Electronic phase separation due to magnetic polaron formation in the semimetallic ferromagnet EuB6 — A weakly-nonlinear-transport study
We report measurements of weakly nonlinear electronic transport, as measured by third-harmonic voltage generation V 3ω , in the low-carrier density semimetallic ferromagnet EuB 6 , which exhibits an unusual magnetic ordering with two consecutive transitions at = 15.6K and = 12.5K. In contrast to the...
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Published in: | Journal of the Korean Physical Society Vol. 62; no. 10; pp. 1489 - 1494 |
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Main Authors: | , , , |
Format: | Journal Article |
Language: | English |
Published: |
Seoul
The Korean Physical Society
01-05-2013
한국물리학회 |
Subjects: | |
Online Access: | Get full text |
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Summary: | We report measurements of weakly nonlinear electronic transport, as measured by third-harmonic voltage generation
V
3ω
, in the low-carrier density semimetallic ferromagnet EuB
6
, which exhibits an unusual magnetic ordering with two consecutive transitions at
= 15.6K and
= 12.5K. In contrast to the linear resistivity, the third-harmonic voltage is sensitive to the microgeometry of the electronic system. Our measurements provide evidence for magnetically-driven electronic phase separation consistent with the picture of percolation of magnetic polarons (MP), which form highly conducting magnetically ordered clusters in a paramagnetic and less conducting background. Upon cooling in zero magnetic field through the ferromagnetic transition, the dramatic drop in the linear resistivity at the upper transition
coincides with the onset of nonlinearity, and upon further cooling is followed by a pronounced peak in
V
3ω
at the lower transition
. Likewise, in the paramagnetic regime, a drop of the material’s magnetoresistance
R
(
H
) precedes a magnetic-fieldinduced peak in nonlinear transport. A striking observation is a linear temperature dependence of
V
3ω
peak
. We suggest a picture where at the upper transition
the coalescing MP form a conducting path giving rise to a strong decrease in the resistance. The MP formation sets in at around
T
* ∼ 35K below which these entities are isolated and strongly fluctuating, while growing in number. The MP then start to form links at
, where percolative electronic transport is observed. The MP merge and start forming a continuum at the threshold
. In the paramagnetic temperature regime
<
T
<
T
*, MP percolation is induced by a magnetic field, and the threshold accompanied by charge carrier delocalization occurs at a single critical magnetization. |
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Bibliography: | G704-000411.2013.62.10.039 |
ISSN: | 0374-4884 1976-8524 |
DOI: | 10.3938/jkps.62.1489 |