Dynamic lower mode control of a light beam wave front in a nonlinear medium

1987 ◽  
Vol 30 (4) ◽  
pp. 320-324
Author(s):  
V. A. Trofimov
1978 ◽  
Vol 21 (12) ◽  
pp. 1003-1004
Author(s):  
V I Bespalov ◽  
A A Betin ◽  
G A Pasmanik
Keyword(s):  

1978 ◽  
Vol 126 (12) ◽  
pp. 688-689
Author(s):  
V.I. Bespalov ◽  
A.A. Betin ◽  
G.A. Pasmanik
Keyword(s):  

1995 ◽  
Vol 62 (1) ◽  
pp. 179-181 ◽  
Author(s):  
V. I. Borisov ◽  
V. I. Lebedev
Keyword(s):  

2002 ◽  
Vol 16 (25) ◽  
pp. 955-962 ◽  
Author(s):  
HARI PRAKASH ◽  
DEVENDRA K. SINGH

The effect of an intense plane wave on a co-propagating weak plane wave in a lossy isotropic nonlinear medium is studied using the exact solution of H. Prakash et al.1 The presence of a plane-polarized intense beam changes the initial circular polarization of the weak beam to elliptical in general. The plane containing the direction of the major axis and the propagation oscillates about the plane of polarization of the intense beam. At the extreme positions, the elliptical polarization reduces to plane polarization and switches its handedness. For the lossless case, the plane of the major axis remains fixed at 45° to the plane of polarization of the intense beam and the polarization oscillates between circular and plane, switching the handedness when the plane polarization occurs, and there effects are periodic in distance within the medium. The presence of a circularly polarized intense beam changes the initial plane polarization of the weak beam to elliptical, whose major axis rotates in propagation. For the lossless case, the weak beam remains plane-polarized and rotates at a uniform rate in propagation. Suggestions for experimental observations of these effects are given and the values of observable quantities estimated for carbon disulfide.


1983 ◽  
Vol 26 (2) ◽  
pp. 129-134
Author(s):  
N. S. Ginzburg ◽  
N. D. Milovskii ◽  
N. Yu. Rusov
Keyword(s):  

1980 ◽  
Vol 39 (4) ◽  
pp. 1143-1145
Author(s):  
I. S. Granik ◽  
L. K. Martinson

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