The Chebyshev differential equation of the first kind is
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(1)
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for . The Chebyshev differential equation has regular singular points at
, 1, and
.
A power series solution about
uses the expansions
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(2)
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(3)
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|
(4)
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Substituting these expansions into (1) gives
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(5)
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|
(6)
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|
(7)
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(8)
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(9)
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so
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(10)
|
|
(11)
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and equating the remaining coefficients gives
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(12)
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for , 3, ....
The equations for and
are special cases, so the recurrence
relation
|
(13)
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holds for , 1, .... It determines all coefficients
from
and
. For the even-indexed
coefficients,
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(14)
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(15)
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(16)
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and for the odd-indexed coefficients,
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(17)
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(18)
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(19)
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Both product formulas hold for , 1, ..., with the products
taken to be 1 when
.
For even ,
the coefficients can also be expressed using the
gamma function as
|
(20)
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and for odd as
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(21)
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At parameter values where the gamma function expressions are indeterminate, their limits give the finite products above. The general solution is obtained by combining the even and odd parts of the power series,
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(22)
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The change of variables ,
with
, transforms (1) into
|
(23)
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so for
the general solution is
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(24)
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For , the limiting form is
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(25)
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For , an equivalent form of the general
solution is
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(26)
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where
and
are Chebyshev polynomials of the
first kind and Chebyshev polynomials
of the second kind, respectively, extended to noninteger orders when necessary.
Another equivalent form of the general solution
for
is
|
(27)
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The Chebyshev differential equation of the second kind is
|
(28)
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For a nonnegative integer , the Chebyshev
polynomial of the second kind
is a solution (NIST Digital Library of Mathematical Functions,
Table 18.8.1). Differentiating (1) at
gives the second-kind equation for the derivative
of a first-kind solution.