Ginzburg-Landau-Schrodinger equation: Difference between revisions

Revision as of 14:26, 9 August 2006

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The Ginsberg-Landau-Schrodinger equation is

iu_{t}^{\epsilon }+\Delta u^{\epsilon }={\frac {1}{\epsilon ^{2}}}(|u^{\epsilon }|^{2}-1)u^{\epsilon }.

The main focus of study for this equation is the formation of vortices and their dynamics in the limit $\epsilon \to 0$ .

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-This a stub and needs to updated.
+{{stub}}
-[[Category:Stubs]]
+The '''Ginsberg-Landau-Schrodinger''' equation is
+<center><math>i u^\epsilon_t + \Delta u^\epsilon = \frac{1}{\epsilon^2} (|u^\epsilon|^2 - 1)u^\epsilon.</math></center>
+The main focus of study for this equation is the formation of vortices and their dynamics in the limit <math>\epsilon \to 0</math>.
+[[Category:Schrodinger]]
 [[Category:Equations]]