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<record version="2" id="787">
 <title>time-dependent harmonic oscillators</title>
 <name>TimeDependentHarmonicOscillators</name>
 <created>2009-05-29 13:46:17</created>
 <modified>2009-05-29 13:50:10</modified>
 <type>Topic</type>
 <creator id="441" name="bci1"/>
 <modifier id="441" name="bci1"/>
 <author id="441" name="bci1"/>
 <classification>
	<category scheme="msc" code="00."/>
	<category scheme="msc" code="02."/>
	<category scheme="msc" code="03."/>
	<category scheme="msc" code="03.65.Fd"/>
 </classification>
 <defines>
	<concept>Ermakov systems</concept>
 </defines>
 <keywords>
	<term>time-dependent harmonic oscillators</term>
 </keywords>
 <preamble></preamble>
 <content>\section{Time-dependent harmonic oscillators}
Nonlinear equations are of increasing interest in Physics; Riccati and Ermakov systems enter the formalism of quantum theory in the study of cases where exact analytic Gaussian wave packet (WP) solutions of the time-dependent
Schr\"odinger equation (SE) do exist, and in particular, in the harmonic oscillator (HO) and the free motion cases.

One of the simplest examples of such nonlinear equations is the Milne--Pinney equation:
$$d^2x/dt^2 = −\omega^2(t)x +k x^3,$$ (1)

where $k$ is a real constant with values depending on the field in which the equation is to be applied.

\subsection{Ermakov systems}
This equation was introduced in the nineteenth
century by V.P. Ermakov, as a way of looking for a first integral for the time-dependent harmonic oscillator. He employed some of Lie's ideas for dealing with ordinary differential equations with the tools of classical geometry. Lie had previously obtained a characterisation of non-autonomous systems of first-order differential equations admitting a superposition rule.


\textbf{[More to come]}</content>
</record>
