Crossover scaling functions for exchange anisotropy:X Yand planar models

1975 ◽  
Vol 11 (9) ◽  
pp. 3445-3456 ◽  
Author(s):  
Surjit Singh ◽  
David Jasnow
Keyword(s):  
2015 ◽  
Vol 67 (3) ◽  
pp. 1275-1294 ◽  
Author(s):  
Ryuichi ASHINO ◽  
Takeshi MANDAI ◽  
Akira MORIMOTO

2013 ◽  
Vol 2013 ◽  
pp. 1-6 ◽  
Author(s):  
Suchitra Rajput ◽  
Sujeet Chaudhary

We report on the analyses of fluctuation induced excess conductivity in the - behavior in the in situ prepared MgB2 tapes. The scaling functions for critical fluctuations are employed to investigate the excess conductivity of these tapes around transition. Two scaling models for excess conductivity in the absence of magnetic field, namely, first, Aslamazov and Larkin model, second, Lawrence and Doniach model, have been employed for the study. Fitting the experimental - data with these models indicates the three-dimensional nature of conduction of the carriers as opposed to the 2D character exhibited by the HTSCs. The estimated amplitude of coherence length from the fitted model is ~21 Å.


2011 ◽  
Vol 182 (1) ◽  
pp. 226-228 ◽  
Author(s):  
Chien-Fu Chen ◽  
An-Chung Cheng ◽  
Yi-Duen Wang ◽  
Chai-Yu Lin

Fractals ◽  
2001 ◽  
Vol 09 (02) ◽  
pp. 165-169
Author(s):  
GANG CHEN ◽  
ZHIGANG FENG

By using fractal interpolation functions (FIF), a family of multiple wavelet packets is constructed in this paper. The first part of the paper deals with the equidistant fractal interpolation on interval [0, 1]; next, the proof that scaling functions ϕ1, ϕ2,…,ϕr constructed with FIF can generate a multiresolution analysis of L2(R) is shown; finally, the direct wavelet and wavelet packet decomposition in L2(R) are given.


1998 ◽  
Vol 38 (21) ◽  
pp. 3259-3263 ◽  
Author(s):  
Steven L Buck ◽  
Roger Knight ◽  
Garth Fowler ◽  
Brian Hunt

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