In Mathematical, a continuation of orthogonal polynomials is a infinite continuation of Polynôme S p 0 ( X ), p 1 ( X ), p 2 ( X )…, in which each p N ( X ) has a degree N and so that the polynomials of the continuation are orthogonal two to two, with the following direction:
We can define the scalar Produit functions, (by analogy with the scalar product for the Vecteur S), in integral the product of these functions:
more generally, we can introduce a " function poids" W ( X ) in the integral:
With this definition of scalar product, two functions are orthogonal between them if their scalar product is equal to zero (same manner that two vectors are orthogonal (perpendiculars) if their scalar product equalizes zero).
Such a made scalar product of the whole of all the functions of standard finished, a Space of Hilbert.
The interval of integration is called interval of orthogonality . It can be infinite on one or two terminals.
This field of the orthogonal polynomials was developed during the XIXe century by the study of the continued fractions by Stieltjes. In rose from multiple applications in mathematics and Physique.
They all are orthogonal on:
The function weight must be strictly positive in the field of integration. In certain cases, it can be null or infinite at the boundaries of the integral. The integral of the product of the function weight by a polynomial must be finished.
Any continuation of polynomials , where each is of degree K , is a base of the vector space (of infinite size) of all the polynomials. A succession of orthogonal polynomials is simply a continuation which includes/understands an orthogonal base for this space, relative with this scalar product.
The Procédé of Gram-Schmidt can transform any base of a vector space (provided with a scalar product) into an orthogonal base. One starts with a vector and while incorporating, one by one, of new vectors in such a way that each new vector is orthogonal with all the precedents. This is carried out by withdrawing a linear Combinaison preceding vectors. This is often a exercise for the first elementary courses of Linear algebra. It results the polynomials from them from Legendre.
When an orthogonal base is built, one can be tried to make it orthonormal , i.e., in which . In the case of the polynomials, it often results from it from dreadful square roots for the coefficients. In the place, the polynomials are transformed, in a way approved by the mathematicians, so that the coefficients give simpler formulas. One calls that standardization . The polynomials " classiques" enumerated below were standardized. Typically, their coefficients of the term moreover high degree were put at a given quantity. This standardization does not have mathematical significance, it is right a convention. Standardization implies also a scaling of the function weight.
Once the continuation of polynomials standardized, one can define the standard. That is to say
The standard is the square root of this. The values of for standardization are enumerated in the table below. We have
where δmn is the Delta of Kronecker.
Lemma 1: Being taken an action pursuant of orthogonal polynomials , any polynomial of degree N can be expressed in a single way like a linear combination of . I.e., there exist coefficients such as
Lemma 2: Being given a succession of orthogonal polynomials, any element of this continuation is orthogonal with any polynomial of strictly lower degree.
The coefficients has , B , and C depends on N . They also depend on the standardization, obviously.
The values of , and can be calculated directly. Are and the first two coefficients of :
and the scalar product of by itself:
One obtains
Any polynomial of a succession of orthogonal polynomials of which degree N is equal to or higher than 1 admits N distinct roots, all real, and located strictly inside the interval of integration.
(Whoever already drew the curve representative of a polynomial, knows at which point it is rare, for a polynomial whose coefficients were randomly selected, to have all its real roots.)
where Q is a given quadratic polynomial and L a given linear polynomial. The function F and the constant λ are the unknown factors.
(To notice that a polynomial solution has all its direction for such an equation.
The solutions of this differential equation have singularities, unless λ does not take specific values. The continuation of numbers leads to a succession of polynomials solutions if one of the following assertions is checked:
Q is really quadratic, L is linear, Q has two distinct real roots, the root of L is located between the two roots of Q, and the terms moreover high degree of Q and L have the same sign.
These three cases lead respectively to the polynomials of Jacobi , Laguerre and Hermite .
For each one of these cases:
the solution is a succession of polynomials , each having a degree N, and corresponding to the number .
Because of the constant of integration, the quantity R (X) is defined except for a multiplicative constant. The table low gives the values " officielles" R (X) and W (X).
better known equation under the name of “formula of Rodrigues”. She is often written:
where the numbers E N depend on standardization. The values of E N are given in the table low.
With the assumptions of the preceding section,
(Since is quadratic and linear, and is constant, they are indeed numbers.)
With .
Then
By multiplying the differential equation now
by R/Q, one obtains
or
It is forms it standardized Sturm-Liouville of the equation.
By posing .
Then:
By multiplying the differential equation now
by S/Q, one obtains:
or
But , therefore
or, by posing U = Sy ,
| Random links: | Neptunism | Tama (instrument) | Crow of Sinaloa | Brooklyn 62nd | Paul D. Clément |