Neutron scattering from a collective spin fluctuation mode in aCuO2bilayer

1996 ◽  
Vol 53 (9) ◽  
pp. 5149-5152 ◽  
Author(s):  
N. Bulut ◽  
D. J. Scalapino
2005 ◽  
Vol 13 (1-3) ◽  
pp. 45-48
Author(s):  
H. Kawano-Furukawa ◽  
M. Urata ◽  
T. Nagata ◽  
H. Yoshizawa ◽  
H. Kadowaki ◽  
...  

2004 ◽  
Vol 73 (11) ◽  
pp. 2967-2970 ◽  
Author(s):  
Takeshi Matsumura ◽  
Hideaki Ishida ◽  
Taku J. Sato ◽  
Kenichi Katoh ◽  
Yuzuru Niide ◽  
...  

2000 ◽  
Vol 62 (22) ◽  
pp. 15204-15207 ◽  
Author(s):  
F. Venturini ◽  
U. Michelucci ◽  
T. P. Devereaux ◽  
A. P. Kampf

2001 ◽  
Vol 15 (04) ◽  
pp. 373-377
Author(s):  
TAO LI

A model with interlayer pairing is proposed to explain the sinusoidal modulation of the resonant neutron scattering in high temperature superconductors. It is found that the interlayer pairing has s-wave symmetry in the CuO 2 plane and has comparable magnitude with the d-wave intralayer pairing. It is also found that the interlayer pairing mainly affects momentum close to the hot spots on the Fermi surface while its effect on the gap nodes is negligible. It is pointed out that these characteristics of the interlayer pairing can be understood in a model in which the superconducting pairing originates from the exchange of the antiferromagnetic spin fluctuation.


Author(s):  
T. Egami ◽  
H. D. Rosenfeld ◽  
S. Teslic

Relaxor ferroelectrics, such as Pb(Mg1/3Nb2/3)O3 (PMN) or (Pb·88La ·12)(Zr·65Ti·35)O3 (PLZT), show diffuse ferroelectric transition which depends upon frequency of the a.c. field. In spite of their wide use in various applications details of their atomic structure and the mechanism of relaxor ferroelectric transition are not sufficiently understood. While their crystallographic structure is cubic perovskite, ABO3, their thermal factors (apparent amplitude of thermal vibration) is quite large, suggesting local displacive disorder due to heterovalent ion mixing. Electron microscopy suggests nano-scale structural as well as chemical inhomogeneity.We have studied the atomic structure of these solids by pulsed neutron scattering using the atomic pair-distribution analysis. The measurements were made at the Intense Pulsed Neutron Source (IPNS) of Argonne National Laboratory. Pulsed neutrons are produced by a pulsed proton beam accelerated to 750 MeV hitting a uranium target at a rate of 30 Hz. Even after moderation by a liquid methane moderator high flux of epithermal neutrons with energies ranging up to few eV’s remain.


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