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Research Area Summary:
The Center studies a broad range of magnetic materials, from
hard magnetic materials to dilute magnetic
semiconductors. Some of these materials form the basis of current
magnetoelectronic technologies, while others -- both soft and hard
magnets -- are being studied for future applications.
Magnetism in Metals:
 | FIG. 1.
This plot of the Fermi surface of Ag2NiO2 illustrates
the effect of magnetism on transport properties. The left panel shows
the spin-majority Fermi surface, and the right panel the spin-minority
one. The minority surface contains
fast electrons derived from Ag s and p bands, while the majority
surface contains both slow electrons (central cylinder and outside
edge of hexagonal network) and fast electrons (inside edge of
network).
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We are interested in a broad class of physical problem related to
magnetism in metals. This includes such diverse issues as microscopic
understanding of magnetic anisotropy, nuclear magnetic resonance in
metals, and the theory of spectroscopic probes of spin polarization. In the
last few years the main topics of our research in this area were
itinerant ferromagnetism near a quantum critical point and
frustrated low-dimensional magnetism. Strongly correlated magnets,
especially oxides, are also a subject of intensive
investigation. These subjects are intimately related to
spin-fluctuation properties and, as such, to unconventional
superconductivity.
Further Reading:
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Charge order to remove orbital degeneracy in triangular antiferromagnet AgNiO2
E. Wawrzynska, R. Coldea, E.M. Wheeler, I.I. Mazin, M.D. Johannes, et al., Phys. Rev. Lett. 99, 157204 (2007)
- Charge ordering as alternative to Jahn-Teller distortion
I.I. Mazin, D.I. Khomskii, R. Lengsdorf, et al., Phys. Rev. Lett. 98, 176406 (2007)
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Ab initio investigation of magnetic interactions in the frustrated triangular magnet NiGa2S4
I.I. Mazin, Phys. Rev. B - Rapid Comm. 76, 140406(R) (2007)
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CeMnNi4: an impostor half-metal I.I. Mazin, Phys. Rev. B 73, 012415 (2006)
- Why Ni3Al is an itinerant ferromagnet but Ni3Ga is not, A. Aguayo, I. I. Mazin and D.J. Singh,
Phys. Rev. Lett. 92, 147201 (2004)
Points of contact:
Igor.Mazin@nrl.navy.mil
(Privacy Advisory) |
Michelle.Johannes@nrl.navy.mil (Privacy Advisory)
Magnetic Semiconductors:
In the late 1980s and early 1990s, researchers in Japan and the United
States showed that semiconductors could be made magnetic by doping
them with manganese. An early finding was that II-VI semiconductors
(such as ZnSe) were antiferromagnetic when doped with Mn, while III-V
semiconductors (such as GaAs) were ferromagnetic. This suggests a
competition between two interactions: a weak antiferromagnetic
interaction due to superexchange, and a ferromagnetic
interaction due to an indirect exchange mechanism mediated by free carriers.
When a divalent dopant such as Mn substitutes for a Group III atom
such as Ga, a hole is introduced; this is the reason GaAs becomes
ferromagnetic while ZnSe does not.
In 2001, Jonker and coworkers at NRL developed the first ferromagnetic
semiconductor based on an elemental host, Mn-doped germanium. To help
understand the origins of ferromagnetism in this material, we used
density-functional theory to compute the effective coupling strength
between Mn spins as a function of their separation (see "Further
Reading" below). Interestingly, this coupling is antiferromagnetic
for nearest-neighbor Mn atoms, but ferromagnetic for all separations
greater than this. To calculate the Curie temperature (as a function
of Mn concentration), we then used a simple percolation theory based
on our computed coupling strengths. The predicted Curie temperature
increases approximately linearly with Mn concentration, in agreement
with experiment, but the absolute temperatures are too large by
roughly a factor 4-5.
 | FIG. 2.
Potential energy surface for Mn adsorption on GaAs(001),
plotted in a plane normal to the surface and containing the As surface
dimer. The minimum energy adsorption site is the subsurface
interstitial site labeled i; the corresponding surface
geometry is shown (light gray for As, dark gray for Ga, yellow for
Mn). Typical adsorption pathways funnel Mn adatoms into the
interstitial site (heavy curves) or a cave site
c (light curves). Inset: Binding energy of a Mn adatom centered
on the As-dimer; for comparison, results are also
shown for a Ga adatom. When additional As is deposited, the metastable
substitutional site, s, becomes more favorable and leads to
partial incorporation of substitutional Mn.
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The reason for this overestimate is two-fold. First, the local-density
approximation to density-functional theory generally overestimates
spin coupling strengths by similar factors. Second, the actual
materials (both Mn-doped Ge and Mn-doped GaAs) are found to be
strongly compensated: that is, their measured hole concentrations are
much lower than expected based on the measured Mn
concentrations. Recently we proposed that the source of this
compensation is Mn in interstitial sites (rather than substitutional
sites). We have shown that even though the substitutional site is
strongly preferred in the bulk crystal, during the growth process Mn
atoms can follow a very low-energy pathway starting from the gas phase
and come to rest at a subsurface interstitial site (see Fig. 2). In
the bulk crystal environment interstitial Mn is an electron donor,
with each interstitial Mn compensating two substitutional Mn.
We are also conducting theoretical research on other types of magnetic
semiconductor systems. Our current projects include: a computational
search for promising new ferromagnetic semiconductors in the chalcopyrite family; a
first-principles investigation of the structure of Fe/GaAs interfaces;
a study of Co-doped TiO2, a relatively new dilute magnetic
semiconductor with Curie temperatures reported to be 700 K or higher;
studies of magnetic impurities in diamond; and a theoretical
assessment of spin injection from the magnetic semiconductor
CdCr2Se4 into semiconductors such as Si and
GaAs.
Further Reading:
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Thermodynamics of Carrier-Mediated Ferromagnetism in
Semiconductors A.G. Petukhov, I. Zutic,
and S.C. Erwin. Physical Review Letters (December 21, 2007)
- Spin Injection and
Detection in Silicon I. Zutic and
S.C. Erwin. Physical Review Letters (July 14, 2006)
- Determination of Interface Atomic
Structure and Its Impact on Spin Transport Using Z-Contrast Microscopy
and Density-Functional Theory.
T.J. Zega, A.T. Hanbicki, S.C. Erwin, I. Zutic, G. Kioseoglou, C.H. Li,
B.T. Jonker, and R.M. Stroud. Physical Review Letters (May 16, 2006)
- Tailoring ferromagnetic chalcopyrites S.C. Erwin and I. Zutic. Nature Materials (June 6, 2004)
[see also this News and Views article by S. Picozzi]
- Cross-sectional STM of Mn-doped GaAs: Theory and experiment J.M. Sullivan, G.I. Boishin, L.J. Whitman, A.T. Hanbicki, B.T. Jonker, and S.C. Erwin. Physical Review B (December 23, 2003)
- Predicted absence of ferromagnetism in manganese-doped diamond S.C. Erwin and C.S. Hellberg. Physical Review B (December 30, 2003)
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Electrical spin injection and transport in semiconductor spintronic devices
B.T. Jonker, S.C. Erwin, A. Petrou, and A.G. Petukhov. MRS Bulletin (October 10, 2003)
- Theory of dopants and defects in Co-doped
TiO2 anatase J.M. Sullivan and S.C. Erwin. Physical Review B (April 18, 2003)
- Self-Compensation in Manganese-Doped Ferromagnetic Semiconductors S.C. Erwin and A.G. Petukhov. Physical Review Letters (November 25, 2002)
- First-principles study of nucleation, growth, and interface structure of Fe/GaAs S.C. Erwin, S.-H. Lee, and M. Scheffler.
Physical Review B (May 22, 2002)
- A Group-IV Ferromagnetic Semiconductor: Mn(x)Ge(1-x) PDF (109 kB) Y.D. Park, A. Hanbicki, S.C. Erwin, C.S. Hellberg, J.M. Sullivan,
J.E. Mattson, T.F. Ambrose, A. Wilson, G. Spanos, and B.T. Jonker. Science (January 25, 2002)
Point of contact:
Steven.Erwin@nrl.navy.mil (Privacy Advisory)
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