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		<id>https://en.formulasearchengine.com/index.php?title=Descriptivist_theory_of_names&amp;diff=12509</id>
		<title>Descriptivist theory of names</title>
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		<updated>2013-10-13T18:31:18Z</updated>

		<summary type="html">&lt;p&gt;93.5.162.23: /* See also */ added onomastics link&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Maxwell&#039;s Equations]], when converted to [[cylindrical coordinates]], and with the boundary conditions for an [[optical fiber]] while including [[birefringence]] as an effect taken into account, will yield the coupled [[nonlinear Schrödinger equation]]s. After employing the [[Inverse scattering transform]] (a procedure analogous to the [[Fourier Transform]] and [[Laplace Transform]]) on the resulting equations, the Manakov system is then obtained. The most general form of the Manakov system is as follows:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;v_{1}&#039;=-i\,\xi\,v_{1}+q_{1}\,v_{2}+q_{2}\,v_{3}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v_{2}&#039;=-q_{1}^{*}\,v_{1}+i\,\xi\,v_{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v_{3}&#039;=-q_{2}^{*}\,v_{1}+i\,\xi\,v_{3}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It is a coupled system of linear [[ordinary differential equations]]. The functions &amp;lt;math&amp;gt;q_{1}, q_{2}&amp;lt;/math&amp;gt; represent the envelope of the electromagnetic field as an initial condition.&lt;br /&gt;
&lt;br /&gt;
For theoretical purposes, the [[integral equation]] version is often very useful. It is as follows:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\lim_{x\to a}e^{i\xi x}v_{1}-\lim_{x\to b}e^{i\xi x}v_{1}=\int_{a}^{b}[e^{i\xi x}\,q_{1}\,v_{2}+e^{i\xi x}\,q_{2}\,v_{3}]\,dx&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\lim_{x\to a}e^{-i\xi x}v_{2}-\lim_{x\to b}e^{-i\xi x}v_{2}=-\int_{a}^{b}e^{-i\xi x}\,q_{1}^{*}\,v_{1}\,dx&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\lim_{x\to a}e^{-i\xi x}v_{3}-\lim_{x\to b}e^{-i\xi x}v_{3}=-\int_{a}^{b}e^{-i\xi x}\,q_{2}^{*}\,v_{1}\,dx&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
One may make further substitutions and simplifications, depending on the limits used and the assumptions about boundary or initial conditions. One important concept is that &amp;lt;math&amp;gt;\xi&amp;lt;/math&amp;gt; is complex; assumptions must be made about this [[eigenvalue]] parameter.  If a non-zero solution is desired, the imaginary part of the eigenvalue cannot change [[Sign (mathematics)|sign]]; accordingly, most researchers take the imaginary part to be [[Positive number|positive]].&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*C. Menyuk, &#039;&#039;Application of multiple-length-scale methods to the study of optical fiber transmission&#039;&#039;, Journal of Engineering Mathematics 36: 113-136, 1999, Kluwer Academic Publishers, Netherlands.&lt;br /&gt;
*D. Kaup, B. Malomed, &#039;&#039;Soliton Trapping and Daughter Waves in the Manakov Model&#039;&#039;, Physical Review A, Vol. 48, No. 1, July 1993.&lt;br /&gt;
*S. V. Manakov, &#039;&#039;Remarks on the Integrals of the Euler Equations of the n-dimensional Heavy Top&#039;&#039;, Functional Anal. Appl., Vol. 10, pp.&amp;amp;nbsp;93–94, 1976.&lt;br /&gt;
&lt;br /&gt;
[[Category:Fiber optics]]&lt;br /&gt;
[[Category:Ordinary differential equations]]&lt;/div&gt;</summary>
		<author><name>93.5.162.23</name></author>
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