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1)  lattice relaxation
晶格弛豫
1.
Study on the lattice relaxation caused by lead vacancy in PbWO_4 crystal;
PbWO_4晶体中铅空位周围晶格弛豫的研究
2.
The results show that,the models of lattice relaxations resulted by stacking fault are alike in these 4 metals.
计算结果表明,四种金属中由层错导致的晶格弛豫方式都一样,既层错发生处的4个{111}晶面间膨胀,而其他晶面间距被不同程度的压缩;不同的金属其晶格弛豫对层错能的影响不同。
2)  Spin-lattice relaxation
自旋-晶格弛豫
3)  spin lattice relaxation
自旋晶格弛豫
1.
The extended Solomon equations are used to describe the 13 C spin lattice relaxation with the 1H RF field irradiation It is shown that the 13 C spin lattice relaxation with the 1H RF field irradiation is generally a triple exponential course, which can be reduced to a single exponential course in the absence of the 1H initial magnetization and with strong enough RF field irradiation.
用扩展的Solomon方程描述1H受到射频 (RF)场照射时13 C的自旋晶格弛豫过程 。
4)  grain boundary relaxation
晶界弛豫
1.
This article gives an overview of the early development and recent progress of the study of grain boundary relaxation by Chinese scientists, ranging from, the invention of the torsion pendulum for internal friction measurement to the discovery of a critical temperature for the grain boundary relaxation.
文章综述了我国科学工作者50年来关于晶界弛豫研究的早期开拓和近期发展。
5)  crystalline relaxtion
结晶弛豫
6)  proton spin-lattice relaxation rate
质子自旋-晶格弛豫速率
补充资料:自旋-晶格弛豫


自旋-晶格弛豫


  磁共振成像术语。又称纵向弛豫(longitudinal relaxation)或T1弛豫。指平行于外磁场B0方向的磁化矢量的指数性恢复的过程。磁共振成像时,对置于外磁场B0中的自旋系统施加射频脉冲,则自旋系统被激励,其净磁化矢量指向偏转,不再与外磁场B0方向平行(如与B0垂直)。射频脉冲终止后,被激励的质子与周围环境(晶格)之间发生能量交换,把能量传递给周围的晶格,同时其净磁化矢量指向逐渐恢复与外磁场方向平行。该过程在自旋与晶格之间有能量交换,故自旋-晶格弛豫又称热弛豫。自旋-晶格弛豫与外磁场场强有关。
  
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