A F Ioffe Physical Technical Institute, 26 Politekhnicheskaya, St Petersburg 194021, Russia.
J Phys Condens Matter. 2012 Aug 29;24(34):346002. doi: 10.1088/0953-8984/24/34/346002. Epub 2012 Aug 7.
Spin-wave excitations revealed in the dynamically equilibrated one-dimensional superlattices formed due to phase separation and charge carrier self-organization in doped single crystals of Eu(0.8)Ce(0.2)Mn(2)O(5) and Tb(0.95)Bi(0.05)MnO(3) multiferroics are discussed. Similar excitations, but having lower intensities, were also observed in undoped RMn(2)O(5) (R=Eu, Er, Tb, Bi). This suggests that a charge transfer between manganese ions with different valences, which give rise to the superlattice formation, occurs in undoped multiferroics as well. The spin excitations observed in the native superlattices represent a set of homogeneous spin-wave resonances excited in individual superlattice layers. The positions of these resonances depend on the relation between the numbers of Mn(3+) and Mn(4+) ions, charge carrier concentrations, and barrier depths in the superlattice layers. It has been found that the spin-wave excitations observed in the frequency interval studied (30-50 GHz) form two spin-wave minibands with a gap between them.
在掺杂的 Eu(0.8)Ce(0.2)Mn(2)O(5) 和 Tb(0.95)Bi(0.05)MnO(3) 多铁单晶中,由于相分离和载流子自组织形成的动态平衡一维超晶格中揭示了自旋波激发。在未掺杂的 RMn(2)O(5)(R=Eu、Er、Tb、Bi)中也观察到了类似的激发,但强度较低。这表明,在未掺杂的多铁体中也发生了导致超晶格形成的不同价态锰离子之间的电荷转移。在本征超晶格中观察到的自旋激发代表了在各个超晶格层中激发的一组均匀的自旋波共振。这些共振的位置取决于 Mn(3+)和 Mn(4+)离子的数量、载流子浓度以及超晶格层中的势垒深度之间的关系。已经发现,在所研究的频率间隔(30-50 GHz)中观察到的自旋波激发形成了两个自旋波微带,它们之间存在间隙。