The term "Lebesgue constants" refers to either of two commonly used sets. The first is related to approximation of functions via Fourier series, while the other arises in the computation of Lagrange interpolating polynomials.
Assume a function is integrable over the interval
and
is the
th partial sum of the Fourier
series of
,
so that
|
(1)
| |||
|
(2)
|
and
|
(3)
|
If
|
(4)
|
for all ,
then
|
(5)
|
and
is the smallest possible constant for which this holds for all continuous
functions
.
The first few values of
are
|
(6)
| |||
|
(7)
| |||
|
(8)
| |||
|
(9)
| |||
|
(10)
| |||
|
(11)
| |||
|
(12)
|
Some sum formulas for include
|
(13)
| |||
|
(14)
|
(Zygmund 1959) and integral formulas include
|
(15)
| |||
|
(16)
|
(Hardy 1942). For large ,
|
(17)
|
This result can be generalized for a -periodic function with
continuous derivatives, where
is an integer, satisfying
|
(18)
|
for all .
In this case,
|
(19)
|
where
|
(20)
|
(Kolmogorov 1935, Zygmund 1959).
Watson (1930) showed that
|
(21)
|
where
|
(22)
| |||
|
(23)
| |||
|
(24)
|
(OEIS A243277), where is the gamma function,
is the Dirichlet lambda function, and
is the Euler-Mascheroni constant.
For a positive integer and
distinct nodes
with
, define the
th Lebesgue constant for the Lagrange
interpolating polynomial by
|
(25)
|
It is then true that
|
(26)
|
The efficiency of Lagrange interpolating polynomial approximation is related to the rate at which increases. Erdős (1961) proved that there exists
a positive constant such that
|
(27)
|
for all .
For the nodes given by the roots of the Chebyshev
polynomial of the first kind
, Erdős (1961) notes that
|
(28)
|
where
is a positive constant independent of
. Thus the leading coefficient
of
in (27) cannot be increased.