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Measuring Electroweak Quantum Numbers of Color Sextet Resonances at the LHC
High Energy Physics - Phenomenology · Submitted 22 Feb 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We utilize this feature and the energy distributions of the final state jets and leptons to distinguish among the three possible color sextet resonances, taking into account various SM background processes at the $13$ TeV LHC.
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The abstract, sentence by sentence
We study the prospect of measuring the electroweak quantum numbers of beyond the Standard Model (SM) color sextet particles that decay into same-sign top quark pairs. Among these particles, the color sextet scalars give rise to top quarks with the same chirality, while the top quarks coming from the color sextet vector would have opposite chirality. This difference gets encoded in the angular distributions of the bottom quarks and leptons originating from the decays of the top quarks. We utilize this feature and the energy distributions of the final state jets and leptons to distinguish among the three possible color sextet resonances, taking into account various SM background processes at the $13$ TeV LHC.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the prospect of measuring the electroweak quantum numbers of beyond the Standard Model (SM) color sextet particles that decay into same-sign top quark pairs. | contribution 0.99 | 0.69 | 0.07 | hedged possibility 0.60 |
| s1 | Among these particles, the color sextet scalars give rise to top quarks with the same chirality, while the top quarks coming from the color sextet vector would have opposite chirality. | background 0.54 | 0.22 | 0.10 | asserted 1.00 |
| s2 | This difference gets encoded in the angular distributions of the bottom quarks and leptons originating from the decays of the top quarks. | method 0.34 | 0.28 | 0.07 | asserted 1.00 |
| s3 | We utilize this feature and the energy distributions of the final state jets and leptons to distinguish among the three possible color sextet resonances, taking into account various SM background processes at the $13$ TeV LHC. | method 0.64 | 0.90 | 0.41 | asserted 0.99 |
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The paper
Original abstract
We study the prospect of measuring the electroweak quantum numbers of beyond the Standard Model (SM) color sextet particles that decay into same-sign top quark pairs. Among these particles, the color sextet scalars give rise to top quarks with the same chirality, while the top quarks coming from the color sextet vector would have opposite chirality. This difference gets encoded in the angular distributions of the bottom quarks and leptons originating from the decays of the top quarks. We utilize this feature and the energy distributions of the final state jets and leptons to distinguish among the three possible color sextet resonances, taking into account various SM background processes at the $13$ TeV LHC.
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References
How the literature uses it
1 arXiv paper cite this in 1 sentence
What it cites · 19 sentences without a confident label
Uses the method or tool of 8 papers
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We calculate the signal significance [ref] using [equation] where $s$ and $b$ stand for the total number of signal and background events surviving after cuts.
Asymptotic formulae for likelihood-based tests of new physics · Results · 1.00
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Events are then passed to PYTHIA8.2 [ref] for showering and hadronization, followed by fast detector simulation in Delphes v3.4.2 [ref] .
An Introduction to PYTHIA 8.2 · Results · 1.00
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Events are then passed to PYTHIA8.2 [ref] for showering and hadronization, followed by fast detector simulation in Delphes v3.4.2 [ref] .
DELPHES 3, A modular framework for fast simulation of a generic collider experiment · Results · 1.00
Uses data or values from 3 papers
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We note that there is an upper bound of $1.2$ pb on the $tt$ production cross-section given by CMS coming from the same-sign di-lepton, missing energy, and jets search [ref] .
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For example, for a lepton, $α_l=1$, whereas for a $b$-quark, $α_b=-0.4$ [ref] .
A model independent spin analysis of fundamental particles using azimuthal asymmetries · Observable · 0.93
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Assuming $CP$ conservation and taking $x≈4×10^-3$ [ref] , we get $Re(λ_1,ccλ_1,uu^*) < 3×10^-7$ for $m_ϕ= 1 TeV$.
2106.03744 · Model · 1.00
Cites as support 2 papers
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Therefore, the top quarks coming from the sextet decay would carry definite polarization and this plays a crucial role in extracting the quantum numbers of the sextet states [ref] .
Color Sextet Scalars in Early LHC Experiments · Introduction · 0.98
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Therefore, the top quarks coming from the sextet decay would carry definite polarization and this plays a crucial role in extracting the quantum numbers of the sextet states [ref] .
Color Sextet Vector Bosons and Same-Sign Top Quark Pairs at the LHC · Introduction · 0.98
Cites as background 15 papers
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The phenomenology and ultraviolet origin of such color sextet diquarks have been discussed extensively in the literature, see, e.g., [ref] .
Diquark Higgs at LHC · Introduction · 0.99
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The phenomenology and ultraviolet origin of such color sextet diquarks have been discussed extensively in the literature, see, e.g., [ref] .
Color Sextet Scalars at the CERN Large Hadron Collider · Introduction · 0.99
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The phenomenology and ultraviolet origin of such color sextet diquarks have been discussed extensively in the literature, see, e.g., [ref] .
Minimal Matter at the Large Hadron Collider · Introduction · 0.99
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