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Measurement of Double Charmonium Production in $e^+e^-$ Annihilations at $\sqrt{s}=10.6$ GeV
High Energy Physics - Experiment · Submitted 24 Jun 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We observe signals for $\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$ in the recoil mass distribution, thus confirming previous measurements.
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The abstract, sentence by sentence
We study $e^+e^-\to J/\psi c\bar{c}$ by measuring the invariant mass distribution recoiling against fully reconstructed $J/\psi$ decays, using 124 fb$^{-1}$ of data collected with a center-of-mass energy of 10.6 GeV with the $BaBar$ detector. We observe signals for $\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$ in the recoil mass distribution, thus confirming previous measurements. We measure $\sigma(e^+e^-\to J/\psi+c\bar{c}) {\cal B} (c\bar{c} \to >2 \mathrm{charged})$ to be $17.6\pm2.8\textrm{(stat)}^{+1.5}_{-2.1}\textrm{(syst)}$ fb, $10.3\pm2.5\textrm{(stat)}^{+1.4}_{-1.8}\textrm{(syst)}$ fb, and $16.4\pm3.7\textrm{(stat)}^{+2.4}_{-3.0}\textrm{(syst)}$ fb with $c\bar{c}=\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$, respectively.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study $e^+e^-\to J/\psi c\bar{c}$ by measuring the invariant mass distribution recoiling against fully reconstructed $J/\psi$ decays, using 124 fb$^{-1}$ of data collected with a center-of-mass energy of 10.6 GeV with the $BaBar$ detector. | method 0.81 | 0.97 | 0.04 | asserted 0.97 |
| s1 | We observe signals for $\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$ in the recoil mass distribution, thus confirming previous measurements. | result 0.97 | 0.90 | 0.24 | asserted 1.00 |
| s2 | We measure $\sigma(e^+e^-\to J/\psi+c\bar{c}) {\cal B} (c\bar{c} \to >2 \mathrm{charged})$ to be $17.6\pm2.8\textrm{(stat)}^{+1.5}_{-2.1}\textrm{(syst)}$ fb, $10.3\pm2.5\textrm{(stat)}^{+1.4}_{-1.8}\textrm{(syst)}$ fb, and $16.4\pm3.7\textrm{(stat)}^{+2.4}_{-3.0}\textrm{(syst)}$ fb with $c\bar{c}=\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$, respectively. | result 1.00 | 0.97 | 0.64 | asserted 1.00 |
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The paper
Original abstract
We study $e^+e^-\to J/\psi c\bar{c}$ by measuring the invariant mass distribution recoiling against fully reconstructed $J/\psi$ decays, using 124 fb$^{-1}$ of data collected with a center-of-mass energy of 10.6 GeV with the $BaBar$ detector. We observe signals for $\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$ in the recoil mass distribution, thus confirming previous measurements. We measure $\sigma(e^+e^-\to J/\psi+c\bar{c}) {\cal B} (c\bar{c} \to >2 \mathrm{charged})$ to be $17.6\pm2.8\textrm{(stat)}^{+1.5}_{-2.1}\textrm{(syst)}$ fb, $10.3\pm2.5\textrm{(stat)}^{+1.4}_{-1.8}\textrm{(syst)}$ fb, and $16.4\pm3.7\textrm{(stat)}^{+2.4}_{-3.0}\textrm{(syst)}$ fb with $c\bar{c}=\eta_c(1S)$, $\chi_{c0}$, and $\eta_c(2S)$, respectively.
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References
How the literature uses it
44 arXiv papers cite this in 58 sentences
Papers citing it · 36 sentences without a confident label
Uses its data or values 9 papers
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Later in the year 2005, another independent measurement was finished by BABAR [ref] , and the total cross section is $σ[J/ψ+η_c] ×B^η_c[≥2] = (17.6±2.8^+1.5_-2.1) fb$.
Next-to-next-to-leading-order QCD corrections to $J/\psi$ plus $\eta_c$ production at the $B$ factories · Introduction · 0.97
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The BABAR Collaboration has also measured this quantity, and obtains $σ[e^+e^-→J/ψ+η_c]×B_> 2=17.6±2.8±2.1 fb$ (Ref. [ref] ).
Resummation of Relativistic Corrections to e+ e- -> J/psi+eta_c · Introduction · 0.89
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Later the Belle Collaboration updated the value as $25.6±2.8±3.4$ fb [ref] and the BABAR Collaboration also reported a large cross section of $17.6±2.8±2.1$ fb [ref] , where the values include the branching fraction of the system recoiling against the $J/ψ$ into two or more charged tracks.
Recent Developments in Heavy-Quarkonium Phenomenology · Relativistic corrections to quarkonium processes · 0.98
Compares with it 1 paper
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We find the theoretical value of $σ[e^+e^-⟶J/Ψη_c]=21.75fb$, which is broadly in agreement with the Babar's data $σ[e^+e^-⟶J/Ψη_c]=(17.6±2.8±2.1)fb$ [ref] and the Belle's data, $σ[e^+e^-⟶J/Ψη_c]=(25.6±2.8±3.4)fb$ [ref] .
Cross section for double charmonium production in electron-positron annihilation at energy $\sqrt{s}$= 10.6 GeV · Discussion · 0.93
Cites it as support 2 papers
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For example, in the case of double charmonia production at B-factories Belle and BaBar there is about an order of magnitude difference between LC and NRQCD results and only LC solves the long standing contradiction between theory and experiment [ref]
Charmonia Production in $W\to (c\bar{c}) D_{s}^{(*)}$ Decays · Introduction · 0.96
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Recently, however, an attempts were made to use it also for heavy quarkonia production at B-factories Belle and BaBar at $√(s_ee)=10.6$ GeV (see [ref] ) and agreement between obtained theoretical predictions and experimental data shows us that light-cone formalism can be used also to describe reactions with heavy quarkonium mesons.
Double Charmonia Production in Exclusive $Z$ Boson Decays · Light Cone Expansion · 0.96
Cites it as background 9 papers
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The measurements of the cross section for exclusive $J/ψ+η_c$ production from $e^+e^-$ annihilation carried out by the Belle [ref] and BABAR [ref] collaborations have triggered rapid progress in the heavy-quarkonium theory based on the nonrelativistic QCD (NRQCD) factorization approach [ref] .
Exclusive heavy quarkonium + gamma production from e+ e- annihilation into a virtual photon · Introduction · 0.81
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Over the past decades, the research on double charmonium at various high-energy colliders has been made considerable progress both experimentally and theoretically [ref] .
Next-to-leading-order QCD correction to the exclusive double charmonium production via $Z$ decays · Introduction · 0.99
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The benchmark processes, exemplified by $e^+e^-→J/ψ+H$, with $H=η_c, χ_c0,1,2,…$ representing a $C$-even charmonium that recoils against $J/ψ$, are first observed at two $B$ factories in the beginning of this century [ref] .
${\mathcal O}(\alpha_s^2)$ corrections to $J/\psi+\chi_{c0,1,2}$ production at $B$ factories · Introduction · 0.81
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