<p>We have applied the effective field theory (EFT) approach to achieve the astrophysical s-factor for the transition to the first <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mn>2</mn> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>−</mo> </msup> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$2P_{1/2^{-}}$</EquationSource> </InlineEquation> excited state of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>L</mi> <mprescripts /> <none /> <mn>7</mn> </mmultiscripts> <mi>i</mi> </math></EquationSource> <EquationSource Format="TEX">$^{7}Li$</EquationSource> </InlineEquation> nucleus in the <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq7.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="90" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>H</mi> <mprescripts /> <none /> <mn>3</mn> </mmultiscripts> <msup> <mrow> <mo stretchy="false">(</mo> <mi>α</mi> <mo>,</mo> <mi>γ</mi> <mo stretchy="false">)</mo> </mrow> <mn>7</mn> </msup> <mi>L</mi> <mi>i</mi> </math></EquationSource> <EquationSource Format="TEX">$^{3}H(\alpha ,\gamma )^{7}Li$</EquationSource> </InlineEquation> radiative capture reaction. The <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mn>1</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$E_{1}$</EquationSource> </InlineEquation> electrical transition from the <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq9.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mn>2</mn> <msub> <mi>S</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msub> <mo>,</mo> <mn>2</mn> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$2S_{1/2}, 2P_{1/2}$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mn>3</mn> <msub> <mi>S</mi> <mn>1</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$3S_{1}$</EquationSource> </InlineEquation> incoming states have studied in the range of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>E</mi> <mo>≤</mo> <mn>1.5</mn> </math></EquationSource> <EquationSource Format="TEX">$E\leq 1.5$</EquationSource> </InlineEquation> MeV up to leading order (LO) in the presence of Coulomb effects. This work has been performed in continuation of our studies on the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq12.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>H</mi> <mprescripts /> <none /> <mn>3</mn> </mmultiscripts> <mo>−</mo> <mi>α</mi> </math></EquationSource> <EquationSource Format="TEX">$^{3}H-\alpha $</EquationSource> </InlineEquation> reaction for the transition to the ground <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq13.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mn>2</mn> <msub> <mi>P</mi> <mrow> <mn>3</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>−</mo> </msup> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$2P_{3/2^{-}}$</EquationSource> </InlineEquation> state of <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>L</mi> <mprescripts /> <none /> <mn>7</mn> </mmultiscripts> <mi>i</mi> </math></EquationSource> <EquationSource Format="TEX">$^{7}Li$</EquationSource> </InlineEquation>. Both the results have been summed up to obtain the <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10509_2024_4385_Article_IEq15.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mn>34</mn> </msub> <mo stretchy="false">(</mo> <mi>E</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$S_{34}(E)$</EquationSource> </InlineEquation> and compared with the available theoretical and experimental data.</p>

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EFT calculations of \(S_{34}(E)\) for the \(^{3}H(\alpha ,\gamma )^{7}Li\) radiative capture reaction

  • H. Sadeghi,
  • M. Khoddam

摘要

We have applied the effective field theory (EFT) approach to achieve the astrophysical s-factor for the transition to the first 2 P 1 / 2 $2P_{1/2^{-}}$ excited state of L 7 i $^{7}Li$ nucleus in the H 3 ( α , γ ) 7 L i $^{3}H(\alpha ,\gamma )^{7}Li$ radiative capture reaction. The E 1 $E_{1}$ electrical transition from the 2 S 1 / 2 , 2 P 1 / 2 $2S_{1/2}, 2P_{1/2}$ and 3 S 1 $3S_{1}$ incoming states have studied in the range of E 1.5 $E\leq 1.5$ MeV up to leading order (LO) in the presence of Coulomb effects. This work has been performed in continuation of our studies on the H 3 α $^{3}H-\alpha $ reaction for the transition to the ground 2 P 3 / 2 $2P_{3/2^{-}}$ state of L 7 i $^{7}Li$ . Both the results have been summed up to obtain the S 34 ( E ) $S_{34}(E)$ and compared with the available theoretical and experimental data.