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 />
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