paper

Magnetoelectric effects in single crystals of the cubic ferrimagnetic helimagnet Cu2OSeO3

arXiv:1204.3783 · doi:10.1103/PhysRevB.85.224413

Abstract

We present magnetodielectric measurements in single crystals of the cubic spin-1/2 compound CuOSeO. A magnetic field-induced electric polarization () and a finite magnetocapacitance (MC) is observed at the onset of the magnetically ordered state ( K). Both and MC are explored in considerable detail as a function of temperature (T), applied field , and relative field orientations with respect to the crystallographic axes. The magnetodielectric data show a number of anomalies which signal magnetic phase transitions, and allow to map out the phase diagram of the system in the -T plane. Below the 3up-1down collinear ferrimagnetic phase, we find two additional magnetic phases. We demonstrate that these are related to the field-driven evolution of a long-period helical phase, which is stabilized by the chiral Dzyalozinskii-Moriya term $D \vec{M} \cdot(\bs{\nabla}\times\vec{M})$ that is present in this non-centrosymmetric compound. We also present a phenomenological Landau-Ginzburg theory for the ME effect, which is in excellent agreement with experimental data, and shows three novel features: (i) the polarization has a uniform as well as a long-wavelength spatial component that is given by the pitch of the magnetic helices, (ii) the uniform component of points along the vector , and (iii) its strength is proportional to , where is the longitudinal and is the transverse (and spiraling) component of the magnetic ordering. Hence, the field dependence of P provides a clear signature of the evolution of a conical helix under a magnetic field. A similar phenomenological theory is discussed for the MC.

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