<p>We present the complete set of measured inelastic angular distributions (ADs) for d<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(+^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mo>+</mo> <mn>9</mn> </msup> </math></EquationSource> </InlineEquation>Be system at a deuteron beam energy (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(E_\textrm{d}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mtext>d</mtext> </msub> </math></EquationSource> </InlineEquation>) of 14.5 MeV, corresponding to the (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\frac{1}{2}^+\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(E_x=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>x</mi> </msub> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 1.684 MeV) and (<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\frac{5}{2}^+\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mfrac> <mn>5</mn> <mn>2</mn> </mfrac> <mo>+</mo> </msup> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(E_x =\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>x</mi> </msub> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 3.049 MeV) excited states of <sup>9</sup>Be. These measured inelastic <sup>9</sup>Be(d,d)<sup>9</sup>Be* ADs, along with the previously measured <sup>9</sup>Be(d,d)<sup>9</sup>Be elastic ADs at <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(E_\textrm{d }=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mtext>d</mtext> </msub> <mspace width="0.333333em" /> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 7–35 MeV, were analysed in various nuclear potentials. The inelastic AD data for the studied <sup>9</sup>Be excited states were modelled within the coupled-channel (CC) framework and the corresponding deformation parameters were extracted. Additionally, we present the measured ADs for the <sup>9</sup>Be(d,t)<sup>9</sup>Be neutron pickup transfer reaction at <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(E_\textrm{d }=\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mtext>d</mtext> </msub> <mspace width="0.333333em" /> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 14.5 MeV, populating the (0<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mo>+</mo> </mmultiscripts> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(E_x =\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>x</mi> </msub> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 0.0 MeV) and (2<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mo>+</mo> </mmultiscripts> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(E_x =\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>x</mi> </msub> <mo>=</mo> </mrow> </math></EquationSource> </InlineEquation> 3.04 MeV) states of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Be. The <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(^{9}\hbox {Be(d,t)}^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> <msup> <mtext>Be(d,t)</mtext> <mn>9</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>Be transfer reaction was analysed using the method of distorted waves Born approximation (DWBA) and the optimal spectroscopic amplitudes (SAs) of the configurations <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Be<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\rightarrow ^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mo stretchy="false">→</mo> <mn>9</mn> </msup> </math></EquationSource> </InlineEquation>Be + n and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>9</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Be<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\rightarrow ^{9}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mo stretchy="false">→</mo> <mn>9</mn> </msup> </math></EquationSource> </InlineEquation>Be* <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(+ \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>+</mo> </math></EquationSource> </InlineEquation>n were determined and cross-checked with the existing literature values.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Study of (d, d) scattering and (d, t) reaction on 9Be nuclei at 14.5 MeV

  • Maulen Nassurlla,
  • S K Sakhiyev,
  • N Burtebayev,
  • S B Sakuta,
  • Marzhan Nassurlla,
  • R A Khojayev,
  • K A Talpakova,
  • A Nurpeisov,
  • D A Issayev,
  • Awad A Ibraheem,
  • SH Hamada,
  • Ahmed Hammad Amer

摘要

We present the complete set of measured inelastic angular distributions (ADs) for d \(+^{9}\) + 9 Be system at a deuteron beam energy ( \(E_\textrm{d}\) E d ) of 14.5 MeV, corresponding to the ( \(\frac{1}{2}^+\) 1 2 + , \(E_x=\) E x = 1.684 MeV) and ( \(\frac{5}{2}^+\) 5 2 + , \(E_x =\) E x = 3.049 MeV) excited states of 9Be. These measured inelastic 9Be(d,d)9Be* ADs, along with the previously measured 9Be(d,d)9Be elastic ADs at \(E_\textrm{d }=\) E d = 7–35 MeV, were analysed in various nuclear potentials. The inelastic AD data for the studied 9Be excited states were modelled within the coupled-channel (CC) framework and the corresponding deformation parameters were extracted. Additionally, we present the measured ADs for the 9Be(d,t)9Be neutron pickup transfer reaction at \(E_\textrm{d }=\) E d = 14.5 MeV, populating the (0 \(^+\) + , \(E_x =\) E x = 0.0 MeV) and (2 \(^+\) + , \(E_x =\) E x = 3.04 MeV) states of \(^{9}\) 9 Be. The \(^{9}\hbox {Be(d,t)}^{9}\) 9 Be(d,t) 9 Be transfer reaction was analysed using the method of distorted waves Born approximation (DWBA) and the optimal spectroscopic amplitudes (SAs) of the configurations \(^{9}\) 9 Be \(\rightarrow ^{9}\) 9 Be + n and \(^{9}\) 9 Be \(\rightarrow ^{9}\) 9 Be* \(+ \) + n were determined and cross-checked with the existing literature values.