Solid State Chemistry Laboratory, Zernike Institute for Advanced Materials, Rijksuniversiteit Groningen, Nijenborgh 4, 9747AG Groningen, The Netherlands.
J Phys Condens Matter. 2010 Feb 24;22(7):075902. doi: 10.1088/0953-8984/22/7/075902. Epub 2010 Feb 2.
We have studied the magnetodieletric coupling of polycrystalline samples of the spinels MCr(2)O(4) (M = Mn, Co and Ni). Dielectric anomalies are clearly observed at the onset of the magnetic spiral structure (T(s)) and at the 'lock-in' transition (T(f)) in MnCr(2)O(4) and CoCr(2)O(4), and also at the onset of the canted structure (T(s)) in NiCr(2)O(4). The strength of the magnetodielectric coupling in this system can be explained by spin-orbit coupling. Moreover, the dielectric response in an applied magnetic field scales with the square of the magnetization for all three samples. Thus, the magnetodielectric coupling in this state appears to originate from the P(2)M(2) term in the free energy.
我们研究了尖晶石 MCr(2)O(4)(M = Mn、Co 和 Ni)多晶样品的磁电耦合。在 MnCr(2)O(4) 和 CoCr(2)O(4)中,在磁性螺旋结构(T(s))和“锁定”转变(T(f))开始时以及在 NiCr(2)O(4)中在倾斜结构(T(s))开始时,明显观察到介电异常。在该系统中,磁电耦合的强度可以通过自旋轨道耦合来解释。此外,对于所有三个样品,在施加磁场时的介电响应与磁化强度的平方成正比。因此,这种状态下的磁电耦合似乎源于自由能中的 P(2)M(2)项。