The Silicon Inner Tracker for LHCb - LHCb - CERN
The Silicon Inner Tracker for LHCb - LHCb - CERN The Silicon Inner Tracker for LHCb - LHCb - CERN
LHCb Inner Tracker Memo 2002-003 8 International Conference on Instrumentation for Colliding Beam Physics ¡ Novosibirsk — February 28 - March 06, 2002 The Silicon Inner Tracker for LHCb ¢ ¢ ¢ ¢ Olaf Steinkamp Requirements and Layout Silicon Sensors and Ladders Read-Out Chip Outlook Physik Institut der Universität Zürich Winterthurerstrasse 190 CH-8057 Zürich olaf.steinkamp@physik.unizh.ch
- Page 2 and 3: LHCb Experiment Dedicated experimen
- Page 4 and 5: ( largest station 6 m 5 m ) Inner T
- Page 6 and 7: Radiation Dose and Particle Fluxes
- Page 8 and 9: Design aims: Sensor Support simple,
- Page 10 and 11: ¡ four-layer Amoco K1100 shelf dum
- Page 12 and 13: leakage current [nA] 3000 2500 2000
- Page 14 and 15: As function of efficiency 1 0.95 0.
- Page 16 and 17: 110mm 108mm Region Strips Pitch Wid
- Page 18 and 19: Beetle 1.1 Total Ionizing Dose Irra
- Page 20 and 21: Beetle 1.2, submission April 2002:
- Page 22 and 23: Read-Out Link Readout rate (L0-trig
- Page 24: Main requirements: 22 cm long ladde
<strong>LHCb</strong> <strong>Inner</strong> <strong>Tracker</strong> Memo 2002-003<br />
8 International Conference<br />
on Instrumentation <strong>for</strong> Colliding Beam Physics<br />
¡<br />
Novosibirsk — February 28 - March 06, 2002<br />
<strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong><br />
¢<br />
¢<br />
¢<br />
¢<br />
Olaf Steinkamp<br />
Requirements and Layout<br />
<strong>Silicon</strong> Sensors and Ladders<br />
Read-Out Chip<br />
Outlook<br />
Physik Institut der Universität Zürich<br />
Winterthurerstrasse 190 CH-8057 Zürich<br />
olaf.steinkamp@physik.unizh.ch
<strong>LHCb</strong> Experiment<br />
Dedicated experiment <strong>for</strong> B-physics at LHC<br />
CP Violation and rare decays<br />
production at LHC strongly <strong>for</strong>ward peaked<br />
¡<br />
Special attention on:<br />
<strong>for</strong>ward spectrometer 250 mrad ¢ 300 mrad<br />
£ vertexing: VELO ( ¤ talk by J.Libby )<br />
£ particle identification: RICH detectors ( ¤ talk by C.Matteuzzi )<br />
£<br />
£<br />
triggering: VELO, calorimeters, muon detector<br />
tracking, momentum reconstruction: dipole spectrometer<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
<strong>LHCb</strong> Spectrometer<br />
4 Tm dipole magnet ( bending plane horizontal )<br />
Nine planar tracking stations<br />
positions optimized <strong>for</strong> “upstream” tracking<br />
Each station four detection layers<br />
δp/p (per mille)<br />
8<br />
7<br />
6<br />
5<br />
4<br />
3<br />
2<br />
1<br />
0<br />
wire/strip orientation vertical, +5 ¡ , -5 ¡ , vertical<br />
optimized <strong>for</strong> momentum resolution, pattern recognition<br />
0 20 40 60 80 100 120 140 160 180 200<br />
p (GeV)<br />
– track reconstruction efficiency ¢ 95 %<br />
<strong>for</strong> B decay tracks<br />
– average momentum resolution £ 0.4 %,<br />
dominated by mult.scatt. up to 100 GeV<br />
¤<br />
watch material budget!<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
( largest station 6 m<br />
5 m )<br />
<strong>Inner</strong> <strong>Tracker</strong>: cross-shaped layout<br />
¡<br />
¡<br />
¡<br />
¡<br />
¡<br />
four detector boxes<br />
each box four detection layers<br />
each layer seven silicon ladders<br />
each ladder two 6” silicon sensors<br />
¤<br />
total surface 9 stations 14 m£<br />
Tracking Stations<br />
©<br />
Track density strongly <strong>for</strong>ward peaked<br />
¡<br />
¡<br />
¡<br />
¡<br />
¡<br />
up to 10¢<br />
charged part./ cm£<br />
near beam pipe<br />
falling off with ¤<br />
each station: two detector technologies<br />
borderline determined by track density<br />
“Outer <strong>Tracker</strong>”: straw drift chambers<br />
¦¨§ ¥<br />
“<strong>Inner</strong> <strong>Tracker</strong>”: silicon-strip detector<br />
34.53 52.9 34.53<br />
121.96<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp<br />
21.8<br />
59.76
Fraction of charge<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0.7523E-02/ 11<br />
P1 0.9481<br />
P2 31.20<br />
P3 61.79<br />
0<br />
0 25 50 75 100 125 150 175 200 225<br />
Position<br />
Amplitude, a. u.<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0<br />
Detector Simulation<br />
GEANT description of active and dead material<br />
Digitization within <strong>LHCb</strong> Gaudi framework:<br />
0 20 40 60 80<br />
Time, ns<br />
signal generation<br />
charge sharing ( from laser tests )<br />
amplifier response ( from Beetle prototype )<br />
gaussian noise<br />
clustering<br />
Cluster size<br />
3<br />
2.5<br />
2<br />
1.5<br />
1<br />
0.5<br />
0<br />
0 2 4 6 8 10 12<br />
Station number<br />
0.07<br />
0.06<br />
0.05<br />
0.04<br />
0.03<br />
0.02<br />
0.01<br />
0<br />
0 2 4 6 8 10 12<br />
eta function signal shape cluster size occupancies<br />
Occupancy<br />
Station number<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Radiation Dose and Particle Fluxes<br />
Detailed Fluka description of detector<br />
and cave<br />
careful analysis of <strong>Inner</strong> <strong>Tracker</strong> region<br />
to be done<br />
From previous study:<br />
integrated dose 20 Mrad<br />
5 ¡<br />
£¥¤<br />
¢<br />
¦<br />
1-MeV equiv. neutrons / cm§<br />
after 10 years of operation in hottest spot<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Cost read-out electronics:<br />
“long” ladders, “large” pitch<br />
Tracking per<strong>for</strong>mance, station layout:<br />
22 cm long ladders<br />
readout pitch about 250¡ m<br />
Material budget:<br />
“thin” sensors<br />
LHC bunch crossing frequency:<br />
<strong>Silicon</strong> Sensor Design<br />
shaping time 25 ns to avoid pile-up<br />
¢<br />
small £<br />
/¤<br />
Radiation environment:<br />
¥<br />
5<br />
§©¨<br />
¦<br />
to minimize capacitance<br />
1-MeV equiv. n / cm<br />
/ year<br />
locally ( not our biggest worry ) <br />
<br />
<br />
<br />
110<br />
108<br />
78<br />
76<br />
135<br />
150<br />
Technology p<br />
<br />
-on-n<br />
Thickness 320 m<br />
Sensitive 108 mm 76 mm <br />
Number strips 320 (384)<br />
Strip pitch 237.5 m (198 m)<br />
Implant width 0.2 <br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp<br />
<br />
<br />
0.3
Design aims:<br />
Sensor<br />
Support<br />
simple, robust construction<br />
modularity<br />
material budget<br />
cooling ( sensors at -5<br />
¡<br />
C )<br />
Ladder Design<br />
Pitch Adaptor<br />
Front−End Chip<br />
Layout:<br />
Readout Hybrid<br />
Balcony<br />
U-shaped carbon-fibre support<br />
ceramic pitch adaptor<br />
kapton read-out hybrid<br />
cooling “balcony”<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
2.5<br />
Detector Box Design<br />
78<br />
one box <strong>for</strong> four detection layers<br />
common “cooling plate” carrying<br />
cooling pipe<br />
thermal contact and positioning via<br />
individual balconies<br />
cold, dry nitrogen atmosphere<br />
insulation box (not shown)<br />
– light-weight foam <strong>for</strong> thermal<br />
insulation<br />
– thin aluminium foil <strong>for</strong> electrical<br />
shielding<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
¡<br />
four-layer Amoco K1100 shelf<br />
dummy silicon sensors and hybrid<br />
Kapton heat elements<br />
Ladder Prototype<br />
temperature probes / thermal camera<br />
test mechanical and thermal properties<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Detector Box Prototype<br />
¤<br />
First prototype <strong>for</strong> thermal tests:<br />
box from mold-injected polyurethane<br />
foam<br />
C¡ F¢ £<br />
liquid cooling<br />
aluminium cooling plate / balconies<br />
mock-up ladders with kapton heat elements<br />
validate cooling concept<br />
Next: identify low-weight materials<br />
balconies magnesium matrix composite<br />
(magnesium-infiltrated carbon fibres)<br />
cooling plate carbon-carbon material<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
leakage current [nA]<br />
3000<br />
2500<br />
2000<br />
1500<br />
1000<br />
500<br />
0<br />
1st Prototype Sensors from SPA-Detector, Kiev<br />
0 20 40 60 80 100 120 0<br />
bias voltage [V]<br />
p¡<br />
-on-n, 300 m thick ¢<br />
64 strips, 6.66 cm long, 240 m pitch ¢<br />
implant width 48, 60, 72 m ¢<br />
fast turnaround, attractive price!<br />
sensors work fine, except junction<br />
breakdown at too low bias voltages<br />
signal right strip [mV]<br />
200<br />
150<br />
100<br />
50<br />
£<br />
IR laser test<br />
80 V<br />
¤¥<br />
§ ¦<br />
0 50 100 150 200<br />
signal left strip [mV]<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp<br />
¨
N<br />
6000<br />
4000<br />
2000<br />
£<br />
1st Test Beam with SPA Prototype Sensors<br />
resolution:<br />
m<br />
¢<br />
¥ ¤<br />
¦<br />
Constant 4870.<br />
Mean -0.2990E-02<br />
Sigma 0.1959<br />
0<br />
-2 -1 0 1 2<br />
Δ [strips]<br />
Cluster Charge [ADC]<br />
9 GeV pions ( <strong>CERN</strong>-T7 test beam )<br />
one-sensor and three-sensor ladders<br />
¡<br />
6.7 cm and 20 cm long<br />
unirradiated sensors at room temp.<br />
Helix read-out chip (HERA-B)<br />
¡<br />
30<br />
20<br />
10<br />
¢<br />
fastest shaping time 50 ns<br />
short ladder<br />
long ladder<br />
0<br />
0 100 200<br />
trigger delay [ns]<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
As function of<br />
efficiency<br />
1<br />
0.95<br />
0.9<br />
0.85<br />
Detection Efficiency 20 cm-long Ladder<br />
sensor 2 w/p=0.2<br />
¡¢<br />
( <strong>for</strong> £<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
As function of £<br />
efficiency<br />
1.02<br />
1<br />
0.98<br />
0.96<br />
¡¢<br />
80 V w/p=0.2<br />
¨<br />
0.2<br />
0.94<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
£<br />
¤¥<br />
§ ¦<br />
¨<br />
¤¥<br />
§ ¦<br />
( <strong>for</strong><br />
efficiency<br />
1.02<br />
0.98<br />
0.96<br />
80 V £<br />
1<br />
¡¢<br />
¤¥<br />
§ ¦<br />
efficiency<br />
¨<br />
1<br />
0.95<br />
0.9<br />
0.85<br />
¨<br />
90 V w/p=0.2<br />
90 V ):<br />
sensor 2 w/p=0.25<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
0.2 ):<br />
0.94<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
¤¥<br />
§ ¦<br />
¨<br />
¡¢<br />
¨<br />
efficiency<br />
90 V £<br />
0.25<br />
1.02<br />
1<br />
0.98<br />
0.96<br />
100 V w/p=0.2<br />
efficiency<br />
1<br />
0.95<br />
0.9<br />
0.85<br />
0.94<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
¤¥<br />
§ ¦<br />
¨<br />
sensor 2 w/p=0.3<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
efficiency<br />
100 V £<br />
¡¢<br />
1.02<br />
1<br />
0.98<br />
0.96<br />
¨<br />
0.3<br />
110 V w/p=0.2<br />
0.94<br />
0 0.2 0.4 0.6 0.8 1<br />
track position<br />
¤¥<br />
§ ¦<br />
¨<br />
110 V<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
S/N<br />
60<br />
40<br />
20<br />
Charge Collection Efficiency<br />
0<br />
30 31 32 33 34 35<br />
strip number<br />
S/N<br />
60<br />
40<br />
20<br />
0<br />
30 31 32 33 34 35<br />
strip number<br />
one-strip clusters two-strip clusters<br />
Reduced charge collection efficiency in between strips<br />
¢¤£<br />
effect decreases ¡<br />
with increasing<br />
effect decreases with increasing overbiassing<br />
Interpretation:<br />
Cure:<br />
low-field region in between strips<br />
charges get trapped or arrive too late ( fast shaping time! )<br />
( simulation in preparation )<br />
optimized strip geometry<br />
higher overbiassing<br />
¥<br />
new sensors with better HV per<strong>for</strong>mance !<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
110mm<br />
108mm<br />
Region<br />
Strips<br />
Pitch<br />
Width<br />
Prototype Sensors from Hamamatsu<br />
38mm<br />
78mm<br />
76mm<br />
A B C D E<br />
1−64 65−128 129−192 193−272 273−352<br />
197.9 197.9 197.9 237.5 237.5<br />
50 60 70 70 85<br />
<br />
<br />
Full-size multi-geometry sensors:<br />
p¡<br />
-on-n, 320 ¢ m thick<br />
198 ¢ m and 237.5 ¢ m pitch<br />
£¤<br />
¥<br />
¦<br />
§<br />
¨©<br />
Sensors received last Friday:<br />
¦<br />
testbeam at <strong>CERN</strong> end May<br />
£¤<br />
<br />
select strip geometry <strong>for</strong> <strong>LHCb</strong><br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Beetle Readout Chip<br />
128-channel pipelined r/o chip, custom design at ASIC lab Heidelberg<br />
basic RD20 front-end architecture<br />
0.25 m CMOS ¡<br />
analog and binary pipeline<br />
prompt binary readout<br />
programmable via I<br />
¢<br />
C interface<br />
<strong>LHCb</strong> front-end requirements<br />
40 MHz sampling rate<br />
1 MHz read-out rate<br />
160 cell analog pipeline<br />
16 event internal buffer<br />
900 ns max. read-out time<br />
Beetle 1.1 submitted March 2001<br />
Test<br />
Input<br />
Analog<br />
In<br />
6.1 mm<br />
Itp<br />
Testpulse<br />
Generator<br />
Vfp<br />
Ipre<br />
preamplifier<br />
128 Analogue Input Pads<br />
FETestOut PipeampTestOut<br />
Vfs<br />
Isha Ibuf<br />
shaper<br />
Vfp<br />
Vfs<br />
Ipre<br />
Isha<br />
Ibuf<br />
Icomp<br />
Ithmain<br />
Ithdelta<br />
Itp<br />
Frontend<br />
Bias−Generator<br />
Frontend Amplifiers<br />
Comparators<br />
buffer<br />
Testchannel<br />
Pipeline<br />
Control<br />
comparator<br />
Polarity<br />
Icomp<br />
Ithmain<br />
Ithdelta<br />
5.5 mm<br />
D Q<br />
CompClk<br />
1 of 160+16+10 cells<br />
Write<br />
Read<br />
I2C Interface<br />
Pipeline<br />
Pipeline/<br />
Readout<br />
Control<br />
pipeline<br />
Vd<br />
Or Mux LVDS @ 80 MHz<br />
Vdcl<br />
Ivoltbuf<br />
Vd<br />
Dummy channel<br />
1 of 128 channels<br />
pipeline<br />
readout−amplifier<br />
Vdcl<br />
Reset<br />
Reset<br />
Ipipe Ivoltbuf<br />
1 of 16 channels<br />
CompOut<br />
notCompOut<br />
Ipipe<br />
Icurrbuf<br />
Isf<br />
Backend<br />
Bias−Generator<br />
multiplexer<br />
4 x (32 to 1)<br />
Isf<br />
current<br />
buffer<br />
Icurrbuf<br />
Out[3:0]<br />
notOut[3:0]<br />
8 Comparator Outputs<br />
Pipeline Readout<br />
Amplifiers<br />
Multiplexers<br />
Backend Bias Block<br />
8 Comparator Outputs<br />
Frontend Bias Block<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Beetle 1.1 Total Ionizing Dose Irradiation<br />
Four chips irradiated at <strong>CERN</strong> X-ray facility<br />
[V]<br />
full functionality up to 45 Mrad<br />
trigger / readout and slow control<br />
per<strong>for</strong>mance degradation small<br />
0.14<br />
0.12<br />
0.1<br />
0.08<br />
0.06<br />
0.04<br />
0.02<br />
0<br />
−0.02<br />
0 Mrad<br />
15 Mrad<br />
30 Mrad<br />
45 Mrad<br />
−0.04<br />
0 25 50 75 100<br />
time [ns]<br />
125 150 175 200<br />
Pulse shape at C¡<br />
£ ¤ ¢<br />
¥<br />
[%]<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
Cp = 3 pF<br />
Cp = 7 pF<br />
Cp = 10 pF<br />
Cp = 13 pF<br />
Cp = 25 pF<br />
Cp = 36 pF<br />
0 5 10 15 20 25 30 35 40 45<br />
dose [Mrad]<br />
¦pF Amplitude remainder after 25 ns<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
45<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
0<br />
1st Test Beam with Beetle 1.1 Read-Out Chip<br />
resolution:<br />
¢¤£<br />
¥¦<br />
§ m<br />
-0.04 -0.02 0 0.02 0.04<br />
Residual [cm]<br />
¡<br />
120 GeV muons ( <strong>CERN</strong>-X7 test beam )<br />
SPA prototype sensor ladders<br />
6.7 cm and 20 cm long<br />
successful, reliable operation of chips<br />
14<br />
12<br />
10<br />
8<br />
6<br />
4<br />
2<br />
( S / N limited by DAQ setup )<br />
0<br />
150 151 152 153 154 155 156 157 158 159<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Beetle 1.2, submission April 2002:<br />
few bug fixes<br />
SEU redundant logic<br />
fully differential output driver<br />
improved front-ends<br />
Beetle — Next Steps<br />
Measured on test chips (Beetle-FE 1.1):<br />
remainder after 25 ns<br />
ENC<br />
§<br />
<br />
¡<br />
30% <strong>for</strong> ¢<br />
¨©<br />
<br />
S/N §<br />
<br />
<br />
<br />
<br />
<br />
<br />
£<br />
¥ ¦ ¤<br />
<br />
up to 30 pF<br />
<br />
¢<br />
£<br />
¥ ¦ ¤<br />
/ pF<br />
<strong>for</strong> 22 cm long ladder<br />
gain (1 MIP = 23.200e) [mV]<br />
ENC [e]<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
3000<br />
2500<br />
2000<br />
1500<br />
1000<br />
BeetleFE 1.1 - Set 2c<br />
(Vfp=0V, Vfs=0V, Ipre=600uA, Isha=80uA, Ibuf=80uA)<br />
cp = 0pF<br />
cp = 3pF<br />
cp = 10pF<br />
cp = 20pF<br />
cp = 30pF<br />
cp = 40pF<br />
0 50 100<br />
time [ns]<br />
500<br />
ENC BeetleFE 1.1 - Set 2c<br />
(Vfp=0V, Vfs=0V, Ipre=600uA, Isha=80uA, Ibuf=80uA)<br />
0<br />
0 10 20<br />
cp [pF]<br />
30 40<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Read-Out Hybrid<br />
Four-layer kapton hybrid <strong>for</strong> three Beetle chips<br />
1. digital/analog power 3. traces<br />
2. digital/analog ground 4. components<br />
Two-layer “tails” <strong>for</strong> control signals and read-out of analog signals<br />
Separate pitch adaptor ( thin-film ceramic? )<br />
prototypes in production<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
Read-Out Link<br />
Readout rate (L0-trigger accept rate): 1.1 MHz<br />
Beetle output: 4¡<br />
40 MHz analog<br />
8-bit digitization:<br />
1.28 Gbit/s per Beetle, 3.84 Gbit/s per ladder, 134 Gbit/s per Box<br />
Design criteria read-out link:<br />
radiation hardness components, material budget, cost<br />
BEETLE<br />
40 MHz<br />
analog<br />
FADC<br />
FADC<br />
FADC<br />
FADC<br />
8<br />
8<br />
8<br />
8<br />
<strong>CERN</strong> GOL<br />
1 of 12<br />
12x VCSEL<br />
fibre transmitter<br />
5−10 m<br />
<strong>Silicon</strong> ladder Service box on Outer <strong>Tracker</strong> frames<br />
19,2 Gbit/s<br />
digital<br />
100 m<br />
to counting room<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp
¡<br />
“<strong>LHCb</strong>-Light”<br />
Common ef<strong>for</strong>t <strong>for</strong> overall re-optimization of <strong>LHCb</strong> detector<br />
Two major changes to tracking system under investigation:<br />
a) reduce number of tracking stations<br />
improved per<strong>for</strong>mance<br />
due to lower material budget<br />
baseline scenario: four stations<br />
very promising results<br />
¡<br />
8.84<br />
23.17 52.9 23..17<br />
143.5<br />
144.84<br />
b) use station in Level-1 trigger<br />
1¢<br />
£<br />
improved per<strong>for</strong>mance<br />
from momentum in<strong>for</strong>mation<br />
may need all silicon (6.8 m<br />
careful study still needed<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp<br />
10.8<br />
¤<br />
21.8<br />
52.14<br />
)<br />
117.04
Main requirements:<br />
22 cm long ladders,<br />
Summary and Outlook<br />
large pitch ( 80 ¡ m resolution sufficient )<br />
fast shaping <strong>for</strong> 25 s bunch crossing rate<br />
material budget!!!<br />
Main D: R¢<br />
sensors: 6” p<br />
readout chip: Beetle<br />
£<br />
-on-n , 320 ¡ m thick, 198 ¡ m or 237.5 ¡ m pitch<br />
ladder supports, detector boxes: modular design, low-weight materials<br />
digital optical read-out link<br />
Upcoming:<br />
May/June — testbeam with full-size prototype sensors<br />
¤<br />
validation of sensor design, choice of strip geometry<br />
October — submission Technical Design Report<br />
March 02, 2002 <strong>The</strong> <strong>Silicon</strong> <strong>Inner</strong> <strong>Tracker</strong> <strong>for</strong> <strong>LHCb</strong> Olaf Steinkamp