harold g. kirk brookhaven national laboratory target baseline ids-nf plenary cern march 23-24, 2009
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![Page 1: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/1.jpg)
Harold G. KirkBrookhaven National Laboratory
Target Baseline
IDS-NF Plenary
CERN March 23-24, 2009
![Page 2: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/2.jpg)
Harold G. Kirk
The Neutrino Factory Target Concept
![Page 3: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/3.jpg)
Harold G. Kirk
IronPlug
ProtonBeam
NozzleTube
SC-1SC-2 SC-3 SC-4
SC-5Window
MercuryDrains
MercuryPool
Water-cooledTungsten ShieldMercury
Jet
ResistiveMagnets
Neutrino Factory Study 2 Target Concept
ORNL/VGMar2009
SplashMitigator
Path toward a Target System Design
![Page 4: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/4.jpg)
Harold G. Kirk
Alternative Collection System
Another containment approach includes a shortened Hg container
Drain lines exit cryostat between SC-3 and SC-4
This would trap container in the cryostat, preventing future replacement
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Harold G. Kirk
The Hg Jet Nozzle
Nozzle performance:
The Issue
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Harold G. Kirk
The Jet/Beam Dump Interaction
T. Davonne, RAL
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Harold G. Kirk
Fluka Simulation - Energy deposition in mercury pool with 24GeV beam
How much of the beam energy is absorbed in the beam dump?
T. Davonne, RAL
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Harold G. Kirk
Eruption of mercury pool surface due to 24GeV proton beam
Autodyne simulationSplash following pulse of 20Terra protons
![Page 9: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/9.jpg)
Harold G. Kirk
Splash Mitigation
Study 2 assumed a particle bed of tungsten balls to minimize effects of jet entering pool
Many other feasible concepts to accomplish this function
Simulation/analytical studies may be useful to limit options
Pool circulation and drainage locations also need to be studied
Prototypic testing needed for comparison & final determination
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Harold G. Kirk
Containment Design Requirements
Material compatible with high-field magnets Must also withstand some number of full-power beam
pulses with no Hg in vessel (accident scenario)
Desire no replaceable components
Provide support for Hg weight ~220 liters, 3 metric tons
Sloped (1°-2°) for gravity drain
Overflow drain for 20m/s jet (1.6 liter/s)
Vent for gas transfer
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Harold G. Kirk
Toward a Target Prototype
Esatablish a coherent, engineered design concept
Design and test an improved nozzle Design an Hg handling system Design and test a CW Hg delivery system
Design, fabricate and beam test a target prototype
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Harold G. Kirk
Hg Jet Target Geometry
Previous results: Radius 5mm, θbeam =67mrad Θcrossing = 33mrad
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Harold G. Kirk
The Target/Collection System
Count all the pions and muons that cross the transverse plane at z=50m.
For this analysis we select all pions and muons with 40 < KE< 180 MeV.
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Harold G. Kirk
50GeV Beam-Mesons at 50m
40MeV<KE<180MeV
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Harold G. Kirk
Mesons at 50m
Mesons/Proton Mesons/Proton normalized to beam power
ISS Results reported April, 2006
Fixed Parameters: R=5mm; Beam Angle=67mrad; Jet/Beam = 33mrad
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Harold G. Kirk
Vary the Target Radius
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Harold G. Kirk
Optimized Target Radius 2 to 100 GeV
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Harold G. Kirk
Beam Angle and Jet/Beam Crossing Angle
Beam Angle Crossing Angle
![Page 19: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/19.jpg)
Harold G. Kirk
Mars14 vs Mars15 Comparison
0 20 40 60 80 1000
20000
40000
60000
80000
100000
120000
140000
160000
180000
200000
220000
Mes
ons
Proton Kinetic Energy, GeV
MARS15 MARS14
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Harold G. Kirk
Normalized to Beam Power
![Page 21: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/21.jpg)
Harold G. Kirk
Normalized to Peak
![Page 22: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/22.jpg)
Harold G. Kirk
Summary
Peak meson production efficiency for a Neutrino Factory Hg Target system occurs in the region of 6 to 8 GeV At 20 GeV we have a 25% loss in efficiency At 40 GeV we have a 45% loss in efficiency At 80 GeV we have a 50% loss in efficiency
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Harold G. Kirk
Backup Slides
![Page 24: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/24.jpg)
Harold G. Kirk
Optimized Target Parameters
Target Radius Beam Angle
Beam/Jet Crossing angle
![Page 25: Harold G. Kirk Brookhaven National Laboratory Target Baseline IDS-NF Plenary CERN March 23-24, 2009](https://reader031.vdocuments.site/reader031/viewer/2022032310/56649d535503460f94a2ef96/html5/thumbnails/25.jpg)
Harold G. Kirk
Optimized Target Parameters
Target Radius Proton Beam Angle
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Harold G. Kirk
Beam/Jet Crossing Angle
!
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Harold G. Kirk
Meson Production Normalized to Beam Power
!
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Harold G. Kirk
Process mesons through Cooling
Consider mesons within acceptance ofε┴ = 30π mm and εL = 150π mmafter cooling
180 MeV
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Harold G. Kirk
Compare 50m to Post-Cooling
!
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Harold G. Kirk
Step 1: Vary the Target Radius
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.022000
24000
26000
28000
30000
32000
10GeV Beam at 67mrad beam angle and 33mrad beam/jet crossing angle
Mes
ons
Target Radius, cm
Positives+Negatives Polynomial Fit(3rd order)
Rmax=0.48cm
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Harold G. Kirk
Proton Driver Parameters
Proton driver power: 4 MW
Proton driver repetition rate: 50 Hz
Proton energy: around 10 GeV
3 proton bunches in train 1.7×1013 protons per bunch at 10 GeV
Bunch length 1–3 ns
Train length at least 200 μs
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Harold G. Kirk
Optimizing Soft-pion Production
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Harold G. Kirk
Step 2: Vary the Beam Angle
20 40 60 80 100 120 140 160 180 200 22016000
18000
20000
22000
24000
26000
28000
30000
32000
10GeV Beam-Mesons at 0.48cm target radiusand 33mrad beam/jet crossing angle
Positives+Negatives Polynomial Fit (3rd Order)
Mes
ons
Beam Angle, mrad
beam=89mrad
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Harold G. Kirk
Step 3: Vary the Beam/Jet Crossing Angle
10 20 30 40 50 60
28000
29000
30000
31000
32000
33000
10GeV Beam at 0.48cm target radius and 89mrad bem angle
Mes
ons
Angle between Beam and Jet, mrad
Positives+Negatives Polynomial Fit(3rd order)
crossing=25mrad
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Harold G. Kirk
Post-cooling 30π Acceptance