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Precision Electroweak Measurements and Constraints on the Standard Model
High Energy Physics - Experiment · Submitted 6 Dec 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
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The abstract, sentence by sentence
This note presents constraints on Standard Model parameters using published and preliminary precision electroweak results measured at the electron-positron colliders LEP and SLC. The results are compared with precise electroweak measurements from other experiments, notably CDF and D{\O}at the Tevatron. Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | This note presents constraints on Standard Model parameters using published and preliminary precision electroweak results measured at the electron-positron colliders LEP and SLC. | contribution 1.00 | 0.42 | 0.16 | asserted 0.99 |
| s1 | The results are compared with precise electroweak measurements from other experiments, notably CDF and D{\O}at the Tevatron. | method 0.85 | 0.41 | 0.04 | asserted 0.99 |
| s2 | Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering. | contribution 0.44 | 0.74 | 0.38 | asserted 1.00 |
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The paper
Original abstract
This note presents constraints on Standard Model parameters using published and preliminary precision electroweak results measured at the electron-positron colliders LEP and SLC. The results are compared with precise electroweak measurements from other experiments, notably CDF and D{\O}at the Tevatron. Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
Human review
References
How later papers used it
54 later papers cite it
13 later papers by other authors are listed below: 13 used its data or values. 1 more paper by the same authors is listed: 1 built on it.
Builds on it 1 paper · 1 by the same authors
By the same authors
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Updated its previous analysis of this paper.
Precision Electroweak Measurements and Constraints on the Standard Model (2008) (same authors) · 0.81 · paraphrased: the licence does not allow quoting
Uses its data or values 13 of 24 papers with this label
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Used this paper's current experimental result of LEP2/Tevatron, M_W = 80.398 ± 0.025, in its plot.
Test of the Littlest Higgs model through the correlation among W boson, top quark and Higgs masses (2008) · 1.00 · paraphrased: the licence does not allow quoting
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Used the 68% and 95% confidence level contours in the (S,T) plane obtained from the LEP Electroweak Working Group, citing this paper.
Electroweak precision constraints on the Lee-Wick Standard Model (2008) · 0.92 · paraphrased: the licence does not allow quoting
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Used this paper's average value of the effective weak mixing angle, 0.23153 ± 0.00016.
Global Electroweak Fits and the Higgs Boson Mass (2008) · 1.00 · paraphrased: the licence does not allow quoting
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Used this paper's experimental estimate of sin^2 theta_eff^lep = 0.2324 ± 0.0012.
Fitting the Phenomenological MSSM (2009) · 1.00 · paraphrased: the licence does not allow quoting
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Used this paper's value alpha_s(M_Z) = 0.1191 ± 0.0027 from hadronic Z decays.
Tau Physics: Theory Overview (2008) · 0.81 · paraphrased: the licence does not allow quoting
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Matched this paper's R(m_Z^2) value from the LEP Collaboration by taking Lambda = 227 MeV.
Thresholds in FAPT: Euclid vs Minkowski (2008) · 0.98 · paraphrased: the licence does not allow quoting
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Derived a 95% C.L. upper limit of 182 GeV using this paper's bound.
Gamma rays from the annihilation of singlet scalar dark matter (2008) · 0.97 · paraphrased: the licence does not allow quoting
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Combined with the precise determination of the $Z$-boson decay rate into hadrons at LEP [ref] this has led to one of the most precise determinations of the strong coupling constant $α_s(M_Z)$.
R(s) and Z decay in order \alpha_s^4: complete results (2012) · Introduction · 0.89
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Used this paper's current LEP 2 average of M_W = 80.399 ± 0.025 GeV.
Electroweak Theory for the Tevatron, LHC, and ILC (2008) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's present experimental uncertainty of ±0.0026 in the extraction of alpha_s.
Complete QCD Corrections to Hadronic $Z$--Decays in Order $\alpha_s^4$ (2012) · 0.89 · paraphrased: the licence does not allow quoting
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Used this paper's indirect constraint that the Higgs mass be below 190 GeV when taking into account the direct bound.
Searches and Prospects for Standard Model Higgs boson at the Tevatron (2008) · 0.85 · paraphrased: the licence does not allow quoting
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Showed this paper's precise constraint on the Higgs mass in terms of Delta chi^2 relative to the best-fit point.
Physics searches at the LHC (2009) · 0.93 · paraphrased: the licence does not allow quoting
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Used this paper's best estimate of sin^2 theta = 0.2324 ± 0.0012.
Supersymmetry vis-\`a-vis Observation: Dark Matter Constraints, Global Fits and Statistical Issues (2011) · 1.00 · paraphrased: the licence does not allow quoting
How the literature uses it
54 arXiv papers cite this in 75 sentences
Papers whose main result relates to this one's
States the same result 5 papers
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Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
Precision Electroweak Measurements and Constraints on the Standard Model · 0.97
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Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\"o}ller scattering, and neutrino-nucleon scattering.
A Combination of Preliminary Electroweak Measurements and Constraints on the Standard Model · 0.94
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Constraints on the input parameters of the Standard Model are derived from the combined set of results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
Precision Electroweak Measurements and Constraints on the Standard Model · 0.91
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Constraints on the input parameters of the Standard Model are derived from the results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, Moller scattering, and neutrino-nucleon scattering.
A Combination of Preliminary Electroweak Measurements and Constraints on the Standard Model · 0.88
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Constraints on the input parameters of the Standard Model are derived from the combined set of results obtained in high-$Q^2$ interactions, and used to predict results in low-$Q^2$ experiments, such as atomic parity violation, M{\o}ller scattering, and neutrino-nucleon scattering.
Precision Electroweak Measurements and Constraints on the Standard Model · 0.83
Papers citing it · 33 sentences without a confident label
Builds on it 1 paper
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This report updates our previous analysis [ref] .
Precision Electroweak Measurements and Constraints on the Standard Model · Introduction · 0.81
Uses its method or tool 1 paper
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The SM computations use the programs TOPAZ0 and ZFITTER (for more details see [ref] ).
Global Electroweak Fits and the Higgs Boson Mass · ELECTROWEAK FITS · 0.95
Uses its data or values 24 papers
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Very recently, Fermilab CDF collaboration has reported the most precise single measurement of the $W$ boson mass to date from Run II of the Tevatron [ref] , [equation] and updated the world average [ref] to [equation] In addition, the world average result of $M_t$ from the Tevatron experiments CDF and D0 has been given [ref] by [equation]
Test of the Littlest Higgs model through the correlation among W boson, top quark and Higgs masses · Introduction · 0.97
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To obtain a better understanding of the importance of the $S$ and $T$ parameters in constraining the model we show in Fig. [ref] the $68%$ and $95%$ Confidence Level contours in the $(S,T)$ plane, as obtained from the LEP Electroweak Working Group [ref] , together with the LWSM predictions for several values of the LW-masses.
Electroweak precision constraints on the Lee-Wick Standard Model · Analysis of the EWPT · 0.92
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There are six determinations of the effective weak mixing angle, giving an average value $$=0.23153 $±$ 0.00016 [ref] .
Global Electroweak Fits and the Higgs Boson Mass · PRECISION ELECTROWEAK DATA · 1.00
Cites it as background 4 papers
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The precise measurement of the electroweak parameters at LEP and SLC are discussed in detail in [ref] .
Measuring Supersymmetry · Abstract · 0.93
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This quantity is an important ingredient for global EW fits, where precision measurements of EW observables are compared to accurate predictions of various parameters of the EW sector of the SM [ref] .
The muon $g$-2 and $\Delta \alpha$ connection · Introduction · 0.99
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The Standard Model Electroweak (EW) Field Theory was confirmed as the correct physics theory of electromagnetic and weak interactions between elementary particles by precision measurements of the LEP experiments [ref] .
QED Exponentiation for quasi-stable charged particles: the $e^-e^+\to W^-W^+$ process · Introduction · 0.88
What it cites · 1 sentence without a confident label
Uses data or values from 2 papers
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Including also the recent result on $$ based on Run-II data by CDF [ref] , the combined results are: $= 80429±39$, $= 2078±87$.[The combined Tevatron result quoted for $$ and used here does not take into account the very recently published CDF result based on Run-II data, $= 2.032±0.073$ [ref] .] Combining these results with the preliminary combination [ref] ,
First Measurement of the W Boson Mass in Run II of the Tevatron · Measurements · 0.90
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Including also the recent result on $$ based on Run-II data by CDF [ref] , the combined results are: $= 80429±39$, $= 2078±87$.[The combined Tevatron result quoted for $$ and used here does not take into account the very recently published CDF result based on Run-II data, $= 2.032±0.073$ [ref] .] Combining these results with the preliminary combination [ref] ,
A direct Measurement of the W Boson Width in ppbar Collisions at sqrt(s) = 1.96 TeV · Measurements · 0.90
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