Hemme P, Philippe J-C, Medeiros A, Alekhin A, Houver S, Gallais Y, Sacuto A, Forget A, Colson D, Mantri S, Xu B, Bellaiche L, Cazayous M
Laboratoire Matériaux et Phénomènes Quantiques, Université Paris Cité, CNRS, 10 rue Alice Domon et Léonie Duquet, 75205 Paris Cedex 13, France.
Synchrotron SOLEIL, L'Orme des Merisiers Saint-Aubin, BP 48, 91192 Gif-sur-Yvette, France.
Phys Rev Lett. 2023 Sep 15;131(11):116801. doi: 10.1103/PhysRevLett.131.116801.
More than twenty years ago, multiferroic compounds combining in particular magnetism and ferroelectricity were rediscovered. Since then, BiFeO_{3} has emerged as the most outstanding multiferroic by combining at room temperature almost all the fundamental or applicative properties that may be desired: electroactive spin wave excitations called electromagnons, conductive domain walls, or a low band gap of interest for magnonic devices. All these properties have so far only been discontinuously strain engineered in thin films according to the lattice parameter imposed by the substrate. Here we explore the ferroelectricity and the dynamic magnetic response of BiFeO_{3} bulk under continuously tunable uniaxial strain. Using elasto-Raman spectroscopy, we show that the ferroelectric soft mode is strongly enhanced under tensile strain and driven by the volume preserving deformation at low strain. The magnonic response is entirely modified with low energy magnon modes being suppressed for tensile strain above pointing out a transition from a cycloid to an homogeneous magnetic state. Effective Hamiltonian calculations show that the ferroelectric and the antiferrodistortive modes compete in the tensile regime. In addition, the homogeneous antiferromagnetic state becomes more stable compared to the cycloidal state above a +2% tensile strain close to the experimental value. Finally, we reveal the ferroelectric and magnetic orders of BiFeO_{3} under uniaxial strain and how the tensile strain allows us to unlock and to modify in a differentiated way the polarization and the magnetic structure.
二十多年前,人们重新发现了一类特别结合了磁性和铁电性的多铁性化合物。从那时起,BiFeO₃已成为最杰出的多铁性材料,因为它在室温下几乎结合了所有可能期望的基本或应用特性:被称为电磁子的电活性自旋波激发、导电畴壁,或对磁振子器件有意义的低带隙。到目前为止,所有这些特性仅根据衬底施加的晶格参数在薄膜中通过不连续的应变工程来实现。在这里,我们探索了BiFeO₃块体在连续可调单轴应变下的铁电性和动态磁响应。利用弹性拉曼光谱,我们表明铁电软模在拉伸应变下强烈增强,并在低应变下由体积保持变形驱动。磁振子响应被完全改变,对于高于[具体应变值]的拉伸应变,低能磁振子模式被抑制,这表明从摆线磁状态向均匀磁状态的转变。有效哈密顿量计算表明,铁电模式和反铁畸变模式在拉伸状态下相互竞争。此外,在接近实验值的 +2%拉伸应变以上,均匀反铁磁状态比摆线状态变得更稳定。最后,我们揭示了单轴应变下BiFeO₃的铁电和磁有序,以及拉伸应变如何使我们以不同的方式解锁和修改极化和磁结构。