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solving a Schwartz derivative

A computation related to the link between a second order linear differential equation and a Ricatti equation gives a solution to a Schwartz differential equation

$\displaystyle \{w,z\}$ = 2Q(z) (314)

where
$\displaystyle \{w,z\}$ = $\displaystyle \left\{\frac{w''}{w'}\right\}'-\frac{1}{2}\left(\frac{w''}{w'}\right)^2.$ (315)

Suppose that y1 and y2 are two solutions of the second order equation

y'' + 2Q(z) = 0 (316)

whose nonvanishing and linear indepencence is established by their having a unit Wronskian,
$\displaystyle \left\vert
\begin{array}{cc} y_1(z) & y_2(z) \\  y_1'(z) & y_2'(z) \end{array}\right\vert$ = 1. (317)

Starting with the definition

w(z) = $\displaystyle \frac{y_1(z)}{y_2(z)},$ (318)

there follow
w'(z) = [y2(z)]-2, (319)
$\displaystyle \frac{w''}{w'}$ = $\displaystyle -2\frac{y_2'(z)}{y_2(z)},$ (320)
$\displaystyle \left(\frac{w''(z)}{w'(z)}\right)'$ = $\displaystyle -2\frac{y_2(z)'}{y_2(z)} +
2\left(\frac{y_2'(z)}{y_2(z)}\right)^2,$ (321)
  = $\displaystyle 2Q(z) + \frac{1}{2}\left(\frac{w''(z)}{w'(z)}\right)^2,$ (322)

according to which such a quotient solves the equation. The involvement of the Ricatti equation arises from concluding that the only other solutions of the Schwartz equation result from a change of basis from the two solutions y1(z) and y2(z), which would enter w in the form of a fractional linear transformation. But we already know that invariance under fractional linear transformation and invariance of the Schwartz derivative are two sides of the same coin.


next up previous contents
Next: Functions of mathematical physics Up: Second order differential equations Previous: projective coordinates and Ricatti's
Microcomputadoras
2001-04-05