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Forward-backward asymmetry and differential cross section of top quark in flavor violating $Z'$ model at $\mathscr{O}(\alpha_s^2 \alpha_X)$
High Energy Physics - Phenomenology · Submitted 13 Jun 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim After including the new higher order correction, the differential cross section can fit the data better than those only including the leading contributions from $Z'$, while the forward-backward asymmetry is still in agreement with the measurement.
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The abstract, sentence by sentence
In this paper, forward-backward asymmetry and differential cross section of top quark in flavor violating $Z'$ model up to $\mathscr{O}(\alpha_s^2 \alpha_X)$ at Tevatron are calculated. In order to account for the top observed large forward-backward asymmetry, the new coupling $g_X$ among $Z'$ and quarks will be not much less than strong coupling constant $g_s$. After including the new higher order correction, the differential cross section can fit the data better than those only including the leading contributions from $Z'$, while the forward-backward asymmetry is still in agreement with the measurement.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper, forward-backward asymmetry and differential cross section of top quark in flavor violating $Z'$ model up to $\mathscr{O}(\alpha_s^2 \alpha_X)$ at Tevatron are calculated. | contribution 1.00 | 0.94 | 0.11 | asserted 0.99 |
| s1 | In order to account for the top observed large forward-backward asymmetry, the new coupling $g_X$ among $Z'$ and quarks will be not much less than strong coupling constant $g_s$. | interpretation 0.71 | 0.39 | 0.28 | asserted 0.58 |
| s2 | After including the new higher order correction, the differential cross section can fit the data better than those only including the leading contributions from $Z'$, while the forward-backward asymmetry is still in agreement with the measurement. | result 0.98 | 0.91 | 0.54 | asserted 0.95 |
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The paper
Original abstract
In this paper, forward-backward asymmetry and differential cross section of top quark in flavor violating $Z'$ model up to $\mathscr{O}(\alpha_s^2 \alpha_X)$ at Tevatron are calculated. In order to account for the top observed large forward-backward asymmetry, the new coupling $g_X$ among $Z'$ and quarks will be not much less than strong coupling constant $g_s$. After including the new higher order correction, the differential cross section can fit the data better than those only including the leading contributions from $Z'$, while the forward-backward asymmetry is still in agreement with the measurement.
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References
How the literature uses it
29 arXiv papers cite this in 37 sentences
Papers citing it · 13 sentences without a confident label
Uses its method or tool 1 paper
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However, we carry out independent calculations [ref] with the help of FeynCalc [ref] , FormCalc [ref] and QCDLoop [ref] .
One-side Forward-backward Asymmetry in Top Quark Pair Production at CERN Large Hadron Collider · Introduction · 0.82
Cites it as background 20 papers
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Similarly, model-independent analyses were performed [ref] and new physics models were invoked [ref] to explain earlier D0 and CDF measurements of the inclusive asymmetry [ref] .
Implications of the CDF t \bar t Forward-Backward Asymmetry for Hard Top Physics · Introduction · 0.94
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However, from a phenomenological point of view, these models mainly fall into only two categories according to the nature of the new particle exchange: (i) $s$-channel exchange of vector mediators (e.g. axigluon models) [ref] or (ii) $t$-channel exchange of flavor-violating mediators [ref] [There is another class of models that can create effective axial QCD coupling from NP [ref] . ].
Tevatron Top $A_{FB}$ Versus LHC Top Physics · Introduction · 0.85
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Models proposed thus far in the literature that generate the observed Tevatron $$ at tree level while not grossly disrupting the top pair production cross section fall into two categories according to the nature of the new particle exchange: (i) $s$-channel exchange of vector mediators with axial couplings (e.g. axigluon models) [ref] or (ii) $t$-channel exchange of flavor-violating mediators [ref] .
On Models of New Physics for the Tevatron Top A_FB · Introduction · 0.82
What it cites · 12 sentences without a confident label
Uses the method or tool of 3 papers
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Two cutoff phase space slicing method [ref] is applied for such processes.
The two cutoff phase space slicing method · Contributions at $𝒪(α^2_s α_X)$ · 1.00
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The calculations are carried out with the help of FeynCalc [ref] , FormCalc [ref] and QCDloop [ref] .
Scalar one-loop integrals for QCD · Contributions at $𝒪(α^2_s α_X)$ · 1.00
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The calculations are carried out with the help of FeynCalc [ref] , FormCalc [ref] and QCDloop [ref] .
Automatized One-Loop Calculations in 4 and D dimensions · Contributions at $𝒪(α^2_s α_X)$ · 1.00
Compares with 1 paper
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Histograms are drawn here in order to compare conveniently with the experimental measurements [ref] .
First Measurement of the $\lowercase{\ttbar}$ Differential Cross Section $\lowercase{d\sigma/d}M_{\lowercase{{t\overline{t}}}}$ in $\lowercase{\ppbar}$ Collisions at $\sqrt{\lowercase{s}}=1.96$ TeV · Numerical Results · 0.80
Cites as background 14 papers
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SM predictions have been estimated in Refs. [ref] .
Charge asymmetry of heavy quarks at hadron colliders · Introduction · 0.87
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SM predictions have been estimated in Refs. [ref] .
Top Quarks, Axigluons and Charge Asymmetries at Hadron Colliders · Introduction · 0.87
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SM predictions have been estimated in Refs. [ref] .
Charge asymmetry in hadroproduction of heavy quarks · Introduction · 0.87
Discussion
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