The Silicon Inner Tracker for LHCb - LHCb - CERN

The Silicon Inner Tracker for LHCb - LHCb - CERN The Silicon Inner Tracker for LHCb - LHCb - CERN

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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

<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

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