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The Underlying-Event Model in PYTHIA (6&8) - Peter Skands - Cern

The Underlying-Event Model in PYTHIA (6&8) - Peter Skands - Cern

The Underlying-Event Model in PYTHIA (6&8) - Peter Skands - Cern

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P. <strong>Skands</strong><br />

pQCD<br />

2→2<br />

= Sum of<br />

≈ Rutherford<br />

(t-channel gluon)<br />

!"#$%&'()*+,'*,-<br />

./.,)&0.%<br />

")&,'(12/)%<br />

MPI a la <strong>PYTHIA</strong><br />

Multiple Perturbative Parton-Parton Interactions<br />

A) Start from perturbative model (dijets) and extend to IR<br />

Multiparton <strong>in</strong>teractions<br />

Regularise cross section with p ⊥0 as free parameter<br />

IR Regularization<br />

dˆσ<br />

dp 2 ⊥<br />

with energy dependence<br />

Energy Scal<strong>in</strong>g<br />

∝ α2 s (p 2 ⊥ )<br />

p 4 ⊥<br />

p ⊥0(E CM) =p ref<br />

⊥0 ×<br />

→ α2 s (p 2 ⊥0 + p2 ⊥ )<br />

(p 2 ⊥0 + p2 ⊥ )2<br />

<br />

ECM<br />

Eref ɛ CM<br />

Matter profile <strong>in</strong> impact-parameter space<br />

gives time-<strong>in</strong>tegrated overlap which determ<strong>in</strong>es level of activity:<br />

simple Gaussian or more peaked variants<br />

Normalize to<br />

ISR total and cross MPI section: compete for beam momentum → PDF rescal<strong>in</strong>g<br />

+ flavour effects (valence, qq pair companions, . . . )<br />

+ Resum/Unitarize → Probability<br />

+ correlated primordial k⊥ and colour <strong>in</strong> beam remnant<br />

for a 2→2 <strong>in</strong>teraction at xT1 =<br />

Many partons produced close <strong>in</strong> space–time ⇒ colour rearrangement;<br />

reduction → This is of now total our str<strong>in</strong>g basic length (UV & ⇒IR) steeper 2→2 cross 〈p section<br />

⊥〉(nch) See, e.g., new MCnet Review: “General-purpose event generators for LHC physics”, arXiv:1101.2599<br />

4

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