After division by , the equation is . Every is an ordinary point. The origin is singular, but it is a regular singular point because and are analytic there. An ordinary point has analytic normalized coefficients ; a singular point failing the displayed regularity test is irregular.
The Frobenius method ansatz gives the indicial equation , , and
For nonintegral , two independent solutions are
For integral , put . In the recurrence the denominator vanishes at , so that series fails or coincides in the exceptional case. Up to scale the single Frobenius series is
For , , so
Its integral contains both and ; multiplying by leaves a pole and a logarithmic term. Thus the reduction-of-order solution is not a power series at zero.
For
a finite point is a regular singular point when and extend holomorphically to . A singularity at infinity is classified by applying this criterion after the change of variable .
For the displayed Bessel differential equation,
At , the functions and are holomorphic, so zero is regular singular. To inspect infinity, write . The equation becomes
Here is not holomorphic at zero, so infinity is an irregular singular point. Thus
Set . Direct differentiation makes every lower-order term cancel:
Hence , and on any domain carrying a branch of two linearly independent solutions are
Near the regular singular point, these behave as and , the two Frobenius exponents. At infinity their combinations are ; after these contain , the exponential behavior characteristic of an irregular singular point.