论文标题

Fe掺杂的Ca $ _ {3} $ ru $ _ {2} $ o $ $ $ _ {7} $极性金属的μsr调查

μSR investigation of the Fe-doped Ca$_{3}$Ru$_{2}$O$_{7}$ polar metal

论文作者

Lamura, G., Das, D., Shang, T., Peng, J., Wang, Y., Mao, Z. Q., Shiroka, T.

论文摘要

ca $ _ {3} $ ru $ _ {2} $ o $ $ _ {7} $是属于多型磁性材料类的极性金属。在这里,RU位点中少量的Fe掺杂会带来电子和磁性的巨大变化,并产生复杂的H-T相图。迄今为止,在没有磁场的情况下,这种系统的基态尚不了解。通过执行5%Fe掺杂的CA $ _ {3} $ RU $ _ {2} $ o $ $ $ $ _ {7} $单晶的测量值($μ$ SR)测量值,我们在本地级别研究了其电子属性。横向场$ $ $ SR的结果表明,在T $ _ {n} $ = 79.7(1)K处的非常清晰的正常到抗磁力过渡,仅宽度为1k。零元素$μ$ SR的测量值,在磁性降低的状态下,我们可以确定本地领域B $ _ _ {I} i} $ site site n site n sitimant site n n n sitimant。通过对称性,Muons停在RUO $ _ {2} $飞机附近,仅检测弱核偶极场,而在顶端氧气旁边停止的磁极磁场则感觉磁场高达150吨。在与名义上掺杂的杰出同意的情况下,$ \ sim $ 6%的少数族裔感觉略低,反映了铁离子引起的局部磁性挫败感。最后,b $ _ {i} $在金属到绝缘体的过渡中没有显示出近40 K的重大变化。我们将这种令人惊讶的缺乏对晶体孪生的敏感性缺乏敏感性。

Ca$_{3}$Ru$_{2}$O$_{7}$ is a polar metal that belongs to the class of multiferroic magnetic materials. Here, tiny amounts of Fe doping in the Ru sites bring about dramatic changes in the electronic and magnetic properties and generate a complex H-T phase diagram. To date, not much is known about the ground state of such a system in the absence of magnetic field. By performing muon-spin spectroscopy ($μ$SR) measurements in 5% Fe-doped Ca$_{3}$Ru$_{2}$O$_{7}$ single crystals, we investigate its electronic properties at a local level. Transverse-field $μ$SR results indicate a very sharp normal-to-antiferromagnetic transition at T$_{N}$ = 79.7(1) K, with a width of only 1 K. Zero-field $μ$SR measurements in the magnetically ordered state allow us to determine the local fields B$_{i}$ at the muon implantation sites. By symmetry, muons stopping close to the RuO$_{2}$ planes detect only the weak nuclear dipolar fields, while those stopping next to apical oxygens sense magnetic fields as high as 150 mT. In remarkable agreement with the nominal Fe-doping, a $\sim$ 6% minority of the these muons feel slightly lower fields, reflecting a local magnetic frustration induced by iron ions. Finally, B$_{i}$ shows no significant changes across the metal-to-insulator transition, close to 40 K. We ascribe this surprising lack of sensitivity to the presence of crystal twinning.

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