U(As1−xSex)solid solutions. I. Resonant x-ray and neutron scattering study of the magnetic phase diagram

2001 ◽  
Vol 63 (13) ◽  
Author(s):  
M. J. Longfield ◽  
W. G. Stirling ◽  
E. Lidström ◽  
D. Mannix ◽  
G. H. Lander ◽  
...  
1987 ◽  
Vol 63-64 ◽  
pp. 151-154 ◽  
Author(s):  
P. Burlet ◽  
D. Bonnisseau ◽  
S. Quezel ◽  
J. Rossat-Mignod ◽  
J.C. Spirlet ◽  
...  

Author(s):  
P. BURLET ◽  
D. BONNISSEAU ◽  
S. QUEZEL ◽  
J. ROSSAT-MIGNOD ◽  
J.C. SPIRLET ◽  
...  

2010 ◽  
Vol 12 (10) ◽  
pp. 105006 ◽  
Author(s):  
D Haug ◽  
V Hinkov ◽  
Y Sidis ◽  
P Bourges ◽  
N B Christensen ◽  
...  

1998 ◽  
Vol 266 (1-2) ◽  
pp. 230-233 ◽  
Author(s):  
S. Danilkin ◽  
H. Fuess ◽  
E. Jadrowski ◽  
T. Wieder ◽  
H. Wipf

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3411-3414 ◽  
Author(s):  
R. Gilardi ◽  
S. Streule ◽  
J. Mesot ◽  
A. J. Drew ◽  
U. Divakar ◽  
...  

The magnetic phase diagram of slightly overdoped La 2-x Sr x CuO 4 (x=0.17) is characterised by a field-induced hexagonal to square transition of the vortex lattice at low fields (~ 0.4 Tesla) [R. Gilardi et al., Phys. Rev. Lett.88, 217003 (2002)]. Here we report on a small angle neutron scattering study of the vortex lattice at higher fields, that reveals no further change of the coordination of the square vortex lattice up to 10.5 Tesla applied perpendicular to the CuO 2 planes. Moreover, it is found that the diffraction signal disappears at temperatures well below Tc, due to the melting of the vortex lattice.


ChemInform ◽  
2010 ◽  
Vol 29 (22) ◽  
pp. no-no
Author(s):  
S. DANILKIN ◽  
H. FUESS ◽  
E. JADROWSKI ◽  
T. WIEDER ◽  
H. WIPF

2009 ◽  
Vol 404 (19) ◽  
pp. 3264-3266 ◽  
Author(s):  
H.C. Walker ◽  
R.A. Ewings ◽  
F. Fabrizi ◽  
D. Mannix ◽  
C. Mazzoli ◽  
...  

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