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Observation of psi(3770) --> gamma chi_c0
High Energy Physics - Experiment · Submitted 16 May 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We report the first observation of such decays for J=0 with a branching ratio of (0.73+-0.07+-0.06)%.
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The abstract, sentence by sentence
From e+e- collision data acquired with the CLEO-c detector at CESR, we search for the non-DDbar decays psi(3770) -> gamma chi_cJ, with chi_cJ reconstructed in four exclusive decays modes containing charged pions and kaons. We report the first observation of such decays for J=0 with a branching ratio of (0.73+-0.07+-0.06)%. The rates for different J are consistent with the expectations assuming psi(3770) is predominantly a 1^3D_1 state of charmonium, but only if relativistic corrections are applied.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | From e+e- collision data acquired with the CLEO-c detector at CESR, we search for the non-DDbar decays psi(3770) -> gamma chi_cJ, with chi_cJ reconstructed in four exclusive decays modes containing charged pions and kaons. | method 0.81 | 0.94 | 0.04 | asserted 0.76 |
| s1 | We report the first observation of such decays for J=0 with a branching ratio of (0.73+-0.07+-0.06)%. | result 1.00 | 0.97 | 0.80 | asserted 1.00 |
| s2 | The rates for different J are consistent with the expectations assuming psi(3770) is predominantly a 1^3D_1 state of charmonium, but only if relativistic corrections are applied. | interpretation 0.99 | 0.74 | 0.22 | hedged possibility 0.88 |
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The paper
Original abstract
From e+e- collision data acquired with the CLEO-c detector at CESR, we search for the non-DDbar decays psi(3770) -> gamma chi_cJ, with chi_cJ reconstructed in four exclusive decays modes containing charged pions and kaons. We report the first observation of such decays for J=0 with a branching ratio of (0.73+-0.07+-0.06)%. The rates for different J are consistent with the expectations assuming psi(3770) is predominantly a 1^3D_1 state of charmonium, but only if relativistic corrections are applied.
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References
How the literature uses it
3 arXiv papers cite this in 3 sentences
Papers citing it
Uses its data or values 1 paper
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The E1 widths associated with the ground-state scalar $χ_c0$, i.e., $Γ_χ_c0 →J/ψγ$, $Γ_ ψ(2S) →χ_c0 γ$, and $Γ_ψ(3770) →χ_c0 γ$, and with the $C$-odd axial vector $h_c$, i.e., $Γ_h_c →η_c(1S) γ$, $Γ_η_c(2S) →h_c γ$, have been measured by several experiments [ref] and compiled by PDG [ref] .
Shedding light on charmonium · Numerical results · 0.88
Compares with it 1 paper
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To further support our claim we would like to quote that CLEO [ref] has reported the observation of the $ψ(3770)$ decay into $γχ_c0(1P)$ which has a decay width of 172 KeV, about two orders of magnitude bigger than our results for $γX(3700)$.
The radiative decay of $\psi(3770)$ into the predicted scalar state X(3700) · Radiative Decay · 0.81
Cites it as background 1 paper
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The research on charm hadron physics has experienced a renewed interest in the last years, after the discovery of a few meson states which could not be easily described as $qq̅$ states of quark model potentials, such as the $D_s0(2317)$, the $D_s1(2460)$ [ref] , in the open-charm sector, and the $X(3872)$ [ref] , the $X(3940)$ [ref] , the $Y(3940)$ [ref] or the $Z(3930)$ [ref] , in the hidden-charm sector.
Radiative decays of dynamically generated charmed baryons · Introduction · 0.91
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