Low temperature and high magnetic field study of UBe13, U0.97Th0.03Be13 and UBe12.94Cu0.06

1986 ◽  
Vol 64 (3) ◽  
pp. 299-304 ◽  
Author(s):  
H. M. Mayer ◽  
U. Rauchschwalbe ◽  
F. Steglich ◽  
G. R. Stewart ◽  
A. L. Giorgi
1993 ◽  
Vol 56 (2-3) ◽  
pp. 2725-2730 ◽  
Author(s):  
A. Rotger ◽  
C. Schlenker ◽  
J. Dumas ◽  
J. Marcus ◽  
S. Dubois ◽  
...  

2000 ◽  
Vol 7 (3-4) ◽  
pp. 976-980 ◽  
Author(s):  
T Omiya ◽  
F Matsukura ◽  
T Dietl ◽  
Y Ohno ◽  
T Sakon ◽  
...  

2011 ◽  
Vol 273 ◽  
pp. 012110 ◽  
Author(s):  
H Q Yuan ◽  
L Jiao ◽  
J Singleton ◽  
F F Balakirev ◽  
G F Chen ◽  
...  

1980 ◽  
Vol 40 (3) ◽  
pp. 227-231 ◽  
Author(s):  
R. Plumier ◽  
M. Sougi ◽  
M. Lecomte ◽  
A. Miedan-Gros

1987 ◽  
Vol 01 (05n06) ◽  
pp. 245-250 ◽  
Author(s):  
C.Y. HUANG ◽  
Y. SHAPIRA ◽  
P.H. HOR ◽  
R.L. MENG ◽  
C.W. CHU

The magnetization of antiferromagnetic superconducting GdBa2Cu3O6+δ has been measured for ~1.5<T≤4.2 K for field up to ~20 T. We found that all Gd3+ spins are nearly parallel at very high field, and that this saturated spin subsystem coexists with superconductivity. Below the Néel temperature, 2.22 K, we observed the transition from the “canted” phase to the paramagnetic phase by the application of a high magnetic field.


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