Abstract

$N$-jettiness subtractions provide a general approach for performing fully-differential next-to-next-to-leading order (NNLO) calculations. Since they are based on the physical resolution variable $N$-jettiness, $\mathcal{T}_N$, subleading power corrections in $\tau=\mathcal{T}_N/Q$, with $Q$ a hard interaction scale, can also be systematically computed. We study the structure of power corrections for $0$-jettiness, $\mathcal{T}_0$, for the $gg\to H$ process. Using the soft-collinear effective theory we analytically compute the leading power corrections $\alpha_s \tau \ln\tau$ and $\alpha_s^2 \tau \ln^3\tau$ (finding partial agreement with a previous result in the literature), and perform a detailed numerical study of the power corrections in the $gg$, $gq$, and $q\bar q$ channels. This includes a numerical extraction of the $\alpha_s\tau$ and $\alpha_s^2 \tau \ln^2\tau$ corrections, and a study of the dependence on the $\mathcal{T}_0$ definition. Including such power suppressed logarithms significantly reduces the size of missing power corrections, and hence improves the numerical efficiency of the subtraction method. Having a more detailed understanding of the power corrections for both $q\bar q$ and $gg$ initiated processes also provides insight into their universality, and hence their behavior in more complicated processes where they have not yet been analytically calculated.

Highlights

  • Our ability to perform next-to-next-to-leading order (NNLO) calculations for cross sections of phenomenological importance is crucial for theory predictions to match the precision of Run 2 measurements at the LHC

  • We focus on improving the understanding of the infrared structure of N-jettiness subtractions [7,8], which is a nonlocal subtraction method based on the N-jettiness resolution variable T N [9,10]

  • The simplicity of the analytic results, and their close relation to those for quark-initiated processes suggests a degree of universality in the subleading soft and collinear limits, similar to that which is observed at leading power

Read more

Summary

INTRODUCTION

Our ability to perform next-to-next-to-leading order (NNLO) calculations for cross sections of phenomenological importance is crucial for theory predictions to match the precision of Run 2 measurements at the LHC. The leading-logarithmic (LL) terms at subleading order in τ were analytically computed at NLO and NNLO for Drell-Yan like processes in Refs. We perform a detailed numerical study using H þ 1 jet NLO results from MCFM8 [18,42,43,44] This provides both a confirmation of our analytic calculation, and enables us to study the extent to which the power corrections are well described by the LL approximation.

N-JETTINESS SUBTRACTIONS
CALCULATION
Comparison with Drell-Yan
NUMERICAL RESULTS
RAPIDITY DEPENDENCE AND OBSERVABLE DEFINITION
CONCLUSIONS
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.