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Reviving the interference: framework and proof-of-principle for the anomalous gluon self-interaction in the SMEFT

Celine Degrande, Matteo Maltoni

TL;DR

In SMEFT, interference between the SM and a dimension-6 operator can cancel across phase space, suppressing sensitivity to the linear term in $C_G/Λ^2$. The authors propose a differential-measurement framework that defines the measurable interference $σ^{|meas|}$ and identifies observables—most notably the transverse sphericity $Sph_T$ and transverse thrust—that efficiently separate positive- and negative-interference regions in three-jet production. Their LO studies show that linear-term bounds on $C_G/Λ^2$ from carefully chosen differential distributions can be competitive with bounds from the squared amplitude, with $Sph_T$ achieving efficiencies above 80%. The approach provides a practical, model-agnostic route to probe anomalous gluon self-interactions and can be extended to other BSM scenarios, pending NLO/PS refinements.

Abstract

Interferences are not positive-definite and can change sign over the phase space. If the contributions of the regions where they are positive and negative nearly cancel each other, their effects can be hard to measure. In this paper, we propose a method to quantify the ability of an observable to separate these opposite contributions and therefore to revive the interference effects at experiments. We apply this strategy to the anomalous gluon operator in the SMEFT, for which the linear-term suppression is well known. We show that we can get, for the first time, constraints on its coefficient from the interference only that are similar to those from the square of the new-physics amplitude.

Reviving the interference: framework and proof-of-principle for the anomalous gluon self-interaction in the SMEFT

TL;DR

In SMEFT, interference between the SM and a dimension-6 operator can cancel across phase space, suppressing sensitivity to the linear term in . The authors propose a differential-measurement framework that defines the measurable interference and identifies observables—most notably the transverse sphericity and transverse thrust—that efficiently separate positive- and negative-interference regions in three-jet production. Their LO studies show that linear-term bounds on from carefully chosen differential distributions can be competitive with bounds from the squared amplitude, with achieving efficiencies above 80%. The approach provides a practical, model-agnostic route to probe anomalous gluon self-interactions and can be extended to other BSM scenarios, pending NLO/PS refinements.

Abstract

Interferences are not positive-definite and can change sign over the phase space. If the contributions of the regions where they are positive and negative nearly cancel each other, their effects can be hard to measure. In this paper, we propose a method to quantify the ability of an observable to separate these opposite contributions and therefore to revive the interference effects at experiments. We apply this strategy to the anomalous gluon operator in the SMEFT, for which the linear-term suppression is well known. We show that we can get, for the first time, constraints on its coefficient from the interference only that are similar to those from the square of the new-physics amplitude.

Paper Structure

This paper contains 6 sections, 9 equations, 2 figures, 3 tables.

Figures (2)

  • Figure 1: Differential cross-section distributions for the leading jet p_T ( top) and the transverse sphericity ( bottom) in three-jet production, with p_T^j > 200 GeV. The red (blue) histograms represent the differential cross-section contributions to the interference by the positive- (negative-) weighted events. Their differences, in orange, are the differential linear terms; the dotted portion in the bottom plot is the opposite of the negative part. The black lines reproduce the SM distributions divided by 100, while the green lines show the squared ones. The last bin of the top plot contains the overflow
  • Figure 2: 95% CL upper bounds on Λ (for C_G = 1) as functions of the upper cut over the CoM energy √{s}, inferred from the best distribution for the 200 and 1000 GeV p_T^j cut. The orange (green) lines show the bounds from the linear (quadratic) order. The dotted lines reproduce the limits obtained through the S_T variable alone. The axes on top quantify the percentage of events, in the interference sample, that are discarded because of the cut on √{s}. The shaded areas cover the region where √{s} is larger than the bound on Λ