Monolithic CMOS Pixel Detectors in Particle and Nuclear ... - SLAC
Monolithic CMOS Pixel Detectors in Particle and Nuclear ... - SLAC
Monolithic CMOS Pixel Detectors in Particle and Nuclear ... - SLAC
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PIXEL2002 - International Workshop on Semiconductor <strong>Pixel</strong> <strong>Detectors</strong> for <strong>Particle</strong>s <strong>and</strong> X-Rays<br />
Carmel Mission CA, USA, September 9-12, 2002<br />
Motivation for <strong>Monolithic</strong> <strong>Pixel</strong> Devices<br />
<br />
<br />
<br />
Vertex <strong>Detectors</strong> (VXD)<br />
Quarks from primary <strong>in</strong>teraction hadronize<br />
with<strong>in</strong> typical distances of a few fermi (they are<br />
not seen),<br />
Hadronization of quarks yields <strong>in</strong> jets of<br />
particles, which reta<strong>in</strong> the direction <strong>and</strong> the<br />
energy of the parent,<br />
F<strong>in</strong>al states with large number of jets;<br />
b, c, τ present <strong>in</strong> most f<strong>in</strong>al states of <strong>in</strong>terest,<br />
Future Vertex <strong>Detectors</strong> should :<br />
• allow assign<strong>in</strong>g each track to its<br />
vertex orig<strong>in</strong> ,<br />
• allow reconstruct<strong>in</strong>g Q, M, E <strong>and</strong> 2 ry - 3 ry vertices<br />
• allow reconstruct<strong>in</strong>g the flavour of each vertex <strong>in</strong><br />
a high particle density multi-jets environment,<br />
Untill today the flagship are Charge Cupled Devices...<br />
but VXDs should also ...<br />
• provide constant performances under relatively<br />
harsh radiation environment,<br />
• allow fast readout - to cope with background.<br />
rσ+ r σ<br />
σ =<br />
1 1 2 2<br />
IP 2<br />
( r2 − r1)<br />
<strong>Monolithic</strong> <strong>CMOS</strong> <strong>Pixel</strong> <strong>Detectors</strong><br />
<strong>in</strong> <strong>Particle</strong> <strong>and</strong> <strong>Nuclear</strong> Physics<br />
Grzegorz DEPTUCH<br />
deptuch@lepsi.<strong>in</strong>2p3.fr<br />
Impact parameter precision<br />
<strong>and</strong> Multiple Coulomb Scatter<strong>in</strong>g<br />
13.<br />
6 MeV x ⎡ ⎛ x ⎞⎤<br />
Θ<br />
0<br />
= z ⎢1+<br />
0. 038ln⎜<br />
⎟⎥<br />
βcp X0 ⎣ ⎝X0<br />
⎠⎦<br />
The solution be<strong>in</strong>g sought is very granular,<br />
ultra light, radiation hard, poly-layer VXD<br />
<strong>in</strong>stalled close to the IP.<br />
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