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Imaging Local Effects of Voltage and Boron Doping on Spin Reversal in Antiferromagnetic Magnetoelectric Cr2O3 Thin Films and Devices
Advanced Functional Materials ( IF 18.5 ) Pub Date : 2024-08-02 , DOI: 10.1002/adfm.202408542 Adam Erickson 1 , Syed Qamar Abbas Shah 2 , Ather Mahmood 2 , Pratyush Buragohain 2, 3 , Ilja Fescenko 4 , Alexei Gruverman 2 , Christian Binek 2 , Abdelghani Laraoui 1, 2
Advanced Functional Materials ( IF 18.5 ) Pub Date : 2024-08-02 , DOI: 10.1002/adfm.202408542 Adam Erickson 1 , Syed Qamar Abbas Shah 2 , Ather Mahmood 2 , Pratyush Buragohain 2, 3 , Ilja Fescenko 4 , Alexei Gruverman 2 , Christian Binek 2 , Abdelghani Laraoui 1, 2
Affiliation
Chromia (Cr2O3) is a magnetoelectric oxide that permits voltage-control of the antiferromagnetic (AFM) order, but it suffers technological constraints due to its low Néel Temperature (TN ≈307 K) and the need of a symmetry-breaking applied magnetic field to achieve reversal of the Néel vector. Recently, boron (B) doping of Cr2O3 films led to an increase TN >400 K and allowed the realization of voltage magnetic-field free controlled Néel vector rotation. Here, the impact of B doping is directly imaged on the formation of AFM domains in Cr2O3 thin films and elucidates the mechanism of voltage-controlled manipulation of the spin structure using nitrogen-vacancy (NV) scanning probe magnetometry. A stark reduction and thickness dependence of domain size in B-doped Cr2O3 (B:Cr2O3) films is found, explained by the increased germ density, likely associated with the B doping. By reconstructing the surface magnetization from the NV stray-field maps, a qualitative distinction between the undoped and B-doped Cr2O3 films is found, manifested by the histogram distribution of the AFM ordering, that is, 180° domains for pure films, and 90° domains for B:Cr2O3 films. Additionally, NV imaging of voltage-controlled B-doped Cr2O3 devices corroborates the 90° rotation of the AFM domains observed in magnetotransport measurement.
中文翻译:
电压和硼掺杂对反铁磁电 Cr2O3 薄膜和器件自旋反转的局部效应成像
铬氧化物 (Cr2O3) 是一种磁电氧化物,允许对反铁磁 (AFM) 级进行电压控制,但由于其低 Néel 温度 (TN ≈307 K) 并且需要打破对称性的施加磁场来实现 Néel 矢量的反转,因此它受到技术限制。最近,Cr2O3 薄膜的硼 (B) 掺杂导致 TN >400 K 的增加,并允许实现电压无磁场控制的 Néel 矢量旋转。在这里,B 掺杂对 Cr2O3 薄膜中 AFM 结构域形成的影响直接成像,并使用氮空位 (NV) 扫描探针磁力计阐明了自旋结构的电压控制操纵机制。发现 B 掺杂的 Cr2O3 (B:Cr2O3) 薄膜中畴大小的明显减少和厚度依赖性,这可以通过细菌密度增加来解释,这可能与 B 掺杂有关。通过从 NV 杂散场图重建表面磁化强度,发现了未掺杂和 B 掺杂的 Cr2O3 薄膜之间的定性区别,表现为 AFM 排序的直方图分布,即纯薄膜为 180° 域,B:Cr2O3 薄膜为 90° 域。此外,电压控制 B 掺杂 Cr2O3 器件的 NV 成像证实了在磁传输测量中观察到的 AFM 域旋转 90°。
更新日期:2024-08-02
中文翻译:
电压和硼掺杂对反铁磁电 Cr2O3 薄膜和器件自旋反转的局部效应成像
铬氧化物 (Cr2O3) 是一种磁电氧化物,允许对反铁磁 (AFM) 级进行电压控制,但由于其低 Néel 温度 (TN ≈307 K) 并且需要打破对称性的施加磁场来实现 Néel 矢量的反转,因此它受到技术限制。最近,Cr2O3 薄膜的硼 (B) 掺杂导致 TN >400 K 的增加,并允许实现电压无磁场控制的 Néel 矢量旋转。在这里,B 掺杂对 Cr2O3 薄膜中 AFM 结构域形成的影响直接成像,并使用氮空位 (NV) 扫描探针磁力计阐明了自旋结构的电压控制操纵机制。发现 B 掺杂的 Cr2O3 (B:Cr2O3) 薄膜中畴大小的明显减少和厚度依赖性,这可以通过细菌密度增加来解释,这可能与 B 掺杂有关。通过从 NV 杂散场图重建表面磁化强度,发现了未掺杂和 B 掺杂的 Cr2O3 薄膜之间的定性区别,表现为 AFM 排序的直方图分布,即纯薄膜为 180° 域,B:Cr2O3 薄膜为 90° 域。此外,电压控制 B 掺杂 Cr2O3 器件的 NV 成像证实了在磁传输测量中观察到的 AFM 域旋转 90°。