Ferroelectric phase transitions of 3d -spin origin in Eu1-x Yx Mn O3
Ferroelectric phase transitions of 3d -spin origin in Eu1-x Yx Mn O3
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DOI:
10.1103/physrevb.76.184418
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发表时间:
2007-11
影响因子:
3.7
通讯作者:
Y. Yamasaki;S. Miyasaka;T. Gotō;H. Sagayama;T. Arima;Y. Tokura
中科院分区:
文献类型:
--
作者:
Y. Yamasaki;S. Miyasaka;T. Gotō;H. Sagayama;T. Arima;Y. Tokura
Perovskite-type rare-earth manganites(and Dy) undergo the ferroelectric transitions concomitantly with the collinear to noncollinear magnetic transitions of Mnspins, in which the electric polarization direction can be controlled by an external magnetic field. To clarify how the magnetic transition of Mnspins is correlated with the ferroelectric transition, we have investigated a mixed-crystal system of perovskite-typewithout themagnetic moments of the rare earth ions. The choice of the present system has enabled us to systematically investigate the correlation between dielectric, magnetic (of Mn spin origin), and superlattice properties with varying the perovskite lattice distortion or equivalently the competing Mn spin superexchange interactions. The compounds withand 0.4 undergo the ferroelectric transitions with the spontaneous polarization along theaxis, which is associated with the formation of a-plane cycloidal spin structure with the modulation vector along theaxis. Among them, thecompound was found to undergo the polarization flop from along theaxis to theaxis as induced not only thermally but also by a magnetic field applied along theaxis. The magnetic-field induced polarization flop and its mechanism forcan be fully accounted for in terms of the rotation of the cycloidal spin plane fromtostemming from the Mn spin flops. This is contrasted by the case ofandwith the rare-earthIsing moments coupled to the Mnspins, in which magnetic fields along theaxis and theaxis, but not along theaxis (up to), can flop the polarization from along theaxis to theaxis.