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000202820 1001_ $$0P:(DE-HGF)0$$aFritsch, V.$$b0$$eCorresponding author
000202820 245__ $$aRole of the tuning parameter at magnetic quantum phase transitions
000202820 260__ $$aBerlin$$bSpringer$$c2015
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000202820 520__ $$aHeavy-fermion systems, with their competition betweenKondo and RKKY interactions, offer a rich variety of materials thatmay be driven to a magnetic quantum phase transition. Quite often,a quantum critical point can be approached by chemical substitution,notably of isoelectric ligands of Ce, as in CeCu6−xAux andCePd1−xNixAl. While in the former we compare pressure and concentrationtuning of the magnetic structure, the latter has the additionalfeature of geometric frustration due to the distorted kagom´e sublatticeof Ce atoms in the basal plane. We further present the systemCeAu2Ge2 where minor structural differences between crystals grownfrom Sn or Au-Ge flux lead to pronounced differences in the magneticstructure, with several field-induced phases in samples grown fromAu-Ge flux. Finally, non-isoelectronic substitution of Ti by V is studiedin CeTi1−xVxGe3 where CeTiGe3 is a ferromagnet, thus allowingthe study of ferromagnetic quantum criticality, a rare case for heavyfermionsystems.
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000202820 7001_ $$0P:(DE-HGF)0$$aStockert, O.$$b1$$eCorresponding author
000202820 7001_ $$0P:(DE-HGF)0$$aHuang, C.-L.$$b2
000202820 7001_ $$0P:(DE-HGF)0$$aBagrets, N.$$b3
000202820 7001_ $$0P:(DE-HGF)0$$aKittler, W.$$b4
000202820 7001_ $$0P:(DE-HGF)0$$aTaubenheim, C.$$b5
000202820 7001_ $$0P:(DE-HGF)0$$aPilawa, B.$$b6
000202820 7001_ $$0P:(DE-HGF)0$$aWoitschach, S.$$b7
000202820 7001_ $$0P:(DE-HGF)0$$aHuesges, Z.$$b8
000202820 7001_ $$0P:(DE-HGF)0$$aLucas, S.$$b9
000202820 7001_ $$0P:(DE-Juel1)156579$$aSchneidewind, A.$$b10
000202820 7001_ $$0P:(DE-HGF)0$$aGrube, K.$$b11
000202820 7001_ $$0P:(DE-HGF)0$$aLöhneysen, H. v.$$b12$$eCorresponding author
000202820 773__ $$0PERI:(DE-600)2267176-6$$a10.1140/epjst/e2015-02443-6$$gVol. 224, no. 6, p. 997 - 1019$$n6$$p997 - 1019$$tEuropean physical journal special topics$$v224$$x1951-6401$$y2015
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