HIGH-FIELD MAGNETIC TRANSITIONS IN THE R2T17 COMPOUNDS

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-505-C8-506 ◽  
Author(s):  
J. J. M. Franse ◽  
R. J. Radwaski ◽  
S. Sinnema
2004 ◽  
Vol 17 (1) ◽  
pp. 241-248 ◽  
Author(s):  
A Bouguerra ◽  
S Khène ◽  
S de Brion ◽  
G Chouteau ◽  
G Fillion

2006 ◽  
Vol 51 ◽  
pp. 231-234 ◽  
Author(s):  
V Sandu ◽  
C Zhang ◽  
C C Almasan ◽  
B J Taylor ◽  
M B Maple

2002 ◽  
Vol 16 (20n22) ◽  
pp. 3041-3044 ◽  
Author(s):  
S. CHANG ◽  
H. NAKOTTE ◽  
A. M. ALSMADI ◽  
A. H. LACERDA ◽  
M. H. JUNG ◽  
...  

UIrGe crystallizes in the orthorhombic TiNiSi structure and undergoes an antiferromagnetic transition around 14.1 K. The low-temperature longitudinal magnetoresistance (I // B) exhibits a pronounced field-induced step at about 13 T (14 T) and a much weaker step at about 17 T (out of field range) for B // b axis (c axis). No transition was seen for B // a. Here, we report on the magnetization results in fields up to 38 T applied along the principle directions. In addition, we present new magnetoresistance results taken in the transverse (I ⊥ B)configuration in fields up to 18 T applied along the c axis. The data show intriguing differences in comparison to those taken in the longitudinal configuration. The results are discussed in terms of field-induced magnetic transitions and/or Fermi-surface changes.


2017 ◽  
Vol 96 (10) ◽  
Author(s):  
V. Paul-Boncour ◽  
M. Guillot ◽  
O. Isnard ◽  
A. Hoser

Author(s):  
T. F. Kelly ◽  
P. J. Lee ◽  
E. E. Hellstrom ◽  
D. C. Larbalestier

Recently there has been much excitement over a new class of high Tc (>30 K) ceramic superconductors of the form A1-xBxCuO4-x, where A is a rare earth and B is from Group II. Unfortunately these materials have only been able to support small transport current densities 1-10 A/cm2. It is very desirable to increase these values by 2 to 3 orders of magnitude for useful high field applications. The reason for these small transport currents is as yet unknown. Evidence has, however, been presented for superconducting clusters on a 50-100 nm scale and on a 1-3 μm scale. We therefore planned a detailed TEM and STEM microanalysis study in order to see whether any evidence for the clusters could be seen.A La1.8Sr0.2Cu04 pellet was cut into 1 mm thick slices from which 3 mm discs were cut. The discs were subsequently mechanically ground to 100 μm total thickness and dimpled to 20 μm thickness at the center.


1998 ◽  
Vol 184-185 (1-2) ◽  
pp. 339-342 ◽  
Author(s):  
L Parthier
Keyword(s):  

1971 ◽  
Vol 32 (C1) ◽  
pp. C1-943-C1-945
Author(s):  
M. W. van TOL ◽  
M. MATSUURA ◽  
N. J. POULIS
Keyword(s):  

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