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Strong correlation effects in theoretical STM studies of magnetic adatoms

机译:在磁性吸附原子的理论STM研究中具有强相关性

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We present a theoretical study for the scanning tunneling microscopy (STM) spectra of surface-supported magnetic nanostructures, incorporating strong correlation effects. As concrete examples, we study Co and Mn adatoms on the Cu(111) surface, which are expected to represent the opposite limits of Kondo physics and local moment behavior, using a combination of density functional theory and both quantum Monte Carlo and exact diagonalization impurity solvers. We examine in detail the effects of temperature T, correlation strength U, and impurity d electron occupancy N_d on the local density of states. We also study the effective coherence energy scale, i.e., the Kondo temperature T_K, which can be extracted from the STM spectra. Theoretical STM spectra are computed as a function of STM tip position relative to each adatom. Because of the multiorbital nature of the adatoms, the STM spectra are shown to consist of a complicated superposition of orbital contributions, with different orbital symmetries, self-energies, and Kondo temperatures. For a Mn adatom, which is close to half-filling, the STM spectra are featureless near the Fermi level. On the other hand, the quasiparticle peak for a Co adatom gives rise to strongly position-dependent Fano line shapes.
机译:我们目前对表面支撑的磁性纳米结构的扫描隧道显微镜(STM)光谱进行理论研究,并纳入了强相关效应。作为具体示例,我们将结合密度泛函理论和量子蒙特卡罗理论以及精确的对角化杂质,研究Cu(111)表面上的Co和Mn原子,它们有望代表近藤物理学和局部矩行为的相反极限。解算器。我们详细研究了温度T,相关强度U和杂质d电子占有率N_d对局部态密度的影响。我们还研究了可从STM光谱中提取的有效相干能级,即近藤温度T_K。 STM理论光谱是根据STM尖端相对于每个原子的位置计算的。由于吸附原子的多轨道性质,显示STM光谱由复杂的轨道贡献叠加组成,具有不同的轨道对称性,自能和近藤温度。对于接近半填充的Mn原子,STM光谱在费米能级附近没有任何特征。另一方面,Co原子的准粒子峰产生了与位置密切相关的Fano线形。

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  • 来源
    《Physical review》 |2016年第11期|115123.1-115123.14|共14页
  • 作者单位

    Institute for Theoretical Solid State Physics, JARA-FIT and JARA-HPC, RWTH Aachen University, 52056 Aachen, Germany;

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich & JARA, D-52425 Juelich, Germany;

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich & JARA, D-52425 Juelich, Germany;

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich & JARA, D-52425 Juelich, Germany;

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