<p>The decay widths of <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_5975_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="99" /> </InlineMediaObject> <EquationSource Format="TEX">\(V \rightarrow K(\pi ) l \bar{\nu }_l \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo stretchy="false">→</mo> <mi>K</mi> <mrow> <mo stretchy="false">(</mo> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> <mi>l</mi> <msub> <mover accent="true"> <mrow> <mi>ν</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mi>l</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> are calculated within the Nambu–Jona-Lasinio model, where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_5975_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="115" /> </InlineMediaObject> <EquationSource Format="TEX">\(V=K^*, \rho , \omega , \phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mo>=</mo> <msup> <mi>K</mi> <mo>∗</mo> </msup> <mo>,</mo> <mi>ρ</mi> <mo>,</mo> <mi>ω</mi> <mo>,</mo> <mi>ϕ</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10773_2025_5975_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(l=\mu , e\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>l</mi> <mo>=</mo> <mi>μ</mi> <mo>,</mo> <mi>e</mi> </mrow> </math></EquationSource> </InlineEquation>. The results are obtained using the previously fixed model parameters without introducing any arbitrary parameters. The obtained results are considered as predictions due to the absence of experimental data.</p>

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Weak Semileptonic Decays of Vector Mesons in the NJL Model

  • M. K. Volkov,
  • A. A. Pivovarov,
  • K. Nurlan

摘要

The decay widths of \(V \rightarrow K(\pi ) l \bar{\nu }_l \) V K ( π ) l ν ¯ l are calculated within the Nambu–Jona-Lasinio model, where \(V=K^*, \rho , \omega , \phi \) V = K , ρ , ω , ϕ and \(l=\mu , e\) l = μ , e . The results are obtained using the previously fixed model parameters without introducing any arbitrary parameters. The obtained results are considered as predictions due to the absence of experimental data.