Complex polarization topologies in nanostructured light (Conference Presentation)

Author(s):  
Peter Banzer
Keyword(s):  
Plasmonics ◽  
2012 ◽  
Vol 8 (2) ◽  
pp. 571-579 ◽  
Author(s):  
Jed I. Ziegler ◽  
Richard F. Haglund

2010 ◽  
Author(s):  
Chen Haifeng ◽  
Luo Guoan ◽  
Hou Aiyuan ◽  
Zhao Gulling ◽  
Lei Na

Appleton’s magneto-ionic theory of the propagation of wireless waves in the ionosphere has been discussed by several authors, usually for the case when incidence is vertical and damping due to electronic collisions is neglected. Two salient features of the theory which appear upon the removal of these restrictions are described in the present paper. In sections 3, 4, and 5 the effect of collisional friction on vertical propagation is examined and the nature of the transition from longitudinal to transverse propagation is described. Curves are drawn (in section 5) showing this transition when there is a small constant value of friction and the Lorentz polarization therm is neglected. In some respects this part of the paper resembles the treatment in a recent paper by Taylor, but there appears to be a difference between her conclusions and ours. In section 6 the further complication of oblique incidence is considered with particular reference to the relation between the polarization of downcoming magneto-ionic components. A description of the relation between the complex polarization and the elliptical polarization which it represents is included in section 4.


2016 ◽  
Vol 12 (6) ◽  
pp. 2661-2667 ◽  
Author(s):  
Zilvinas Rinkevicius ◽  
Jaime A. R. Sandberg ◽  
Xin Li ◽  
Mathieu Linares ◽  
Patrick Norman ◽  
...  

2018 ◽  
Vol 43 (23) ◽  
pp. 5757 ◽  
Author(s):  
M. Alameer ◽  
A. Jain ◽  
M. G. Rahimian ◽  
H. Larocque ◽  
P. B. Corkum ◽  
...  

1991 ◽  
Vol 81 (2) ◽  
pp. 611-621
Author(s):  
William Menke ◽  
Arthur Lerner-Lam

Abstract We measure the polarization of compressional waves from seismograms of chemical explosion of the Ontario-New York-New England refraction experiment recorded by the seven element ECO array in the New York Adirondack mountains. After careful instrument calibration, a precision of about 5° is achieved in measuring the azimuth of the compressional wave polarization direction. The azimuth of the polarization of the onset of the P wave differs from the geometrical source-receiver azimuth by as much as 20°, possible due to deflection of the first-arriving ray by lateral variation in crustal structure. Shortly after the onset of P, the polarization changes from the linear polarization expected of a compressional wave to become very complex. The time of this transition increases with source-receiver distance, from about 0.4 to 0.5 sec at 50 km distance and 0.7 to 0.8 sec at 150 km distance. The complex polarization may be due to the arrival of strongly scattered waves that have propagated mainly in the shallow crust, which would imply that the upper 1 to 2 km of the crust is particularly heterogeneous.


Sign in / Sign up

Export Citation Format

Share Document