## LFNM 2003: Proceedings of LFNM 2003 : 5th International Workshop on Laser and Fiber-optical Networks Modeling : Alushta, Crimea, Ukraine, 19-20 September 2003 |

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Page 156

In consequence surfaces waves with spatial soliton are formed . Now if the

saturation

nonlinear interface ( Figure 2 ) and the reflected beam is near to nonlinear

medium .

In consequence surfaces waves with spatial soliton are formed . Now if the

saturation

**coefficient**is increased , the beam is transmitted and reflected bynonlinear interface ( Figure 2 ) and the reflected beam is near to nonlinear

medium .

Page 216

22h ; + y ? , ng = Vē , and y = a + iß – is the propagation constant , a - is the

absorption

, K ( v ) Jo ( u ) are the well - known [ 3 ] Bessel functions of the first kind and ...

22h ; + y ? , ng = Vē , and y = a + iß – is the propagation constant , a - is the

absorption

**coefficient**, ß – is the phase**coefficient**and Jo ( u ) , Ji ( u ) and Ko ( v ), K ( v ) Jo ( u ) are the well - known [ 3 ] Bessel functions of the first kind and ...

Page 256

7 and

cmo K . The violation of conservation of the electron wave vector at optical

transitions provides a second power dependence of jtn ~ T ' [ 4 , 5 ] . Involving

highlying ...

7 and

**coefficient**a for different laser materials covers the interval of 0 . 2 to 3 A /cmo K . The violation of conservation of the electron wave vector at optical

transitions provides a second power dependence of jtn ~ T ' [ 4 , 5 ] . Involving

highlying ...

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### Contents

LFNM Plenary Sessions | 7 |

Transformation of the Polarization Distribution in the CrossSection of Light Beam by Self | 18 |

Extraction of Spectra and Theresholds from FullWave Lasing Eigenvalue Problems Invited | 19 |

Copyright | |

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