1993
DOI: 10.1103/physrevlett.71.2110
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Transition offelectron nature from itinerant to localized: Metamagnetic transition inCeRu2Si2

Abstract: We report the measurements of the de Haas-van Alphen (dHvA) effect for field ranges below and above the metamagnetic transition field (//m) in CeRu2Si2. The dHvA frequency branches and the effective masses ranging from 1.5A^7O to 120mo observed below Hm agree with the predictions of the itinerant / electron model, whereas those above Hm can be explained well with the localized / electron model. All the dHvA frequencies change abruptly around Hm-The effective masses decrease considerably around Hm and then cont… Show more

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Cited by 219 publications
(123 citation statements)
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“…17(b). 1,106,107,111,117 The effective mass of the ω oscillation is spin dependent and the other oscillation with the heavier mass may have the effective mass of the order of several tens of m 0 .…”
Section: Fermi Surface Properties Above the Metamagnetic Transitionmentioning
confidence: 99%
“…17(b). 1,106,107,111,117 The effective mass of the ω oscillation is spin dependent and the other oscillation with the heavier mass may have the effective mass of the order of several tens of m 0 .…”
Section: Fermi Surface Properties Above the Metamagnetic Transitionmentioning
confidence: 99%
“…4,5 Recent experiments on CeRu 2 Si 2 , however, suggest that the localization scenario might not be appropriate. 6 This was already pointed out in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…7, in which static magnetization measurements ruled out the possibility of a first order phase transition, at odds with the existent de Haas-van Alphen measurements. 5 On the basis of Hall effect and magnetoresistance measurements, the authors of Ref. 6 proposed that the MMT anomalies result from a continuous evolution of the Fermi surface in which the spin-split sheet corresponding to the heaviest electrons shrinks to a point.…”
Section: Introductionmentioning
confidence: 99%
“…So far, CeRu 2 Si 2 has eagerly been studied in order to elucidate the mechanism of the metamagnetic transition which occurs at H m ∼ 7.7 T. 15,16 According to the de Haas-van Alphen (dHvA) studies, 17 the Fermi surface (FS) of CeRu 2 Si 2 approaches to that of LaRu 2 Si 2 above H m due to the localization of the 4f electrons. However, the dHvA results of CeRu 2 Si 2 can not fully be explained by the band structure calculations under H < H m .…”
Section: Introductionmentioning
confidence: 99%