<p>Highly oriented pyrolytic graphite (HOPG) is frequently adopted as the reaction target in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C+<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C fusion reaction experiments owing to its superior purity. In this study, we investigate the reaction yield dependence on the accumulated beam dose on HOPG target using a novel detection system consisting of a time-projection chamber and silicon array. The reaction yields are significantly reduced under intense beam bombardment owing to radiation damage to the HOPG surface. The <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq9.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(p_{0,1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>p</mi> <mrow> <mn>0</mn> <mo>,</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> yields decrease by 51.5% and 25%, respectively, when the <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq12.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> beam dose accumulates at 5&#xa0;C. Using the novel detection system and HOPG target, the <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq9.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> yield is determined to be <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq14.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(2.68^{+4.69}_{-1.69}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>.</mo> <msubsup> <mn>68</mn> <mrow> <mo>-</mo> <mn>1.69</mn> </mrow> <mrow> <mo>+</mo> <mn>4.69</mn> </mrow> </msubsup> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq15.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\times\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>×</mo> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(10^{-17}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>10</mn> <mrow> <mo>-</mo> <mn>17</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>/<InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C after correcting for the yield loss due to radiation damage. Our result represents the highest sensitivity achieved to date in direct measurements of <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C(<InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>C,<InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq9.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1714_Article_IEq21.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{20}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>20</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Ne.</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

12C+12C fusion reaction at astrophysical energies using HOPG target

  • Shuo Wang,
  • Yun-Zhen Li,
  • Long-Hui Ru,
  • Xin-Yu Wang,
  • Ning-Tao Zhang,
  • Yi-Hua Fan,
  • Yu-Cheng Feng,
  • Bing-Shui Gao,
  • Hao Huang,
  • Tao-Yu Jiao,
  • Hao Jian,
  • Kuo-Ang Li,
  • Jia-Qing Li,
  • Li-Bin Li,
  • Xiao-Bin Li,
  • Chen-Gui Lu,
  • En-Qiang Liu,
  • Bing-Feng Lv,
  • Hong-Yi Ma,
  • Hooi-Jin Ong,
  • Fu-Shuai Shi,
  • Liang-Ting Sun,
  • Xiao-Dong Tang,
  • Yu Tang,
  • Bing Wang,
  • Hou-Qing Wang,
  • Yao Yang,
  • Yu-Han Zhai,
  • Jin-Long Zhang,
  • Bo Zhang,
  • Peng Zhang,
  • Zhi-Chao Zhang,
  • Xiao-Dong Xu,
  • Wei-Ping Lin,
  • Chun Wen,
  • De-Hao Xie,
  • Zhi-Yong Zhang,
  • Xiao Fang,
  • Hong-Yi Wu,
  • Tao Tian,
  • Jun-Rui Ma,
  • Cheng-Lin Hao,
  • Yu-Na Yang,
  • Yu-Yang Yu,
  • Xue Liu,
  • Yun-Long Lu,
  • Si-Tao Zhu

摘要

Highly oriented pyrolytic graphite (HOPG) is frequently adopted as the reaction target in \(^{12}\) 12 C+ \(^{12}\) 12 C fusion reaction experiments owing to its superior purity. In this study, we investigate the reaction yield dependence on the accumulated beam dose on HOPG target using a novel detection system consisting of a time-projection chamber and silicon array. The reaction yields are significantly reduced under intense beam bombardment owing to radiation damage to the HOPG surface. The \(\alpha _0\) α 0 and \(p_{0,1}\) p 0 , 1 yields decrease by 51.5% and 25%, respectively, when the \(^{12}\) 12 C \(^{2+}\) 2 + beam dose accumulates at 5 C. Using the novel detection system and HOPG target, the \(\alpha _0\) α 0 yield is determined to be \(2.68^{+4.69}_{-1.69}\) 2 . 68 - 1.69 + 4.69 \(\times\) × \(10^{-17}\) 10 - 17 / \(^{12}\) 12 C after correcting for the yield loss due to radiation damage. Our result represents the highest sensitivity achieved to date in direct measurements of \(^{12}\) 12 C( \(^{12}\) 12 C, \(\alpha _0\) α 0 ) \(^{20}\) 20 Ne.