# Measurement of the top quark polarization and $\mathrm{t\bar{t}}$ spin   correlations using dilepton final states in proton-proton collisions at   $\sqrt{s} =$ 13 TeV

**Authors:** CMS Collaboration

arXiv: 1907.03729 · 2019-10-16

## TL;DR

This paper measures top quark polarization and spin correlations in proton-proton collisions at 13 TeV, providing the first parton-level differential cross sections at this energy and testing the standard model predictions.

## Contribution

It presents the first measurement of parton-level differential cross sections for top quark spin observables at 13 TeV and compares them with advanced theoretical predictions.

## Key findings

- Measurements are consistent with the standard model.
- Constraints on anomalous top quark dipole moments are established.
- First parton-level differential cross sections at 13 TeV are reported.

## Abstract

Measurements of the top quark polarization and top quark pair ($\mathrm{t\bar{t}}$) spin correlations are presented using events containing two oppositely charged leptons (e$^+$e$^-$, e$^\pm\mu^\mp$, or $\mu^+\mu^-$) produced in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were recorded by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb$^{-1}$. A set of parton-level normalized differential cross sections, sensitive to each of the independent coefficients of the spin-dependent parts of the $\mathrm{t\bar{t}}$ production density matrix, is measured for the first time at 13 TeV. The measured distributions and extracted coefficients are compared with standard model predictions from simulations at next-to-leading-order (NLO) accuracy in quantum chromodynamics (QCD), and from NLO QCD calculations including electroweak corrections. All measurements are found to be consistent with the expectations of the standard model. The normalized differential cross sections are used in fits to constrain the anomalous chromomagnetic and chromoelectric dipole moments of the top quark to $-$0.24 $<C_\text{tG}/\Lambda^{2}$ $<$ 0.07 TeV$^{-2}$ and $-$0.33 $< C^{I}_\text{tG}/\Lambda^{2}$ $<$ 0.20 TeV$^{-2}$, respectively, at 95% confidence level.

## Figures

40 figures with captions in the complete paper: https://tomesphere.com/paper/1907.03729/full.md

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Source: https://tomesphere.com/paper/1907.03729