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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 1 Commissioning and Initial Operating Experience with the SNS Accelerator Complex
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 2 Beam and Neutronics Project Completion goals were met 10 13 protons delivered to the target The SNS Construction Project was formally Completed in June 2006 We have officially started SNS Operations First Beam on Target, First Neutrons and Technical Project Completion Goals Met April 28, 2006
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 3 SNS Accelerator Complex 945 ns 1 ms macropulse Current mini-pulse Current 1ms Front-End: Produce a 1-msec long, chopped, H- beam 1 GeV LINAC Accumulator Ring: Compress 1 msec long pulse to 700 nsec Chopper system makes gaps Ion Source 2.5 MeV1000 MeV87 MeV CCL SRF, = 0.61 SRF, =0.81 186 MeV387 MeV DTL RFQ Accumulator Ring RTBT Target HEBT InjectionExtraction RF Collimators Liquid Hg Target
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 4 SNS High-Level Design Parameters Ring is designed for 2 MW at 1 GeV; installed for 1.3 GeV (mostly)
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 5 The SNS Partnership ORNL Accelerator Systems Division responsible for integration, installation, commissioning and operation
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 6 Spring 1999
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 7 Now
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 8 Front-End Systems Front-End H - Injector was designed and built by LBNL 402.5 MHz Radiofrequency quadrupole accelerates beam to 2.5 MeV Medium Energy Beam Transport matches beam to DTL1 input parameters Front-end delivers 38 mA peak current, chopped 1 msec beam pulse H - Ion Source has been tested at baseline SNS parameters in several endurance runs >40 mA, 1.2 msec, 60 Hz
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 9 Accumulator Ring and Transport Lines Circum 248 m Energy 1 GeV f rev 1 MHz Q x, Q y 6.23, 6.20 x, y -7.9, -6.9 Accum turns1060 Final Intensity1.5x10 14 Peak Current52 A RF Volts (h=1) 40 kV (h=2) 20 kV Injected p/p 0.27% Extracted p/p 0.67% HEBT Accumulator Ring RTBT Injection Collimation RF Extraction Target Designed and built by Brookhaven National Lab
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 10 Ring and Transport Lines HEBT Arc Injection Ring Arc RTBT/Target
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 11 Target Region Within Core Vessel Core Vessel water cooled shielding Core Vessel Multi-channel flange Outer Reflector Plug Target Target Module with jumpers Moderators Proton Beam
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 12 Normal Conducting Linac: Front-End Output Emittance and Bunch Length MEBT inline emittance system allows routine measurement Expect 0.3 mm mrad, rms, norm Results ( mm mrad, rms, norm) X = 0.29 Y = 0.26 Bunch length measured with mode-locked laser system RMS Bunch Length (deg) Rebuncher phase (deg)
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 13 DTL and CCL RF Setpoints by Phase Scan Signature Matching CCL Module 2 RF Phase BPM Phase Diff (deg) J. Galambos, A. Shishlo To tune up the linac requires finding phase and amplitude setpoints for 95 RF systems within 1%/1 deg (specification) Model-based methods utilizing time-of-flight data have been developed Normal conducting linac phase and amplitude setpoints determined by Phase- Scan Signature Matching Plot shows data (lines) compared to model (pts) for two CCL2 amplitudes
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 14 CCL Module 1 Longitudinal Bunch Shape Monitor Measurements Measured values are close to the predicted bunch length Measurements were motivated by earlier observations of a longer bunch, presumably due to longitudinal mismatch BSM107 BSM111
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 15 Superconducting Linac Tuneup by Phase Scan Fit varies input energy, cavity voltage and phase offset in the simulation to match measured BPM phase differences Relies on absolute BPM phase calibration With a short, low intensity beam, results are insensitive to detuning cavities intermediate to measurement BPMs SCL phase scan for first cavity Solid = measured BPM phase diff Dot = simulated BPM phase diff Red = cosine fit Cavity phase BPM phase diff
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 16 Low-level RF Feedforward Beam turn-on transient gives RF phase and amplitude variation during the pulse, beyond bandwidth of feedback LLRF Feedforward algorithms have been commissioned (Champion, Kasemir, Ma, Crofford) Without Feed-forward With Feed-forward
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 17 SCL Operations: Fault Recovery (Galambos) We have successfully tested a cavity fault recovery algorithm in which the phase of all downsteam cavities are adjusted in response to a change in setpoint of a given cavity Cavity 3a turned off Final cavity phase found within 1 degree, output energy within 1 MeV Turned on cavity 4a, reduced fields in 11 downstream cavities
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 18 Ring/RTBT/Target Commissioning Timeline January-May 2006 Jan. 12:Received approval for beam to Extraction Dump. Jan. 13:First beam to Injection Dump. Jan. 14:First beam around ring. Jan. 15:>1000 turns circulating in ring Jan. 16:First beam to Extraction Dump. Jan. 26:Reached 1.26E13 ppp to Extraction Dump. Feb. 11:~8 uC bunched beam (5x10 13 ppp) Feb. 12:~16 uC coasting beam (1x10 14 ppp) Feb. 13:End of Ring commissioning run April 3-7: Readiness Review for RTBT/Target April 27: Received approval for Beam on Target April 28: First beam on target and CD4 beam demonstration
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 19 Accumulation and Extraction of 1.3x10 13 protons/pulse (January 26, 2006) Ring Beam Current Monitor 200 turn accumulation extraction Extraction Dump Current Monitor
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 20 Ring Orbit Correction: H,V Bumps are Due to Injection Kickers Horizontal Orbit BPM Amplitude Vertical Orbit
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 21 Ring Optics Measurements: Betatron Phase Advance and Chromaticity VertHoriz Natural Chromaticity (Design) -6.9-7.9 Natural Chromaticity (Measured) -7.2-8.2 Corrected Chromaticity (Meas) 0.00.1 Plots show measured betatron phase error vs. model-based fit Data indicates that the linear lattice is already very close to design
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 22 High Intensity Studies (Danilov, Cousineau, Plum) Beam intensity records (protons/pulse): 5x10 13 in bunched beam, transported to target 1x10 14 unbunched, coasting beam We searched for instabilities by i) delaying extraction, ii) operating with zero chromaticity, iii) storing a coasting beam No instabilities seen thus far in “normal” conditions See instability centered at 6 MHz, growth rate 860 us for 10 14 protons in the ring, driven, as predicted by extraction kicker impedance Z calc 22-30 kOhm/m Z meas 28 kOhm/m. In coasting beam also see very fast instability at 0.2-1x10 14 protons in the ring, consistent with e-p. Growth rate 20-200 turns. f 30-80 MHz depending on beam conditions. Scaling these observations to nominal operating conditions predicts threshold > 2 MW for extraction kicker (as previously predicted) Slow: Extraction Kicker Fast: electron-proton
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 23 Phase Space Painting Stripping Foil Injected Beam Initial Closed Orbit Final Closed Orbit X pxpx Wei et. al., PAC 2001, 2560 X-Y space after 1060 Turns
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 24 Phase Space Painting 65 mm 80 mm Beam on Target View Screen Beam profiles in RTBT
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 25 Summary of Achieved Beam Parameters ParameterBaseline/ Design Achieved in Commissioning/AP Achieved in Operation Units Linac Transverse Output Emittance 0.40.3 (H), 0.3 (V)0.4 mm-mrad (rms,norm) CCL1 bunch length344degrees rms Linac Peak Current38> 3820mA Linac Output Energy10001012890MeV Linac Average Current1.61.05 (DTL1 run) 0.003 (SCL run) 0.067mA Linac H-/pulse1.6x10 14 1.3x10 14 (DTL1) 8.0x10 13 (SCL run) 1.0x10 14 (Ring run) 4.3x10 13 Ions/pulse Linac Pulse length/Rep- rate/Duty Factor 1.0/60/6.01.0/60/3.8 (DTL1 run) 0.85/0.2/0.017 (SCL) 0.6/5/0.3msec/Hz/% Extracted protons/pulse1.5x10 14 0.96x10 14 0.43x10 14 Protons/pulse Beam Power1440460kW
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 26 Beam-Power-on-Target History Beam Power [0-65 kW] Beam power administratively limited to 10 kW until November 8 Feb 1, 2007 May 1, 2006
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 27 FY 2007 Integrated Beam Power by Day and Cumulative 6.3 MW-hrs delivered in Run 2007-1
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 28 Technical Challenges: Equipment Reliability Beam Chopper Systems Repeated failures in Low-energy and Medium-energy Beam Transport chopper systems New, more robust, designs will be designed and manufactured this year (FY07 Accelerator Improvement Project) High-Voltage Converter Modulators A number of weak components limit MTBF to 2700 Hrs Several prototype improvements are in test in single operational units Improvements will be deployed this year on full system of 14 modulators (FY07 Accelerator Improvement Project) Ion Source and Low Energy Beam Transport System Water Systems Problems associated with clogging flow restrictors, failed gaskets, poor conductivity monitoring and control, etc. Reliability improvements have been underway since CD-4 (also FY07 AIP) Cryogenic Moderator System Thermal capacity degraded in 3 week cycle prior to December 2006 Manufacturer attempted repair in December Capacity improved, but some sign of degradation remains Mercury Pump Seal failed end of November Operating the pump now with failed seal, mitigated by installation of a cover plate to direct gas to the Mercury Off-Gas Treatment System Replacement Mercury Pump in expected to be available for installation in September
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 29 Technical Challenges: Beam Power Beam losses must be kept below 1 Watt/m to limit residual activation We measure higher than desired losses in the Ring Injection area We are unable to simultaneously transport waste beams (from stripping process) to the injection dump and properly accumulate in the ring Internal Review of Injection Dump performance was held in November and follow-up meeting in December Short-term fixes allow >100 kW operation; mid-term fixes (April 2007) are in preparation; long-term fix requires redesign of injection dump beamline and 2 new magnets An aggressive accelerator physics program has reduced losses and activation while allowing increased beam power We are not operating 9 Superconducting RF cavities (out of 81) out of concern for potential failures Recent tests indicate that 6 of these 9 cavities are operable up to 15 Hz repetition rate Those tests also show that the behaviour of individual cavities is the same at higher repetition rates, up to the full 60 Hz We are building infrastructure to provide cryomodule repair and maintenance capabilities on-site. We are formulating plans to restore operation of all cavities, and to procure spare cryomodules
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 30 Outlook: Performance Goals FY08FY07 FY09 SNS Beam Power Upgrade Project will increase linac output energy to 1.3 GeV and provide 3 MW beam power
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 31 E-P Feedback Experiment at the PSR We formed a collaboration to carry out an experimental test of active damping of the e-p instability at the LANL PSR (ORNL, LBNL, IU, LANL) We deployed a broadband transverse feedback system designed and built by ORNL/SNS and demonstrated for the first time damping of an e-p instability in a long-bunch machine We observed a 30% increase in e-p instability threshold with feedback on.
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 32 We have observed > 90% H- to proton stripping efficiency in proof-of-principle tests at SNS Laser Beam H-H- proton H0H0 H 0* Step 1: Lorentz Stripping Step 2: Laser Excitation Step 3: Lorentz Stripping High-field Dipole Magnet H - H 0 + e - H 0 (n=1) + H 0* (n=3)H 0* p + e - Laser-Stripping Injection Proof-of- Principle Experiment H- to protons
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 33 Yes, We’ve Had a Few Surprises RFQ resonant frequency shifted by 100 kHz Never found the cause; retuned in 2003 Bunch length 3x design in CCL1; also had difficulty keeping DTL5 at design field Found a charred piece of paper in DTL Tank 5 in 2004 Large local losses and poor trajectory near SCL/HEBT transition Found large dipole deflection with orbit response studies Found current shunted around one quad coil Beam is rotated about 6 degrees on target view screen Excessive fundamental power through two SCL HOM feedthroughs; others impacted Large local losses in injection dump line
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 34 Summary Completed 7 beam commissioning runs, amounting to more than 1 year of dedicated beam commissioning and operating time Achieved beam and neutron project completion requirements within project schedule SNS construction project was formally completed in June 2006 on-budget and on-schedule We are now in the early operations stage with local users We are beginning to ramp up the beam power of the SNS accelerator complex
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 35 SNS Beam Diagnostic Systems RING 44 Position 2 Ionization Profile 70 Loss 1 Current 5 Electron Det. 12 FBLM 2 Wire 1 Beam in Gap 2 Video 1 Tune RING 44 Position 2 Ionization Profile 70 Loss 1 Current 5 Electron Det. 12 FBLM 2 Wire 1 Beam in Gap 2 Video 1 Tune SCL 32 Position 86 Loss 9 Laser Wire 24 PMT Neutron SCL 32 Position 86 Loss 9 Laser Wire 24 PMT Neutron RTBT 17 Position 36 Loss 4 Current 5 Wire 1 Harp 3 FBLM RTBT 17 Position 36 Loss 4 Current 5 Wire 1 Harp 3 FBLM HEBT 29 Position 1 Prototype Wire-S 46 BLM, 3 FBLM 4 Current HEBT 29 Position 1 Prototype Wire-S 46 BLM, 3 FBLM 4 Current IDump 1 Position 1 Wire 1 Current 6 BLM IDump 1 Position 1 Wire 1 Current 6 BLM EDump 1 Current 4 Loss 1 Wire EDump 1 Current 4 Loss 1 Wire LDump 6 Loss 6 Position 1 Wire,1 BCM LDump 6 Loss 6 Position 1 Wire,1 BCM CCL/SCL Transition 2 Position 1 Wire 1 Loss 1 Current CCL/SCL Transition 2 Position 1 Wire 1 Loss 1 Current CCL 10 Position 9 Wire 8 Neutron, 3BSM, 2 Thermal 28 Loss 3 Bunch 1 Faraday Cup 1 Current CCL 10 Position 9 Wire 8 Neutron, 3BSM, 2 Thermal 28 Loss 3 Bunch 1 Faraday Cup 1 Current Operational MEBT 6 Position 2 Current 5 Wires 2 Thermal Neutron 3 PMT Neutron 1 fast faraday cup 1 faraday/beam stop D-box video D-box emittance D-box beam stop D-box aperture Differential BCM MEBT 6 Position 2 Current 5 Wires 2 Thermal Neutron 3 PMT Neutron 1 fast faraday cup 1 faraday/beam stop D-box video D-box emittance D-box beam stop D-box aperture Differential BCM DTL 10 Position 5 Wire 12 Loss 5 Faraday Cup 6 Current 6 Thermal and 12 PMT Neutron DTL 10 Position 5 Wire 12 Loss 5 Faraday Cup 6 Current 6 Thermal and 12 PMT Neutron Not Operating
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 36 Baseline SNS Ion Source Performance LBNL H - ion source + ORNL antennas Source performed well during SNS commissioning. Successful commissioning would not be possible without use of longer- lived antennas. 10-40 mA routinely delivered at ~0.1% duty-factor. Availability improved: 86% ~100% during later commissioning periods (target comm: 77 days). Largest availability gain redesigning LEBT insulators Antennas: Welton et al, RSI 73 (2002) 1008 + Beam attenuation ~5 mA/day Run #9 ran for 16 days / 33 mA / 0.4 mA/day. 3 Typical Test Runs Our Best Run (employs new operating procedure) Catastrophic antenna failure ~10 lifetime tests performed at full 7% duty-factor and max current. Best results shown Outcome: Insufficient beam current, frequent antenna failures and poor beam stability with time Vigorous R&D program to meet SNS operational requirement of 40 mA and SNS-PUP requirement of 60 mA.
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 37 Recent Ion Source R&D Accomplishments Ionization Cone Cs injection collar Air duct Cs Line Extractor electrode ions Elemental Cs system 65 mA-1.2 ms, 70 mA-0.2 ms pulses achieved at 10Hz! ~2x increase in RF power efficiency. Multi-day runs show excellent beam stability. Multiple cesiations show excellent reproducibility. ~5% droop and good ~30 us rise times. Beam emittance is expected to be similar to baseline source. Al 2 O 3 insulator Anode Cooling channel Plasma stream Cathode Ions Multi-year lifetime achieved at DESY at <1% duty-factor Plasma gun enhances H - ~50% 51 mA – 0.2 ms pulses achieved with no Cs and no B-field confinement. 65 mA – 0.2 ms, 50 mA – 1.2 ms pulses achieved with Cs and no confinement. Welton et al, LINAC 2006, Knoxville External Antenna & Plasma Gun Welton et al, LINAC 2006, Knoxville
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 38 Energy Stability – Pulse to Pulse (J. Galambos) RMS energy difference jitter is 0.35 MeV, extreme = + 1.3 MeV Parameter list requirement is max jitter < +1.5 MeV 865 MeV beam ~ 1000 pulses 20 sec pulse 12 mA beam
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 39 SCL Laser Profile Measurements SCL laser profiles (H + V) were available at 7 locations 3 at medium beta entrance, 3 at high beta entrance and 1 at the high beta end Measured horizontal profile after SCL cryomodule 4
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 40 Neutrons: 4-methyl pyridine N-oxide 5 kWatt, 3 hour, ¼ detector, T = 3 K 4 eV
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O AK R IDGE N ATIONAL L ABORATORY U. S. D EPARTMENT OF E NERGY 41 The Spallation Neutron Source The SNS is a short-pulse neutron source, driven by a 1.4 MW proton accelerator SNS will be the world’s leading facility for neutron scattering research with peak neutron flux ~20–100x ILL, Grenoble SNS construction project, a collaboration of six US DOE labs, was funded through DOE-BES at a cost of 1.4 B$ SNS will have 8x beam power of ISIS, the world’s leading pulsed source Stepping stone to other high power facilities
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