Prometeusz Jasinski

Transcription

Prometeusz Jasinski
A Luminosity Detector
for the
PANDA Experiment
at FAIR
Prometeusz Jasinski
on behalf of the PANDA collaboration
25.02.2014
INSTR14 BINP, Novosibirsk
25.02.2014
Prometeusz Jasinski
1
PANDA – Experiment at FAIR
Straw tubes
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2
PANDA – Experiment at FAIR
Straw tubes
High
HighEnergy
EnergyStorage
StorageRing
Ring(HESR)
(HESR)
Beam properties
Beam
properties
(high
luminosity
mode)
(high luminosity mode)
Particles
Particles
Momentum p
Momentum p
Dp/p
Dp/p
Luminosity L
Luminosity L
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Prometeusz Jasinski
Anti-Protons
Anti-Protons
1.5–15 GeV/c
1.5–15 GeV/c
< 1 x 10-4-4
< 1 x 10
2 x 103232cm-2s-2-1-1
2 x 10 cm s
3
PANDA – Experiment at FAIR
Straw tubes
Physics
PhysicsTopics
Topics
Hadron
HadronSpectroscopy
Spectroscopy
Nucleon
NucleonStructure
Structure
Hadrons
HadronsininMatter
Matter
Hypernuclei
Hypernuclei
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Determination of Luminosity
event rate
ΔN
= L⋅σ
Δt
Luminosity
L=
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ΔN 1
⋅σ
Δt
with
Prometeusz Jasinski
cross section
ΔL
<4 %
L
5
Elastic Proton Anti-Proton scattering
pp
pp
c.m.s.
p
q
t
p
q
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Elastic scattering as reference
Measure
Measureatat
small
smallmomentum
momentumtransfers
transfers|t||t|
small
smallscattering
scatteringangles
anglesQQ
→
→ reduction
reductionofofuncertainties
uncertaintiesby
bymodel
model
hadronic
electromagnetic (Coulomb)
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Particle track reconstruction
top view
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Measurement close to the Beam
Requirements
Requirementsfor
forthe
thedetector:
detector:
minimal track distortion by material
minimal track distortion by material
maximum acceptance elastic events
maximum acceptance elastic events
measurement at smallest angles
measurement at smallest angles
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Measurement close to the Beam
Requirements
Requirementsfor
forthe
thedetector:
detector:
Requirements
Requirementsby
bythe
thestorage
storagering:
ring:
minimal track distortion by material
minimal track distortion by material
high vacuum < 10-9-9mbar
high vacuum < 10 mbar
maximum acceptance elastic events
maximum acceptance elastic events
maximum acceptance of the beam
maximum acceptance of the beam
measurement at smallest angles
measurement at smallest angles
slow changes of beam pipe diameter
slow changes of beam pipe diameter
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Vacuum Box Prototype
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Beam Pipe Prototype
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Differential Pumping Scheme
transition region
beam
beam pipe
vacuum box
turbo molecular pump
turbo molecular pump
Scroll fore pump
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First Pumping Tests
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First Pumping Tests
After 2.5 weeks of pumping
6.37·10-8 mbar
4.50·10-7 mbar
Next: Testing with an additional getter pump
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Retractable Detector Halves
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Retractable Detector Halves
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Retractable Detector Halves
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Vacuum Box Deformations
10 µm
420 µm
265 µm
Finite Element Model (FEM)
at a pressure difference of 1 bar
(Inventor 2014)
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Displacement Measurement in Vacuum
Capacitive probes:
Capacitec 208-ACU
2 mm range ~ 40 nm resolution
Aquisition via 18-bit differential ADC
and microcontroller with CAN interface
DCS via Epics: Florian Feldbauer Sat 9:00 am
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Vacuum Box Deformations
10 µm
70 µm
420 µm 1530 µm
simulation vs measurement
265 µm
900 µm
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The Tracking System
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Simulations on cooling
Simulations with up to
7 mW/mm²
43°C
-20°C
clamp
AutoDesk CFD 2014
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Simulations vs. Reality
Testing contact materials for the module clamp and a copper dummy
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Simulations vs. Reality
„worst case“
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A Support Structure as a Heat Sink
Aluminum
Cooling of up to 250 W per plane half
Coolant: -20°C cold Ethanol
frontend electronics attached to the surface
V2A pipe
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Production of Heat Sink Supports
Original idea: LHCb Velo Detector
melting AlMg4.5Mn alloy for
730°C 90 min in argon atmosphere
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Production of Heat Sink Supports
Right now:
Tests of the
cooling performance
in vacuum
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Track Reconstruction
4 planes with distances of 20-10-10 cm in between
(Geant 4 simulation model)
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Material Budget of one Plane
one side of a module
flex cable
Al
Al
resin < 15 µm
polymide 10 µm
resin < 15 µm
Al layer 14 µm
Poly-p-xylylen 5 µm
resin < 15 µm
HV-MAPS
50 µm
resin < 15 µm
CVD-diamond
200 µm
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Prometeusz Jasinski
X/X0 (2 sides) = 0.37%
( eq. 350 µm thick silicon )
35
Resolution at the Detector
Luminosity detector
interaction point
hits
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Resolution after back propagation
Luminosity detector
interaction point
hits
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Fit of the Luminosity at 1.5 GeV/c
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What's next?
Upcoming tests:
- A full cooling circuit at full load
- More on the mechanical precision
- Glued flex print vacuum feed throughs
- Gluing of thin sensors
- Systematic fit studies
Our goal: finalizing our TDR this year!
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Simulations with PANDAROOT (Geant)
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Differential Pumping Sheme
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Cooling stations for cooling liquids
versus
Cooling power @-20°C
1.9 kW
2.2kW
max. pumping speed
105 l/min
45 l/min
max. pumping pressure
2.5 bar(special version)
2.9 bar
Huber Unistate 425 w
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Lauda XT 550 (W)
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Dimensions of the current design
T-cross
BPM
Width: 370 mm
Missing for the full length:
Valves and bellows
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Geometrical Acceptance
Acceptance at 1.5 GeV/c beam momentum
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Connection of cooling pipes and the module supports
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First Pumping Tests
8.66·10-6
2.63·10-2
vacuum box turbo pump off
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