In normalized form, the coefficients are and . They are analytic near zero, so .
At each of , has a simple pole and at most a simple pole. The products and are analytic, so both are regular singular points. More precisely their limiting values are and zero, giving indicial equation , with exponents .
To classify infinity, set and . The transformed equation is
After division, its coefficients satisfy
Both are analytic at , while itself has a pole. Hence , with indicial exponents . These classifications remain valid at , when the exponents at infinity coincide.
Because zero is an ordinary point, substitute . Matching powers gives
Even and odd coefficients evolve independently. Taking and constructs solutions
Their initial values and derivatives give , so they are linearly independent. These power series of the Chebyshev differential equation span the local solution space. A useful check is and , with at .
For a nonterminating parity series, consecutive nonzero terms satisfy
The ratio test therefore gives for each nonterminating series. The nearest singular coefficient points are , both distance one from the expansion centre.
The polynomial exception is essential here. If is an integer, the series of the same parity as terminates and has ; the opposite-parity independent series remains nonterminating with radius one. For noninteger , both have radius one. A regular singular point can be removable for one particular solution, so its presence does not force every individual solution to have finite convergence radius.
If is an integer, the recurrence has zero numerator at . Choosing the parity containing therefore makes all later coefficients vanish. Conversely, for a nonzero polynomial of degree , the coefficient of in the differential equation is , so is necessary.
Normalizing the terminating series by gives the first Chebyshev polynomials:
Substitution verifies each differential equation and endpoint value. More generally, ; its recurrence also establishes polynomiality and the normalization.

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