<p>As an approximate Goldstone boson with zero quantum number and zero standard model charge, the long-lived <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1708_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> meson exhibits the decay processes that offer a unique opportunity to explore physics beyond the standard model and new sources of charge parity violation. Further, they facilitate the testing of the low-energy quantum chromodynamics theory and measurement of the fundamental parameters of light quarks. To pursue these goals, we propose a plan to construct a super <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1708_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> factory at HIAF high-energy terminal or at CiADS after its energy upgrade. The high-intensity proton beam at HIAF enables the production of many <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1708_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> samples, exceeding <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1708_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="TEX">\(10^{13}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>10</mn> <mn>13</mn> </msup> </math></EquationSource> </InlineEquation> events per year during the first stage, utilizing multiple layers of thin targets composed of light nuclei. This paper presents the physics goals, the first-version conceptual design of the spectrometer, and preliminary simulation results.</p>

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Plan for a super η factory at Huizhou accelerator complex

  • Xurong Chen,
  • Xiong-Hong He,
  • Qiang Hu,
  • De-Xu Lin,
  • Yang Liu,
  • Hao Qiu,
  • Xu Sun,
  • Ye Tian,
  • Rong Wang,
  • Hong-Lin Zhang,
  • Ya-Peng Zhang,
  • Cheng-Xin Zhao

摘要

As an approximate Goldstone boson with zero quantum number and zero standard model charge, the long-lived \(\eta\) η meson exhibits the decay processes that offer a unique opportunity to explore physics beyond the standard model and new sources of charge parity violation. Further, they facilitate the testing of the low-energy quantum chromodynamics theory and measurement of the fundamental parameters of light quarks. To pursue these goals, we propose a plan to construct a super \(\eta\) η factory at HIAF high-energy terminal or at CiADS after its energy upgrade. The high-intensity proton beam at HIAF enables the production of many \(\eta\) η samples, exceeding \(10^{13}\) 10 13 events per year during the first stage, utilizing multiple layers of thin targets composed of light nuclei. This paper presents the physics goals, the first-version conceptual design of the spectrometer, and preliminary simulation results.