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Metamagnetism

About: Metamagnetism is a research topic. Over the lifetime, 2023 publications have been published within this topic receiving 38108 citations.


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01 Mar 1999
TL;DR: In this paper, a field-induced metamagnetic transition for the magnetic field along the c-axis is observed, which is caused by the switching of the different magnetic anisotropy states.
Abstract: Abstract High-field magnetization measurements in single crystalline CeCu 2 , TbCu 2 and DyCu 2 with the orthorhombic CeCu 2 -type crystal structure have been carried out. A field-induced metamagnetic transition for the magnetic field along the c -axis is observed, which is caused by the switching of the different magnetic anisotropy states. The origin of the transition is discussed on the basis of the quadrupolar interaction and crystalline electric field.

5 citations

Journal ArticleDOI
TL;DR: In this paper, the spin dependence of the quasiparticle masses on the two small ellipsoidal Fermi surface sheets of CeRu 2 Si 2 via the dHvA effect was measured.
Abstract: We have measured the spin dependence of the quasiparticle masses on the two small ellipsoidal Fermi surface sheets of CeRu 2 Si 2 via the dHvA effect. The field variation of the effective masses above the metamagnetic transition was obtained for the β ′ and γ ′ oscillations. We find that m ↓ * ( β ′ ) ≈ 5 m ↑ * ( β ′ ) , m ↓ * ( γ ′ ) ≈ 3 m ↑ * ( γ ′ ) .

5 citations

Journal ArticleDOI
TL;DR: In this article, the magnetization and magnetoresistance of a heavy-fermion antiferromagnet YbAgGe have been measured under pressures P up to 2.7 GPa and magnetic fields B up to 9.5 T.
Abstract: The magnetization M and magnetoresistance of a heavy-fermion antiferromagnet YbAgGe have been measured under pressures P up to 2.7 GPa and magnetic fields B up to 9.5 T. This compound crystallizing in the hexagonal ZrNiAl-type structure with a quasi-kagome lattice of Yb ions has two magnetically ordered phases, namely, phase I ( T ≤ T M2 = 0.65 K) and phase II ( T M2 ≤ T ≤ T M1 = 0.8 K). With increasing pressure to 2.2 GPa, M ( B || a = 9.5 T) at 0.3 K increases from 1.5 µ B /Yb to 1.8 µ B /Yb, while M ( B || c = 9.5 T) hardly changes. The metamagnetic transition field in M ( B || a ) decreases from 4.6 T for P = 0 to 3.3 T for P = 2.2 GPa. As the pressure exceeds P * = 1.6 GPa, both T M and the initial slope of M ( B || a ) steeply increase and the area of phase I for B || a expands. These observations suggest that the magnetic frustration of the Yb quasi-kagome lattice is partially suppressed by the application of pressure above 1.6 GPa or magnetic field B || a above 4.5 T. Detailed B – T phase diagrams...

5 citations

Journal ArticleDOI
TL;DR: In this article, pressure effects on the magnetic properties of a series of quasi-one-dimensional molecular magnets have been studied and it is suggested that the subtle change of the relative arrangement of chain structures affects the interchain ferromagnetic interactions.
Abstract: Pressure effects on the magnetic properties of a series of quasi-one-dimensional molecular magnets have been studied. The complexes of Mn(hfac) 2 (hfac = hexafluoroacethylacetonate) with 1,3-bis(N-tert-buthylaminoxyl)benzene and it's 5-halo- derivatives, abbreviated as 1 x (X = H, F, Cl and Br), have almost the same ferrimagnetic chain structure. The difference is seen in the interchain molecular arrangement. The complexes of 1 H and IF are metamagnets with weak interchain antiferromagnetic interactions, whereas 1 Cl and 1 Br are ferrimagnets with weak interchain ferromagnetic interactions. In two metamagnets (1 H , 1 F ), the pressurization simply results in the enhancement of the interchain antiferromagnetic interactions, which is reflected by the higher transition temperature and spin-flipping field. On the other hand, in the ferrimagnet (1 Cl ), the metamagnetic behavior is observed under pressure. It is suggested that the subtle change of the relative arrangement of chain structures affects the interchain ferromagnetic interactions.

5 citations

Journal ArticleDOI
TL;DR: In this paper, a single crystal of Tb 5 Sn 3 has been successfully grown by the Czochralski method and the effective paramagnetic moment obtained from reciprocal susceptibility is 10.3 μ B along the c-axis and 10.0 μ B in the c -plane.

5 citations

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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
202320
202249
202117
202015
201937
201837