Воздействие слабого импульсного магнитного поля на ионную проводимость суперионного проводника Pb-=SUB=-0.67-=/SUB=-Cd-=SUB=-0.33-=/SUB=-F-=SUB=-2-=/SUB=-

Николай Иванович Сорокин, В. М. Каневский
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Abstract

A magnetoconductometric effect was found under pulsed magnetic action (B = 0.1–1 T) on a single crystal of the superionic conductor Pb0.67Cd0.33F2 (cubic symmetry, space group Fm¯3m, unit cell parameter a = 5.7575 A). The static electrical conductivity σdc was determined from impedance spectra in the frequency range (5–5)×105 Hz. In the absence of magnetic influence (B = 0) the ionic conductivity of a superionic crystal is σdc = 1.4×10–4 S/cm. When applying a magnetic field (B = (0.1−1) T) it increases, reaching σdc = 9.5 10−4 S/cm and σdc(B)/σdc(0) = 6.8 at B = 1 T. The nature of the magnetoconductometric effect in the superionic Pb0.67Cd0.33F2 is discussed in connection with the features its atomic structure.
脉冲磁场对超导电性Pb-= -0.67-= -Cd-=SUB - 33-= =SUB -2-= =SUB -
在脉冲磁作用(B = 0.1-1 T)下,超离子导体Pb0.67Cd0.33F2(立方对称,空间群fm¯3m,晶胞参数A = 5.7575 A)单晶产生了磁导效应,并在(5-5)×105 Hz频率范围内测定了其静态电导率σdc。在无磁影响条件下(B = 0),超离子晶体的离子电导率为σdc = 1.4×10-4 S/cm。当施加(B =(0.1−1)T)磁场时,磁导效应增大,在B = 1 T时达到σdc = 9.5 10−4 S/cm, σdc(B)/σdc(0) = 6.8。结合超离子Pb0.67Cd0.33F2的原子结构特征,讨论了磁导效应的性质。
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