1995
DOI: 10.1016/0925-8388(94)05057-0
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Anisotropies of the electrical resistivity and Hall effect in UAsSe

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Cited by 22 publications
(15 citation statements)
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“…Additionally, yet in the case of UPS and UAsSe only, below about 0.5T C the resistivity exhibits an anomalous upturn towards low temperatures [6,7,9]. This latter feature has recently attracted much attention being interpreted [6,9,10] in terms of non-magnetic Kondo effect in a two-level-system (TLS) scenario [11]. It was argued that the Kondo-like resistivity behavior arises in UPS and UAsSe due to anion disorder, i.e.…”
Section: Introductionmentioning
confidence: 99%
“…Additionally, yet in the case of UPS and UAsSe only, below about 0.5T C the resistivity exhibits an anomalous upturn towards low temperatures [6,7,9]. This latter feature has recently attracted much attention being interpreted [6,9,10] in terms of non-magnetic Kondo effect in a two-level-system (TLS) scenario [11]. It was argued that the Kondo-like resistivity behavior arises in UPS and UAsSe due to anion disorder, i.e.…”
Section: Introductionmentioning
confidence: 99%
“…The first term is described by the well known the Bloch-Grüneisen (B-G) formula while the second term, representing the OK scattering, is described here by Arai given formula [13]. This formula was found previously [3] to describe well ρ K (T) in UAsSe ferromagnet characterized by T C = 102 K at temperatures 4.2 ÷ 430 K. Here the sum of resistivity components xρ ph + yρ K + ρ 0 was fitted to the ∆ρ(T) curve at T > T C = 123.4 K and extrapolated to the low temperature range as shows the curve 1 in Fig. 3.…”
Section: Resultsmentioning
confidence: 96%
“…Here we used the best- fitted value of C equal to 2.15. This method is a generalization of earlier approach applied for resolving of UAsSe resistivity into their magnetic, Kondo and phonon contributions [3]. The determined ∆ρ(T) dependence is composed of two temperature dependent terms: ∆ρ ph = ( c ρ ph -2.15 a ρ ph ) ~ xρ ph (T) and…”
Section: Resultsmentioning
confidence: 99%
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