status of the micro vertex detector of the cbm experiment n. bialas 1, n. chon-sen 2, g. claus 2, c....
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Status of the Micro Vertex Status of the Micro Vertex Detector of the CBM ExperimentDetector of the CBM Experiment
N. Bialas1, N. Chon-Sen2, G. Claus2, C. Colledani2, R. De Masi2, M. Deveaux1, D. Doering1, M. Domachowski1, A. Dorokhov2,
C. Dritsa1;2;3, W. Dulinski2, H. Düring2, J. C. Fontaine2, I. Fröhlich1, T. Galatyuk1, M. Goffe2, A. Himmi2, C. Hu2, K. Jaaskelainen2,
M. Koziel2, J. Michel2, F. Morel2, C. Müntz1, S. Ottersbach1, F. Rami2,P. Scharrer11, C. Schrader1, S. Seddiki1;2, M. Specht2, J. Stroth1, T. Tischler1,
C.Trageser1, I. Valin2, F. M. Wagner4, B. Wiedemann2, and M. Winter2
1Institut für Kernphysik, Goethe Universität Frankfurt am Main — 2Institut Pluridisciplinaire Hubert Curien (IPHC), Strasbourg/France — 3GSI, Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt —
4Forschungsneutronenquelle Heinz-Maier-Leibnitz (FRM II), Technische Universität München
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 2
Sensors for the MVD
CBM
wish list
MAPS*
(2003)
MAPS*
(2009)
MIMOSA-26
Binary, 0
Single point res. ~ 5 µm 1.5 µm 1 µm 4 µm
Material budget < 0.3% X0 ~ 0.1% X0 ~ 0.05% X0 ~ 0.05% X0
Rad. hard. non-io. >1013 neq 1012 neq/cm² >3x1013 neq few 1012 neq
Rad. hard. io > 3 Mrad 200 krad > 1 Mrad > 300 krad
Time resolution < 30 µs ~ 1 ms ~ 25 µs 110 µs
Optimized for one parameter Current compromise
Monolithic Active Pixel Sensors(MAPS, also CMOS-Sensors)
• Invented by industry (digital camera)• Modified for charged particle detection since 1999 by IPHC Strasbourg • Also foreseen for ILC, STAR… => Sharing of R&D costs.
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 3
Chapter 1
Sensor R&D
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 4
Radiation hardness studies
Undepleted MAPS
Depleted MAPS
Radiation tolerance of MAPS as function of pixel pitch
Sensor ok if det. eff > 95%
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 5
Sensor R&D: MIMOSA-26
Analog pixel outputs for tests
JTAG slow control On-chipvoltagegenerators
1152 discriminators
zero suppr. logic
Output memories
3 mm
Suited for up to 9 hits/line => ~ 1% occupancy
21.2 x 10.6 mm²18.6 µm pixel pitch
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 6
First analysis resultsFirst analysis results
6
Mimosa26 Spectrum
Mimosa26 Noise
First tests successfully performed at T= -20°C and .
Prelim
inary
D. D
oering
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 7
Comparison standard and depleted sensor
7
0 50 100 150 200 250 300 350 400 450 500 550 600 6500
100
200
300
400
500
600
unirradiated
6 1012 neq/cm²
Ent
ries
in h
isto
gram
Charge collected [ADC]
Depleted sensor 400 Epitaxial layer: 15µm
Fe-554 pixel clusterT=-20°C
Fe-55 4 pixel cluster T=-20°CShift afterirradiation No shift
Very uniform charge collectionproperties but: Strong radiationeffect.
Sensor not uniform (as partiallydepleted): Reduced radiation effect.
D. D
oering
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 8
Sensors for the MVD
CBM
wish list
MAPS*
(2003)
MAPS*
(2009)
MIMOSA-26
Binary, 0
Single point res. ~ 5 µm 1.5 µm 1 µm 4 µm
Material budget < 0.3% X0 ~ 0.1% X0 ~ 0.05% X0 ~ 0.05% X0
Rad. hard. non-io. >1013 neq 1012 neq/cm² >3x1013 neq few 1012 neq
Rad. hard. io > 3 Mrad 200 krad > 1 Mrad > 300 krad
Time resolution < 30 µs ~ 1 ms ~ 25 µs 110 µs
Optimized for one parameter Current compromise
Monolithic Active Pixel Sensors(MAPS, also CMOS-Sensors)
• Invented by industry (digital camera)• Modified for charged particle detection since 1999 by IPHC Strasbourg • Also foreseen for ILC, STAR… => Sharing of R&D costs.
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 9
Annealing studies with combined radiation irradiated MAPSAnnealing studies with combined radiation irradiated MAPS
9
Temperature profile
T[°C]
Time
20°C
80°C
Neutronradiation
1 year
X-rayradiation
Measurementsat T=20°C (280h)
Heating at T=80°C (73h)
Measurements and storage at T=20°C (191h)
2h transport
D. D
oering
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 10
Annealing studies
0 40 80 120 160 200 240 280 320 3600
50
100
150
200
250
300
350
400
450
irradiated with 200 krad X-ray
1013 neq
/cm²
xRay + neutrons no radiationLe
akag
e cu
rren
t [f
A]
Net anneal time [h]
T=20°C T=80°C
-70%
Annealing dims ionizing radiation substantiallyNo trace of reverse annealing (yet) => Recover detector on the fly(?)
D. D
oering
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 11
Chapter 3: Data rates and performances
1 fake hit / hit in the MVD
Measurement of the dark rate of irradiated MIMOSA-18
hits/pixel/readout
M. D
omachow
ski
To be used as input for the MVD-Digitizer
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 12
Chapter 2:
System integration (1)
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 13
Design of a ladder for the MVD
CBM-AcceptanceLow material
5 cm
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 14
Steps of a system integration: The MVD-Demonstrator
Idea
Thermal simulation
CAD-Design
Construction
Power: ~ 1W /cm²
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 15
Achievements:
System design validatedGood noise: 21 e- ENCSpatial res.: < 6µm
Steps of a system integration: The MVD-Demonstrator
Construction
Beamtest @ CERN-SPS(Nov 2009)
signal (a.u.)
Shadow of trigger scintillator
Prelim
inary
Demonstrator project
accomplished
S. A
mar-Y
oucef
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 16
Towards the MVD: HP-2 ULISI
Build an ultra thin ladder. Partners: IPHC, IKF, IMEC
Chip on polyamide: Technology demonstrator by IMEC, Belgium
Build a “prototype” with:• Fast digital sensors• FEE/DAQ for multiple sensors• “Close to real detector” performance
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 17
Towards the MVD: HP-2 ULISI
Diamond 200-300 µm
~ 60(1) -150(2) µm Si
< 200 µm Si
~ 60(1) -150(2) µm Si
~ 320(1)-500(2) µm Si
Polyamide SensorMetal lines
Build an ultra thin ladder.Partners: IPHC, IKF, IMEC
(1) first MVD station(2) last MVD station
Project kick off: Dec. 2009First Prototype: Apr. 2010First results: End 2010
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 18
Chapter 2:
Simulation
.
.
.
.
.
.
.
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 19
Open charm simulation with delta-electrons and pile-up
• Thickness of sensors - Geometry used– Pixel pitch : 18.4 × 18.4 µm2 (From MIMOSA 26)
• Time resolution = 30 µs (MIMOSIS-2)
Station Z [cm]Thickness
[µm]Rinner [mm] Router [mm]
1 5 300 5.5 25
2 10 500 5.5 50
Collision rate(interactions/s)
Collisions/year(mbias)
D0 →π+K-
(generated) *
No pile up 3 ·10 4 1.5·1011 68 000
Pile up 5 1.5 ·10 5 7.5·1011 340 000
C. D
ritsa
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 20
Analogue readout: PV sigma
Pile UpSignal Efficiency
(PV>3)
Background rejection
(PV>3)
0 30.0 % 99.4 %
5 29.8 % 98.0 %
10 30.8 % 92.2 %
C. D
ritsa
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 21
Hit merging and track reconstruction
1: High P track
2: Low P track
MVD STS
• The high P track will be reconstructed first and will “own” the hit.• The track parameters will be slightly modified.• Hit sharing is not implemented in the MVD: The low momentum
track does not “find” the hit. There is a probability to pick up a wrong neighbouring hit (?)
C. D
ritsa
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 22
Open Charm reconstruction
No pile-upC
. Dritsa
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 23
~ 2500 D0
~ 700 D0
Significance
Operating with pile-up seems mandatory but:• Hardware has to be optimized – review detector position and geometry• Pattern recognition should be studied – reduce background
C. D
ritsa
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 24
Chapter 3:
FEE and DAQ
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 25
Data rates for 1.5 x 105 coll/s
Data rate of the sensors was simulated accounting for:
pile-up, delta electrons, clustering,fake hits rates , data protocols....
S. S
eddi
ki
No multiplexers in vacuum vessel (cooling, radiation dose) => more than 200 differential links ( > 10 GB/s compressed data)
100 GB/s for 3D-Sensors
S. S
eddiki
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 26
DAQ-system for the MVD
Slow control:JTAG
Time stampingSensor Control
Data concentrationFPGA based:• Cluster finding (?)• Fake rejection (?)• Pattern recognition (?)
PC interface:4x 3.8 Gbit/s•GPU based data processing•Interface to FLES
All hardware components shown are available (HADES TRBNet)Prototype MVD-DAQ: • Compact radiation hard and vacuum compatible FEE-boards• System validation (Firmware, Data concentration algorithms)• Speed up TRBNet (So far designed for 200 MB/s with 2 Gbit/s links)
C. S
chrader
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 27
Summary and Conclusion
The MVD – demonstrator project was successfully completed.• Readout chain shows good noise performance in beam• Spatial resolution obtained in beam test fits CBM-requirements
The feasibility of open charm reconstruction with pile-up 5 and delta electrons was demonstrated => 1.5 x 105 coll/s with MIMOSIS-2.
• Relatively high background => Improve hit finder, MVD-tracking.• High occupancy: Review mag. field, detector position
Radiation hardness tests are progressing: • Test of MIMOSA-26 HR show first promising results • Annealing tests suggest that ionizing radiation damage can be partially recovered in installed detector.
Outlook: Build prototype with “close to real detector”-performance• Study silicon in polyamide technology => would match material budget goals• Study realistic FEE-DAQ based on Hades TRBNet
M. Deveaux, 15th CBM collaboration meeting , 14th April 2010, GSI 28
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