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NLO single-top production matched with shower in POWHEG: s- and t-channel contributions (0907.4076v2)

Published 23 Jul 2009 in hep-ph

Abstract: We present a next-to-leading order calculation of single-top production interfaced to Shower Monte Carlo programs, implemented according to the POWHEG method. A detailed comparison with MC@NLO and PYTHIA is carried out for several observables, for the Tevatron and LHC colliders.

Citations (898)

Summary

  • The paper introduces a POWHEG method that accurately simulates NLO single-top production in both s- and t-channels.
  • It employs specific techniques like the Frixione-Kunszt-Signer subtraction and Sudakov form factors to handle initial- and final-state singularities.
  • The study demonstrates enhanced predictions for top-quark kinematics and decay spin correlations compared to traditional approaches.

Overview of NLO Single-Top Production Matched with Shower in POWHEG

The paper presents a next-to-leading order (NLO) calculation of single-top production in both ss- and tt-channels interfaced with Shower Monte Carlo (SMC) programs using the POWHEG method. This paper is significant as it addresses a process involving both initial- and final-state singularities, and seeks to enhance the reliability of simulating single-top quark production events in hadronic collisions. POWHEG is noted for its ability to generate events with positive weights and compatibility with various SMC programs, offering advantages over traditional methods.

Key Aspects of the POWHEG Implementation

  • Amplitude Calculations: The paper explores both the Born and virtual contributions, providing explicit outcomes using MadGraph for verification. The Frixione-Kunszt-Signer subtraction method is employed to handle divergences in both initial- and final-state emissions.
  • Sudakov Form Factor and Kinematics: The implementation utilizes the Sudakov form factor for radiation, creating variables that account for the transverse momentum emphasizing the subtleties of initial-state radiation (ISR) and final-state radiation (FSR) kinematics. This approach ensures better adherence to the realistic environment of hadron colliders.
  • Decay Spin Correlations: The POWHEG framework in the paper includes spin correlation effects in the top-quark decay phase, improving upon the precision of predictions over various SMC programs that assume spin-averaged decay processes.

Results and Comparisons

The authors conduct detailed comparisons between the POWHEG NLO implementation and results from MCFM, as well as SMC programs such as MC@NLO and PYTHIA. The comparisons address:

  • Top and Jet Kinematics: The transverse momentum and pseudorapidity distributions of top quarks and the hardest jets show fair agreement across the NLO and SMC results, albeit with minor deviations that highlight shower effects in the softer transverse momentum regime.
  • Rapidity Distributions: The paper addresses a central concern regarding the presence of dips in rapidity distributions observed in MC@NLO outputs, providing insights into the underlying mechanics of POWHEG and showcasing its capacity to reconcile with fixed-order NLO outputs.
  • Decayed Events: Ensuring pertinence to experimental observables, the analysis incorporates leptonic decay channels, showcasing POWHEG's nuanced handling of angular correlations and differential distributions ensuing from top decay—an area where it outperforms PYTHIA's spin-averaged decay model.

Implications and Future Directions

The successful integration of NLO corrections with shower algorithms using POWHEG has sizable implications in experimental physics—particularly in improving the accuracy of simulations for processes involving heavy quarks at colliders like the LHC and Tevatron. The methodological advancements outlined enable better modeling of complex processes, facilitating more precise measurements and statistical significance in searches for new physics phenomena.

Looking forward, similar implementations could extend to include electroweak corrections or even interface with higher-order perturbative QCD corrections, further bridging the gap between theoretical calculations and empirical data. Enhanced computational strategies in high-energy physics simulations continue to be of paramount significance, providing the impetus for a deeper understanding of the Standard Model and beyond.

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