scholarly journals Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1−xEuxPt4Ge12

2018 ◽  
Vol 98 (6) ◽  
Author(s):  
R. B. Adhikari ◽  
D. L. Kunwar ◽  
I. Jeon ◽  
M. B. Maple ◽  
M. Dzero ◽  
...  
2010 ◽  
Vol 470 ◽  
pp. S703-S704 ◽  
Author(s):  
F. Kanetake ◽  
H. Mukuda ◽  
Y. Kitaoka ◽  
H. Sugawara ◽  
K. Magishi ◽  
...  

2017 ◽  
Vol 53 (1) ◽  
pp. 323-332 ◽  
Author(s):  
Lili Chen ◽  
Jiyu Fan ◽  
Wei Tong ◽  
Dazhi Hu ◽  
Lei Zhang ◽  
...  

2005 ◽  
Vol 38 (18) ◽  
pp. 3343-3347 ◽  
Author(s):  
Fèlix Casanova ◽  
Sophie de Brion ◽  
Amílcar Labarta ◽  
Xavier Batlle

1990 ◽  
Vol 2 (32) ◽  
pp. 6801-6806 ◽  
Author(s):  
X Obradors ◽  
J Bassas ◽  
J Rodriguez ◽  
J Pannetier ◽  
A Labarta ◽  
...  

1996 ◽  
Vol 8 (24) ◽  
pp. 4411-4428 ◽  
Author(s):  
Arturo Marcello Allega ◽  
Hideki Matsumoto ◽  
Satoru Odashima

2010 ◽  
Vol 168-169 ◽  
pp. 497-500
Author(s):  
E.A. Tishchenko ◽  
O.E. Omelyanovskii ◽  
A.V. Sadakov ◽  
D.G. Eshchenko ◽  
A.A. Bush ◽  
...  

The low temperature investigations of the magnetic properties of non-twinning LiCu2O2+δ crystals showed that a new spontaneous magnetization phase arises in the compound at temperatures less than T~150 K along with the basic long-range helimagnet phase at T<24 K. The increase of an extra oxygen Оδ concentration intensifies ferromagnetic response of this phase. We suggested a cluster model for the new phase as an antiferromagnet structure with a short-range order with the weak and hidden ferromagnetism on the basis of both the theoretical group analysis of the magnetic and crystal lattice symmetry and the analysis of the temperature, field, hysteresis and anisotropy properties of spontaneous magnetization.


2000 ◽  
Vol 14 (29n31) ◽  
pp. 3374-3379
Author(s):  
N. BULUT ◽  
U. YAZ

The NMR and neutron scattering experiments on YBa 2 Cu 3 O 7 with Li and Zn impurities are compared using a simple framework exhibiting short-range antiferromagnetic correlations. The model parameters are determined by fitting the NMR rate [Formula: see text] of the pure system, and the effective impurity potential is approximated by a static extended form. The results of the calculations are compared with the experimental data, and their implications are discussed.


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