Abstract <p>The formation of the multineutron systems <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{2}n\)</EquationSource> <!--NuclPhys2560004Gurov-m5--> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{3}n\)</EquationSource> <!--NuclPhys2560004Gurov-m6--> </InlineEquation> was studied in the reactions of stopped pion absorption by <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{9}\)</EquationSource> <!--NuclPhys2560004Gurov-m7--> </InlineEquation>Be nuclei. Measurements were carried out at low energy pion channel of LANL using two-arm multilayer semiconductor spectrometer. The bound states of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{2}n\)</EquationSource> <!--NuclPhys2560004Gurov-m8--> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{3}n\)</EquationSource> <!--NuclPhys2560004Gurov-m9--> </InlineEquation> have not been found. In the missing mass spectrum of the reaction <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{9}\)</EquationSource> <!--NuclPhys2560004Gurov-m10--> </InlineEquation>Be(<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi^{-}\)</EquationSource> <!--NuclPhys2560004Gurov-m11--> </InlineEquation>, <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(t^{4}\)</EquationSource> <!--NuclPhys2560004Gurov-m12--> </InlineEquation>He), a peak was observed near the threshold, which is due to the formation of the <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq13.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(s\)</EquationSource> <!--NuclPhys2560004Gurov-m13--> </InlineEquation>-wave virtual state of the dineutron. Indications of the existence of two states of the <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{3}n\)</EquationSource> <!--NuclPhys2560004Gurov-m14--> </InlineEquation> with resonant energies (<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq15.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_{r}\approx 6\)</EquationSource> <!--NuclPhys2560004Gurov-m15--> </InlineEquation> MeV, and <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq16.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\approx}14\)</EquationSource> <!--NuclPhys2560004Gurov-m16--> </InlineEquation> MeV) were first obtained in the reactions <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{9}\)</EquationSource> <!--NuclPhys2560004Gurov-m17--> </InlineEquation>Be(<InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi^{-}\)</EquationSource> <!--NuclPhys2560004Gurov-m18--> </InlineEquation>, <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq19.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(d^{4}\)</EquationSource> <!--NuclPhys2560004Gurov-m19--> </InlineEquation>He) and <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{9}\)</EquationSource> <!--NuclPhys2560004Gurov-m20--> </InlineEquation>Be(<InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi^{-}\)</EquationSource> <!--NuclPhys2560004Gurov-m21--> </InlineEquation>, <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11450_2025_3542_Article_IEq22.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(t^{3}\)</EquationSource> <!--NuclPhys2560004Gurov-m22--> </InlineEquation>He). Comparison with theoretical and experimental results obtained by other authors was performed.</p>

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Formation of the Multineutron Systems \({}^{{2}}{n}\) and \({}^{{3}}{n}\) in the Reactions of Stopped Pion Absorption

  • Yu. B. Gurov,
  • B. A. Chernyshev,
  • S. A. Evseev,
  • S. V. Rozov,
  • V. G. Sandukovsky,
  • M. V. Tel’kushev

摘要

Abstract

The formation of the multineutron systems \({}^{2}n\) and \({}^{3}n\) was studied in the reactions of stopped pion absorption by \({}^{9}\) Be nuclei. Measurements were carried out at low energy pion channel of LANL using two-arm multilayer semiconductor spectrometer. The bound states of \({}^{2}n\) and \({}^{3}n\) have not been found. In the missing mass spectrum of the reaction \({}^{9}\) Be( \(\pi^{-}\) , \(t^{4}\) He), a peak was observed near the threshold, which is due to the formation of the \(s\) -wave virtual state of the dineutron. Indications of the existence of two states of the \({}^{3}n\) with resonant energies ( \(E_{r}\approx 6\) MeV, and \({\approx}14\) MeV) were first obtained in the reactions \({}^{9}\) Be( \(\pi^{-}\) , \(d^{4}\) He) and \({}^{9}\) Be( \(\pi^{-}\) , \(t^{3}\) He). Comparison with theoretical and experimental results obtained by other authors was performed.