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NMR study of the magnetization of superfluid helium-3-boron and NMR of superfluid helium-3 in aerogel .

机译:气凝胶中超流动氦3-硼的磁化和超流动氦3的NMR的研究。

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摘要

Pulsed NMR measurements of superfluid 3He confined in 98.2% porosity silica aerogel are reported. The aerogel suppressed the superfluid transition temperature TC and the order parameter magnitude from their bulk values in qualitative agreement with impurity scattering models. Magnetization measurements showed that the superfluid is an equal spin pairing state (ESP). The superfluid exhibited positive NMR frequency shifts with similar temperature dependence to those of the bulk A-phase, only smaller. TC was independent of the magnetic field for H 1.8 kOe to within the experimental error. At 2.18 kOe an increased suppression of TC and the order parameter was observed. Two layers of solid 3He were adsorbed to the aerogel strands. When these were replaced with solid 4He a non-ESP superfluid state was observed.; An experimental cell for measuring the heat capacity of 3He in aerogel was designed and fabricated. It was tested without aerogel by measuring the heat capacity of liquid 3He over a range of temperatures from 1 to 25 mK and at pressures of 7.0, 14.0, and 28.0 bar. The measurements in both the normal and superfluid phases were consistent with the data of Greywall.; The discrepancy between static and dynamic measurements of the magnetization of superfluid 3He-B was characterized over a region of the phase diagram by comparison of nuclear magnetic resonance (NMR) data and recent SQUID data from other researchers. At the B- to A-phase transition, TAB, the discrepancy was absent at low pressure, but increased to 20% at 26.6 bar and 1.2 kOe. The NMR data were consistent with the weak-coupling-plus (wcp) theory at TAB for most pressures and fields. The Ginzburg-Landau strong-coupling parameter gz/( gz)wcp was determined from NMR results to equal 1.00 +/- 0.03 for all pressures. Combinations of the Ginzburg-Landau beta-parameters are reported that are consistent with this observation.
机译:据报道,超流体3He的脉冲NMR测量仅限于98.2%孔隙度的二氧化硅气凝胶中。气凝胶从其体积值抑制了超流体转变温度TC和有序参数幅度,与杂质散射模型定性一致。磁化测量表明,超流体是等自旋配对状态(ESP)。超流体表现出正NMR频移,与本体A相的温度依赖性相似,但温度依赖性较小。对于H <1.8 kOe,在实验误差范围内,TC与磁场无关。在2.18 kOe时,观察到TC和阶数参数的增加。两层固体3He被吸附到气凝胶丝上。当用固体4He代替这些时,观察到非ESP超流体状态。设计并制作了一个用于测量气凝胶中3He热容量的实验电池。通过在1至25 mK的温度范围内以及7.0、14.0和28.0 bar的压力下测量液体3He的热容量,在没有气凝胶的情况下进行了测试。正常相和超流体相的测量值均与Greywall数据一致。通过比较核磁共振(NMR)数据和其他研究人员的最新SQUID数据,在相图区域上表征了超流体3He-B磁化强度静态和动态测量之间的差异。在B相到A相过渡TAB时,低压不存在差异,但在26.6 bar和1.2 kOe时差异增加到20%。对于大多数压力和场,NMR数据与TAB的弱耦合加(wcp)理论一致。从NMR结果确定对于所有压力,Ginzburg-Landau强耦合参数gz /(gz)wcp。据报道,Ginzburg-Landauβ参数的组合与该观察结果一致。

著录项

  • 作者

    Haard, Thomas Michael.;

  • 作者单位

    Northwestern University.;

  • 授予单位 Northwestern University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2001
  • 页码 315 p.
  • 总页数 315
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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