Searcharxiv⌕ Search

arXiv · cond-mat/0601291

Influence of Roughness and Disorder on Tunneling Magnetoresistance

Abstract

A systematic, quantitative study of the effect of interface roughness and disorder on the magnetoresistance of FeCo$|$vacuum$|$FeCo magnetic tunnel junctions is presented based upon parameter-free electronic structure calculations. Surface roughness is found to have a very strong effect on the spin-polarized transport while that of disorder in the leads (leads consisting of a substitutional alloy) is weaker but still sufficient to suppress the huge tunneling magneto-resistance (TMR) predicted for ideal systems.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

P. X. Xu, V. M. Karpan, K. Xia, M. Zwierzycki, I. Marushchenko, P. J. Kelly. 2006-05-30. Influence of Roughness and Disorder on Tunneling Magnetoresistance. https://doi.org/10.1103/physrevb.73.180402

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Chiral Majorana hinge modes on a curved surface with magnetic impurities

Chiral Majorana modes, a key ingredient for topological quantum computation, arise on the surface of a three-dimensional time-reversal-invariant topological superconductor when a magnetic field induces a sign-changing surface mass. In practice, the orbital response of the superconductor tilts the surface spectrum and overwhelms the Zeeman term as the field grows. Here we show that magnetic impurities on a spherical surface can instead generate this mass term through their exchange coupling, so that only a weak field is required. The Ising surface Majorana modes mediate a ferromagnetic Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction, derived here on the curved surface, that orders the radial impurity moments into an inversion-breaking hedgehog at zero field. An axial field instead stabilizes a domain wall across which the radial magnetization reverses sign, leaving a single chiral Majorana mode along the equator and realizing an inversion-protected second-order topological superconductor.

cond-mat.mes-hall↗

Scalar Spin Chirality from Dissipative Pumping and Lamb-Shift Precession

How electrical driving generates and reverses scalar spin chirality in an interacting system with a real Hamiltonian and no magnetic flux remains a fundamental open question. We show that dissipative tunneling prepares an orbital pseudospin, while virtual charge fluctuations generate a noncollinear Lamb field that rotates it toward the chiral direction. Bias changes their relative orientation and thereby reverses the current. This reservoir-induced orbital Hanle effect converts a nonchiral orbital polarization into scalar spin chirality. Within the ground-state space, the circulating current is determined by the scalar spin chirality. Hierarchical-equations-of-motion calculations show that the low-bias reversal survives beyond the second-order weak-coupling description, while the quadratic growth of chirality after a sudden voltage switch identifies precession. More broadly, time-reversal-odd responses can emerge in open quantum systems from the interplay between dissipative state preparation and coherent precession.

cond-mat.mes-hall↗

Anisotropic Boltzmann transport in a tight-binding superlattice: Exact results for power-law energy-dependent scattering

We develop a complete Boltzmann transport theory for the in-plane ($σ_{xx}$) and out-of-plane ($σ_{zz}$) conductivities of an electronic superlattice consisting of a periodic stack of two-dimensional (2D) parabolic-band layers coupled along the superlattice axis by nearest-neighbor tunneling $t$, in the physically relevant regime $t\ll E_F$ where the Fermi surface is an open, corrugated cylinder. Within the relaxation-time approximation with a power-law energy-dependent scattering time $τ(E)\propto E^{p}$, we study the seven models $p=0,\pm1,\pm3/2,\pm2$ as functions of the 2D electron density $n$ per layer and temperature $T$. For $p=-2$ (in plane) and $p\le -1$ (out of plane), long-lived carriers at the miniband bottom can dominate transport at finite temperature. For $p=-2$, these carriers produce a pronounced peak in $σ_{zz}(T)$ at $T\sim E_F$. We find that the temperature dependence of the anisotropic metallic dc conductivity can be highly counterintuitive depending on $t$, $T$, and $p$, with no generic increase or decrease with temperature. The Lorenz ratio is determined by the energy variance of the current-carrying electrons; the Wiedemann-Franz (WF) law is exact as $T\to0$ for all models at fixed $t$, with anisotropic corrections at finite temperature. Band-edge carriers first enhance the interlayer Lorenz ratio up to several times its low-temperature value through thermal occupation of separated energy ranges within the same electron band and then suppress it at high temperature by energy filtering. Strong violations of the Wiedemann-Franz law can therefore arise from miniband structure and energy-dependent elastic scattering alone.

cond-mat.mes-hall↗