Research Area: Magnetic Materials


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:  
Fermi Surface of delafossite)
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).
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:  

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.
Mn adsorption on GaAs(001)
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.

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:  

Point of contact:   Steven.Erwin@nrl.navy.mil (Privacy Advisory)


Modification date :  Aug 11, 2008   Send comments or corrections to the webmaster (Privacy Advisory).

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