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Local moment formation and magnetic coupling of Mn guest atoms in Bi$_2$Se$_3$: a low-temperature ferromagnetic resonance study

机译:mn客体原子的局域矩形成和磁耦合   Bi $ _2 $ se $ _3 $:一项低温铁磁共振研究

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摘要

We compare the magnetic and electronic configuration of single Mn atoms inmolecular beam epitaxy (MBE) grown Bi$_2$Se$_3$ thin films, focusing onelectron paramagnetic (ferromagnetic) resonance (EPR and FMR, respectively) andsuperconducting quantum interference device (SQUID) techniques. X-raydiffraction (XRD) and electron backscatter diffraction (EBSD) reveal theexpected increase of disorder with increasing concentration of magnetic guestatoms, however, Kikuchi patterns show that disorder consists majorly ofmum-scale 60deg twin domains in the hexagonal Bi$_2$Se$_3$ structure, which arepromoted by the presence of single unclustered Mn impurities. Ferromagnetismbelow T$_C$ ~ (5.4 +/- 0.3) K can be well described by critical scaling lawsM(T) ~ (1-T/T$_C$)$^\beta$ with a critical exponent $\beta$ = (0.34 +/- 0.2)),suggesting 3D Heisenberg class magnetism instead of e.g. 2D-type couplingbetween Mn-spins in van der Waals gap sites. From EPR hyperfine structure datawe determine a Mn$^{2+}$ (d$^5$, S = 5/2) electronic configuration with ag-factor of 2.002 for -1/2 --> +1/2 transitions. In addition, from the strongdependence of the low temperature FMR fields and linewidth on the fieldstrength and orientation with respect to the Bi$_2$Se$_3$ (0001) plane, wederive magnetic anisotropy energies of up to K1 = -3720 erg/cm3 in MBE-grownMn-doped Bi$_2$Se$_3$, reflecting the first order magneto-crystallineanisotropy of an in-plane magnetic easy plane in a hexagonal (0001) crystalsymmetry. Across the ferromagnetic-paramagnetic transition the FMR intensity issuppressed and resonance fields converge the paramagnetic limit of a Mn$^{2+}$(d$^5$, S = 5/2).
机译:我们比较了单个Mn原子在分子束外延(MBE)上生长的Bi $ _2 $ Se $ _3 $薄膜的磁性和电子结构,重点研究了电子顺磁(铁磁)共振(分别为EPR和FMR)和超导量子干涉装置(SQUID)技术。 X射线衍射(XRD)和电子背向散射衍射(EBSD)揭示了随着磁性客体原子浓度的增加,无序的预期增加,但是,菊池模式显示,无序主要由六角形Bi $ _2 $ Se $ _3中最大的60度双畴组成。单个未团聚的Mn杂质的存在促进了结构的转变。低于T $ _C $〜(5.4 +/- 0.3)的铁磁性可以通过临界比例定律M(T)〜(1-T / T $ _C $)$ ^ \ beta $以及临界指数$ \ beta $ = (0.34 +/- 0.2)),建议使用3D Heisenberg级磁性,而不是例如范德华间隙位置Mn自旋之间的2D型偶联。从EPR超精细结构数据中,我们确定Mn $ ^ {2 +} $(d $ ^ 5 $,S = 5/2)电子构型,其-1-2-> +1/2跃迁的a-因子为2.002。此外,由于低温FMR场和线宽对Bi $ _2 $ Se $ _3 $(0001)平面的场强和取向的强烈依赖性,高达K1 = -3720 erg / cm3的偏磁各向异性能量在MBE生长的Mn掺杂Bi $ _2 $ Se $ _3 $中,反映了六方(0001)晶体对称性中面内磁易平面的一阶磁晶各向异性。跨铁磁-顺磁转变,FMR强度被抑制,共振场收敛到Mn $ ^ {2 +} $(d $ ^ 5 $,S = 5/2)的顺磁极限。

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