drift chamber for super-belle
DESCRIPTION
Drift chamber for super-Belle. Present performance and background Idea for upgrade Upgrade plan Summary. Shoji Uno (KEK) Jan-20 th , 2003 at Super B-factory WS in Hawaii. Wire chamber. Wire chamber is a good device for the central tracker. - PowerPoint PPT PresentationTRANSCRIPT
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Drift chamber for super-Belle
Present performance and background Idea for upgrade Upgrade plan Summary
Shoji Uno (KEK) Jan-20th, 2003 at Super B-factory WS in Hawaii
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Wire chamber Wire chamber is a good device for the centr
al tracker. Less material Good momentum resolution. Cheap It is easy to cover a large region. Established technology Easy construction. Many layers Provide trigger signals and particle
ID information.
Can the wire chamber survive at S-KEKB? Answer is ” Yes”. My talk and Senyo’s talk.
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Momentum Resolution
Thanks for filling He based gas and using Aluminum field wires.
The resolution was calculated using cosmic ray events during a normal physics run.
BaBar data was obtained from a talk in Vancouver WS.
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dE/dx Resolution
Good resolution was obtained.
It is useful to identify hadrons and electrons.
Bhabha Mu pair
M.I.P in Hadronic events
0.35<P<0.88GeV/cwithout any PID.
Electron
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Hit Rate ~200kHz for inner most layers.
Chamber itself was working. No significant gain degradation wa
s observed for four years operation.
Exceeds 0.2C/cm.
5-10KHz for most of layers. Quite small. The gas chamber can work at 20 ti
mes higher beam background.
Inner most part was replaced with a new chamber in the last summer.
At S-KEKB, it will be covered with a silicon detector.
Layer
Hit
rat
e/w
ire (
k Hz)
CDC
Exp 27 Run 206
HER 1.1ALER 1.5AL=9.6x1033cm-1s-1
MainInner
Cathode
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Total Current Draw of CDC
Total CDC current(8400 wires) has kept about 1mA at the maximum beam current for each years.
Vacuum condition is improving from year to year.
Better masking system has been adopted for fixed masks near IP and movable masks in arc section.
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Radiation Damage Test
a: ’93 Plastic tube d: ’94 SUS tubeb: ’93 Plastic tube + O2 filter e: ’94 SUS tube + O2 filterc: ’94 Plastic tube f: ’94 Plastic tube
Total accumulated charge on sense wire(C/cm)
Gai
n de
grad
atio
n
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Simulation Study for Higher Beam Background
Detail will be reported by K.Senyo.
MC +BGx1 MC+BGx20
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Idea for upgrade In order to reduce occupancy,
Smaller cell sizeMore wires. smaller hit rate for each wire.Shorter maximum drift length shorter maximum drift time.
A new small cell drift chamber was constructed((Maximum drift length is 2.5mm).
Inner most three layers were replaced with the new chamber in the last summer.
Faster drift velocityShorter maximum drift time.
One candidate : 100% CH4 Drift time simulation shows maximum drift time is similar to the present gas due to a large Lorentz angle.
More study
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Small Cell Drift Chamber
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Photo of small cell chamber
Installation in the last summerJust after wire stringing
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XT Curve & Max. Drift Time
Small cell(5.4mm)
Normal cell(17.3mm)
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Drift Velocity
Two candidate gases were tested. CH4 and He-CF4
In case of He-CF4, higher electric field is necessary to get fast drift velocity.
In case of CH4, faster drift
velocity by factor two or more can be obtained, even in rather lower electric field.
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dE/dx Resolution
The pulse heights for electron tracks from 90Sr were measured for various gases.
The resolutions for CH4
and He(50%)-C2H6(50%) are same.
The resolution for He-CF
4 is worse than Ar-based
gas(P-10).
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xt curve for 7mm cell
Distance from wire (cm)
Pure CH4
100nsec
Distance from wire (cm)
Dri
ft ti
me
(se
c)
Dri
ft ti
me
(se
c )
He/C2H6 = 50/50
100nsec
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Wire configuration
9 super-layers : 5 axial + 4 stereo(2U+2V)A 160*8, U 160*6, A 192*6, V 224*6, A 256*6, U 288*6, A 320*6, V 352*6, A 388*8
Number of layers : 58 Number of total sense wires : 15104 Number of total wires : ~60000
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Deformation of endplate
Number of wires increase by factor 2. Larger deformation of endplate is expected. It may cause troubles in a wire stringing process and ot
her occasions.
In order to reduce deformation of endplates, The endplate with a different shape is considered. Wire tension of field wires will be reduced.
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Curved Endplate
Deformation of endplate due to wire tension was calculated at design stage of present Belle CDC.
Deformation(mm) 35.2 2.03 1.31
Present New
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Baseline design
CDC
SVD
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Main parameters
Present FutureRadius of inner boundary (mm) 77 160Radius of outer boundary (mm) 880 1140Radius of inner most sense wire (mm) 88 172Radius of outer most sense wire (mm) 863 1120Number of layers 50 58Number of total sense wires 8400 15104Effective radius of dE/dx measurement (mm) 752 978Gas He-C2H6 He-C2H6
Diameter of sense wire (m) 30 30
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Expected performance
OccupancyHit rate : ~140kHz ~7Hz X 20 Maximum drift time : 80-300nsec Occupancy : 1-4% 140kHz X 80-300nsec = 0.01-0.04
Momemtum resolution(SVD+CDC) Pt/Pt = 0.19Pt 0.30/[%] : Conservative Pt/Pt = 0.11Pt 0.30/[%] : Possible 0.19*(863/1118)2
Energy loss measurement 6.9% : Conservative6.4% : Possible 6.9*(752/869)1/2
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Summary
Present CDC is working well.Good momentum resolution is obtained even for low
momentum range.Energy loss measurement is also good. Beam background is manageable range.
Vacuum condition is still improving.
New CDCSmaller cell size for inner most layers.New gas with a fast drift velocity is preferred.Larger outer radius
Better performance is expected.
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Chamber Gas He(50%)-C2H6(50%)
Longer radiation length(680m).Drift velocity is higher than other He-based gas.
Average drift velocity : ~3.3cm/sec in the chamber cell. Maximum drift time : ~400nsec for 18mm cell size.
Good dE/dx resolution.
Gas systemGas circulation( Flow rate : 3.0 liter/min).Fresh gas( Input flow rate : 0.3 liter/min).Keeping an absolute pressure constant. O2 contamination ~50ppm (with O2 filter)
H2O contamination ~500ppm ( no control )
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Momentum Resolution We could obtain a small
constant term using He-based gas and aluminum field wires.
Slop parameter is not so good as compared with expected value. We had to change the electronics
parameters to reduce the cross talk.
HV is slightly lower than the original value.
Alignment is not perfect. More tuning to reject bad points. Some effects from the beam
background.
Transverse Momentum(GeV/c)
(%)/ PtPt
% /35.028.0:~ PtonlyCDC
%/30.019.0:~ PtSVDCDC
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dE/dx Measurement MQT chip (Charge to T
ime conversion) and multi-hit TDC.
80% truncated mean. Relativistic rise.
1.4 for electron.
Good PID performance for lower momentum region.
dE/dx information helps to separate high momentum K/.
log10P(GeV/c)
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Comparison with Babar
Momemtum resolution(SVD+CDC) Pt/Pt = 0.19Pt 0.30/[%] : Belle
Pt/Pt = 0.13Pt + 0.45 [%] : BaBar
Mass(dE) resolution Mass resolution for inclusive J/
9.6 MeV(Belle) vs 12.3 MeV(BaBar)
dE resolution for B0 D+, D K+ 13.8MeV(Belle) vs 19.0MeV(BaBar)
We could obtain better resolution than BaBar. BaBar has a CFRP support cylinder with 2mm thickness between SVD and CDC.
Tracking efficiency for low momemtum particles is worse than BaBar. D*+D*yield(slow eff.) ~0.5(?) x BaBar 3 layers SVD (Belle) vs 5 layers SVD(BaBar)
Energy loss measurement 5.6%(Belle) vs 7%(Babar) for Bhabar events
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Pulse Height Variation
Total accumulated charge.>0.2 coulomb/cm at inner
most layer for 4 years.
No significant deterioration, so far.
2000
2002
Layer 49
Layer 49
Layer 1
Layer 1
Layer 3
Layer 3
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CH4
Faster drift velocityFactor two faster than He(50%)-C2H6(50%)
Long radiation lengthSame as He(50%)-C2H6(50%)
Good dE/dx resolutionSame resolution is expected from a test using electro
n from 90Sr.
Small radiation damageSimilar performance as He(50%)-C2H6(50%)
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Electron Drift Simulation
Electron drift simulation in gas volume was done by A.Sugiyama of Saga Univ., recently.
He/C2H6=50/50(present gas) and pure CH4 under 1.5 Tesla.
Small cell size(7mm) and normal cell size(18mm)
Maximum drift time for pure CH4 is not shorter than the present gas due to large Lorentz angle.
Simulation shows He/CH4 =50/50 is slightly better than the present gas. Smaller ionization loss Worse spatial resolution and worse dE/dx
resolution?
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Drift line for 7mm cell
He/C2H6 = 50/50 Pure CH4
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Wire configuration
Super-layer structure 6 layers for each super-layer
at least 5 layers are required for track reconstruction. Even number is preferred for preamp arrangement on
support board to shorten signal cable between feed-through and preamp.
Additional two layers in inner most super-layer and outer super-most layer. Higher hit rate in a few layers near wall. Inner most layer and outer most layer are consider as
active guard wire.
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Problems and Cures Cross Talk
Coaxial cable between pin and preamp. Better grounding is also effective. We replaced all cables with coaxial ones in summer 2003. Then, electronics parameter will move back original one.
High background around inner most layer Enlarge inner radius : 7.7cm 16cm Smaller cell size : 8.6mm(64 in ) 6.8mm (160 in ) One inner cylinder No additional wall Inner most layer should be considered as a guard wire(active).
3D Tracking(especially, low momentum tracks) 6(?) layers SVD 6 layers in stereo super layer Better track reconstruction program. Charge division?