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Search for same-sign top-quark pair production at sqrt(s) = 7 TeV and limits on flavour changing neutral currents in the top sector
High Energy Physics - Experiment · Submitted 10 Jun 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim These limits disfavour the FCNC interpretation of the Tevatron results.
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The abstract, sentence by sentence
An inclusive search for same-sign top-quark pair production in pp collisions at sqrt(s) = 7 TeV is performed using a data sample recorded with the CMS detector in 2010, corresponding to an integrated luminosity of 35 inverse picobarns. This analysis is motivated by recent studies of p p-bar to t t-bar reporting mass-dependent forward-backward asymmetries larger than expected from the standard model. These asymmetries could be due to Flavor Changing Neutral Currents (FCNC) in the top sector induced by t-channel exchange of a massive neutral vector boson (Z'). Models with such a Z' also predict enhancement of same-sign top-pair production in pp or p p-bar collisions. Limits are set as a function of the Z' mass and its couplings to u and t quarks. These limits disfavour the FCNC interpretation of the Tevatron results.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | An inclusive search for same-sign top-quark pair production in pp collisions at sqrt(s) = 7 TeV is performed using a data sample recorded with the CMS detector in 2010, corresponding to an integrated luminosity of 35 inverse picobarns. | method 0.57 | 0.97 | 0.02 | asserted 0.99 |
| s1 | This analysis is motivated by recent studies of p p-bar to t t-bar reporting mass-dependent forward-backward asymmetries larger than expected from the standard model. | background 1.00 | 0.04 | 0.02 | asserted 0.97 |
| s2 | These asymmetries could be due to Flavor Changing Neutral Currents (FCNC) in the top sector induced by t-channel exchange of a massive neutral vector boson (Z'). | background 0.93 | 0.05 | 0.03 | hedged possibility 1.00 |
| s3 | Models with such a Z' also predict enhancement of same-sign top-pair production in pp or p p-bar collisions. | background 0.96 | 0.07 | 0.04 | asserted 0.92 |
| s4 | Limits are set as a function of the Z' mass and its couplings to u and t quarks. | result 0.78 | 0.94 | 0.13 | asserted 0.99 |
| s5 | These limits disfavour the FCNC interpretation of the Tevatron results. | interpretation 0.97 | 0.86 | 0.83 | asserted 0.97 |
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The paper
Original abstract
An inclusive search for same-sign top-quark pair production in pp collisions at sqrt(s) = 7 TeV is performed using a data sample recorded with the CMS detector in 2010, corresponding to an integrated luminosity of 35 inverse picobarns. This analysis is motivated by recent studies of p p-bar to t t-bar reporting mass-dependent forward-backward asymmetries larger than expected from the standard model. These asymmetries could be due to Flavor Changing Neutral Currents (FCNC) in the top sector induced by t-channel exchange of a massive neutral vector boson (Z'). Models with such a Z' also predict enhancement of same-sign top-pair production in pp or p p-bar collisions. Limits are set as a function of the Z' mass and its couplings to u and t quarks. These limits disfavour the FCNC interpretation of the Tevatron results.
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References
How the literature uses it
39 arXiv papers cite this in 54 sentences
Papers citing it · 38 sentences without a confident label
Contests it 1 paper
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For example, the original light $Z^'$ model [ref] is excluded by the recent CMS data on the same sign top pair production [ref] .
Chiral U(1) flavor models and flavored Higgs doublets: the top FB asymmetry and the Wjj · Introduction · contest 0.82
Uses its method or tool 1 paper
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This work relies heavily on the event selections and background estimation methods of the previous CMS inclusive same-sign dilepton searches not requiring b-tagged jets in the final state [ref] .
Search for new physics in events with same-sign dileptons and b-tagged jets in pp collisions at sqrt(s) = 7 TeV · Introduction · 0.95
Uses its data or values 7 papers
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Finally we enforce that the same-sign leptons (which arise due to the leptonic decays of the produced pair of same-sign tops) cross-section also remains within the LHC non-observation limits [ref] for the current data on such events.
Same-sign Tops: A Powerful Diagnostic Test for Models of New Physics · Numerical Analysis and Results · 0.85
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As no excess above the SM expectation is observed, the $95%$ C.L. upper bound on the number of new-physics events were set in Ref. [ref] .
Search for top quark flavour changing neutral currents in same-sign top quark production · Results · 0.95
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The CMS Collaboration announced the upper bound on the cross section for the same-sign top-quark pair production: $σ^tt < 17$ pb at 95% CL. with a luminosity of 35 pb$^-1$ [ref] , while the limit on the cross sections at ATLAS with a luminosity of $1.04$ fb$^-1$ are $σ^tt < 2$ pb at 95% CL. by using an optimized event selection for the $Z^'$ model and $σ^tt < 4$ pb at 95% CL. by using more inclusive selection, respectively [ref] .
Top A_FB at the Tevatron vs. charge asymmetry at the LHC in chiral U(1) flavor models with flavored Higgs doublets · Generalities and Inputs · 0.99
Compares with it 2 papers
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The CMS collaboration has also performed a search for same-sign top quark production [ref] , however, their model-independent limit on the production cross section, 17 pb, is weaker than the above ATLAS bound.
Tracking Down the Top Quark Forward-Backward Asymmetry with Monotops · Same-sign top quark production · 0.91
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This improves the previous CMS limit [ref] by a factor of 27.
Search for new physics in events with same-sign dileptons and b-tagged jets in pp collisions at sqrt(s) = 7 TeV · Models of pp to tt · 1.00
Cites it as support 2 papers
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Despite the small cross section of the signal channels due to the presence of two anomalous vertices for t$t$ production, this final state has been shown to have very little SM background and is sensitive to new-physics effects [ref] .
Search for top quark flavour changing neutral currents in same-sign top quark production · Introduction · 0.98
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However, flavor-changing $Z'$ exchange implies the production of same-sign top pairs at hadron colliders, which faces strong limits from the Tevatron and the LHC [ref] .
Constraints on W Prime Models for the ttbar Asymmetry · Introduction · 0.96
Cites it as background 2 papers
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The main background to this signal comes from the $t t̅$ (when the events are selected without b-tagging), $t t̅+Z$ and $t t̅+W$ productions, as discussed in Refs. [ref] .
Signature of same-sign top pair production mediated by a nonuniversal $Z^\prime$ with QCD next-to-leading accuracy at the LHC · Signature and background · 0.88
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Both the ATLAS and CMS collaborations have searched for anomalous production of events containing pairs of SS leptons at the LHC, using proton–proton $(pp)$ collision data at $√(s)=7,8$ and 13 [ref] .
Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector · Introduction · 0.93
What it cites · 39 sentences without a confident label
Uses the method or tool of 3 papers
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We used the external model interface in the MadGraph [ref] event generator to calculate at the leading order (LO) the $+j$ cross section as a function of $f_R$ and $M_$.
MadGraph/MadEvent v4: The New Web Generation · Introduction · 1.00
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The fractional systematic uncertainty on the event selection efficiencies was calculated as in Ref. [ref] , and its components are summarized in Table [ref].
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy at the LHC · Introduction · 0.95
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These events were then processed by Pythia [ref] for parton showering, followed by the CMS parametrized event simulation, and the same chain of reconstruction and analysis programs used for collision data.
PYTHIA 6.4 Physics and Manual · Introduction · 1.00
Uses data or values from 1 paper
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In this calculation we used the CTEQ6L [ref] parton distribution functions (PDFs), fixed the top quark mass $M_top$ to be 172.5 GeV, and set the renormalization and factorization scales to be $μ= M_top$.
New Generation of Parton Distributions with Uncertainties from Global QCD Analysis · Introduction · 0.83
Discussion
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