We MIGHT make some headway if we seek an asymptotic approximation in the vicinity of x=0 (i.e, we make a supposition that our unknown function y(x) is defined at x=0)
Let us state an initial condition:
[tex]y(0)=y_{0}>0[/tex]
In addition, we set:
[tex]y'(0)=y'_{0}[/tex]
Define:
[tex]y(x)=Y(x)+y_{0}[/tex],
so that:
[tex]Y(0)=0,Y'(0)=y_{0}'[/tex]
In the vicinity of x=0, we have:
[tex]ln(y)=ln(y_{0}+Y)=ln(y_{0})+ln(1+\frac{Y}{y_{0}})\approx{ln(y_{0})}+\frac{Y}{y_{0}}[/tex]
[tex]yx=y_{0}x+Yx\approx{y}_{0}x[/tex]
Hence, close to x=0, we have the differential equation in Y:
[tex]Y''+\frac{Y}{y_{0}}=y_{0}x-ln(y_{0}), Y(0)=0 (1)[/tex]
The general solution of the homogenous equation (that is, [tex]Y''+\frac{Y}{y_{0}}=0[/tex]) is:
[tex]Y_{h}(x)=A\cos(\frac{x}{\sqrt{y_{0}}})+B\sin(\frac{x}{\sqrt{y_{0}}})[/tex]
A particular solution to (1) is the linear function:
[tex]Y_{p}=y_{0}^{2}x-y_{0}ln(y_{0})[/tex]
We therefore set
[tex]Y(x)=Y_{h}+Y_{p}[/tex]
[tex]Y(0)=0\to{A}=y_{0}ln(y_{0})[/tex]
Whereas:
[tex]Y'(0)=y_{0}'\to{B}=y_{0}'\sqrt{y_{0}}-(y_{0})^{\frac{5}{2}}[/tex]
Hence, we get the asymptotic solution, to first order:
[tex]y(x)=y_{0}+y_{0}ln(y_{0})\cos(\frac{x}{\sqrt{y_{0}}})+(y_{0}'\sqrt{y_{0}}-(y_{0})^{\frac{5}{2}})\sin(\frac{x}{\sqrt{y_{0}}})+y_{0}^{2}x-y_{0}ln(y_{0})[/tex]
I would like to emphasize that this is only a first order approximation, valid in the limit [tex]x\to0[/tex]