injection du LEP L'obtention des faisceaux e + e ? , avec desénergiesélevéesdesénergiesdesénergiesélevées, exige l'utilisation d'une cha??necha??ne complexe d'injection (voir figure 2.1) qui tire parti des différents accélérateurs existants au CERN : le Super Proton Synchrotron (SPS), le Proton Synchrotron (PS) ,
LesélectronsLesélectrons sont envoyés sur une cible de tungstène o` u des pairesélectronpairesélectron-positron sont créées LesélectronsLesélectrons et les positrons sont ensuite guidés vers le LINAC, o` u ils sont accélérés jusqu'` a uné energie de 600 MeV. Ces paquets de particules sont accumulés dans l'Electron Positron Accumulator (EPA) avant d'? etre injectés dans les machines suivantes. D` es que le nombre de particules dans l'EPA est suffisant, les paquets sont envoyés dans le PS o` u ils subissent une accélération jusqu'` a 3.5 GeV. La phase suivante consistè a introduire les faisceaux e + e ? dans le pas utilisé pour estimer l'incertitude systématique. Dans ces modèles, la probabilité de recombinaison de couleur est maximal pour la configuration correspondantàcorrespondant`correspondantà des " longueurs ,
Le modèle EG ne reproduit pas les multiplicités des particules observées dans les données expérimentales et il est désormais abandonné. Le modèle SK est fondé sur le modèle des cordes de Lund dans lequel des cordes entre les partons des deux W se croisent. La probabilité de recombinaison de couleur est proportionnelle au volume d'espace temps lors du croisement de ces " tubes de couleur " . Les deux principaux scénario sont appelés SKI et SKII et feront l ,
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