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Measurement of the Jet Energy Scale in the CMS experiment ... - IIHE

Measurement of the Jet Energy Scale in the CMS experiment ... - IIHE

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130 CHAPTER 6: ConclusionUnc.(∆ε l )(%)765Unc.(∆ε b )(%)10846324120 100 200 300 400 500 600 700 800 900 1000 -1Lum<strong>in</strong>osity (pb )0 100 200 300 400 500 600 700 800 900 1000 -1Lum<strong>in</strong>osity (pb )Figure 6.1: The absolute statistical (curved l<strong>in</strong>e) as well as <strong>the</strong> systematical (straightl<strong>in</strong>e) uncerta<strong>in</strong>ties on <strong>the</strong> (left) light and (right) b jet energy corrections as a function<strong>of</strong> <strong>the</strong> lum<strong>in</strong>osity. From some po<strong>in</strong>t onward <strong>the</strong> systematical uncerta<strong>in</strong>ties dom<strong>in</strong>ate<strong>the</strong> statistical uncerta<strong>in</strong>ties.values on simulation, also this is a limit <strong>of</strong> <strong>the</strong> precision <strong>of</strong> ∆E.Although <strong>the</strong> method is able to estimate <strong>the</strong> jet energy corrections <strong>in</strong>clusively, ithas also <strong>the</strong> capability to provide a differential estimation <strong>of</strong> <strong>the</strong> jet energy corrections.When larger amounts <strong>of</strong> statistics are recorded, <strong>the</strong> jets can be categorized <strong>in</strong> terms<strong>of</strong> <strong>the</strong>ir k<strong>in</strong>ematics, such as pseudorapidity η or transverse momentum p T . Then, <strong>the</strong>same method can be applied on <strong>the</strong> events which populate a particular b<strong>in</strong> <strong>of</strong> <strong>the</strong>sek<strong>in</strong>ematic variables and consequently <strong>the</strong> estimated results would be obta<strong>in</strong>ed for thatregion <strong>of</strong> <strong>the</strong> phase space. This yields to obta<strong>in</strong> a differential estimation <strong>of</strong> <strong>the</strong> jetenergy corrections. With 36pb −1 where a low number <strong>of</strong> events survived <strong>the</strong> selectioncuts, a differential estimation is not feasible. Us<strong>in</strong>g a higher amount <strong>of</strong> statistics <strong>of</strong> forexample 2fb −1 , <strong>the</strong>re are sufficient events rema<strong>in</strong><strong>in</strong>g <strong>in</strong> <strong>the</strong> various regions <strong>of</strong> <strong>the</strong> phasespace that makes <strong>the</strong> differential method applicable and would result <strong>in</strong> mean<strong>in</strong>gfulestimations. More detailed <strong>in</strong>formation on this aspect can be found <strong>in</strong> [106].The calibration method expla<strong>in</strong>ed <strong>in</strong> this <strong>the</strong>sis will help <strong>the</strong> search for new physicsphenomena at <strong>the</strong> LHC, because when jets are better calibrated, <strong>the</strong> k<strong>in</strong>ematic topology<strong>of</strong> <strong>the</strong> new physics events can be better reconstructed and differentiated from <strong>the</strong>backgrounds. Moreover, s<strong>in</strong>ce <strong>in</strong> almost all <strong>the</strong> analyses, <strong>the</strong> jet energy scale calibrationis <strong>the</strong> ma<strong>in</strong> source <strong>of</strong> systematical uncerta<strong>in</strong>ty, a precise determ<strong>in</strong>ation <strong>of</strong> <strong>the</strong> energy<strong>of</strong> <strong>the</strong> jets would also reduce <strong>the</strong> uncerta<strong>in</strong>ties orig<strong>in</strong>at<strong>in</strong>g from <strong>the</strong> jet energy scalecalibration factors and makes it possible to perform precision tests even at hadroncolliders like <strong>the</strong> LHC.

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