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Probing electroweak precision physics via boosted Higgs-strahlung at the LHC

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TLDR
In this article, the authors studied the process of reconstructing the Higgs boson at high energies using subjet techniques using the standard model effective field theory (SMEFT).
Abstract
We study the process pp → Zðlþl−Þhðbb¯Þ in the standard model effective field theory (SMEFT) at high energies using subjet techniques to reconstruct the Higgs boson. We show that at high energies this process probes four directions in the dimension-6 EFT space, namely the operators that contribute to the four contact interactions, hZμf¯ γμf, where f ¼ uL; uR; dL and dR. These four directions are, however, already constrained by the Z-pole and diboson measurements at LEP. We show that by utilizing the energy growth of this process in the SMEFT and the accuracy that can be achieved by using subjet techniques at the High Luminosity LHC, one can obtain bounds on these operators that are an order of magnitude better than existing LEP bounds.

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Higgs Physics at the HL-LHC and HE-LHC

Maria Cepeda, +376 more
TL;DR: The potential reach and opportunities in Higgs physics during the High Luminosity phase of the LHC were summarized in this article, with an expected dataset of pp collisions at 14 TeV, corresponding to an integrated luminosity of 3 ab$^{-1}$.
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Top, Higgs, diboson and electroweak fit to the Standard Model effective field theory

TL;DR: In this article, a global analysis with SMEFT operators of dimension 6 included linearly is presented, and the constraints on the coefficients of these operators, both individually and when marginalised, in flavour-universal and top-specific scenarios, studying the interplay of these datasets and the correlations they induce in the SM EFT.
Journal ArticleDOI

On the impact of dimension-eight SMEFT operators on Higgs measurements

TL;DR: In this article, the effect of dimension-8-SM interference and dimension-6-squared terms appeared at the same order in an expansion in 1/Λ, and the authors showed that the effect on the inferred new physics scale is small, with some variation depending on the relative signs of the dimension8 coefficients.
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Diboson at the LHC vs LEP

TL;DR: In this paper, the authors use the current CMS and ATLAS data for the leptonic pp → WW, WZ channels to show that diboson production is, for a broad class of flavour models, already competitive with LEP-1 measurements for setting bounds on the anomalous couplings between the quarks and the electroweak gauge bosons, at least under the assumption that any new particle is heavier than a few TeV.
References
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Journal ArticleDOI

The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations

TL;DR: MadGraph5 aMC@NLO as discussed by the authors is a computer program capable of handling all these computations, including parton-level fixed order, shower-matched, merged, in a unified framework whose defining features are flexibility, high level of parallelisation and human intervention limited to input physics quantities.
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An Introduction to PYTHIA 8.2

TL;DR: Pythia 8.2 is the second main release after the complete rewrite from Fortran to C++, and now has reached such a maturity that it offers a complete replacement for most applications, notably for LHC physics studies.
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FastJet User Manual

TL;DR: FastJet as mentioned in this paper is a C++ package that provides a broad range of jet finding and analysis tools, including efficient native implementations of all widely used 2→1 sequential recombination jet algorithms for pp and e − − collisions.
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FeynRules 2.0 - A complete toolbox for tree-level phenomenology

TL;DR: FeynRules is a Mathematica-based package which addresses the implementation of particle physics models, which are given in the form of a list of fields, parameters and a Lagrangian, into high-energy physics tools.
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Dimension-Six Terms in the Standard Model Lagrangian

TL;DR: In this paper, the authors considered the Standard Model as an effective low-energy theory, higher dimensional interaction terms appear in the Lagrangian and performed their classification once again from the outset.
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