, 77 2.5.3 Reconstruction et identification des objets, p.82
, 96 3.2.2 Canaux bruyants isolés 100 3.2.4 Court circuit de lignes haute tension 101 3.2.4.1 Distribution de la haute tension 101 3.2.4.2 Les phases de la haute tension 105 3.3 ´ Etude de l'effet des variations de la haute tension sur la qualité des données 106 3.3.1 Motivations de l Configuration des runs spéciaux, Définition et traitement desprobì emes liés aux calorimètrescalorimètresà argon liquide 95 3.2.1 Bruit cohérent, p.115
, 96 3.2.2 Canaux bruyants isolés, p.106
, 106 3.3.2 ´ Etude des runs spéciaux 107 3.3.2.1 Configuration des runs spéciaux Stratégie de l'analyse et résultats, p.117
, 159 5.4.2.1 Reconstruction des bosons Z et Z ( * )
, 163 5.4.3.1 Prise en compte des photons radiatifs dans l'´ etat final 164 5.4.3.2 Correction de m 4 ` a l'aide de contraintes sur la masse du boson, p.165
, 192 5.6.3.1 Mesure des efficacités dans les données, p.202
, 208 5.6.5.1 A partir des efficacités mesurées dans les données, p.211
, La masse reconstruite des candidats bosons Z sont 86.3 GeV et 31.6 GeV. CetévénementCetévénement a ´ eté enregistré le 10 Juin, se désintégrant en 4 muons, p.31, 20122012.
, Les paires d'´ electrons formant les candidats boson Z, dont les masses reconstruite sont 70.6 GeV et 44.7 GeV, sont colorées en rouge et bleu. CetévénementCetévénement a ´ eté enregistré le, p.11, 2012201220-03-18.
, ´ electrons (vert) et de muons (rouge) Les candidats boson Z ont des masses reconstruite de 97
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