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Integer quantum Hall effect in graphene channel with p-n junction at domain wall in a strained ferroelectric film

机译:应变铁电薄膜畴壁上具有p-n结的石墨烯通道中的整数量子霍尔效应

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摘要

We revealed that 180 degrees domain walls in a strained ferroelectric film can induce p-n junctions in a graphene channel and lead to the nontrivial temperature and gate voltage dependences of the perpendicular modes of the integer quantum Hall effect (IQHE). In particular, the number of perpendicular modes nu(perpendicular to), corresponding to the p-n junction across the graphene channel, varies with the gate voltage increase from small integers to higher non-integer numbers, e.g., nu(perpendicular to) = 1.9, 2, ..., 5.1, 6.875, ..., 9.1, ..., 23,..., 37.4, in the vicinity of the transition temperature from the ferroelectric to paraelectric phase. The non-integer numbers and their irregular sequence principally differ from the sequence of non-integer numbers v = 3/2, 5 3, ... reported earlier. The unusual nu(perpendicular to)-numbers originate from significantly different numbers of the edge modes, v(1) and v(2), corresponding to different concentrations of carriers in the left (n(1)) and right (n(2)) domains of the p-n junction boundary. The concentrations n(1) and n(2) are determined by the gate voltage and spontaneous polarization contributions, and so their difference originates from different directions of the spontaneous polarization in different domains of the strained ferroelectric film. The difference between n(1) and n(2) disappears with the vanishing of the film spontaneous polarization in a paraelectric phase. The temperature transition from the ferroelectric to paraelectric phase taking place in a strained ferroelectric film can be varied in a wide temperature range by an appropriate choice of misfit strain so that the first plateaus of the predicted IQHE effect can be observed even at room temperatures.
机译:我们发现,应变铁电薄膜中的180度畴壁会在石墨烯通道中引起p-n结,并导致整数量子霍尔效应(IQHE)的垂直模式的非平凡温度和栅极电压依赖性。特别地,与跨石墨烯通道的pn结相对应的垂直模式nu(垂直于)的数量随栅极电压从小整数到较高的非整数而变化,例如nu(垂直于)= 1.9, 2,...,5.1、6.875,...,9.1,...,23,...,37.4,处于从铁电相到顺电相的转变温度附近。非整数及其不规则序列的原则上与先前报道的非整数v = 3/2,5 3,...的序列不同。不寻常的nu(垂直于)数源自边缘模式v(1)和v(2)的明显不同数量,对应于左侧(n(1))和右侧(n(2 ))pn结边界的域。浓度n(1)和n(2)由栅极电压和自发极化贡献决定,因此它们的差异源自应变铁电薄膜不同域中自发极化的不同方向。随着薄膜在顺电相中自发极化的消失,n(1)和n(2)之间的差异消失。通过适当选择失配应变,可以在较宽的温度范围内改变在应变铁电薄膜中发生的从铁电相到顺电相的温度转变,从而即使在室温下也可以观察到预测的IQHE效应的第一个平稳期。

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  • 来源
    《Journal of Applied Physics》 |2019年第8期|082525.1-082525.10|共10页
  • 作者单位

    Natl Acad Sci Ukraine, V Lashkariov Inst Semicond Phys, Pr Nauky 4-1, UA-03028 Kiev, Ukraine|Taras Shevchenko Kyiv Natl Univ, Radiophys Fac, Pr Akad Hlushkova 4g, UA-03022 Kiev, Ukraine;

    Natl Acad Sci Ukraine, V Lashkariov Inst Semicond Phys, Pr Nauky 4-1, UA-03028 Kiev, Ukraine;

    Natl Acad Sci Ukraine, Inst Phys, Pr Nauky 46, UA-03028 Kiev, Ukraine|Natl Acad Sci Ukraine, Bogolyubov Inst Theoret Phys, 14-B Metrolohichna Str, UA-03680 Kiev, Ukraine;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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