Beam Induced Fluorescence (BIF) Monitor for Transverse...
Transcript of Beam Induced Fluorescence (BIF) Monitor for Transverse...
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BBeam eam IInducednduced FFluorescenceluorescence ((BIFBIF) Monitor) Monitorfor Transverse Profile Determination for Transverse Profile Determination of 5 to 750 MeV/u Heavy Ion Beamsof 5 to 750 MeV/u Heavy Ion Beams
F. Becker1, C. Andre1, P. Forck1, D.H.H. Hoffmann1,2
1) Gesellschaft für Schwerionenforschung mbH GSI, Darmstadt2) Technische Universität Darmstadt
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OutlineOutline
• Introduction– Detectors for high beam power– BIF-detection principle
• Experiment– Setup– Data Analysis– Results
• Conclusion
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Comparison of Profile MonitorsComparison of Profile Monitors
HV−electrode
IPM with 175 x 175 mm clearance
300 mm flange
MCP: 100 x 30 mm
63 wires, 2 mm spacing
beam2
Secondary-Electron-Monitor (SEM) Grid+ Standard tool, compact design+ Low background level- Limited spacial resolution (wire spacing)-- Melts in high power beams!
Residual Gas Monitor (RGM)+ Non-intercepting monitoring+ Measures even high power beams+ Very sensitive a used in synchrotrons- Lot of mechanics inside vacuum
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Beam Beam InducedInduced Fluorescence (Fluorescence (BIFBIF))
ION beam
Blackened wallsVacuum gauge
Valve
Viewport
150mm flange
LensImage-IntensifierCCD FireWire-Camera
N2 as fluorescent gasequally distributed
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How a Profile is obtainedHow a Profile is obtained
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How a Profile is obtainedHow a Profile is obtained
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How a Profile is obtainedHow a Profile is obtained
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Advantages of Advantages of BIFBIF
25 cmShort insertion length
No mechanics in the vacuum
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Advantages of Advantages of BIFBIF
25 cmShort insertion length
No mechanics in the vacuum
Reproduction scale can be matched by the focal distance.
Image intensifier performs single photon detection.
12-bit VGA camera with digital fire-wire interface.
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Advantages of Advantages of BIFBIF
25 cmShort insertion length
No mechanics in the vacuum
Reproduction scale can be matched by the focal distance.
Image intensifier performs single photon detection.
12-bit VGA camera with digital fire-wire interface.
Commercial Components
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Detection PrincipleDetection Principle
Photon
Fiber optics
VG
A-C
AM
CCD
UV-enhanced S-20photocathode
Fast P-46 phosphor-screen (blue-light)
Solid angle limitedby viewport-apperture
Wide-angle lens system
Ω
Atomic collisions N2
+ ⇔Beam Ions.Excitating vibration-levels, 391 nm, 427 nm, ...
V-stack MCPHV a gain ~ 106
Single photon detection!
BEAM
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Expected Photon YieldExpected Photon Yield
nn sprojectileIon
photons ldl
ZpdEπ
β4
),,( 2 Ω∆∝
~ integration time~ number of particles per pulse
l∆Ω depends on setup geometry
SYNC/ Low energy lossHEBT: typical: 60-2000 MeV/u
1010 particles per cycle
LINAC: High energy losstypical: 5-11 MeV/u2,5 mA ~ 1012 particles pp.
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Areas of ApplicationAreas of Application
beam direction
viewport size
aver. pixel int.
beam direction
viewport size
aver. pixel int.
Detection-efficiency adjusted by pressure
LINAC: 2,5 mA ~ 1011 Ar10+
@4,4 MeV/u
p=5 10-6 mbarsingle shot
SYNC-HEBT: 2,3 109 Xe48+ @200 MeV/u
p=10-3 mbaraveraged over 20 shots
- Background is larger at HEBT energies
+ Application had been proven!
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Areas of ApplicationAreas of Application
beam direction
viewport size
aver. pixel int.
beam direction
viewport size
aver. pixel int.
Detection-efficiency adjusted by pressure
LINAC: 2,5 mA ~ 1011 Ar10+
@4,4 MeV/u
p=5 10-6 mbarsingle shot
SYNC-HEBT: 2,3 109 Xe48+ @200 MeV/u
p=10-3 mbaraveraged over 20 shots
- Background is larger at HEBT energies
+ Application had been proven!
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Pressure Variation
Signal amplitude increases proportional to p
For higher beam intensities lower pressures should be sufficient!
LINAC: 1E10 Ni(6+) @ 4.54 MeV/u and p=1E-6 mbar to p=1E-3 mbar
HEBT: 2E9 Xe(48+) @ 200 MeV/u and p=1E-3 mbar to p=1E-6 mbar
p changed by 6 orders of magnitude
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Pressure Variation
Signal amplitude increases proportional to p
For higher beam intensities lower pressures should be sufficient!
LINAC: 1E10 Ni(6+) @ 4.54 MeV/u and p=1E-6 mbar to p=1E-3 mbar
HEBT: 2E9 Xe(48+) @ 200 MeV/u and p=1E-3 mbar to p=1E-6 mbar
p changed by 6 orders of magnitude
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Pressure VariationPressure Variation
p changed by 6 orders of magnitude
LINAC: 1E10 Ni(6+) @ 4.54 MeV/u and p=1E-6 mbar to p=1E-3 mbar
HEBT: 2E9 Xe(48+) @ 200 MeV/u and p=1E-3 mbar to p=1E-6 mbar
Profile width remains constant → p is suitable parameter to match signal strength!
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Energy VariationEnergy VariationIntegrated signal amplitude scales with Bethe-Bloch function.Good accordance for all ions normalized by their charge and mass with respect to U73+
Background level encreases with approximately E2.It is generated by thermal NEUTRONShitting the photo-cathode.
Signal to background ratio decreases two oders of magnitude.Short gating during fast extraction improves the ratio by a factor 4, for Xe and Ta.
a Background reduction is major challange!
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Energy VariationEnergy VariationIntegrated signal amplitude scales with Bethe-Bloch function.Good accordance for all ions normalized by their charge and mass with respect to U73+
Background level encreases with approximately E2.It is generated by thermal NEUTRONShitting the photo-cathode.
Signal to background ratio decreases two oders of magnitude.Short gating during fast extraction improves the ratio by a factor 4, for Xe and Ta.
60 MeV/u
350 MeV/u
750 MeV/u
a Background reduction is major challange!
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Background DistributionBackground Distribution
- Neutron ´afterglow´ longerthan µs beam delivery
- Simulation and experimentagree well!
⇒ Reduction by short gating (improvement: factor 4)
Simulation by PHITS:
- Neutrons are backscatteredfrom walls
- Neutron flux in whole cave
⇒ Reduction by moderation and absorbtion in shielding
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Shielding ConceptShielding Concept
Effective neutron SHIELDING: Moderation and Absorbtion
Distance extension by ~1 millionfiberoptics boundlewithout loosing solid angle!
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Shielding ConceptShielding Concept
Effective neutron SHIELDING: Moderation and Absorbtion
Distance extension by ~1 millionfiberoptics boundlewithout loosing solid angle!
Commercial Systems →
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How Excitation affects ProfilesHow Excitation affects Profiles
IonXN +Σ)( 12
vr
IoneBN u ++Σ −++ )( 22
vr+
)471390()( 22 nmXN g ≤≤+Σ++ λγ
hE∆
=υphoton
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How Excitation affects ProfilesHow Excitation affects Profiles
IonXN +Σ)( 12
vr
)471390()( 22 nmXN g ≤≤+Σ++ λγ
hE∆
=υphoton
IoneBN u ++Σ −++ )( 22
vr+
Vibrational spectrum [Huges, Philpot 1961]for 100 keV protons.Strongest lines at 391,4 nm and 427,8 nm.Optical glasses + photocathode have to be UV-enhanced. ~60 ns lifetime.
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How Excitation affects ProfilesHow Excitation affects Profiles
IonXN +Σ)( 12
vr
)471390()( 22 nmXN g ≤≤+Σ++ λγ
hE∆
=υphoton
IoneBN u ++Σ −++ )( 22
vr+
Vibrational spectrum [Huges, Philpot 1961]for 100 keV protons.Strongest lines at 391,4 nm and 427,8 nm.Optical glasses + photocathode have to be UV-enhanced. ~60 ns lifetime.
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Fluorescence LevelsFluorescence Levels
Contribution of fluorescence levels remains constant up to p=10-3 mbar
Contribution by 2-step excitation can be neglected!
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ConclusionConclusion
• General functionality of BIF had been proven!– Profile determination in SINGLE PASS MODE!
• Careful investigation concerning:– Signal strength → linear with p, Bethe-Bl. with E– Profile width → constant with p– Background contribution → ~E2, neutron shielding– Fluorescence levels → even for high p no distortion
• Future Improvements:– Optimizing geometry, lens, intensifier and camera– Development of shielding using fiberoptics bundle– Further investigation to establish BIF as standard tool!
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Thank You
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