Abstract:We provide a comprehensive global analysis of Run II top measurements at the LHC in terms of dimension-6 operators. A distinctive feature of the top sector as compared to the Higgs-electroweak sector is the large number of four-quark operators. We discuss in detail how they can be tested and how quadratic terms lead to a stable limit on each individual Wilson coefficient. Predictions for all observables are computed at NLO in QCD. Our SFitter analysis framework features a detailed error treatment and shows tha… Show more
“…Refs. [48,49] report comparatively loose bounds obtained from studying tZ production which also confirm that electroweak corrections to tt are apparently the strongest probe available at the LHC.…”
Section: Resultsmentioning
confidence: 87%
“…Global fits of New Physics contributions in terms of dimension-six operators relevant for the top quark sector have been carried out in refs. [48][49][50]. The resulting constraints on New Physics are substantial (see e.g.…”
We calculate the O(α) weak corrections to top quark pair production at the LHC and include anomalous electroweak interactions from dimension-six operators. The loop calculation and renormalization are consistently done within the Standard Model Effective Field Theory. Sensitivity to the involved operators is exposed through the virtual corrections, which receive enhancement from electroweak Sudakov logarithms. We investigate the prospects of using this feature for probing New Physics at the LHC that so far has only been studied in final states with on-shell sensitivity such as tt + Z or t → bW . We find that the large tt production rate and the excellent perturbative control allow compensating the loop suppression and yield remarkably strong constraints that are competitive with those from tt + Z.
“…Refs. [48,49] report comparatively loose bounds obtained from studying tZ production which also confirm that electroweak corrections to tt are apparently the strongest probe available at the LHC.…”
Section: Resultsmentioning
confidence: 87%
“…Global fits of New Physics contributions in terms of dimension-six operators relevant for the top quark sector have been carried out in refs. [48][49][50]. The resulting constraints on New Physics are substantial (see e.g.…”
We calculate the O(α) weak corrections to top quark pair production at the LHC and include anomalous electroweak interactions from dimension-six operators. The loop calculation and renormalization are consistently done within the Standard Model Effective Field Theory. Sensitivity to the involved operators is exposed through the virtual corrections, which receive enhancement from electroweak Sudakov logarithms. We investigate the prospects of using this feature for probing New Physics at the LHC that so far has only been studied in final states with on-shell sensitivity such as tt + Z or t → bW . We find that the large tt production rate and the excellent perturbative control allow compensating the loop suppression and yield remarkably strong constraints that are competitive with those from tt + Z.
“…Each of these coefficients is constrained directly and also through correlations with other coefficients from LHC measurements of top observables. Several global analyses of top-pair production, single-top production and boson-associated top production have been performed [5,6,7,8]. In Figure 1 we show the results of the most recent global fit to LHC top data from Run I and Run II [8].…”
Section: Top Observables At the Lhcmentioning
confidence: 99%
“…• identify the top's chirality in four-quark operators; Figure 1: Global analysis of LHC data for top observables in SMEFT [8]. Shown are 95% (light red/green/blue) and 68% (dark red/green/blue) CL bounds on top operators from global fits to LHJC data on top-pair production (blue), single top (green) and to the full data set of top-pair, single-top and bosonassociated top production (red).…”
“…Stronger bounds can be obtained indirectly, e.g. through global fits [56,57,58,59,60,61,62,63,64], among other methods. 2 However there are assumptions build into any indirect analysis.…”
A common problem in a high energy physics experiment is extracting a signal from a much larger background. Posed as a classification task, there is said to be an imbalance in the number of samples belonging to the signal class versus the number of samples from the background class. In this work we provide a brief overview of class imbalance techniques in a high energy physics setting. Two case studies are presented: (1) the measurement of the longitudinal polarization fraction in same-sign W W scattering, and (2) the decay of the Higgs boson to charm-quark pairs.
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