Slepton pair production at next-to-leading power

A bstract Near threshold, cross sections for the production of heavy particles are sensitive to large logarithmic terms, which must be resummed to all orders in perturbation theory. Current state-of-the art calculations for inclusive slepton pair production at hadron colliders has focused on higher-order logarithms in the leading power of the threshold variable. Here, we evaluate the next-to-leading power contribution in the threshold variable to leading logarithmic accuracy. We find that the next-to-leading power contributions can be significant compared to the next-to-leading logarithmic terms at leading power, and that existing calculations underestimate the scale error for large slepton masses. We include results for a potential future FCC-hh machine at $$ \sqrt{s} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> </mml:math> = 85 TeV.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-04-27
DOI
https://doi.org/10.1007/jhep04(2026)213
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Slepton pair production at next-to-leading power

Lasse Lorentz Braseth, Are Raklev, Tore Klungland
Journal of High Energy Physics
Particle physics theoretical and experimental studies
article

Slepton pair production at next-to-leading power

Lasse Lorentz Braseth, Are Raklev, Tore Klungland
article en

Abstract

A bstract Near threshold, cross sections for the production of heavy particles are sensitive to large logarithmic terms, which must be resummed to all orders in perturbation theory. Current state-of-the art calculations for inclusive slepton pair production at hadron colliders has focused on higher-order logarithms in the leading power of the threshold variable. Here, we evaluate the next-to-leading power contribution in the threshold variable to leading logarithmic accuracy. We find that the next-to-leading power contributions can be significant compared to the next-to-leading logarithmic terms at leading power, and that existing calculations underestimate the scale error for large slepton masses. We include results for a potential future FCC-hh machine at $$ \sqrt{s} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> </mml:math> = 85 TeV.

Journal of High Energy PhysicsVol. 2026(4)
University of Oslo (NO)
Norges Forskningsråd
Openalex Percentile: Top 97%
Particle physics theoretical and experimental studies
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