论文标题

观察零场横向电阻$ _x $/srtio $ _3 $接口设备

Observation of zero-field transverse resistance in AlO$_x$/SrTiO$_3$ interface devices

论文作者

Krantz, P. W., Chandrasekhar, V.

论文摘要

Domain walls in AlO$_x$/SrTiO$_3$ (ALO/STO) interface devices at low temperatures give a rise to a new signature in the electrical transport of two-dimensional carrier gases formed at the surfaces or interfaces of STO-based heterostructures: a finite transverse resistance observed in Hall bars in zero external magnetic field.这种横向电阻取决于局部域壁的配置,因此随温度,门电压,热循环和沿样品的位置而变化,甚至可以随着这些参数的函数而更改符号。横向电阻在$ \ simeq $ 70 K以下观察到,但增长和变化明显低于$ \ simeq $ 40 K,域壁变得越来越极性。令人惊讶的是,与(001)方向的异质结构相比,(111)方向的异质结构(111)异质结构的横向电阻更大。电容界面与施加到基板的电极之间的电容的测量,该电极反映了STO的介电常数,这表明当在[111]中施加电场时,这种差异可能与电场在电场上施加电场时与温度依赖性介电常数的更大变化有关。有限的横向电阻可以解释由于电流沿域壁的优先运输而与注射电流的标称方向共线,因此电流流动不均匀。

Domain walls in AlO$_x$/SrTiO$_3$ (ALO/STO) interface devices at low temperatures give a rise to a new signature in the electrical transport of two-dimensional carrier gases formed at the surfaces or interfaces of STO-based heterostructures: a finite transverse resistance observed in Hall bars in zero external magnetic field. This transverse resistance depends on the local domain wall configuration and hence changes with temperature, gate voltage, thermal cycling and position along the sample, and can even change sign as a function of these parameters. The transverse resistance is observed below $\simeq$ 70 K but grows and changes significantly below $\simeq$40 K, the temperature at which the domain walls become increasingly polar. Surprisingly, the transverse resistance is much larger in (111) oriented heterostructures in comparison to (001) oriented heterostructures. Measurements of the capacitance between the conducting interface and an electrode applied to the substrate, which reflect the dielectric constant of the STO, indicate that this difference may be related to the greater variation of the temperature dependent dielectric constant with electric field when the electric field is applied in the [111] direction. The finite transverse resistance can be explained inhomogeneous current flow due to the preferential transport of current along domain walls that are not collinear with the nominal direction of the injected current.

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