TRANSPORT ANISOTROPY IN ErNi2B2C ALONG c-AXIS

2010 ◽  
Vol 24 (30) ◽  
pp. 5861-5866
Author(s):  
W. C. LEE

The resistivities along c-axis ρc(H, T) of ErNi 2 B 2 C have been measured with H⊥ and H‖c-axis for 2 < T < 300 K and the superconducting upper critical field Hc2(T) curves of ErNi 2 B 2 C were constructed for each magnetic fields. Our Hc2(T) curves have been compared and discussed with those from ρab(H, T) measurements which explain the anisotropy and its temperature dependence of Hc2(T) are thought to arise from magnetic pair breaking and the anisotropic field dependence of Néel temperature TN originated from Er +3 sublattice.

2001 ◽  
Vol 294-295 ◽  
pp. 427-430 ◽  
Author(s):  
Y. Shimojo ◽  
A.E. Kovalev ◽  
S. Kamiya ◽  
E. Ohmichi ◽  
T. Ishiguro ◽  
...  

2007 ◽  
Vol 148 (5-6) ◽  
pp. 743-747
Author(s):  
Todd E. Sherline ◽  
E. Dwight Adams ◽  
Yasu Takano

2013 ◽  
Vol 87 (13) ◽  
Author(s):  
S. I. Vedeneev ◽  
B. A. Piot ◽  
D. K. Maude ◽  
A. V. Sadakov

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3598-3603 ◽  
Author(s):  
L. Krusin-Elbaum ◽  
T. Shibauchi ◽  
C. H. Mielke

The orientational anisotropy of the pseudogap closing field Hpg is investigated in magnetic fields up to 60 T applied parallel (||ab) and normal (||c) to CuO 2 planes in Bi 2 Sr 2 CaCu 2 O 8+y. We find that, in contrast to large field anisotropy related to the orbital motion of Cooper pairs below the upper critical field Hc2, the temperature-independent and small anisotropy of Hpg is due to anisotropy of the g-factor: [Formula: see text], indicating correlations only in the spin-channel.


1986 ◽  
Vol 57 (10) ◽  
pp. 1259-1262 ◽  
Author(s):  
B. S. Shivaram ◽  
T. F. Rosenbaum ◽  
D. G. Hinks

1997 ◽  
Vol 291 (1-2) ◽  
pp. 41-48 ◽  
Author(s):  
T.Geetha Kumary ◽  
S. Kalavathi ◽  
M.C. Valsakumar ◽  
Y. Hariharan ◽  
T.S. Radhakrishnan

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