Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 5Kharkiv State University of Radio Electronics, 2003 - Fiber optics |
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Page 137
... plane and light distribution is measured in the second focal plane . However in the general case when the subject is not in the focus its spatial spectrum is distorted by quadratic phase shifts . If the plane object is illuminated by ...
... plane and light distribution is measured in the second focal plane . However in the general case when the subject is not in the focus its spatial spectrum is distorted by quadratic phase shifts . If the plane object is illuminated by ...
Page 198
... plane ( in the incidence plane , fig . 1 ) . Periods of the structures were measured by the autocollimation scheme . For the horizontal torch it satisfied the equation for TMo - modes . With the AgCl thickness of h = 125 nm ( calculated ...
... plane ( in the incidence plane , fig . 1 ) . Periods of the structures were measured by the autocollimation scheme . For the horizontal torch it satisfied the equation for TMo - modes . With the AgCl thickness of h = 125 nm ( calculated ...
Page 226
... plane . For antisymmetric zigzag of optic axis in xy , yz , or zx - planes cross - polarized the Bragg reflections ( HE and EH ) are absent . For the zigzag in yz - plane only co - polarized reflection of TM waves occur . Formulas ( 3 ) ...
... plane . For antisymmetric zigzag of optic axis in xy , yz , or zx - planes cross - polarized the Bragg reflections ( HE and EH ) are absent . For the zigzag in yz - plane only co - polarized reflection of TM waves occur . Formulas ( 3 ) ...
Contents
LFNM Plenary Sessions | 1 |
Extraction of Spectra and Theresholds from FullWave Lasing Eigenvalue Problems Invited | 19 |
Design and Evaluation of High Speed DBR Lasers for Analog and Digital Transmission Invited | 32 |
Copyright | |
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