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:
y(0)=y_{0}>0
In addition, we set:
y'(0)=y'_{0}
Define:
y(x)=Y(x)+y_{0},
so that:
Y(0)=0,Y'(0)=y_{0}'
In the vicinity of x=0, we have:
ln(y)=ln(y_{0}+Y)=ln(y_{0})+ln(1+\frac{Y}{y_{0}})\approx{ln(y_{0})}+\frac{Y}{y_{0}}
yx=y_{0}x+Yx\approx{y}_{0}x
Hence, close to x=0, we have the differential equation in Y:
Y''+\frac{Y}{y_{0}}=y_{0}x-ln(y_{0}), Y(0)=0 (1)
The general solution of the homogenous equation (that is, Y''+\frac{Y}{y_{0}}=0) is:
Y_{h}(x)=A\cos(\frac{x}{\sqrt{y_{0}}})+B\sin(\frac{x}{\sqrt{y_{0}}})
A particular solution to (1) is the linear function:
Y_{p}=y_{0}^{2}x-y_{0}ln(y_{0})
We therefore set
Y(x)=Y_{h}+Y_{p}
Y(0)=0\to{A}=y_{0}ln(y_{0})
Whereas:
Y'(0)=y_{0}'\to{B}=y_{0}'\sqrt{y_{0}}-(y_{0})^{\frac{5}{2}}
Hence, we get the asymptotic solution, to first order:
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})
I would like to emphasize that this is only a first order approximation, valid in the limit x\to0