Chebyshev constant
A numerical invariant $ \tau = \tau ( E) $
of a compact set $ E $
in the complex plane that is used in the theory of best approximation.
Let $ K _ {n} $ be the class of all polynomials
$$ p _ {n} ( z) = z ^ {n} + c _ {1} z ^ {n-} 1 + \dots + c _ {n} $$
of degree $ n $, and let
$$ M ( p _ {n} ) = \max \{ {| p _ {n} ( z) | } : {z \in E } \} , $$
$$ m _ {n} = \inf \{ {M ( p _ {n} ) } : {p _ {n} \in K _ {n} } \} ,\ \tau _ {n} = {m _ {n} } ^ {1/n} . $$
There exists a polynomial $ t _ {n} ( z) \in K _ {n} $ for which $ M ( t _ {n} ) = m _ {n} $; it is called the Chebyshev polynomial for $ E $. Moreover, the limit
$$ \lim\limits _ {n \rightarrow \infty } \tau _ {n} = \tau $$
exists, and is called the Chebyshev constant for $ E $.
Restricting oneself to the class $ \widetilde{K} _ {n} $ of all polynomials
$$ \widetilde{p} _ {n} ( z) = z ^ {n} + \dots + \widetilde{c} _ {n} $$
all zeros of which lie in $ E $, one obtains corresponding values $ \widetilde{m} _ {n} , \widetilde \tau _ {n} , \widetilde \tau $ and a polynomial $ \widetilde{t} _ {n} ( z) $ for which $ M ( \widetilde{t} _ {n} ) = \widetilde{m} _ {n} $( it is also called the Chebyshev polynomial).
It is known that $ \tau = \widetilde \tau = C ( E) = d $, where $ C ( E) $ is the capacity of the compact set $ E $, and $ d $ is its transfinite diameter (cf., for example, [1]).
The concept of the Chebyshev constant generalizes to compact sets $ E $ in higher-dimensional Euclidean spaces $ \mathbf R ^ {m} $ starting from potential theory. For a point $ x \in \mathbf R ^ {m} $, let
$$ H ( | x | ) = \left \{ \begin{array}{ll} \mathop{\rm ln} \frac{1}{| x | } & \textrm{ for } m = 2 , \\ \frac{1}{| x | ^ {m-} 2 } & \textrm{ for } m \geq 3 , \\ \end{array} \right .$$
be the fundamental solution of the Laplace equation, and for a set $ ( x _ {j} ) _ {j=} 1 ^ {n} \subset E $, let
$$ \sigma _ {n} ( E) = \sup \left \{ {\min \left \{ { \frac{1}{n} \sum _ { j= } 1 ^ { n } H ( | x - x _ {j} | ) } : {x \in E } \right \} } : {( x _ {j} ) _ {j=} 1 ^ {n} \subset E } \right \} . $$
Then for $ m = 2 $ one obtains the relation
$$ \tau = \widetilde \tau = C ( E) = \mathop{\rm exp} \left ( - \lim\limits _ {n \rightarrow \infty } \ \sigma _ {n} ( E) \right ) , $$
and for $ m \geq 3 $ one obtains (cf. [2]):
$$ \tau = C ( E) = \frac{1}{\lim\limits _ {n \rightarrow \infty } \sigma _ {n} ( E) } . $$
References
[1] | G.M. Goluzin, "Geometric theory of functions of a complex variable" , Transl. Math. Monogr. , 26 , Amer. Math. Soc. (1969) (Translated from Russian) |
[2] | L. Carleson, "Selected problems on exceptional sets" , v. Nostrand (1967) |
Comments
References
[a1] | M. Tsuji, "Potential theory in modern function theory" , Chelsea, reprint (1975) |
[a2] | J.L. Walsh, "Interpolation and approximation by rational functions in the complex domain" , Amer. Math. Soc. (1956) |
Chebyshev constant. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Chebyshev_constant&oldid=46327