Master Thesis Open Access
Schillinger, Bettina
<?xml version='1.0' encoding='UTF-8'?>
<record xmlns="http://www.loc.gov/MARC21/slim">
<leader>00000nam##2200000uu#4500</leader>
<datafield tag="980" ind1=" " ind2=" ">
<subfield code="a">user-cms</subfield>
</datafield>
<datafield tag="980" ind1=" " ind2=" ">
<subfield code="a">user-etp</subfield>
</datafield>
<datafield tag="542" ind1=" " ind2=" ">
<subfield code="l">open</subfield>
</datafield>
<datafield tag="856" ind1="4" ind2=" ">
<subfield code="s">4119111</subfield>
<subfield code="u">https://publish.etp.kit.edu/record/22009/files/masterthesis_schillinger_bettina_27Apr2020.pdf</subfield>
<subfield code="z">md5:2e8ac8ce3df3038db1ad8cc26f3ec0ec</subfield>
</datafield>
<datafield tag="980" ind1=" " ind2=" ">
<subfield code="a">thesis</subfield>
<subfield code="b">master-thesis</subfield>
</datafield>
<controlfield tag="005">20210803090215.0</controlfield>
<datafield tag="520" ind1=" " ind2=" ">
<subfield code="a"><p>In this thesis, the investigation of the cross section ratio of two established processes<br>
occurring in proton-proton collisions is performed. This choice is motivated by the fact,<br>
that the comparison of two separate measurements in the form of cross section ratios<br>
promises to benefit from reduced uncertainties.<br>
The first observable of interest is the inclusive dijet cross section. Dijet events are occurring<br>
at high rates at the LHC, due to the abundant production of jets at hadron colliders.<br>
Investigation of the dijet spectrum allows for tests of QCD, as the particles within the jets follow the laws of the strong nuclear force. Furthermore, these QCD events are<br>
the background for many other physics searches, and consequently have to be precisely<br>
understood in order to increase the accuracy of other measurements. Another advantage<br>
of the dijet event topology is the fact that it covers a wide kinematic range.<br>
The second process of choice is the inclusive Z+jet cross section. The Z boson has been<br>
studied in various experiments and its properties are very well known. This process allows<br>
for precise measurements, because it leaves a clear signal in the detector. Together with<br>
the leading jet in the Z+jet event, this final state can be studied in an analogous manner<br>
as the dijet final state.<br>
&nbsp;</p></subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="a">Measurement of the Ratio of inclusive Jet Cross Sections in Events with and without a high-pT Z Boson</subfield>
</datafield>
<datafield tag="909" ind1="C" ind2="O">
<subfield code="o">oai:publish.etp.kit.edu:22009</subfield>
<subfield code="p">user-cms</subfield>
<subfield code="p">user-etp</subfield>
</datafield>
<datafield tag="041" ind1=" " ind2=" ">
<subfield code="a">eng</subfield>
</datafield>
<controlfield tag="001">22009</controlfield>
<datafield tag="100" ind1=" " ind2=" ">
<subfield code="a">Schillinger, Bettina</subfield>
<subfield code="u">KIT/ETP</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Rabbertz, Klaus</subfield>
<subfield code="u">KIT/ETP</subfield>
<subfield code="4">ths</subfield>
</datafield>
<datafield tag="700" ind1=" " ind2=" ">
<subfield code="a">Voutilainen, Mikko</subfield>
<subfield code="u">University of Helsinki/HIP</subfield>
<subfield code="4">ths</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">QCD</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">dijets</subfield>
</datafield>
<datafield tag="653" ind1=" " ind2=" ">
<subfield code="a">Z+jet</subfield>
</datafield>
<datafield tag="260" ind1=" " ind2=" ">
<subfield code="c">2020-04-27</subfield>
</datafield>
</record>