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| 001 | 202820 | ||
| 005 | 20210129220233.0 | ||
| 024 | 7 | _ | |a 10.1140/epjst/e2015-02443-6 |2 doi |
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| 100 | 1 | _ | |a Fritsch, V. |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Role of the tuning parameter at magnetic quantum phase transitions |
| 260 | _ | _ | |a Berlin |c 2015 |b Springer |
| 300 | _ | _ | |a 23p. |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |m journal |
| 336 | 7 | _ | |a Review |b review |m review |0 PUB:(DE-HGF)36 |s 1438683706_16989 |2 PUB:(DE-HGF) |
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| 520 | _ | _ | |a Heavy-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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| 693 | _ | _ | |a Forschungs-Neutronenquelle Heinz Maier-Leibnitz |e PANDA: Cold three axes spectrometer |f SR2 |1 EXP:(DE-MLZ)FRMII-20140101 |0 EXP:(DE-MLZ)PANDA-20140101 |5 EXP:(DE-MLZ)PANDA-20140101 |6 EXP:(DE-MLZ)SR2-20140101 |x 0 |
| 700 | 1 | _ | |a Stockert, O. |0 P:(DE-HGF)0 |b 1 |e Corresponding author |
| 700 | 1 | _ | |a Huang, C.-L. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Bagrets, N. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Kittler, W. |0 P:(DE-HGF)0 |b 4 |
| 700 | 1 | _ | |a Taubenheim, C. |0 P:(DE-HGF)0 |b 5 |
| 700 | 1 | _ | |a Pilawa, B. |0 P:(DE-HGF)0 |b 6 |
| 700 | 1 | _ | |a Woitschach, S. |0 P:(DE-HGF)0 |b 7 |
| 700 | 1 | _ | |a Huesges, Z. |0 P:(DE-HGF)0 |b 8 |
| 700 | 1 | _ | |a Lucas, S. |0 P:(DE-HGF)0 |b 9 |
| 700 | 1 | _ | |a Schneidewind, A. |0 P:(DE-Juel1)156579 |b 10 |
| 700 | 1 | _ | |a Grube, K. |0 P:(DE-HGF)0 |b 11 |
| 700 | 1 | _ | |a Löhneysen, H. v. |0 P:(DE-HGF)0 |b 12 |e Corresponding author |
| 773 | _ | _ | |a 10.1140/epjst/e2015-02443-6 |g Vol. 224, no. 6, p. 997 - 1019 |0 PERI:(DE-600)2267176-6 |n 6 |p 997 - 1019 |t European physical journal special topics |v 224 |y 2015 |x 1951-6401 |
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