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CERN-THESIS-2012-153 26/07/2012 - CERN Document Server

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2.5 Top Quark Physics Beyond the Standard Model<br />

As mentioned at the beginning of this chapter, the SM has proven rather successful in the description of<br />

experimental results. Figure 2.9 shows a summary of the SM production cross-section for different processes<br />

measured by the ATLAS experiment and compared to the theoretical expectations. Similar measurements<br />

can be found for the CMS experiment. There are, however, a number of shortcomings with the SM. For<br />

instance, the SM does not account for the existence of dark matter and dark energy, the baryon asymmetry<br />

of the universe, non-zero mass of the neutrinos, and furthermore it does not solve the hierarchy problem.<br />

Another question, directly related to the top quark, can be raised: why are the masses of the charged leptons<br />

as they are? Some of these questions might actually be answered, or hints given, at the LHC as more data<br />

is being collected. However, as of now, divergences from the SM are yet to be found. Several extensions to<br />

the SM have been formulated, in an attempt to answer some of those questions. One of the most common<br />

examples of those theories is SUSY, which postulates a fermion-boson symmetry, and provides a solution to<br />

the hierarchy problem.<br />

[pb]<br />

total<br />

σ<br />

10<br />

5<br />

4<br />

10<br />

3<br />

10<br />

2<br />

10<br />

10<br />

1<br />

­1<br />

35 pb<br />

­1<br />

35 pb<br />

­1<br />

1.0 fb<br />

­1<br />

1.0 fb<br />

­1<br />

4.7 fb<br />

ATLAS Preliminary<br />

LHC pp<br />

Theory<br />

­1<br />

4.6 fb<br />

s = 7 TeV<br />

­1<br />

Data 2010 (L = 35 pb )<br />

­1<br />

Data 2011 (L = 1.0 ­ 4.7 fb )<br />

LHC pp<br />

Theory<br />

s = 8 TeV<br />

­1<br />

Data <strong>2012</strong> (L = 5.8 fb )<br />

­1<br />

2.1 fb<br />

­1<br />

4.7 fb<br />

W Z tt t WW WZ Wt ZZ<br />

Figure 2.9: Summary of several Standard Model total production cross section measurements performed<br />

by the ATLAS experiment compared to the corresponding theoretical expectations. The error bars include<br />

the full uncertainty, both statistical and systematic. All theoretical expectations were calculated at NLO or<br />

higher.<br />

Top quark physics, because of its recent discovery, is a rather new field. Several analyses currently<br />

on-going, will provide more precision to known quantities, and possibly hints of new physics will be found.<br />

Some of those analysis specifically aim for physics BSM. Examples of these are analyses are: studies related<br />

21<br />

­1<br />

5.8 fb

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