Write a power series . Substitution gives
The lowest coefficients give , , with free. For , matching the coefficient of gives the recurrence
All odd coefficients consequently vanish. For the first solution, , , so the first three nonzero terms, when , are
For the second, , , giving
If its prescribed constant is zero, the corresponding solution is identically zero and has no nonzero terms.
For the change of variable, put , , with . The chain rule gives
After division by , the coefficient of is and that of is . A genuine constant-coefficient equation requires , which both removes and makes the final coefficient constant. The transformed equation is .
This quadratic-variable reduction of a singular oscillator yields
It holds on each interval away from zero and both solutions extend smoothly through zero. Here and , so the specified solutions are exactly and . Their Taylor series agree with the recurrences above. Although the original equation has a regular singular point at zero, these two linearly independent smooth solutions supply the required data there.