2022arXiv (Cornell University)Open access

First Observation of the Direct Production of the $χ_{c1}$ in $e^+e^-$ Annihilation

BESIII Collaboration

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Abstract

We study the direct production of the $J^{PC}=1^{++}$ charmonium state $χ_{c1}(1P)$ in electron-positron annihilation by carrying out an energy scan around the mass of the $χ_{c1}(1P)$. The data were collected with the BESIII detector at the BEPCII collider. An interference pattern between the signal process $e^+e^-\to χ_{c1}(1P) \to γJ/ψ\toγμ^+μ^-$ and the background processes $e^+e^-\to γ_{\mathrm{ISR}} J/ψ\toγ_{\rm{ISR}}μ^+μ^-$ and $e^+e^-\toγ_{\rm{ISR}}μ^+μ^-$ are observed by combining all the data samples. The $χ_{c1}(1P)$ signal is observed with a significance of 5.1$σ$. This is the first observation of a $C$-even state directly produced in $e^+e^-$ annihilation. The electronic width of the $χ_{c1}(1P)$ resonance is determined to be $Γ_{ee}=(0.12^{+0.13}_{-0.08})~\mathrm{eV}$, which is of the same order of magnitude as theoretical calculations.

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We study the direct production of the $J^{PC}=1^{++}$ charmonium state $χ_{c1}(1P)$ in electron-positron annihilation by carrying out an energy scan around the mass of the $χ_{c1}(1P)$. The data were collected with the BESIII detector at the BEPCII collider. An interference pattern between the signal process $e^+e^-\to χ_{c1}(1P) \to γJ/ψ\toγμ^+μ^-$ and the background processes $e^+e^-\to γ_{\mathrm{ISR}} J/ψ\toγ_{\rm{ISR}}μ^+μ^-$ and $e^+e^-\toγ_{\rm{ISR}}μ^+μ^-$ are observed by combining all the data samples. The $χ_{c1}(1P)$ signal is observed with a significance of 5.1$σ$. This is the first observation of a $C$-even state directly produced in $e^+e^-$ annihilation. The electronic width of the $χ_{c1}(1P)$ resonance is determined to be $Γ_{ee}=(0.12^{+0.13}_{-0.08})~\mathrm{eV}$, which is of the same order of magnitude as theoretical calculations.

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Available abstract

We study the direct production of the $J^{PC}=1^{++}$ charmonium state $χ_{c1}(1P)$ in electron-positron annihilation by carrying out an energy scan around the mass of the $χ_{c1}(1P)$. The data were collected with the BESIII detector at the BEPCII collider. An interference pattern between the signal process $e^+e^-\to χ_{c1}(1P) \to γJ/ψ\toγμ^+μ^-$ and the background processes $e^+e^-\to γ_{\mathrm{ISR}} J/ψ\toγ_{\rm{ISR}}μ^+μ^-$ and $e^+e^-\toγ_{\rm{ISR}}μ^+μ^-$ are observed by combining all the data samples. The $χ_{c1}(1P)$ signal is observed with a significance of 5.1$σ$. This is the first observation of a $C$-even state directly produced in $e^+e^-$ annihilation. The electronic width of the $χ_{c1}(1P)$ resonance is determined to be $Γ_{ee}=(0.12^{+0.13}_{-0.08})~\mathrm{eV}$, which is of the same order of magnitude as theoretical calculations.

Key concepts: Annihilation, Physics, Electron–positron annihilation, Collider, Nuclear physics, Positron annihilation, Production (economics), Energy (signal processing)

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