<p>The China Spallation Neutron Source (CSNS) is the fourth pulsed accelerator-driven neutron source in the world, and it achieved its design target of 100&#xa0;kW in 2020. The planned China Spallation Neutron Source Phase II (CSNS-II) commenced in 2024. The CSNS-II linac design primarily involves the addition of a radio-frequency ion source and a section of a superconducting linear accelerator composed of two types of superconducting cavities, namely double-spoke and six-cell elliptical cavities, after the drift tube linac (DTL). The development of the double-spoke superconducting cavity began in early 2021, and by January 2023, the welding, post-processing, and vertical tests of two 324&#xa0;MHz double-spoke cavity prototypes were completed, with vertical test gradients of 11.6 and 15&#xa0;MV/m, and <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1716_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(Q_{0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>Q</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1716_Article_IEq2.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ge\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>≥</mo> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1716_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(3\times 10^{10}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo>×</mo> <msup> <mn>10</mn> <mn>10</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> @ <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1716_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="121" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_\text {acc}\le {10}\,\text{MV/m}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mtext>acc</mtext> </msub> <mo>≤</mo> <mn>10</mn> <mspace width="0.166667em" /> <mtext>MV/m</mtext> </mrow> </math></EquationSource> </InlineEquation>. The R&amp;D of the cryomodule began in January 2022. In October 2023, the clean assembly of the double-spoke cavity string and cold mass installation of the cryomodule commenced, with the installation of the cryomodule and valve box completing in two months. In January 2024, a horizontal test of the cryomodule was completed, making it the first double-spoke cavity cryomodule in China. The test results showed that the maximum gradients of the two superconducting cavities at a pulse width of 4&#xa0;ms and repetition frequency of 25&#xa0;Hz were 12.8 and 15.2&#xa0;MV/m, respectively. This article provides a detailed introduction to the double-spoke superconducting cavity, tuner, coupler, and cryomodule, elaborates on the clean assembly of the cavity string and cold mass installation of the cryomodule, and provides a detailed analysis of the horizontal test results.</p>

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Integration and horizontal testing of the CSNS-II double-spoke cavity cryomodule

  • Wei-Min Pan,
  • Wen-Zhong Zhou,
  • Fei-Si He,
  • Rui Ge,
  • Miao-Fu Xu,
  • Zheng-Hui Mi,
  • Jin Dai,
  • Ye Han,
  • Mei Li,
  • Zhe-Xin Xie,
  • Ming Liu,
  • Qun-Yao Wang,
  • Hai-Ying Lin,
  • Bai-Qi Liu,
  • Xiao-Long Wang,
  • Zhen-Qiang He,
  • Tong-Ming Huang,
  • Qiang Ma,
  • Xu Chen,
  • Min-Jing Sang,
  • Ke-Yu Zhu,
  • Tong-Xian Zhao,
  • Chang-Cheng Ma,
  • Rui Ye,
  • Zheng-Ze Chang,
  • Liang-Rui Sun,
  • Meng-Xu Fan,
  • Cong Zhang,
  • Hua-Chang Liu,
  • Zhen-Cheng Mu,
  • Tong Wang,
  • Bin Ye,
  • Yang Meng,
  • Lin-Yang Rong,
  • Hui Zhang,
  • Bo Wang,
  • Ma-Liang Wan,
  • Yun Wang,
  • Sheng Wang

摘要

The China Spallation Neutron Source (CSNS) is the fourth pulsed accelerator-driven neutron source in the world, and it achieved its design target of 100 kW in 2020. The planned China Spallation Neutron Source Phase II (CSNS-II) commenced in 2024. The CSNS-II linac design primarily involves the addition of a radio-frequency ion source and a section of a superconducting linear accelerator composed of two types of superconducting cavities, namely double-spoke and six-cell elliptical cavities, after the drift tube linac (DTL). The development of the double-spoke superconducting cavity began in early 2021, and by January 2023, the welding, post-processing, and vertical tests of two 324 MHz double-spoke cavity prototypes were completed, with vertical test gradients of 11.6 and 15 MV/m, and \(Q_{0}\) Q 0 \(\ge\) \(3\times 10^{10}\) 3 × 10 10 @ \(E_\text {acc}\le {10}\,\text{MV/m}\) E acc 10 MV/m . The R&D of the cryomodule began in January 2022. In October 2023, the clean assembly of the double-spoke cavity string and cold mass installation of the cryomodule commenced, with the installation of the cryomodule and valve box completing in two months. In January 2024, a horizontal test of the cryomodule was completed, making it the first double-spoke cavity cryomodule in China. The test results showed that the maximum gradients of the two superconducting cavities at a pulse width of 4 ms and repetition frequency of 25 Hz were 12.8 and 15.2 MV/m, respectively. This article provides a detailed introduction to the double-spoke superconducting cavity, tuner, coupler, and cryomodule, elaborates on the clean assembly of the cavity string and cold mass installation of the cryomodule, and provides a detailed analysis of the horizontal test results.