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@ARTICLE{Sasioglu:754,
author = {Sasioglu, E. and Sandratskii, L. M. and Bruno, P.},
title = {{R}ole of conduction electrons in mediating exchange
interactions in {M}n-based {H}eusler alloys},
journal = {Physical review / B},
volume = {77},
number = {6},
issn = {1098-0121},
address = {College Park, Md.},
publisher = {APS},
reportid = {PreJuSER-754},
pages = {064417},
year = {2008},
note = {Record converted from VDB: 12.11.2012},
abstract = {Because of the large spatial separation of the Mn atoms in
Heusler alloys (d(Mn-Mn)>4 angstrom), the Mn 3d states
belonging to different atoms do not overlap considerably.
Therefore, an indirect exchange interaction between Mn atoms
should play a crucial role in the ferromagnetism of the
systems. To study the nature of the ferromagnetism of
various Mn-based semi- and full-Heusler alloys, we perform a
systematic first-principles calculation of the exchange
interactions in these materials. The calculation of the
exchange parameters is based on the frozen-magnon approach.
The Curie temperature is estimated within the mean-field
approximation. The calculations show that the magnetism of
the Mn-based Heusler alloys depends strongly on the number
of conduction sp electrons, their spin polarization, and the
position of the unoccupied Mn 3d states with respect to the
Fermi level. Various magnetic phases are obtained depending
on the combination of these characteristics. The magnetic
phase diagram is determined at zero temperature. The results
of the calculations are in good agreement with available
experimental data. Anderson's s-d model is used to perform a
qualitative analysis of the obtained results. The conditions
leading to a diverse magnetic behavior are identified. If
the spin polarization of the conduction electrons at the
Fermi energy is large and the unoccupied Mn 3d states lie
well above the Fermi level, a
Ruderman-Kittel-Kasuya-Yoshida-type ferromagnetic
interaction is dominating. On the other hand, the
contribution of the antiferromagnetic superexchange becomes
important if unoccupied Mn 3d states lie close to the Fermi
energy. The resulting magnetic behavior depends on the
competition of these two exchange mechanisms. The
calculation results are in good correlation with the
conclusions made on the basis of the Anderson s-d model
which provides useful framework for the analysis of the
results of first-principles calculations and helps to
formulate the conditions for high Curie temperature.},
keywords = {J (WoSType)},
cin = {IAS-1 / IFF-1},
ddc = {530},
cid = {I:(DE-Juel1)IAS-1-20090406 / I:(DE-Juel1)VDB781},
pnm = {Kondensierte Materie},
pid = {G:(DE-Juel1)FUEK414},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000253764100054},
doi = {10.1103/PhysRevB.77.064417},
url = {https://juser.fz-juelich.de/record/754},
}