Abstract <p>The reaction <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="181" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\pi }^{ - }}{\text{Be}} \to {\text{A}}{\kern 1pt} \omega (782)\phi (1020)\)</EquationSource> <!--PhysPart2470222Gotman-m1--> </InlineEquation> is studied at the VES setup. In the <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega \phi \)</EquationSource> <!--PhysPart2470222Gotman-m2--> </InlineEquation> mass spectrum, the peak near the threshold with quantum numbers <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\({{J}^{{PC}}}{{ = 0}^{{ + + }}}\)</EquationSource> <!--PhysPart2470222Gotman-m3--> </InlineEquation> dominates. It is identified as <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\({{f}_{0}}(1710)\)</EquationSource> <!--PhysPart2470222Gotman-m4--> </InlineEquation>. The reaction cross section is measured and the product <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="186" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{Br}}({{f}_{0}} \to \pi \pi ){\text{Br}}({{f}_{0}} \to \omega \phi )\)</EquationSource> <!--PhysPart2470222Gotman-m5--> </InlineEquation> is obtained in the one-pion-exchange approximation. The value obtained leads to a large partial width of the radiative decay <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9065_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(J{\text{/}}\psi \to \gamma {{f}_{0}}\)</EquationSource> <!--PhysPart2470222Gotman-m6--> </InlineEquation>, which is the evidence of a significant glueball component for this resonance.</p>

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Study of Scalar Resonance in the ωϕ System in Pion-Be Interaction at Momentum of 29 GeV/c

  • V. G. Gotman,
  • V. A. Dorofeev,
  • A. M. Zaitsev,
  • I. A. Kachaev,
  • V. I. Lisin,
  • V. D. Matveev,
  • E. V. Nazarov,
  • A. N. Plekhanov,
  • D. I. Ryabchikov,
  • V. P. Sugonyaev,
  • Yu. A. Khokhlov,
  • A. A. Shumakov

摘要

Abstract

The reaction \({{\pi }^{ - }}{\text{Be}} \to {\text{A}}{\kern 1pt} \omega (782)\phi (1020)\) is studied at the VES setup. In the \(\omega \phi \) mass spectrum, the peak near the threshold with quantum numbers \({{J}^{{PC}}}{{ = 0}^{{ + + }}}\) dominates. It is identified as \({{f}_{0}}(1710)\) . The reaction cross section is measured and the product \({\text{Br}}({{f}_{0}} \to \pi \pi ){\text{Br}}({{f}_{0}} \to \omega \phi )\) is obtained in the one-pion-exchange approximation. The value obtained leads to a large partial width of the radiative decay \(J{\text{/}}\psi \to \gamma {{f}_{0}}\) , which is the evidence of a significant glueball component for this resonance.