Issue |
Europhys. Lett.
Volume 65, Number 6, March 2004
|
|
---|---|---|
Page(s) | 816 - 822 | |
Section | Condensed matter: electronic structure, electrical, magnetic, and optical properties | |
DOI | https://doi.org/10.1209/epl/i2003-10127-x | |
Published online | 01 March 2004 |
Metamagnetism of itinerant electrons in multi-layer ruthenates
1
Département de physique, Université de Fribourg, Pérolles CH-1700 Fribourg, Switzerland
2
Theoretische Physik, ETH-Hönggerberg - CH-8093 Zürich, Switzerland
Received:
16
September
2003
Accepted:
14
January
2004
The problem of quantum criticality in the context of itinerant
ferro- or metamagnetism has received considerable attention
(Grigera S. A. et al. , Science 294 (2001) 329;
Pfleiderer C. et al. , Nature 414 (2001) 427). It has been
proposed that a new kind of quantum criticality is realised in
materials such as or
. We show,
based on a mean-field theory, that the low-temperature behaviour
of the n-layer ruthenates
n
can be understood
as a result of a Van Hove singularity (VHS). We consider a single
band whose Fermi energy,
, is close to the VHS and
deduce a complex phase diagram for the magnetism as a function of
temperature, magnetic field and
. The location of
with respect to the VHS depends on the number of
layers or can be tuned by pressure. We find that the
ferromagnetic quantum phase transition in this case is not of
second but of first order, with a metamagnetic quantum critical
end-point at high magnetic field. Despite its simplicity, this
model describes well the properties of the uniform magnetism in
the single-, double- and triple-layer ruthenates. We would like
to emphasise that the origin of this behaviour lies in the band
structure.
PACS: 75.30.Kz – Magnetic phase boundaries (including magnetic transitions, metamagnetism, etc.) / 75.10.Lp – Band and itinerant models / 71.27.+a – Strongly correlated electron systems; heavy fermions
© EDP Sciences, 2004
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