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1 | \select@language {french} |
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2 | \addvspace {10\p@ } |
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3 | \addvspace {10\p@ } |
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4 | \contentsline {figure}{\numberline {2.1}{\ignorespaces Unit cell of silicon crystalline structure}}{22}{figure.2.1} |
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5 | \contentsline {figure}{\numberline {2.2}{\ignorespaces Silicon band structure in the energy-impulsion domain}}{23}{figure.2.2} |
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6 | \contentsline {figure}{\numberline {2.3}{\ignorespaces Fermi-Dirac Distribution, $\mu =0$, $g_{i}=1$}}{24}{figure.2.3} |
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7 | \contentsline {figure}{\numberline {2.4}{\ignorespaces The three possible state of a pn junction : at rest (top), forward bias (middle), reverse bias (bottom). The depletion region relative size is shown on the figure with the space-charge sign of each zone of the diode. }}{27}{figure.2.4} |
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8 | \contentsline {figure}{\numberline {2.5}{\ignorespaces !!! Mettre belle Mesure ICI !!!!! Typical pn junction current versus bias characteristics. }}{28}{figure.2.5} |
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9 | \contentsline {figure}{\numberline {2.6}{\ignorespaces Schematics of ionizing particle detection in a reverse biased diode. The free electron hole pairs produced by the particle energy loss drift in the electric field and produce a current in the diode. Thermally generated (green boxes) are also generated in the depleted zone of the diode. }}{30}{figure.2.6} |
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10 | \contentsline {figure}{\numberline {2.7}{\ignorespaces Schematics of the hybrid planar pixel sensor.}}{32}{figure.2.7} |
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11 | \contentsline {figure}{\numberline {2.8}{\ignorespaces Schematics of the hybrid 3D pixel sensor.}}{33}{figure.2.8} |
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12 | \contentsline {figure}{\numberline {2.9}{\ignorespaces Schematics of the High Resistivity Monolithic active pixel sensor (MAPS).}}{34}{figure.2.9} |
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13 | \contentsline {figure}{\numberline {2.10}{\ignorespaces Schematics of radiation damage effect at the silicon-silicon dioxide interface in silicon sensors.}}{42}{figure.2.10} |
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