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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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