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Measurement of the Z boson cross-section in - Harvard University ...

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Chapter 5: Monte Carlo Simulation 153<br />

<strong>in</strong>volved. An event generator program can calculate <strong>cross</strong>-<strong>section</strong>s, i.e. , event rates,<br />

for a process. It can determ<strong>in</strong>e differential <strong>cross</strong>-<strong>section</strong>s as functions <strong>of</strong> k<strong>in</strong>ematic<br />

variables, and <strong>the</strong>n generates hypo<strong>the</strong>tical events to populate <strong>the</strong> phase space <strong>of</strong> <strong>the</strong>se<br />

variables. It provides energy-momentum four-vectors <strong>of</strong> primary particles produced<br />

<strong>in</strong> <strong>the</strong> hard <strong>in</strong>teraction and <strong>of</strong> <strong>the</strong> decay products <strong>of</strong> all unstable particles. Differ-<br />

ential <strong>cross</strong>-<strong>section</strong>s can be estimated us<strong>in</strong>g ei<strong>the</strong>r exact matrix elements to a given<br />

degree <strong>of</strong> accuracy, or an ‘all-order’ approach such as parton shower<strong>in</strong>g or QCD re-<br />

summation. At <strong>the</strong> end <strong>of</strong> <strong>the</strong> decay process, partons are grouped <strong>in</strong>to hadrons us<strong>in</strong>g<br />

a hadronization model (Chapter 1). At a hadron-hadron collider such as <strong>the</strong> LHC,<br />

<strong>the</strong> underly<strong>in</strong>g event must also be modeled 1 .<br />

A second class <strong>of</strong> MC generators are <strong>the</strong> so-called <strong>cross</strong>-<strong>section</strong> <strong>in</strong>tegrators. Unlike<br />

event generators, <strong>the</strong>se programs do not output events with full k<strong>in</strong>ematic <strong>in</strong>forma-<br />

tion, but ra<strong>the</strong>r produce distributions <strong>of</strong> k<strong>in</strong>ematic variables, e.g. , pT spectra, with<br />

high precision. Cross-<strong>section</strong> <strong>in</strong>tegrators are <strong>of</strong>ten used for unambiguous <strong>in</strong>terpreta-<br />

tion <strong>of</strong> experimental results.<br />

In <strong>the</strong> simulation step, f<strong>in</strong>al-state particles from <strong>the</strong> generation step are propa-<br />

gated through a realistic description <strong>of</strong> <strong>the</strong> detector. Ideally, all parts <strong>of</strong> <strong>the</strong> detector,<br />

<strong>in</strong>clud<strong>in</strong>g active detection volumes and <strong>in</strong>active (‘dead’) material, would be <strong>in</strong>cluded<br />

<strong>in</strong> <strong>the</strong> detector description. The simulation program knows what volume a particle is<br />

travers<strong>in</strong>g at a given stage; <strong>in</strong>teractions with <strong>the</strong> material <strong>in</strong> that volume are modeled<br />

accord<strong>in</strong>g to <strong>the</strong> particle type, properties <strong>of</strong> <strong>the</strong> material and known physics. Elec-<br />

1 The underly<strong>in</strong>g event arises from <strong>in</strong>teractions between partons <strong>in</strong> <strong>the</strong> collid<strong>in</strong>g hadrons that did<br />

not participate <strong>in</strong> <strong>the</strong> hard process. These <strong>in</strong>teractions can be significant and can lead to sufficient<br />

activity <strong>in</strong> <strong>the</strong> f<strong>in</strong>al state so as to affect <strong>the</strong> measurement <strong>of</strong> <strong>the</strong> hard process. It is <strong>the</strong>refore essential<br />

that <strong>the</strong> underly<strong>in</strong>g event be accurately described <strong>in</strong> Monte Carlo.

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