scholarly journals The Weyl law of transmission eigenvalues and the completeness of generalized transmission eigenfunctions

2021 ◽  
pp. 109146
Author(s):  
Hoai-Minh Nguyen ◽  
Quoc-Hung Nguyen
1994 ◽  
Vol 08 (08n09) ◽  
pp. 469-478 ◽  
Author(s):  
C. W. J. Beenakker

Recent developments in the scaling theory of phase-coherent conduction through a disordered wire are reviewed. The Dorokhov–Mello–Pereyra–Kumar equation for the distribution of transmission eigenvalues has been solved exactly, in the absence of time-reversal symmetry. Comparison with the previous prediction of random-matrix theory shows that this prediction was highly accurate but not exact: the repulsion of the smallest eigenvalues was overestimated by a factor of two. This factor of two resolves several disturbing discrepancies between random-matrix theory and microscopic calculations, notably in the magnitude of the universal conductance fluctuations in the metallic regime, and in the width of the log-normal conductance distribution in the insulating regime.


1996 ◽  
Vol 10 (15) ◽  
pp. 681-688 ◽  
Author(s):  
M. CASELLE

We discuss the distribution of transmission eigenvalues in the strongly localized regime in the presence of both a magnetic field and spin-orbit scattering. We show that, under suitable conditions, this distribution can be described by a new universality class labelled not only by the index β but also by a new index η. This result is obtained by mapping the problem into that of a suitable Calogero-Sutherland model.


2017 ◽  
Vol 33 (12) ◽  
pp. 125002 ◽  
Author(s):  
S Cogar ◽  
D Colton ◽  
S Meng ◽  
P Monk

2014 ◽  
Vol 2014 ◽  
pp. 1-8
Author(s):  
Yalin Zhang ◽  
Yanling Wang ◽  
Guoliang Shi ◽  
Shizhong Liao

We consider all of the transmission eigenvalues for one-dimensional media. We give some conditions under which complex eigenvalues exist. In the case when the index of refraction is constant, it is shown that all the transmission eigenvalues are real if and only if the index of refraction is an odd number or reciprocal of an odd number.


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