nuclear Physics FacilitiesEHF, AHF, JHF, TRIUMPF II, …
RT Linac 1.2 GeV 30-GeV Main Ring Targets
9-GeV Booster
Stretcher Ring
Typically 20-50 GeV
High-Rep Rate 5-30Hz
Intensity ~ 1013 protons/pulse
Average Power ~ 1-5 MW
AC Efficiency ~ few % (30-50 MW AC Power)
Cyclotron
Continuous Beam
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 5
AGS now and UpgradeAGS
presentAGS
upgradeSNS
Kin. Energy, GeV 28 28 1.0
Protons 1014 / Cycle 0.67 0.89 1.04
Rep. Rate, Hz 1/3 2.5 60
Ave. Power, MW 0.10 1.0 1.0
1.5-GeV Booster
28-GeV AGS200-MeVLinac
1.2-GeVSCL
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 6
Spallation Neutron Sources
Modes of OperationShort Pulse 1 - 2 µs
Long Pulse 1 - 10 ms
Continuous Source
RequirementsAround 1 GeV energy range
1 - 20 MW
> 1015 neutrons/ cm2 / s
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 7
Existing Facilities
LAMPF / LANSCERT Linac 800 MeV 60 Hz / 10 ms 1 MW
PSRAccumulator Ring SP 80 KW
ISISRCS 800 MeV SP 160 kW
ANL - IPNSRCS 500 MeV SP 10 kW
PSICyclotron 600 MeV CW 600 kW
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 8
Layouts
LANL-PSR
ISIS
PSI
70-MeV RTL
800-MeV RCS
Target
800-MeV RTLTarget
Accumulator
600-MeV CyclotronTarget
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 9
Oak Ridge SNS
1.3-GeV SCL injecting in Accumulator Ring
Hg -Target
Short Pulse Mode 1.5 µs
Average Power 1.3 MW
Repetition Rate 60 Hz
Design Requirement: Uncontrolled Losses < 10–4 (< 1 W/m)
1-ms Pulse Duration
SCL Linac
RT Linac
Accumulator
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 10
SuperConducting Linacs (Pulsed)
Medium Front End Low-Energy Energy High-Energy
RT Linac Section Section Section To the AGS
201.25 MHz 805 MHz 1,610 MHz 1,610 MHz
200 MeV 400 MeV 800 MeV 1.2 GeV
Front End Medium-Beta High-Beta DTL CCL Section Section To the SNS
402.5 MHz 805 MHz 805 MHz 805 MHz
185.6 MeV 387 MeV 1.0 GeV
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 11
Proposed Neutron Sources
ESS
BNL-PSNS
1.3-GeV SCL
Double Ion Source Compressor Ring
Targets
2 x 2.5 MW @ 50 Hz
600-MeV RTL 30-Hz RCS
Targets
2 x 2.5 MW @ 60 Hz3.6-GeV RCS
100 mA H–
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 12
Accelerator-based Continuous Neutron Source
Layout of Front End
Ion Source RFQ Buncher10 mA 350 MHz 350 MHz
to 200-MeV RT Linac
35 kV 750 keV
Layout of the SCL for the ACNS
Medium Front End Low-Energy Energy High-Energy
RT Linac Section Section Section To the Target
700 MHz 700 MHz 1,400 MHz 1,400 MHz
200 MeV 400 MeV 800 MeV 1.25 GeV
Side View of SCL
Target Area
Klystron Gallery
30-40 ft Cryo-Plant Service Buildings Beam Dump
Linac Tunnel Transport
SNS AGSUpgrade
ACNS
Kinetic Energy, GeV 1.0 1.2 1.25Ave. Power, MW 1.0 0.045 10Duty Factor, % 6.0 0.18 100Repetition Rate, Hz 60 2.5 --Pulse Length, ms 1.0 0.72 --Peak Power, MW 16.7 25 10Ion Source Current, mA 35 35 10Ave. Beam Current, mA 1.0 0.035 8Peak Beam Current, mA 26 21 8Protons / Bunch, x 108 4.3 8.7 1.43RF, MHz 805 805 – 1,610 700 – 1,400Coupler RF Power, MW 170 - 350 260 - 400 80 - 155Length, m 158 120 163Inj. Energy, MeV 185.6 200 200Cryo. Power (2.1oK), kW 0.5 0.15 5.3Ave. AC Power, MW 3.1 0.28 23Ave. Gradient, MV/m 3.1 – 6.5 5.3 – 10.0 3.3 – 8.7Efficiency, % 26 - 30 9 - 16 35 - 40Cost, M$ 110 97 85Operation Cost, M$ / yr 2.0 0.18 15.2
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 13
Cyclotrons
DeeDee
DeflectorDeflector
Trajectories get densier at Extraction
Step given by Energy Gain
RF Source
Energy & Power Limitation to avoid Activation
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 14
Fixed-Field Alternating Gradient Accelerator
Constant Field Sector Magnets
Large Aperture (~ 1m)
Edge Focusing
Injection from low-energy Linac
Multiturn-Injection (H–)
Space Charge (losses)
Adiabatic Capture & Acceleration
Motion spirals outward
Parking and Stacking Orbit
Extraction with Septum/Kicker
B1 B2
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 15
Induction LinacNo RFSequence of High Power TransformersMoving DC Current (Field) Pulse
Large Transverse Aperture (60 cm)Short Beam Pulse (< 1 µs)High beam Pulse Current (> 100 A)High Repetition RateLow Accelerating Gradient (< 1 MV/m)
Switches
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 16
Induction Linac - FFAG
Induction Linac
FFAGAccelerator
Positive Ion Source
•High-Intensity Short Pulse
•Positive Ions
•One-Turn Injection (No Foil Stripping)
•No Accumulation
•No Stacking
•Reduced Concern of Uncontrolled Activation
A.G. Ruggiero, G. Bauer, A. Faltens, R. Kustom, S.A. Martin, P. Meads, E. Zaplatin, K. Ziegler
ICANS-XIII, Villigen PSI, Switzerland
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 17
Induction Linac – FFAG Injector Parameters
Ave. Beam Power 5 MW
Rep. Rate 200 Hz
Final Energy 1 GeV 3 GeV
Ave. beam Current 1.25 mA 0.42 mA
Positive-Ion Source
Pulse Length 2 µs
Duty Cycle 0.04 %
Peak Current 12. 5 A 4.2 A
Norm. Emittance 30 π mm mrad 10 π mm mrad
Induction Linac
Final Energy 260 MeV 600 MeV
Final Pulse Length 0.15 µs 0.1 µs
Init. Acc. Gradient 36 kV/m
Final Acc. Gradient 1 MV/m
Total Length 380 m 720 m
Int. Core Diameter 60 cm
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 18
Induction Linac – FFAG FFAG Accelerator Parameters
Final Energy 1 GeV 3 GeV
Injection Energy 260 MeV 600 MeV
Circumference 200 m 200 m
Packing Factor 40 % 40 %
Bending Radius 12.74 m 12.74 m
Bending Field 1.95 - 4.44 kG 3.19 - 10.01 kG
Momentum Aperture ±40 % ± 50 %
Max. Dispersion 2.0 m 2.0 m
Max Function 20 m 20 m
Magnet Aperture 1.6 m 2.0 m
Magnet Gap 30 cm 20 cm
Space-Charge 0.3 0.3
Norm. Emittance 400 π mm mrad 220 π mm mrad
Acceleration Period 5 ms 5 ms
Harmonic Number 1 1
RF Frequency 0.93 - 1.31 MHz 1.19 - 1.46 MHz
RF Peak Voltage 400 kV 600 kV
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 19
Multi-Cavity Proton Cyclotron AcceleratorChangbiao Wang, V.P. Yakovlev, J.L. Hirshfield, PAC’03, Portland (OR)
Stage 1 2 3 4 5 6 7 8
RF, MHz 120 112 104 96 88 80 72 64
Radius, cm 92 98 106 110 120 132 144 172
Length, m 206 223 239 281 307 338 392 389
E, MeV 63.6 92.9 80.9 96.1 124.3 135.3 177.0 182.7
952.7 MeV1 MeV
I-peak = 0.915 A I-ave = 0.122 A Beam Radius = 0.9 mm Pulse Period = 125 ns Duration = 16.7 ns Energy Spread = 1.2 keV
TE111
Solenoid Field = 8.1 T
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 20
Accelerator for Production of Tritium(and Nuclear Waste Transmutation)
RT Linac 700-MHz, 4-Cells, Doublet-Focusing SCL
100 MeV 260 MeV 1000 MeV
= 0.43 = 0.62 = 0.88
908 m
= 0.48 = 0.71
50 cm
50 cm
Target
Tungsten / SS
100 MW CW Proton Power
3/16 Tritium Production Goal (1995)
AC Efficiency 40% (250 MW AC-Power)
Thermal energy deposition has a limit (~10kW/cm2)
Shock thermal waves absent in CW mode
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 21
Energy Production
SCL are most AC efficient (~ 40%)Magnets require AC Power (10-20%)Large demand of AC Power of 10’s to 100’s MW
AC Power Limitation (Reactors?)Need of Energy recovery SchemeElectrons can be decelerated, but Protons are depleted on Targets
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 22
Energy Amplifier
Target
Cooling
Heat - Exchange
Steam Turbines
Electric Power Generator
Ion Source12 mA, CW
402.5 MHzRFQ
805 MHzDTLnormal-conducting
805 MHz SuperConducting Linac
0.1 GeV 0.3 GeV 1.0 GeV
10 mA
Power to drive Linac, 25 MW
External Load 400 MW
Facility, 5 MW
proton
1-3 GeV Source
Target is a granular mixture of inertial material (W or Pb) and of fissionable material (232 Th).Neutrons are initially produced by Spallation of the inertial material.Each spallation neutron initiates a chain reaction with the fissionable material, so that more neutrons are produced.Sub-critical Reactor k = 0.98
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 23
Long-Baseline Neutrino OscillationNeutrino FactoriesMuon Collider
proton X e±
µ±
π±
µ e
π
LBNO CERN-GSNL
Fermilab
BNL
Japan
NF CERN
ISIS
US Collaboration
µC International Collaboration
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 24
QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.
CERN - Gran Sasso
500 kW
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 25
BNL Homestake Super Neutrino Beam (28 GeV, 1 MW)
Fermilab (0.5 - 2 MW, 40 GeV primary proton beam)
2540 km
HomestakeBNL
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 26
8-GeV Fermilab SCL
(1) SNS Front-End @ 402.5 MHz
(2) DTL @ 402.5 MHz up to 87 MeV
(3) 805-MHz SNS type SCL in three sections ( = 0.47, 0.61, 0.81)
(4) 1.2 GHz “TESLA” cryomodules from 1.2 to 8 GeV ( = 1)
(1) (2) (3) (4) Main Injector
Active Length 671 m
Repetition Rate 10 Hz
Beam Current 25 mA
Pulse Length 1 ms
Beam Intensity 1.5 x 1014 protons / pulse
Linac Beam Power, Ave. 2 MW
Peak 200 MW
8 GeV
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 27
Collaboration Proposal of - Factory
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 28
Alternative Scheme for Neutrino Factory
a 15-GeV Proton Driver (PD),a π - µ Production Channel (πµPC), that is a solid target immediately followed by a transport channel made of a super-conducting 20-T solenoid magnet where the π mesons decay and the µ mesons are produced, an accelerating section consisting of a 2-GeV SCL with two re-circulating SCLs (µSCL) for the acceleration of the µ mesons to 32 GeV, and a 32-GeV muon Storage Ring (µSR), where the µ mesons circulate until they decay in neutrinos.No Ionization Cooling required
Proton Driver µ SC Linac & Re-circulators
π-µ Production Channel µ Storage Ring
Beam
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 29
15-GeV Proton Driver for -Factory PD Injector 2 GeV 3, 6, 9, 12, 15 GeV
PDRe-circulator
(4-passes)
4, 7, 10, 13 GeV
5, 8, 11, 14 GeVTarget
1 GeV SC Sector LinacsMode of Operation Continuous Wave (CW)Final Kinetic Energy 15 GeVAverage Proton Current 10 mAAverage Proton Power 150 MWSCL-Injector Energy 2 GeVSCL- Injector Frequency 201.25 MHz to 116 MeV
805 MHz to 400 MeV1.61 GHz to 2 GeV
Number of Passes in SCL-Sectors 4 (5 in the first Linac Sector)Energy Gain for each Pass 1 GeVFrequency of SCL-Sectors 1.61 GHzExtracted Beam Emittance 0.3 π mm-mrad (rms, norm.)Extracted Bunch Area 1.0 π MeV-degree at 1.61 GHzrms Momentum Spread < 1 x 10-4
rms Bunch Length < 1 mmBeam Bunching Frequency 201.25 MHz, 1 bunch every 8 rf buckets
at 1.61 GHzBunch Spacing 150 cm
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 30
Muon Acceleration 32-GeV Re-circulator
12-GeV Re-circulator
To µSR
2-GeV SCL
Mode of Operation Continuous Wave (CW)Final Kinetic Energy 32 GeVAverage Muon Current 2 x 0.14 mAAverage Muon Power 2 x 4.5 MWSCL-Injector Energy 2 GeVSCL- Injector Frequency 201.25 MHz to 800 MeV
805 MHz to 2 GeVEnergy of First Re-Circulator 12 GeVEnergy of Second Re-Circulator 32 GeVNumber of Passes in SCL-Sectors 3 (4 in the first Linac Sector of each
Re-Circulator)Energy Gain for each Pass 1 GeV for 1st Re-Circulator
2 GeV for 2nd Re-CirculatorFrequency of Re-Circulator Linacs 1.61 GHzExtracted Beam Emittance 122 π mm-mrad (full)Extracted Bunch Area 0.024 π eV-sMomentum Spread ±3 x 10-3
Bunch Length ±0.2 nsBeam Bunching Frequency 201.25 MHzBunch Spacing 150 cm
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 31
One FFAG Period
Packing Factor /R = 70 %
B (average) = 1.0 Tesla
FODO cells phase advance = 90o
E / turn = 5 MeV
Bunch Area = 2 π eV-µs
Momentum Spread = ± 2 x 10–3
Norm. Emittance (full) = 1 π mm mrad
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 32
Applications
AGS-SCL
PSNS SNS ACNS CERN EAAPT
NWT
Average Power
50 kW 5 MW 1.3 MW 10 MW 20 MW 10 MW 100 MW
Rep. Rate
2.5 Hz 60 Hz 60 Hz CW CW CW CW
Pulse Duration
0.7 ms 1.3 ms 1.0 ms -- -- -- --
InjectionEnergy
200 MeV 100 MeV 187 MeV 200 MeV 200 MeV 200 MeV 100 MeV
Ejection Energy
1.2 GeV 1.3 GeV 1.3 GeV1.25 GeV
2 GeV 1.2 GeV 1.2 GeV
Ave. Current
40 µA 4 mA 1 mA 8 mA 20 mA 8 mA 80 mA
Peak Current
30 mA 100 mA 35 mA 8 mA 20 mA 8 mA 80 mA
(FFAG)
0.025 0.083 0.029 0.0067 0.017 0.0067 0.067
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 33
FFAG (CW)
200 MeV 2.2 GeVNext Stage
Injector
Rep. Rate,
Intensity,
Pulse Length
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 34
FFAG Sector Geometric Design
2Dp2, r2, B2
p1, r1 , B1
F
D
B = B0 ( r / r0 )n p0 = B0 r0
B1,2 = B0 ( r1,2 / r0 )n p1,2 = B1,2 r1,2
r1,2 = r0 (1 ± D / r0) p1,2 = p0 (1 ± D / r0) n + 1
R = (p2 / p1) 1/(n+1)
G = (R + 1) / (R – 1)
r0 = D G
N = number of Sectors
= 2 (F – D) = 2 π / N
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 35
200 MeV - 2.2 GeV CW FFAG Design
FFAG Injection Ejection
Energy MeV 200 2200 (1500)
0.5662 0.9543
Momentum GeV/c 0.6444 2.9947
Magn. Rigidity T-m 2.1496 9.9892
kG 1.678 4.514
r m 12.81 22.13
Period Length m 11.16
Sector Length m 8.93
Drift m 2.23
Circumference m 346.01 (273.27)
- max m 38.11
- max m 6.12
p/p (half) % 0.2 0.02
a (full) mm 7.45 3.46
(full) mm 12.25 1.22
a + mm 19.70 4.68
E mm 83.92 10.71
400 turns = ~ 1 msec
B0 = 2.76 kGn = 109 (76)D = 10 cmLF / LD = 3Pack. Fact. = 0.8 / period = 0.25N = 31E = 5 MeV / turnnorm, full = 1 π mm mrad
DFD lattice with thin-lens calculation to derive , ,
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 36
AGS UpgradeRT Linac: 200 MeV
1 π mm mrad2 π eV-µs± 0.2 %30 mA2.5 Hz (5 Hz)0.7 m (2.4 ms)
Booster : 1.5 GeV201 m50 π mm mrad7.5 Hz3 x (5 x 1012)
AGS: (24) 28 GeV 804 m2.5 Hz (5 Hz)0.9 x 1014 p/p
1.0 MW (2.0 MW)
ASBurner 40 GeV810 m
2.5 Hz (5 Hz)0.9 x 1014 p/p
1.43 MW (2.86 MW)
FFAG 2.2 GeV 210 m CW 2.7 kG
3.2 x 1014 p/AGS pulse 10.2 MW
Booster AGS
Multi-Turn H– Inject.
RTLinac
A
B Multi-Turn H– Inject.
ASBurner
1.2-1.5 GeV SCL
FFAG
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 37
Proton Drivers Layouts
Beam Makers SCL
Target
No Stacking
Accumulator
Compressor
AGS
RCS
MI
Stacking
FFAG
RFRF
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 38
Sector Gradient Magnets: B = B0 (r/r0)n
R2 R1
p1 B1 pcentral = B0 R0
p2 B2
r0
B0 ….. careful !! …. p0 = B0 r0 ≠ pcentral
Machine Centre
Important Condition to be satisfied
1 = 2 that is L1 / R1 = L2 / R2
L / R =
Calculate --> L / p = p / R
Careful again !! p / R ≠ p / r
But p = B(R) R
p /R = B(R) + R B(R) / R etc….
1
2
p / R
July 7-11, 2003 FFAG 03
Alessandro G. Ruggiero 39
Isochronous Condition
LF LD D p2
L2
p0
p1 L0
L1
200 MeV 1.1 GeV 2.2 GeV
L/L0 = x [ (1 + 02 0
2) / (1 + 02 0
2 x2)]
x = p / p0
L = LF + LD + D T = L / c = constant
dT / dp = 0 dL / dp – (L / ) d / dp = 0
d / dp = c / E0 3 dL / dp = cL / 3 E0
Bending Condition
(LF – LD) / R = = constant
R dLF / dp – R dLD / dp =
= (LF – LD) dR / dp