<p>We conducted a theoretical study on the process <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="98" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Sigma ^{+} p \rightarrow \Lambda a_0^{+} p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi mathvariant="normal">Σ</mi> <mo>+</mo> </msup> <mi>p</mi> <mo stretchy="false">→</mo> <mi mathvariant="normal">Λ</mi> <msubsup> <mi>a</mi> <mn>0</mn> <mo>+</mo> </msubsup> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation> based on an effective Lagrangian approach. This model encompasses the excitation of intermediate resonance leading to the production of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1920)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">(</mo> <mn>1920</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> through <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi ^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>π</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(K^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>K</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> meson exchanges between the initial <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Sigma ^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Σ</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> and <i>p</i> baryons, as well as the generation of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1940)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">(</mo> <mn>1940</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> via <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi ^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>π</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho ^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ρ</mi> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation> meson exchanges. We provide predictions for the total and differential cross sections and discuss the potential impacts of cut-off parameters, off-shell effects, and branching ratios of the <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq11.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="111" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1920) \rightarrow a_0 p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mrow> <mo stretchy="false">(</mo> <mn>1920</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msub> <mi>a</mi> <mn>0</mn> </msub> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="111" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1940) \rightarrow a_0 p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mrow> <mo stretchy="false">(</mo> <mn>1940</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msub> <mi>a</mi> <mn>0</mn> </msub> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation> decays. Given the dominance of <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1940)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">(</mo> <mn>1940</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> in the region close to the reaction threshold, this reaction is considered an ideal platform for exploring the features of the <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_6013_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta (1940)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">(</mo> <mn>1940</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> resonance.</p>

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The Theoretical Study of \(\Sigma ^{+} p \rightarrow \Lambda a_0^{+} p\) Reaction

  • Yan Dai,
  • Xuan Luo,
  • Aojia Xu,
  • Gang Li,
  • Mao Song

摘要

We conducted a theoretical study on the process \(\Sigma ^{+} p \rightarrow \Lambda a_0^{+} p\) Σ + p Λ a 0 + p based on an effective Lagrangian approach. This model encompasses the excitation of intermediate resonance leading to the production of \(\Delta (1920)\) Δ ( 1920 ) through \(\pi ^{+}\) π + and \(K^{+}\) K + meson exchanges between the initial \(\Sigma ^{+}\) Σ + and p baryons, as well as the generation of \(\Delta (1940)\) Δ ( 1940 ) via \(\pi ^{+}\) π + and \(\rho ^{+}\) ρ + meson exchanges. We provide predictions for the total and differential cross sections and discuss the potential impacts of cut-off parameters, off-shell effects, and branching ratios of the \(\Delta (1920) \rightarrow a_0 p\) Δ ( 1920 ) a 0 p and \(\Delta (1940) \rightarrow a_0 p\) Δ ( 1940 ) a 0 p decays. Given the dominance of \(\Delta (1940)\) Δ ( 1940 ) in the region close to the reaction threshold, this reaction is considered an ideal platform for exploring the features of the \(\Delta (1940)\) Δ ( 1940 ) resonance.