amplicateur suivant la dose re cue, p.60 ,
Temps de r eponse selon la colonne, p.71 ,
Temps de r eponse selon la colonne, p.71 ,
:, p.81 ,
:, p.82 ,
:, p.85 ,
103 5.10 R esolutions normalis ees S pour des muons. : : : : : : : : : : : : : : : : : : : 104 5.11 R esolution en impulsion transverse vs p T . : : : : : : : : : : : : : : : : : : : : 105 5.12 R esolution en impulsion transverse vs . : : : : : : : : : : : : : : : : : : : : : 106 5.13 R esolutions angulaires vs p T . : : : : : : : : : : : : : : : : : : : : : : : : : : : 107 5.14 R esolution en param etre d'impact vs . : : : : : : : : : : : : : : : : : : : : : 108 5.15 Eets du bruit et des inecacit es sur a0, 109 5.16 R esolution en param etre d'impact vs p T . : : : : : : : : : : : : : : : : : : : : : 109 5.17 R esolution en a 0 obtenues par les trois algorithmes. : : : : : : : : : : : : : : : 110 5.18 R esolution en z 0 vs p T, p.111 ,
114 5.24 R epartition des points dans les pixels : : 115 5.25 R epartition des points dans les micro-pistes. : : : : : : : : : : : : : : : : : : : 115 5.26 Vraisemblance S dans les jets. : : : : : : : : : : : : : : : : : : : : : : : : : : 116 5.27 Probabilit e d e 2 des traces dans les jets. : : : : : : : : : : : : : : : : : : : : 116 5.28 R esolution en param etre d'impact des traces reconstruites dans les jets, p.121 ,
impact sign e et normalis e des traces dans les di erents types de jets (simulation rapide), p.123 ,
impact sign e et normalis e a son erreur des traces reconstruites pour les deux types de jets, p.133 ,
A tlas a un boson de Higgs de masse 80 < m H < 120 GeV=c 2 pendant les trois premi eres ann ees a basse luminosit e ,
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