LEADER 03048nam 2200577 a 450 001 9910300383203321 005 20250609112005.0 010 $a3-319-00810-2 024 7 $a10.1007/978-3-319-00810-3 035 $a(CKB)2670000000423435 035 $a(SSID)ssj0000988286 035 $a(PQKBManifestationID)11546510 035 $a(PQKBTitleCode)TC0000988286 035 $a(PQKBWorkID)10950714 035 $a(PQKB)10533783 035 $a(MiAaPQ)EBC1398601 035 $a(DE-He213)978-3-319-00810-3 035 $a(PPN)172422957 035 $a(MiAaPQ)EBC4439631 035 $a(EXLCZ)992670000000423435 100 $a20130617d2014 uy 0 101 0 $aeng 135 $aurcn||||||||| 181 $ctxt 182 $cc 183 $acr 200 10$aStandard model measurements with the ATLAS detector $eMonte Carlo simulations of the tile calorimeter and measurement of the Z [symbols] cross section /$fJana Novakova 205 $a1st ed. 2014. 210 $aNew York $cSpringer$d2014 215 $axv, 91 p. $cill. (some col.) 225 1 $aSpringer theses : recognizing outstanding Ph.D. research,$x2190-5053 300 $aBibliographic Level Mode of Issuance: Monograph 311 08$a3-319-03294-1 311 08$a3-319-00809-9 320 $aIncludes bibliographical references. 327 $aOverview of the ATLAS experiment at the LHC -- Monte Carlo simulations of the Tile calorimeter -- Electron efficiency measurement -- Z0 ? ? + ? cross section measurement. 330 $aThis thesis deals with two main procedures performed with the ATLAS detector at the Large Hadron Collider (LHC). The noise description in the hadronic calorimeter TileCal represents a very valuable technical job. The second part presents a fruitful physics analysis ? the cross section measurement of the process p + p ? Z0 ? ? + ?. The Monte Carlo simulations of the TileCal are described in the first part of the thesis, including a detailed treatment of the electronic noise and multiple interactions (so-called pile-up). An accurate description of both is crucial for the reconstruction of e.g. jets or hadronic tau-jets. The second part reports a Standard Model measurement of the Z0 ? ? + ? process with the emphasis on the final state with an electron and a hadronically decaying tau-lepton. The Z0 ? ? + ? channel forms the dominant background in the search for Higgs bosons decaying into tau lepton pairs, and thus the good understanding achieved here can facilitate more sensitive Higgs detection. 410 0$aSpringer theses. 606 $aNuclear track detectors 606 $aLarge Hadron Collider (France and Switzerland) 615 0$aNuclear track detectors. 615 0$aLarge Hadron Collider (France and Switzerland) 676 $a539.72 700 $aNovakova$b Jana$00 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910300383203321 996 $aStandard Model Measurements with the ATLAS Detector$91768719 997 $aUNINA