Abstract

We consider idealized parton shower event generators that treat parton spin and color exactly, leaving aside the choice of practical approximations for spin and color. We investigate how the structure of such a parton shower generator is related to the structure of QCD. We argue that a parton shower with splitting functions proportional to $\alpha_s$ can be viewed not just as a model, but as the lowest order approximation to a shower that is defined at any perturbative order. To support this argument, we present a formulation for a parton shower at order $\alpha_s ^k$ for any $k$. Since some of the input functions needed are specified by their properties but not calculated, this formulation does not provide a useful recipe for an order $\alpha_s ^k$ parton shower algorithm. However, in this formulation we see how the operators that generate the shower are related to operators that specify the infrared singularities of QCD.

Highlights

  • Parton shower event generators for hadron collisions, such as HERWIG [1], PYTHIA [2], and SHERPA [3], perform calculations of cross sections according to an approximation to the standard model or its possible extensions

  • We consider an idealized version of a parton shower generator in which one accounts exactly for spin and color

  • The formulas for the shower automatically includes factors that sum threshold logarithms [35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80]. These factors are not included in current parton shower generators at even leading order, except for DEDUCTOR [32,33]

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Summary

INTRODUCTION

Parton shower event generators for hadron collisions, such as HERWIG [1], PYTHIA [2], and SHERPA [3], perform calculations of cross sections according to an approximation to the standard model or its possible extensions. The formulas for the shower automatically includes factors that sum threshold logarithms [35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80] These factors are not included in current parton shower generators at even leading order, except for DEDUCTOR [32,33]. The parton evolution kernels play a role in our formalism, it is not a central role

OVERVIEW
FACTORIZATION
Infrared safety
A more quantitative view of infrared safety
Factorization
PARTONS AND THE DENSITY OPERATOR
Amplitudes and the density operator in spin and color
Scales
Multiplying by parton distribution functions
THE PERTURBATIVE CROSS SECTION
The Born cross section
The higher order cross section
Introduction of the infrared sensitive operator Dðμ2Þ
Subtractions for the perturbative cross section
Properties of the infrared sensitive operator
FROM THE PERTURBATIVE CROSS SECTION TO A PARTON SHOWER
Moving the measurement operator
Introducing shower oriented parton distribution functions
Changing the scale of the subtraction operators
The shower evolution equation
The structure of Vðμ2Þ
SUMMARY AND OUTLOOK
Statistical states in the toy model
The infrared sensitive operator
The perturbative shower evolution operator
The operator Vðμ2sÞ
Renormalization of the QCD coupling
Renormalization of the parton distribution functions
Findings
Renormalization scale dependence
Full Text
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