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The Spallation Neutron Source Project Geneva December 8, 2006 Norbert Holtkamp ITER International Organization 13108 St Paul lez Durance [email protected]

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Page 1: The Spallation Neutron Source Projectcas.web.cern.ch/sites/cas.web.cern.ch/themes/cern... · 2017-01-31 · neutrons produced by fission reactions Continuous neutron beam 1 neutron/fission

The Spallation Neutron Source Project

Geneva

December 8, 2006

Norbert Holtkamp ITER International Organization

13108 St Paul lez Durance [email protected]

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2

The Spallation Neutron Source

• SNS is funded through DOE-BES and has a Baseline Cost of 1.4 B$

• 1.3 GeV facility designed & build to operate at 1 GeV to begin with

• SC linac

• Single ring capable to operate at 1.3 GeV

• One target station

• The peak neutron flux will be ~20–100x ILL

• SNS has begun operation with 3 instruments installed.

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The SNS Mega Terms– What it is and what it is supposed to be in a few years…

• It is:

– The first high energy proton linac largely built with superconducting RF structures (0.812 GeV out of 1.0 GeV).

– The worlds highest energy proton linac (operated with H-)

– The second largest accelerator RF installation in the US.

– The first Multilab collaboration with fully distributed responsibility for accelerator construction.

– A project that finished “On Time and within budget” according to a schedule/budget set in 2000.

• It will have:

– The highest intensity proton storage ring of its kind.

– The highest average beam power available in the world.

– The most advanced Neutron scattering facility with the best in class instruments

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4

Fission

chain reaction

continuous flow

1 neutron/fission

Spallation

no chain reaction

pulsed operation

30 neutrons/proton

Time resolved exp.

Spallation-Evaporation Production of Neutrons and Why to use heavy metal target!

power average MW 21.4 achieve to is Goal:SNS

HzfsecTAIeVEP reppulsebeam

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18 Instruments Now Formally Approved (20+ funded) •Fundamental Physics to Engineering

•Chemistry to “Genomes to Life”

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Backscattering Spectrometer

• 84 m incident flight path designed to provide high energy resolution – 2.5 meV (fwhm) at the elastic line – slow dynamics (100’s psec, 3 – 35 Å)

• Approximately 50 x faster then current world’s best comparable instruments – better Q-resolution simplifies studies involving crystalline materials

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Reactors vs. Accelerator-Driven Sources

Reactor-based source:

• neutrons produced by fission reactions

• Continuous neutron beam

• 1 neutron/fission

Accelerator based source: • Neutrons produced by

spallation reaction

• 25 neutrons/proton for Hg

• Neutrons are pulsed and follow proton beam time structure

• A pulsed beam with precise t0 allows neutron energy measurement via TOF

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Spring 1999

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Spring 2006

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SNS Accelerator Complex

945 ns

1 ms macropulse

Curr

en

t mini-pulse

H- stripped to protons

Curr

en

t

1ms

Front-End: Produce a 1-msec long, chopped, H-

beam

LINAC: Accelerates the beam to

1 GeV

Accumulator Ring: Compress 1 msec long pulse to 700

nsec

Deliver beam to Target

Chopper system makes

gaps

Ion Source

2.5 MeV 1000 MeV 87 MeV

CCL SRF, b=0.61 SRF, b=0.81

186 MeV 387 MeV

DTL RFQ

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Target Region Within Core Vessel

Core Vessel water cooled shielding

Core Vessel Multi-channel flange

Outer Reflector Plug

Target

Target Module with jumpers

Moderators

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Original SNS CDR for CD-1 May 1997

• 1.0 MW 1.0 GeV copper CCL linac with no room for increased energy, only current • HEBT and Ring magnets sized for 1.0 GeV H-

• Orginal Design has very little to do with what was built.

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SNS High Level Baseline Parameters

Beam Energy 1.0 GeV

Average Beam Current 1.4 mA

Beam Power on Target 1.4 MW

Pulse Repetition Rate 60 Hz

Beam Macropulse Duty Factor 6.0 %

H- Peak Linac Current 38 mA

Linac Beam Pulse Length 1.0 ms

Ring Beam Extraction Gap 250 ns

Protons Per Pulse on Target 1.5x1014

Proton Pulse Width on Target 695 ns

Uncontrolled Beamloss Criteria 1 Watt/m

Linac length 335 m

Total Beamline Length 903 m

Target Material Liquid Hg (1 m3; 18 tons)

Energy Per Beam Pulse 24 kJ

Maximum Number Instruments 24

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The Spallation Neutron Source Partnership

~177 M$ ~60 M$

~113 M$ ~20 M$

Description AcceleratorProject Support 75.6Front End Systems 20.8 20.8Linac Systems 311.0 311.0Ring & Transfer Systems 146.6 146.6Target Systems 108.2Instrument Systems 63.3Conventional Facilities 378.9Integrated Control System 58.5 58.5BAC 1,162.9Contingency 29.8

TEC 1,192.7R&D 99.9 79.9

Pre-Operations 119.1 95.3

TPC 1,411.7 712.1

~63 M$

~106 M$

SNS-ORNL Accelerator systems: ~167 M$

At peak : ~500 People

worked on the

construction

of the SNS accelerator

The partners developed and built – SNS/ORNL integrated, installed + operated

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SNS Multilab Organizational

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SNS CD-4 Scope Criteria

Level 0 – DOE Deputy Secretary

• Accelerator-based neutron scattering facility capable of at least 1 megawatt proton beam power on target

Level 1A – Director, Office of Science

• Five specific research instruments

Level 1B – Associate Director BES

• Performance test demonstrating

1.0E+13 protons per pulse (one pulse is enough)

5.0E-3 neutrons/steradian/incident proton, viewing moderator face (~x5-10 under normal moderator performance)

Level 2 – DOE Project Director

• At least 3 of the 5 instruments installed and tested; the other 2 procured and on site

• Trained staff, operating permits, and systems documentation in place

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Budget Driving the Schedule

• DOE supported SNS immensely by making sure that we got the budget to execute the plan that was laid out.

• The schedule had a very aggressive procurement plan, that was based on the idea of an “accelerator in the box”

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Cost Development between 2001 and 2006

• Spend $1.41 Billion dollars in 7 years with a peak of ~ 1 M$/day during peak construction.

• ~ $6.5 M contingency left at the end for scope additions

• Operations budget 160M$/Year

• 450 staff positions

• ~2000 users per year at full capacity.

Nov 2001 [$M] May 2006 [$M] Contingency

1.01 Research & Development 103.8 99.9 -3.8%

1.10 Operations 115.2 119.1 3.4%

Total OPC (Burdened, Escalated Dollars) 219.0 219.0

0.0%

1.02 Project Support 72.3 72.1 -0.3%

1.03 Front End Systems 19.3 20.8 7.9%

1.04 Linac Systems 272.4 311.0 14.2%

1.05 Ring & Transfer System 146.2 146.6 0.3%

1.06 Target Systems 95.3 114.9 20.5%

1.07 Instrument Systems 62.3 63.9 2.6%

1.08 Conventional Facilities 310.7 398.5 28.3%

1.09 Integrated Control Systems 58.6 58.5 -0.1%

Total Line Item (Burdened, Escalated Dollars)

1037.0 1186.3 14.4%

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LBNL: SNS Front-End Systems

• Front-End H- Injector was designed and built by LBNL

• Front-end delivers 38 mA peak current, chopped 1 msec beam pulse

• H- Ion Source has operated at baseline SNS parameters in several endurance runs since 2002.

– >40 mA, 1.2 msec, 60 Hz

Ion Source

Radio-Frequency Quadrupole

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LANL: Normal Conducting Linac & RF Systems

• CCL Systems designed and built by Los Alamos

• 805 MHz CCL accelerates beam to 186 MeV

• System consists of 48 accelerating segments, 48 quadrupoles, 32 steering magnets and diagnostics

• 402.5 MHz DTL was designed and built by Los Alamos

• Six tanks accelerate beam to 87 MeV

• System includes 210 drift tubes, transverse focusing via PM quads, 24 dipole correctors, and associated beam diagnostics

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DTL/CCL Commissioning Results

– Full transmission of accelerated beam to the beamstop (with few % measurement uncertainty)

– Typical beam pulse: 20 mA, 40ms, 1 Hz (limited by intercepting diagnostics and beamstop)

Module Design [MeV] Measured [MeV] Deviation [%]

DTL6 86.83 87.48±0.03 0.75

CCL1 107.16 107.36±0.12 0.19

CCL2 131.14 131.53±0.14 0.40

CCL3 157.21 158.08±0.40 0.55

July 2004

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JLAB: The Superconducting Linac

• Designed and built by Jefferson Laboratory.

• SCL accelerates beam from 186 to 1000 MeV.

• SCL consists of 81 cavities in 23 cryomodules.

• Two types of cavity geometries are used to cover broad range in particle velocities (β=.65, .85).

• Cavities are operated at 2.1 K with He supplied by Cryogenic Plant.

• Operation so far mostly at 4.2 K.

Superconducting RF Advantages: 1. Flexibility gradient and energy are not

fixed 2. More power efficient lower operational

cost 3. High cavity fields less real estate 4. Better vacuum less gas stripping 5. Large aperture less aperture

restrictions reduced beam loss reduced activation

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25

Representative Linac Beam Pulse

• 860 MeV • 18 mA peak

current • 200 msec • 70%

Chopping • 12 mA

average pulse current

• 1.5x1013 H-/pulse

Overlay of 12 linac beam current monitors

August 2005

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Cavity Gradient Performance

0

2

4

6

8

10

12

14

16

1 3 5 7 9 11 13 15 17 19 21 23 25

Ea [MV/m]

Nu

mb

er

of

Ca

vit

ies

2.1 K Closed loop 2.1 K Open loop 4.2 K Open loopMaximum fields

achieved in the

installed cavities.

Operational fields

are kept in general

at 75-80% of the

maximum fields

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Energy Stability – Pulse to Pulse

• RMS energy difference jitter is 0.35 MeV, extreme = + 1.3 MeV (without any energy feedback)

• Parameter list requirement is max jitter < +1.5 MeV

865 MeV beam

~ 1000 pulses

20 msec pulse

12 mA beam

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Low-level RF Feedforward within the Beam Pulse

Without Feed-forward With Feed-forward

• Beam turn-on transient gives RF phase and amplitude variation during the pulse, beyond bandwidth of feedback.

• LLRF Feedforward algorithms have been commissioned.

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Linac RMS Transverse Emittance

• Measured RMS emittance is within specification but beam parameters are different for various runs.

Measured

e (H, V)

norm. p-mm-mrad

Parameter List

e (H, V)

norm. p-mm-mrad

Notes

MEBT Entrance

0.22, 0.25 0.21 RFQ Exit Twiss study

CCL Entrance

0.22, 0.25 0.33 Matching 7 CCL profile sets

SCL Entrance

0.27, 0.35 0.41 Matching 3 SCL profile sets

Linac Dump 0.26, 0.27 0.41 1 wire, vary quads

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Linac RF Systems

81 SCL Klystrons

DTL Klystrons

• 2nd largest klystron and modulator installation in the world!

High Voltage Converter Modulators

• Designed and procured by LANL

• All systems 8% duty factor: 1.3 ms, 60 Hz

• 7 DTL Klystrons: 2.5 MW 402.5 MHz

• 4 CCL Klystrons: 5 MW 805 MHz

• 81 SCL Klystrons: 550 kW, 805 MHz

• 14 IGBT-based modulators

CCL Klystrons

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JLAB: SNS CHL Facility

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Warm Compressors System Status

• 3 warm compressor streets

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4.5K Cold Box has been Commissioned

• 8 kW at 4.5 K

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JLAB + ORNL: The SNS Cryogenic Support System

• ~2 kW @ 2.0 K (→ 40mBar)

• Operated since Oct 2004 uninterrupted. Mainly at 4.5K

• Very reliable and build to accommodate an additional 9 (23->31) cryomodules.

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BNL: Accumulator Ring and Transport Lines

Circum 248 m Energy 1 GeV frev 1 MHz Qx, Qy 6.23, 6.20

Qx,y 0.15 x, y -7.9, -6.9 Accum turns 1060 Final Intensity 1.5x1014 Peak Current 52 A RF Volts (h=1) 40 kV (h=2) 20 kV

HEBT

Accumulator Ring

RTBT

Injection

Collimation

RF

Extraction

Target

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Ring and Transport Lines

HEBT Arc

Injection

Ring Arc

RTBT/Target

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•Instrument floor layout can be seen and target installation began

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The SNS Target: 2-MW Design

• 25 kJ/pulse at 7x15cm beam size sets of transverse and longitudinal shock wave.

• Needs to be exchanged remotely every 3 month at full power operation.

1 mm

Back of Target Service Bay

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Recent Achievements

• Ring commissioning started Jan 12th, 2006.

• Status on January 14th in the picture.

• Quick start up of charge exchange injection, accumulation, and extraction since all diagnostics online at commissioning begin.

7 turn injection

Extraction beam dump

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Push For High Intensity

• Achieved CD4 1.3 x 1013 ppp intensity on Jan 26.

multiturn injection

Extraction beam dump

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High Intensity Results: Beam Loading in the Ring RF System

3x1013 protons per pulse

5x1013 protons per pulse • Shows distortion of

longitudinal profile and beam leaking into gap due to untuned compensation of beam loading in RF

Extraction

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Instability Studies at Up to 1014 Coasting Beam

• During high-intensity studies we searched for instabilities by

– delaying extraction

– operating with zero chromaticity

– storing a coasting beam

• No instabilities seen thus far in “normal” conditions

• First instability observed with central frequency about 6 MHz, growth rate 860 us for 1014 protons in the ring,

• Scaling these observations to nominal operating conditions predicts threshold > 2 MW

0 50 100 1502

2.5

3

3.5

4

4.5

5

5.5

6

Turns

Log

(ma

gin

itu

de(

75t

h H

arm

on

ic))

Evolution of 75th Harmonic

Slow: Extraction Kicker

Fast: electron-proton

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1.6x1013 Protons Delivered to the Target for CD4 Beam Demonstration (April 28, 2006)

Final RTBT Beam Current Monitor

Ring Beam Current Monitor

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Beam on Target: Injection Painting

65 mm 80 mm

Beam on Target View Screen

Beam profiles in RTBT

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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 (5x1013 ppp) Feb. 12: ~16 uC coasting beam (1x1014 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 2 hours later CD4 (>1013) beam demonstration

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Uncontrolled loss

during normal operation

0

0.5

1

1.5

2

2.5

3

0 100 200 300 400 500 600 700 800

Length [m]

Bea

m lo

ss [

W/m

]

SCL

DTL

CCLRING

FE

HEBT RTBT

High rad

areas

Primary Concern for SNS on its Way to Full Power Operation: Uncontrolled Beam Loss

• Hands-on maintenance: no more than 100 mrem/hour residual activation (4 h cool down, 30 cm from surface)

• 1 Watt/m uncontrolled beam loss for linac & ring

• Less than 10-6 fractional beam loss per tunnel meter at 1 GeV; 10-4 loss for ring

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SNS Diagnostics Deployment

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

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

IDump

1 Position

1 Wire

1 Current

6 BLM

EDump

1 Current 4 Loss

1 Wire

LDump

6 Loss

6 Position

1 Wire ,1 BCM

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

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

DTL

10 Position 5 Wire 12 Loss

5 Faraday Cup 6 Current

6 Thermal and 12 PMT Neutron

Not Operating

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Losses in HEBT and Ring

HEBT Inj Dump Ring

Collimators 480 turn accumulation

Relative Idump/Ring losses reduced with smaller spot on foil

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SNS Early Operations: Ramping up Scientific Productivity

Accelerator Availability and Operation

0

500

1000

1500

2000

2500

3000

Ye a rs

Op

s H

ou

rs

40

60

80

100

%

User Ops hours A cc el. P hy ic s B eam P ower/kW Reliability (% )

User Ops hours 0 500 900 1000 1500 1900 1950 2400 2450 2500 625 625 2500

A cc el. P hy ic s 1

B eam P ower/k W

Reliability (% )

• Shared the plan with the community to get them involved early on: “Manage Expectations”

• “This slide was made on plane ride in 2 h and most of the numbers were invented.”

‘06 ‘07 ‘08 ‘09 ‘10 ‘11 ‘12

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Schedule Changes…. And How Did We Make It?

• Its always the first schedule that counts to measure how well a project is doing, not the last one…..

2002 2003 2004 2005 2006

DTL Tanks 1-3

Front-End

DTL Tank 1

DTL/CCL

SCL

Ring

Target

The End

FY

460 days

240 days

2001 plan

2006 actual

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How Much R&D Can One Do/Effort in a Construction Project?

• Quite a bit…and a construction schedule is driving the R&D to be very fast and efficient.

– LASER profile monitor to replace standard carbon wires in the SC part of the linac which can be used while operating a full intensity beam

– Nano-crystaline foil development for high intensity beams, tested at the PSR.

– A fast feedback system to reduce/eliminate the PSR instability

– A H- stripping experiment based on Laser/Magnetic stripping.

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Where Does SNS Stand today?: Performance Goals

0

500

1000

1500

2000

2500

0 12 24 36Months

Beam

Pow

er

(kW

), P

roduction H

rs

50

55

60

65

70

75

80

85

90

95

Relia

bili

ty

Beam Power GoalNeutron Production HoursReliability

FY08 FY07 FY09

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Operations Planning: Ramp-up in Beam Parameters

• Beam repetition rate is consistent with the operations envelope limit

Power Ramp Up

0

10

20

30

40

50

60

70

Oct-

06

Apr-

07

Oct-

07

Apr-

08

Oct-

08

Apr-

09

Oct-

09

RR

(H

z) /

Cu

rre

nt

(mA

)

02004006008001000120014001600

Pu

lse

Le

ng

th (

ms

ec

) /

Po

we

r (k

W)Rep. Rate (Hz)

Peak Current (mA)

Pulse Length (u-sec)

Power (kW)

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Beam-Power-on-Target History

Beam power administratively limited to 10 kW until November 8

Be

am

Po

we

r [0

-60

kW

]

May 1, 2006 Nov 30, 2006

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Run 2007-1: Integrated Beam Power by Day and Cumulative

• 6.3 MW-hrs delivered in Run 2007-1

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Run 2007-1 Statistics

• Run Parameters: – Beam Energy: 890 MeV – 20 kW: 5 Hz rep-rate, 300 msec linac beam pulse, 20 mA peak current

0

10

20

30

40

50

60

70

80

90

100

10/8

/200

6

10/1

5/20

06

10/2

2/20

06

10/2

9/20

06

11/5

/200

6

11/1

2/20

06

11/1

9/20

06

Ho

urs

/Week

0

500

1000

1500

2000

2500

kW

Hrs

/Week

kW Hrs per week

Neutron Production Hours per Week

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Ramp-Up Progress

0

100

200

300

400

500

600

1 3 5 7 9 11 13 15 17 19 21 23 25 27 29

Weeks Since First Beam on Target

kW

-hrs

/day

0

10

20

30

40

50

60

Peak B

eam

Pow

er

(kW

)

Average kW-hrs/Day

Peak Beam Power

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Run 2007-1 Breakdown Statistics

Pulsed power: modulators and beam choppers

Accelerator de-ionized water systems

Mercury pump

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FY07 Accelerator Improvement Projects

Project Description FY07

High-Voltage Converter Modulator Upgrade Phase 1

Upgrade HVCM systems to improve reliability and rep rate; install modulator test stand 1,450

Accelerator Cooling Water System Reliability Upgrade Upgrade water systems to improve reliability 1,150

Beam Diagnostic Upgrade Phase 1 Improve diagnostics instrumentation to reduce beam loss and component activation 1,300

LEBT Chopper Upgrade Redesign LEBT chopper system with greater engineering margin to improve reliability 400

MEBT Chopper Upgrade Redesign MEBT chopper system with greater engineering margin to improve reliability 230

RF System Upgrade Phase 1 Upgrade MEBT RF systems and RFQ couplers for higher reliability; other reliability improvements 1,400

Accelerator Power Supply Lock-out Tag-out System

Install trap-key system and finger-safe terminals for HEBT/Ring/RTBT power supply systems to enable rapid and safer lock-out/tag-out 400

CHL Tie-in to Test Cave Connect RF test cave to CHL; add permanent, movable shielding door to cave 770

Injection Region Upgrade Phase 1 Incorporate additional corrector magnet, vacuum chamber and diagnostics in injection dump line; install optimized primary foil mechanism to reduce beamloss 900

Total AIP $8,000k

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Run 2007-1: Goals vs. Achieved

0

10

20

30

40

50

60

70

80

90

0 13 26 39 52

Weeks

Inte

gra

ted B

eam

Pow

er

[MW

-hrs

]

Quarterly Integrated Beam Power Goal

Actual Integrated Beam Power

• Three goals for this run:

Deliver > 3.9 MW-hrs in neutron production

Demonstrate sustained 30 kW operation

Demonstrate 60 kW capability for > ½ shift

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Summary

• SNS had a very rough start in the 90’s when it was converted from a fission reactor project to an accelerator based neutron source to a sc linac driven source. (each change was accompanied by a new management team)

• The SNS project has officially finished at the end of May, 2006 (end of June 2006) with the signature of the Critical Decision 4 documents at a total project cost of $1,405,2M ($1,411.7M) .

• SNS construction was accompanied by several severe technical setbacks and subsequent MIRACLES on recovery.

• This is probably my last official talk about SNS and it’s a pleasure to give it CERN here in the lecture in front of such a distinguished group.

• Thanks

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Technical Challenges: Beam Loss

• The SNS is a loss-limited accelerator; losses must be kept < 1 W/m to limit residual activation

• We measure higher than desired losses in a few locations: – Ring Injection region

We are unable to simultaneously transport waste beams (from stripping process) to the injection dump and properly accumulate in the ring

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

Internal Review of Injection Dump performance and recovery options was held Nov. 21st with R. Macek from LANL (D. Raparia from BNL will review results in December)

– Coupled cavity linac due to orbit control and sparseness of loss monitors

– Near RTBT Dipole for large painted beams • Active and aggressive accelerator physics studies have reduced

losses and activation while allowing increased beam power

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Technical Challenges: Superconducting Linac Performance

• Superconducting Linac is operating at 892 MeV

• All but 3 (of 81) cavities are operational at low rep-rate (< 5 Hz)

• As a conservative measure, we have turned off 6 additional cavities in order to confidently operate at higher rep-rates (15 Hz)

– Driven by concern over potential Higher-Order-Mode feedthrough failures; certain cavities show HOM waveforms that indicate pathological behaviour

• A plan which follows the 3-year beam power ramp-up curve is being formulated:

– We are working with Jefferson Laboratory to develop plans for

Reworking one high-beta cryomodule (remove in December)

Reworking the medium-beta prototype cryomodule to turn it into an operational spare

– We are preparing a bid package for procurement of spare high-beta cryomodules

• We are establishing cryomodule repair, maintenance and testing capabilities on-site (AIP Project)

– Cleanrooms are on order – RF Test Cave will be ready for first test end of January

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Technical Challenges: Reliability Limitations

• Beam Chopper Systems – Repeated failures in LEBT and MEBT chopper systems – New, more robust, designs will be manufactured this year (FY07 AIP)

• High-Voltage Converter Modulators – A number of weak components limit MTBF to 2700 Hrs – Several prototype improvements are in test in single operational units – Begin upgrade program for better fault detection, replacement of

components with higher engineering margin, (FY07 AIP) • Water Systems

– Flow restrictors continue to clog – Responded to floods from failed gaskets – Have been replacing all gaskets and retorquing flanges in klystron

gallery, service buildings and tunnel – Will remove flow restrictors during December down period, replace with

valves where necessary – Water systems upgrade program included in FY07 AIP plan.

• Cryogenic Moderator System – Thermal capacity degrades-- requires cycling every 2 weeks;

Manufacturer will attempt repair in December • Mercury Pump

– Seal failed Nov. 26; repair strategy being formulated

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DTL and CCL RF Setpoints by Phase Scan Signature Matching

CCL Module 2 RF Phase

BP

M P

hase D

iff (

deg)

J. Galambos, A. Shishlo

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SCL Phase Scan using BPMs

• Matching involves varying input energy, cavity voltage and phase offset in the simulation to match measured BPM phase differences

• Relies on absolute BPM 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

BP

M p

hase d

iff

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Ring Closed Orbit: H,V Bumps are Due to Injection Kickers

Horizontal Orbit

BPM Amplitude

Vertical Orbit

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Turn by Turn Data for Zero Chromaticity

Horizontal Turn-by-turn

Vertical Turn-by-turn

Amplitude Turn-by-turn

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Ring Optics Measurements: Betatron Phase Advance and Chromaticity

Vert Horiz

Natural Chromaticity (Design)

-6.9 -7.9

Natural Chromaticity (Measured)

-7.2 -8.2

Corrected Chromaticity (Meas)

0.0 0.1

Horizontal Fit

-30

-20

-10

0

10

20

30

1 4 7 10 13 16 19 22 25 28 31 34 37 40 43

Beam Position Monitor

Bet

atro

n P

has

e E

rro

r (d

egre

es)

Horizontal Data

Horizontal Fit

Vertical Fit

-30

-20

-10

0

10

20

30

1 4 7 10 13 16 19 22 25 28 31 34 37 40 43

Beam Position Monitor

Be

tatr

on

Ph

as

e E

rro

r (d

eg

ree

s)

Vertical Data

Vertical Fit

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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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

– Expect reliable data beyond 3 sigma during operation.

Measured horizontal profile after SCL cryomodule 4

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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:

• We deployed a transverse feedback system designed and built by ORNL/SNS and in two shifts demonstrated for the first time damping of an e-p instability in a long-bunch machine

• In subsequent studies we observed a 15-30% increase in e-p instability threshold with feedback on.

• Continued investigation of e-p feedback will be pursued, as well as simulations to benchmark experimental results.

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Example Measurements

Position, phase

Bunch shape

Profile (wires)

emittance

Current (toroids)

Current (MEBT beam stop)

Loss (neutron)

Halo

Loss (ion chambers)

Current (DTL Faraday cup)

Current (D-plate beam stop)

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• We are receiving funds from the Lab Directors R&D (LDRD) program to perform a proof-of-principle experiment to test a scheme for laser-stripping injection

• First experimental tests were carried out in early December

• We observed >50% double-stripping efficiency in first attempt in a one-hour run

• Further R&D will continue, with the goal of developing a realistic laser-based scheme

Laser Beam

H- proton

H0 H0*

Step 1: Lorentz Stripping

Step 2: Laser Excitation Step 3: Lorentz Stripping

High-field Dipole Magnet

High-field Dipole Magnet

H- H0 + e- H0 (n=1) + H0* (n=3) H0* p + e-

Laser-Stripping Injection Proof-of-Principle Experiment

Flipped-sign notch on BCM indicates protons

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Thanks for all the congratulations !!!!

Now he

should

leave…