The resistivity of paramagnetic palladium-nickel alloys: an average T-matrix calculation

1972 ◽  
Vol 2 (6) ◽  
pp. 1151-1161 ◽  
Author(s):  
R Harris ◽  
M J Zuckermann
2014 ◽  
Vol 39 (16) ◽  
pp. 4827 ◽  
Author(s):  
Xiaoqiong Qi ◽  
Timo A. Nieminen ◽  
Alexander B. Stilgoe ◽  
Vincent L. Y. Loke ◽  
Halina Rubinsztein-Dunlop

2017 ◽  
Vol 8 ◽  
pp. 614-626 ◽  
Author(s):  
Martin Fruhnert ◽  
Ivan Fernandez-Corbaton ◽  
Vassilios Yannopapas ◽  
Carsten Rockstuhl

Given an arbitrarily complicated object, it is often difficult to say immediately how it interacts with a specific illumination. Optically small objects, e.g., spheres, can often be modeled as electric dipoles, but which multipole moments are excited for larger particles possessing a much more complicated shape? The T-matrix answers this question, as it contains the entire information about how an object interacts with any electromagnetic illumination. Moreover, a multitude of interesting properties can be derived from the T-matrix such as the scattering cross section for a specific illumination and information about symmetries of the object. Here, we present a method to calculate the T-matrix of an arbitrary object numerically, solely by illuminating it with multiple plane waves and analyzing the scattered fields. Calculating these fields is readily done by widely available tools. The finite element method is particularly advantageous, because it is fast and efficient. We demonstrate the T-matrix calculation at four examples of relevant optical nanostructures currently at the focus of research interest. We show the advantages of the method to obtain useful information, which is hard to access when relying solely on full wave solvers.


1974 ◽  
Vol 17 (1-2) ◽  
pp. 179-190 ◽  
Author(s):  
V. Canuto ◽  
J. Lodenquai ◽  
L. Parish ◽  
S. M. Chitre

1973 ◽  
Vol 51 (9) ◽  
pp. 1012-1016 ◽  
Author(s):  
K. H. Bray ◽  
S. N. Bunker ◽  
Mahavir Jain ◽  
K. S. Jayaraman ◽  
C. A. Miller ◽  
...  

A study of the 40Ca(p,2p)39K reaction has been made for two states of 39K, the 1d3/2−1(g.s.) and 2s1/2−1(2.53 MeV). Angular correlations at symmetric, coplanar angles between 30 and 105° have been measured. The data are compared with a distorted wave t-matrix calculation which utilizes a nonlocal bound state wave function. A further comparison is made with the angular correlation for unequal energies of the final state protons.


1973 ◽  
Vol 13 (6) ◽  
pp. 709-713 ◽  
Author(s):  
V. Canuto ◽  
J. Lodenquai ◽  
S.M. Chitre

Author(s):  
M.S. Grewal ◽  
S.A. Sastri ◽  
N.J. Grant

Currently there is a great interest in developing nickel base alloys with fine and uniform dispersion of stable oxide particles, for high temperature applications. It is well known that the high temperature strength and stability of an oxide dispersed alloy can be greatly improved by appropriate thermomechanical processing, but the mechanism of this strengthening effect is not well understood. This investigation was undertaken to study the dislocation substructures formed in beryllia dispersed nickel alloys as a function of cold work both with and without intermediate anneals. Two alloys, one Ni-lv/oBeo and other Ni-4.5Mo-30Co-2v/oBeo were investigated. The influence of the substructures produced by Thermo-Mechanical Processing (TMP) on the high temperature creep properties of these alloys was also evaluated.


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