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Impact of nitrogen doping of niobium superconducting cavities on the sensitivity of surface resistance to trapped magnetic flux

机译:铌超导腔中氮掺杂对表面电阻对俘获磁通量敏感性的影响

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摘要

Future particle accelerators such as the SLAC "Linac Coherent Light Source-Ⅱ" (LCLS-Ⅱ) and the proposed Cornell Energy Recovery Linac require hundreds of superconducting radio-frequency (SRF) niobium cavities operating in continuous wave mode. In order to achieve economic feasibility of projects such as these, the cavities must achieve a very high intrinsic quality factor (Q_0) to keep cryogenic losses within feasible limits. To reach these high Q_0's in the case of LCLS-Ⅱ, nitrogen-doping of niobium cavities has been selected as the cavity preparation technique. When dealing with Q_0's greater than 1 × 10~(10), the effects of ambient magnetic field on Q_0 become significant. Here, we show that the sensitivity to RF losses from trapped magnetic field in a cavity's walls is strongly dependent on the cavity preparation. Specifically, standard electropolished and 120℃ baked cavities show a sensitivity of residual resistance from trapped magnetic flux of ~0.6 and ~0.8 nΩ/mG trapped, respectively, while nitrogen-doped cavities show a higher sensitivity of residual resistance from trapped magnetic flux of ~1 to 5 nΩ/mG trapped. We show that this difference in sensitivities is directly related to the mean free path of the RF surface layer of the niobium: shorter mean free paths lead to less sensitivity of residual resistance to trapped magnetic flux in the dirty limit (ℓ << ξ_0), while longer mean free paths lead to lower sensitivity of residual resistance to trapped magnetic flux in the clean limit (ℓ >> ξ_0). These experimental results are also shown to have good agreement with recent theoretical predictions for pinned vortex lines oscillating in RF fields.
机译:诸如SLAC“ Linac相干光源-Ⅱ”(LCLS-Ⅱ)和拟议的Cornell能量回收直线加速器之类的未来粒子加速器需要以连续波模式运行的数百个超导射频(SRF)铌腔。为了实现此类项目的经济可行性,型腔必须达到很高的固有品质因数(Q_0),以将低温损失保持在可行的范围内。为了在LCLS-Ⅱ的情况下达到这些较高的Q_0,已经选择了氮掺杂铌腔作为腔制备技术。当处理大于1×10〜(10)的Q_0时,环境磁场对Q_0的影响变得明显。在这里,我们表明,腔壁中捕获的磁场对RF损耗的敏感性很大程度上取决于腔的制备。具体而言,标准电抛光和120℃烘烤的型腔分别显示出对被困磁通量的残余电阻敏感度分别为〜0.6和〜0.8nΩ/ mG,而氮掺杂的腔对被捕获的磁通量对残留磁通的敏感度更高。陷获1至5nΩ/ mG。我们表明,灵敏度的这种差异直接与铌的射频表面层的平均自由程有关:平均自由程越短,则在脏极限(ℓ<<ξ_0)中对残留磁通的剩余电阻的敏感性越小,而更长的平均自由程会导致在干净极限内(residual >>ξ_0)剩余电阻对捕获的磁通量的敏感性降低。这些实验结果还显示出与针对RF场中振荡的固定涡旋线的最新理论预测具有良好的一致性。

著录项

  • 来源
    《Journal of Applied Physics》 |2016年第7期|073904.1-073904.7|共7页
  • 作者单位

    Cornell Laboratory for Accelerator-Based Sciences and Education, Ithaca, New York 14853, USA;

    Cornell Laboratory for Accelerator-Based Sciences and Education, Ithaca, New York 14853, USA;

    Cornell Laboratory for Accelerator-Based Sciences and Education, Ithaca, New York 14853, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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