Wicaksono Yusuf, Harfah Halimah, Sunnardianto Gagus Ketut, Majidi Muhammad Aziz, Kusakabe Koichi
Graduate School of Engineering Science, Osaka University 1-3 Machikaneyama-cho Toyonaka Osaka 5608531 Japan
Research Center for Quantum Physics, The National Research and Innovation Agency (BRIN) Kawasan Puspiptek Serpong Tangerang Selatan Banten 15314 Indonesia.
RSC Adv. 2022 May 11;12(22):13985-13991. doi: 10.1039/d2ra00957a. eCollection 2022 May 5.
In this study, we present a theoretical study on the in-plane conductance of graphene partially sandwiched between Ni(111) nanostructures with a width of ∼12.08 Å. In the sandwiched part, the gapped Dirac cone of the graphene was controlled using a pseudospin by changing the magnetic alignment of the Ni(111) nanostructures. Upon considering the antiparallel configuration of Ni(111) nanostructures, the transmission probability calculation of the in-plane conductance of graphene shows a gap-like transmission at - = 0.2 and 0.65 eV from the pd-hybridization and controllable Dirac cone of graphene, respectively. In the parallel configuration, the transmission probability calculation showed a profile similar to that of the pristine graphene. High and colossal magnetoresistance ratios of 284% and 3100% were observed at - = 0.65 eV and 0.2 eV, respectively. Furthermore, a magnetoresistance beyond 3100% was expected at - = 0.65 eV when the width of the Ni(111) nanostructures on the nanometer scale was considered.
在本研究中,我们对部分夹在宽度约为12.08 Å的Ni(111)纳米结构之间的石墨烯的面内电导进行了理论研究。在夹层部分,通过改变Ni(111)纳米结构的磁排列,利用赝自旋控制石墨烯的带隙狄拉克锥。考虑到Ni(111)纳米结构的反平行构型,石墨烯面内电导的传输概率计算表明,由于pd杂化和石墨烯可控狄拉克锥,在能量为 - 0.2 eV和0.65 eV时出现类似能隙的传输。在平行构型中,传输概率计算显示出与原始石墨烯相似的分布。在能量为 - 0.65 eV和0.2 eV时,分别观察到高达284%和3100%的巨大磁阻比。此外,当考虑纳米尺度的Ni(111)纳米结构的宽度时,预计在能量为 - 0.65 eV时磁阻超过3100%。