13.07.2015 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

IntroductionThe Standard Model <strong>of</strong> particle physics describes <strong>the</strong> elementary particles and <strong>the</strong>ir<strong>in</strong>teractions, with <strong>the</strong> exception <strong>of</strong> gravity which is not formulated with<strong>in</strong> <strong>the</strong> model.The model has been tested <strong>in</strong> diverse <strong>experiment</strong>s and its parameters have been measuredwith great precision <strong>in</strong> high energy physics laboratories. However, <strong>the</strong>re is stilla miss<strong>in</strong>g particle which has not yet been detected, be<strong>in</strong>g <strong>the</strong> Standard Model Higgsboson. Also <strong>the</strong>re is evidence which make <strong>the</strong> Standard Model only an effective <strong>the</strong>oryand motivate <strong>the</strong> need to have new physics beyond it. Therefore, efforts are made tobuild <strong>the</strong> most fundamental <strong>the</strong>ory describ<strong>in</strong>g nature. To search for <strong>the</strong> Higgs particleand test <strong>the</strong> new physics ideas beyond <strong>the</strong> Standard Model, <strong>the</strong> Large Hadron Collider(LHC) was constructed.The LHC, located at <strong>the</strong> CERN laboratory near Geneva, has been collid<strong>in</strong>g beams<strong>of</strong> protons at a center <strong>of</strong> mass energy <strong>of</strong> 7 TeV s<strong>in</strong>ce March 2010. The proton-protoncollisions are detected with <strong>the</strong> use <strong>of</strong> detectors <strong>in</strong>stalled at <strong>the</strong> <strong>in</strong>teraction po<strong>in</strong>ts, suchas <strong>the</strong> <strong>CMS</strong> (Compact Muon Solenoid) <strong>experiment</strong>, which is one <strong>of</strong> <strong>the</strong> two generalpurposedetectors at <strong>the</strong> LHC. The energy and momentum <strong>of</strong> particles which are produced<strong>in</strong> <strong>the</strong> f<strong>in</strong>al state <strong>of</strong> proton-proton <strong>in</strong>teractions, are measured by <strong>the</strong> detectors.While <strong>the</strong> energy <strong>of</strong> leptons can be measured with high precision, <strong>the</strong> measurement <strong>of</strong><strong>the</strong> energy <strong>of</strong> <strong>the</strong> quarks, which hadronize to make so-called jets, is quite challeng<strong>in</strong>g.While strategies are developed to calibrate <strong>the</strong> jet energies with<strong>in</strong> <strong>the</strong> <strong>CMS</strong> collaboration,search<strong>in</strong>g for new physics benefits from a more precise measurement <strong>of</strong> <strong>the</strong> jetenergies than <strong>the</strong> ones obta<strong>in</strong>ed by apply<strong>in</strong>g <strong>the</strong> basel<strong>in</strong>e methods. In this analysis, amethod to calibrate <strong>the</strong> energy <strong>of</strong> <strong>the</strong> jets is applied on <strong>the</strong> proton collisions conta<strong>in</strong><strong>in</strong>gtwo top quarks <strong>in</strong> <strong>the</strong> f<strong>in</strong>al state, pp → t¯t. The high rate <strong>of</strong> <strong>the</strong> production <strong>of</strong> <strong>the</strong>top quark pairs <strong>in</strong> proton-proton collisions provides a huge amount <strong>of</strong> statistics. Thisallows <strong>the</strong> top quark pairs to be used as a tool to perform <strong>the</strong> calibration studies.This <strong>the</strong>sis is organized as follows. In Chapter 1, <strong>the</strong> Standard Model <strong>of</strong> particlephysics is reviewed with emphasis on <strong>the</strong> top quark sector followed by a motivationto construct <strong>the</strong> LHC. The description <strong>of</strong> <strong>the</strong> Large Hadron Collider and <strong>the</strong> <strong>CMS</strong><strong>experiment</strong>, is given <strong>in</strong> Chapter 2. The <strong>CMS</strong> <strong>experiment</strong> detects <strong>the</strong> emerg<strong>in</strong>g particlesfrom <strong>the</strong> proton collisions through electronic signals which are subsequently used toreconstruct <strong>the</strong> physics objects as described <strong>in</strong> Chapter 3. The simulation <strong>of</strong> <strong>the</strong> protoncollisions is described <strong>in</strong> Chapter 4 followed by <strong>the</strong> description <strong>of</strong> <strong>the</strong> procedure to selecttop quark events on which <strong>the</strong> calibration method is based. The method to estimate<strong>the</strong> residual jet energy corrections is described <strong>in</strong> detail <strong>in</strong> Chapter 5. The estimatedresults <strong>of</strong> <strong>the</strong> method are obta<strong>in</strong>ed based on both <strong>the</strong> simulated proton collisions aswell as <strong>the</strong> real proton collisions collected <strong>in</strong> 2010 by <strong>the</strong> <strong>CMS</strong> <strong>experiment</strong>. F<strong>in</strong>ally, a1

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!