beam instrumentation performance and plans · 2 managed by ut-battelle for the u.s. department of...
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Beam Instrumentation
Performance and Plans
Alexander Aleksandrov
Beam Instrumentation Group Leader
February 3, 2010
2 Managed by UT-Battellefor the U.S. Department of Energy Presentation_name
SNS Beam Instrumentation Systems are
Numerous and Diverse
RTBT17 Position
26 Loss
4 Current
1 Harp
3 FBLM
1 RTBT Video
CCL/SCL Transition
2 Position and Phase
1 Wire
1 Loss
RING44 Position
54 Loss
1 Current
12 FBLM
2 Video
2 Electron Profile Scanner
2 Transverse feedback system (analog)
SCL32 Position and Phase
32 Loss
8 Laser Wire
24 Neutron Detectors
HEBT29 Position and Phase
26 BLM,
3 FBLM
4 Current
2 BSMs
1 Laser emittance sys
IDump2 Position
1 Wire
6 BLM
2 IDump Video
EDump1 Current
4 Loss
1 Wire
LDump6 Loss
6 Position
1 Wire
CCL10 Position and Phase
8 Wires
8 Loss
1 Faraday Cup
-1 Current (removed)
4 BSMs
10 Neutral Detectors
MEBT6 Position and Phase
2 Current
5 Wires
1 CHUMPS
1 Emittance
DTL10 Position and Phase
5 Wire
4 Loss
5 Faraday Cup
6 Current
18 Neutron Detectors
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Beam Instrumentation Performance and PlansFebruary 22-24, 2009
Outline
• Diagnostics downtime
• New Systems
• Overview of performance improvements upgrades and development progress
– SCL Laser Wire
– Wire Scanners
– Ring Transverse Feedback system
– Laser Stripping Experiment
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Beam instrumentation-related downtime
The old VME BLM IOC processing power was insufficient to perform all desired BLM
functionality. This necessitated partial functionality being distributed to a separate Soft
IOC (IOC without instrumentation hardware).
BLM IOC CPU hardware upgrades have since made this unnecessary.
The Soft IOC functionality has now been rolled back into the VME IOC in order
to reduce system complexity and increase both maintainability and reliability.
• 12 hours for last year
• Mainly related to BLM software upgrade
Soft IOC (Linux PC)
BLM IOC (VME)
Accelerator Network
BLM Detectors
BLM IOC (VME)
Accelerator Network
BLM Detectors
upgrade
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Beam Instrumentation Performance and PlansFebruary 22-24, 2009
New Systems
• 8 HEBT BPMs in operation
• 4 HEBT scrapers read-outs in operation
• 2 MEBT scrapers ` in operation
• 1 MEBT chopper in operation
• 5 Ring Electron Detector read-outs commissioning
• Momentum Dump Diagnostics
– 2 scraper read out commissioning
– 4 Beam Loss Monitors (BLMs) installing
– 1 Wire Scanner (WS) installing
– 1 NanoCurrent Detector (NCD) manufacturing
– 1 Beam Current Transformer (BCM) designing
• Ring Injection Dump Line Upgrade
– 3 BPMs designing
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“In the transverse phase plane, the Laser Wire Scanners are remarkable instruments capable of monitoring transverse beam evolution along the linac and during the pulse. It is regrettable that they cannot presently be used to their full potential, mostly because of stability problems. The committee urges the implementation of the improvements proposed by the beam
instrumentation specialists. ”
AAC’09 Recommendation on Laser Wire
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Laser wire profile scanner
Faraday Cup
Laser
H-
H0
electron
Bending
Magnet
Y-scan
y z
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SCL
1 2 3 4 5 321712 13 14 15
250 m 227 m 25 m160 m
LR Laser room
Laser wire station
Cryomodule number
Camera
Mirror
Power meter32
LR
Ring
Layout of the SCL Laser Wire System
CCLDTL
Target
MEBT
• 4 LW from 200 MeV
• 4 LW from 450 MeV
• 1 LW at 1 GeV
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Periscope box upper mirror – hidden corner –
identified as a major source of the laser
beam vibration
Pipe A: ~ 8 m
Pip
e B
: ~
2.5
m
Mirror
Laser beam
Concrete
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Installed New Mirror Holder
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Feedback Off
-20
0
20
40
60
80
0 100 200 300 400 500 600
Time (sec)
Po
siti
on
(m
m)
0
2
4
6
8
10
Po
wer
(W
)
CAM05_PosY Power Meter 01Feedback Off
-20
0
20
40
60
80
0 300 600 900 1200 1500 1800
Time (sec)
Po
siti
on
(m
m)
0
2
4
6
8
10
Po
we
r (W
)
CAM05_PosY Power Meter01
May 29, 2009 Aug. 12, 2009Beam position Y on Cam5
Laser power measured at LW1
Improvement of laser beam stability
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Profile-Station_02-HORIZ-2009-10-01_16-36-54
0
0.2
0.4
0.6
0.8
1
0 5 10 15 20 25 30 35
Position (mm)
Am
pli
tud
e (V
)
Amp Fit Profile-Station_02-VERT-2009-10-01_16-54-28
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
5 10 15 20 25 30 35 40
Position (mm)
Am
pli
tud
e (V
)
Amp Fit
Profile-Station_01-HORIZ-2009-10-01_17-01-31
0
0.2
0.4
0.6
0.8
1
5 10 15 20 25 30 35 40
Position (mm)
Am
pli
tud
e (V
) Amp Fit Profile-Station_01-VERT-2009-10-01_17-12-53
0
0.2
0.4
0.6
0.8
1
15 20 25 30 35 40 45
Position (mm)
Am
pli
tud
e (V
)
Amp Fit
LW 1
LW 2
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Improvement of profile measurement
(noise reduced by 30-60%)
LW Station # 1 2 3 4 12 13 14 15 32
Previous
run
13.5% (H)
11.0% (V)
12.1
11.8
8.8
10.7
10.0
7.4
7.6
6.8
7.6
6.8
7.3
8.1
6.7
6.8
4.5
4.8
This run
4.2% (H)
5.0% (V)
5.0
4.7
5.4
6.2
6.6
6.6
3.7
3.3
4.3
4.5
3.5
3.5
4.1
4.4
4.1
4.0
STD Measurement Noise
Y. Liu
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Verification of LW data self-consistency
LW 12V Cam17 Pos: (81,88)
Focus Lens
Pos (mm) s_V (mm) Amp_V (V) C_V (mm) E_V (%)
0 3.12 0.94 22.98 5.47
2 3.14 0.89 22.88 3.93
4 3.14 0.79 22.96 4
6 3.18 0.66 23.01 3.98
8 3.17 0.59 23.06 3.49
10 3.14 0.65 22.97 3.28
LW12 Oct.15, 2009
Ion beam power: 800 KW
Laser pulse
energy (mJ) s_H (mm) s_V (mm) Amp_H (V) Amp_V (V) E_H (%) E_V (%) C_H (mm) C_V (mm)
75 2.45 3.07 0.35 0.37 4.9 4.2 19.8 22.95
150 2.46 3.11 0.67 0.64 4.1 4.8 19.76 23.13
225 2.37 3.16 0.9 0.96 4.4 4.1 19.78 23.16
300 2.42 3.13 1.06 1.22 4.3 3.9 19.79 23.02
Beam Center vs. Horizontal Beam Shift
18
20
22
24
26
28
30
32
-6 -4 -2 0 2 4 6
Horizontal Beam Shift (mm)
Mea
sure
d B
eam
Cen
ter
(mm
)
X0 (mm) Y0 (mm)
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Summary of laser wire system status
• Laser Wire system has been improved and verified to give reliable profile measurement.
• Measurement noise has been reduced by 30-60%.
• System is available to AP with help from BIG experts.
• Trained Operation’s Accelerator Specialist in operating the Laser Wire.
• Laser Wire is used often during neutron production
• First Laser Wire journal paper - Laser wire beam profile monitor in the SNS Superconducting linac – published in NIMA.
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On-going efforts
• Laser wire bump compensation magnet (design has been finished, sent out for quotation request).
• Feedback bandwidth improvement (from 1 Hz to 15-30 Hz).
• Laser energy pulse-to-pulse measurement at laser wire station.
• Simultaneous profile measurement at multiple laser wire stations (currently two-station measurement was made available on hardware).
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Laser wire station with the compensation magnet
Magnet for collecting
electrons
Compensating magnet
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Compensating magnet is designed to be connected
to power supply in series with the main magnet
Sent for manufacturing
Plan to install during summer 2010 outage
A. Menshov
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• “…The only possibility to measure transverse beam halo down to the 10-5 level is with the HEBT beam scraper. Transforming this scraper into a fully functional halo monitor is essential to help understand the process of halo formation and minimization….”
– We equipped the HEBT scraper with large dynamic range charge sensitive electronics. AP started to use it ( J. Galambos’s talk)
– We are looking into possibility of increasing measurement dynamic range of all SNS wire scanners
AAC09 Recommendation on large
dynamic range profile measurements
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Limitations in Large Dynamic Range
Measurements with SNS Wire Scanners
Signal in the beam tail is dominated by
the cross-talk between the wires
#1
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Cross-talk between the wires
X
Large separation
between the wires
helps to reduce the
cross talk
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Performance of the CCL WS with diagonal
wire removed
Modified all DTL and HEBT wire scanners during January outage
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• “… In the accumulator ring, the committee is favorably impressed by the preliminary results obtained with the electron scanner and encourages its further development ….”
– Installed magnetic shielding, which improved stability of measurements greatly
– Electron beam energy of 60kV is significant limitation. Initiated collaboration with Budker Institute of Nuclear Physics for increasing operating energy to 100kV
AAC09 Recommendation on ring profile
measurements using electron beam
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Effect of Magnetic Shields on electron beam trace
After shielding: Dipole current at 0 amps (top) and
4000 amps (bottom)
Before shielding: Dipole current at 0 amps (top)
and 4000 amps (bottom)
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Profile measurement repeatability
Twenty profiles taken without changing settings:
– Nice horizontal repeatability
– Still not so great vertical repeatability
W. Blokland
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Electron beam energy is too low
Curvature becomes too strong
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• Status of Large Bandwidth Feedback System for the SNS Ring:
– Tested analog system with beam
– Have demonstrated e-p instability suppression
– Need more study time for better understanding of the system
– Digital controller is on the way
28 Managed by UT-Battellefor the U.S. Department of Energy Presentation_nameTuesday, February 03, 2015
Damper system components in
the ring service building
Amplifier set
Vertical Comb
Filter
Fiber
Optic
Delays
Power
Combiners
Horizontal LLRF
Vertical LLRF
Horizontal
Comb Filter
Broad band 800W amplifier.
1-300 MHz BW
C. Deibele
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Vertical Damper Test Results R. Hardin
OffOn
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New pick up and kicker hardware
Blue = Measured
Red = Simulated
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High power mode-locked laser for laser stripping is
installed in the new laser room
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Laser beam parameters are sufficient for
the next laser stripping experiment
0
0.002
0.004
0.006
0.008
0.01
0.012
0.014
0.016
0.018
0.02
0 2 4 6 8 10
Time (us)
Outp
ut
(volt)
UV power: 2.5 W/macro-pulse
120 uJ/micro-pulse (2.2 MW peak power @ 55 ps)
402.5 MHz
Measured full pulse width: 69 ps (green light).
Estimated UV light pulse width: ~ 55 ps.
Y. Liu
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Beam Instrumentation Performance and PlansFebruary 22-24, 2009
Summary
• Existing Beam Instrumentation is capable to support machine tuning and production runs
• Downtime associated with beam diagnostics is low. Goal is to not exceed 10 hours next year
• Laser wire is brought to routine operation status. Have several improvements in works
• Removing the diagonal wire allowed to demonstrate 10^4 dynamic range on CCL wire scanner. Expanding modification to DTL and HEBT wires.
• Reduction of AP beam time requires Improvement of BI user interface and speed up of measurement
– bringing BSM and MEBT emittance devices to “user friendly” status is main goal for this year