13 research outputs found
Bias asymmetry in the conductance profile of magnetic ions on surfaces probed by scanning tunneling microscopy
The conductance profiles of magnetic transition metal atoms, such as Fe, Co
and Mn, deposited on surfaces and probed by a scanning tunneling microscope
(STM), provide detailed information on the magnetic excitations of such
nano-magnets. In general the profiles are symmetric with respect to the applied
bias. However a set of recent experiments has shown evidence for inherent
asymmetries when either a normal or a spin-polarized STM tip is used. In order
to explain such asymmetries here we expand our previously developed
perturbative approach to electron-spin scattering to the spin- polarized case
and to the inclusion of out of equilibrium spin populations. In the case of a
magnetic STM tip we demonstrate that the asymmetries are driven by the
non-equilibrium occupation of the various atomic spin-levels, an effect that
reminds closely that electron spin-transfer. In contrast when the tip is not
spin-polarized such non-equilibrium population cannot be build up. In this
circumstance we propose that the asymmetry simply originates from the
transition metal ion density of state, which is included here as a
non-vanishing real component to the spin-scattering self-energy
Spin-flip inelastic electron tunneling spectroscopy in atomic chains
We present a theoretical study of the spin transport properties of
mono-atomic magnetic chains with a focus on the spectroscopical features of the
I-V curve associated to spin-flip processes. Our calculations are based on the
s-d model for magnetism with the electron transport treated at the level of the
non-equilibrium Green's function formalism. Inelastic spin-flip scattering
processes are introduced perturbatively via the first Born approximation and an
expression for the associated self-energy is derived. The computational method
is then applied to describe the I-V characteristics and its derivatives of one
dimensional chains of Mn atoms and the results are then compared to available
experimental data. We find a qualitative and quantitative agreement between the
calculated and the experimental conductance spectra. Significantly we are able
to describe the relative intensities of the spin excitation features in the I-V
curve, by means of a careful analysis of the spin transition selection rules
associated to the atomic chains
Magnetism and Antiferroelectricity in MgB
We report on a density functional theory study demonstrating the coexistence
of weak ferromagnetism and antiferroelectricity in boron-deficient MgB6. A
boron vacancy produces an almost one dimensional extended molecular orbital,
which is responsible for the magnetic moment formation. Then, long-range
magnetic order can emerge from the overlap of such orbitals above percolation
threshold. Although there is a finite density of states at the Fermi level, the
localized nature of the charge density causes an inefficient electron
screening. We find that the Mg ions can displace from the center of their cubic
cage, thus generating electrical dipoles. In the ground state these order in an
antiferroelectric configuration. If proved experimentally, this will be the
first material without d or f electrons displaying the coexistence of magnetic
and electric order
Ab initio comparison of spin-transport properties in MgO-spaced ferrimagnetic tunnel junctions based on MnGa and MnAl
We report on first-principles spin-polarised quantum transport calculations
(from NEGF+DFT) in MgO-spaced magnetic tunnel junctions (MTJs) based on two
different Mn-based Heusler ferrimagnetic metals, namely MnAl and MnGa
in their tetragonal DO phase. The former is a fully compensated
half-metallic ferrimagnet, while the latter is a low-moment
high-spin-polarisation ferrimagnet, both with a small lattice mismatch from
MgO. In identical symmetric and asymmetric interface reconstructions across a
3-monolayer thick MgO barrier for both ferrimagets, the linear response
(low-voltage) spin-transfer torque (STT) and tunneling magneto-resistance (TMR)
effects are evaluated. A larger staggered in-plane STT is found in the MnGa
case, while the STT in MnAl vanishes quickly away from the interface
(similarly to STT in ferromagnetic MTJs). The roles are reversed for the TMR,
which is practically 100\% in the half-metallic MnAl-based MTJs (using the
conservative definition) as opposed to 60\% in the MnGa case. The weak
dependence on the exact interface reconstruction would suggest
MnGa-MnAl solid solutions as a possible route towards optimal trade-off
of STT and TMR in the low-bias, low-temperature transport regime.Comment: 6 pages, 4 figure
Multiferroicity of magnesium hexaboride
Hexaborides, MB6 (M=Ca, Sr, Ba), have attracted considerable attention after the observation
of a weak ferromagnetism not involving partially filled d or f orbitals. High melting point,
chemical stability and high hardness are among other properties which raised the interest in
these compounds. Although the above mentioned systems were thoroughly investigated theoretically and experimentally, the properties of the lighter member of the family, namely MgB6,
are largely unknown so far. Our spin-polarized calculations, based on DFT at GGA level, predict multiferroicity in MgB6, which is unique in this class of materials. In fact, MgB6 displays a weak magnetic moment associated to boron vacancies, similar to the ferromagnetism in the related CaB6 and SrB6. In addition, a small Mg cations shift off the center of the simple cubic elementary unit cell breaks the central symmetry and yields the relatively large net electric dipole moment of 7.7 Debye per unit cell. Long range Coulombic interaction lowers the energy of the system further by arranging the dipoles in antiferroelectric order
A pertubative approach to the Kondo effect in magnetic atoms on nonmagnetic substrates
Recent experimental advances in scanning tunneling microscopy make the
measurement of the conductance spectra of isolated and magnetically coupled
atoms on nonmagnetic substrates possible. Notably these spectra are
characterized by a competition between the Kondo effect and spin-flip inelastic
electron tunneling. In particular they include Kondo resonances and a
logarithmic enhancement of the conductance at voltages corresponding to
magnetic excitations, two features that cannot be captured by second order
perturbation theory in the electron-spin coupling. We have now derived a third
order analytic expression for the electron-spin self-energy, which can be
readily used in combination with the non-equilibrium Green's function scheme
for electron transport at finite bias. We demonstrate that our method is
capable of quantitative description the competition between Kondo resonances
and spin-flip inelastic electron tunneling at a computational cost
significantly lower than that of other approaches. The examples of Co and Fe on
CuN are discussed in detail
Spin scattering and spin-polarized hybrid interface states at a metal-organic interface
Spin scattering at the interface formed between metallic Fe and Cu-phthalocyanine molecules is investigated by spin-polarized scanning tunneling spectroscopy and spin-resolved photoemission. The results are interpreted using first-principles electronic structure theory. The combination of experimental and theoretical techniques allows us to shed light on the role of hybrid interface states for the spin scattering. We show that Cu-phthalocyanine acts, via hybrid interface states, as a local spin filter up to room temperature both below and above the Fermi energy, E(F). At the same time, the molecule behaves as a featureless scattering barrier in a region of about 1 eV around E(F). Similar properties are found for both single molecules and self-assembled molecular layers, so that the acquired microscopic knowledge can be transferred to operating devices
FLEUR
FLEUR is an all-electron DFT code based on the full-potential linearized augmented plane-wave method (FLAPW). It is mainly developed at the Forschungsentrum Jülich, Germany and available for the materials research community