1) re-entrant spin glass
重入自旋玻璃
2) re-entrant spin-glass state
重入自旋玻璃态
3) reentrant spin-glass
再入自旋玻璃
4) spin-glass
自旋玻璃
1.
Charge order phase and reentrant spin-glass behavior in half doped Sm_(0.5)Ca_(0.5)MnO_3 manganite;
半掺杂Sm_(0.5)Ca_(0.5)MnO_3体系的电荷有序和再入型自旋玻璃行为
2.
This paper reviews the new progress in the residual entropy of glass systems and the entropy -freezing in spin-glass systems and proposes a new explanations of the existence of residual en tropy.
本文综述了有关一般玻璃系统零点剩余熵研究的新进展，同时介绍了自旋玻璃系统的熵冻结问题。
3.
With the temperature decreasing,the system undergoes a transition from paramagnetic(PM) to ferromagnetic(FM) and further to spin-glass(SG).
随温度的降低样品表现出从顺磁(PM)到铁磁(FM)及自旋玻璃态(SG)等复杂的磁相变行为。
5) spin glass
自旋玻璃
1.
Nonequilibrium properties of Sherrington-Kirkpatric spin glass model
Sherrington-Kirkpatric自旋玻璃模型的非平衡态性质
2.
Characteristic spin glass state occurred near the 225K which is due to the competition between the ferromagnetic and antiferromagnetic properties.
此材料呈现出一种典型的自旋玻璃特性,在T=225K发生自旋冻结。
3.
Quantum Sherrington Kirkpatrick (SK) spin glass model is investigated with the help of the static replica symmetric spin glass theory.
研究了量子Ｓｈｅｒｒｉｎｇｔｏｎ－Ｋｉｒｋｐａｔｒｉｃｋ自旋玻璃模型。
6) second-entering-type spin glass behavior
再入型自旋玻璃行为
补充资料：自旋-自旋弛豫
自旋-自旋弛豫
磁共振成像术语。又称T2弛豫或横向弛豫(transverse relaxation)，指垂直于外磁场B0方向的磁化矢量的指数性衰减过程。磁共振成像时，对置于外磁场B0中的自旋系统施加90°射频脉冲，则自旋系统被激励，其净磁化矢量指向与外磁场B0垂直；射频脉冲终止后，被激励的质子与邻近的原子核之间发生相互作用，逐渐失去相位，净磁化矢量指向恢复与外磁场平行，该过程称自旋-自旋弛豫。自旋-自旋弛豫过程无能量交换。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条