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In mathematics, the Bessel polynomials are an
orthogonal In mathematics, orthogonality is the generalization of the geometric notion of '' perpendicularity''. By extension, orthogonality is also used to refer to the separation of specific features of a system. The term also has specialized meanings in ...
sequence of
polynomial In mathematics, a polynomial is an expression consisting of indeterminates (also called variables) and coefficients, that involves only the operations of addition, subtraction, multiplication, and positive-integer powers of variables. An ex ...
s. There are a number of different but closely related definitions. The definition favored by mathematicians is given by the series :y_n(x)=\sum_^n\frac\,\left(\frac\right)^k. Another definition, favored by electrical engineers, is sometimes known as the reverse Bessel polynomials :\theta_n(x)=x^n\,y_n(1/x)=\sum_^n\frac\,\frac. The coefficients of the second definition are the same as the first but in reverse order. For example, the third-degree Bessel polynomial is :y_3(x)=15x^3+15x^2+6x+1 while the third-degree reverse Bessel polynomial is :\theta_3(x)=x^3+6x^2+15x+15. The reverse Bessel polynomial is used in the design of Bessel electronic filters.


Properties


Definition in terms of Bessel functions

The Bessel polynomial may also be defined using
Bessel function Bessel functions, first defined by the mathematician Daniel Bernoulli and then generalized by Friedrich Bessel, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary ...
s from which the polynomial draws its name. :y_n(x)=\,x^\theta_n(1/x)\, :y_n(x)=\sqrt\,e^K_(1/x) :\theta_n(x)=\sqrt\,x^e^K_(x) where ''K''''n''(''x'') is a modified Bessel function of the second kind, ''y''''n''(''x'') is the ordinary polynomial, and ''θ''''n''(''x'') is the reverse polynomial . For example: :y_3(x)=15x^3+15x^2+6x+1 = \sqrt\,e^K_(1/x)


Definition as a hypergeometric function

The Bessel polynomial may also be defined as a
confluent hypergeometric function In mathematics, a confluent hypergeometric function is a solution of a confluent hypergeometric equation, which is a degenerate form of a hypergeometric differential equation where two of the three regular singularities merge into an irregular ...
:y_n(x)=\,_2F_0(-n,n+1;;-x/2)= \left(\frac 2 x\right)^ U\left(-n,-2n,\frac 2 x\right)= \left(\frac 2 x\right)^ U\left(n+1,2n+2,\frac 2 x \right). A similar expression holds true for the generalized Bessel polynomials (see below): :y_n(x;a,b)=\,_2F_0(-n,n+a-1;;-x/b)= \left(\frac b x\right)^ U\left(n+a-1,2n+a,\frac b x \right). The reverse Bessel polynomial may be defined as a generalized Laguerre polynomial: :\theta_n(x)=\frac\,L_n^(2x) from which it follows that it may also be defined as a hypergeometric function: :\theta_n(x)=\frac\,\,_1F_1(-n;-2n;2x) where (−2''n'')''n'' is the Pochhammer symbol (rising factorial).


Generating function

The Bessel polynomials, with index shifted, have the generating function :\sum_^\infty \sqrt x^ e^x K_(x) \frac =1+x\sum_^\infty \theta_(x) \frac= e^. Differentiating with respect to t, cancelling x, yields the generating function for the polynomials \_ :\sum_^\infty \theta_(x) \frac=\frace^. Similar generating function exists for the y_n polynomials as well: :\sum_^\infty y_(x)\frac=\exp\left(\frac\right). Upon setting t=z-xz^2/2, one has the following representation for the
exponential function The exponential function is a mathematical function denoted by f(x)=\exp(x) or e^x (where the argument is written as an exponent). Unless otherwise specified, the term generally refers to the positive-valued function of a real variable, ...
: :e^z=\sum_^\infty y_(x)\frac.


Recursion

The Bessel polynomial may also be defined by a recursion formula: :y_0(x)=1\, :y_1(x)=x+1\, :y_n(x)=(2n\!-\!1)x\,y_(x)+y_(x)\, and :\theta_0(x)=1\, :\theta_1(x)=x+1\, :\theta_n(x)=(2n\!-\!1)\theta_(x)+x^2\theta_(x)\,


Differential equation

The Bessel polynomial obeys the following differential equation: :x^2\frac+2(x\!+\!1)\frac-n(n+1)y_n(x)=0 and :x\frac-2(x\!+\!n)\frac+2n\,\theta_n(x)=0


Orthogonality

The Bessel polynomials are orthogonal with respect to the weight e^ integrated over the unit circle of the complex plane. In other words, if n \neq m, \int_0^ y_n\left(e^\right) y_m\left(e^\right) ie^ \mathrm\theta = 0


Generalization


Explicit Form

A generalization of the Bessel polynomials have been suggested in literature, as following: :y_n(x;\alpha,\beta):= (-1)^n n! \left(\frac x \beta\right)^n L_n^\left(\frac \beta x\right), the corresponding reverse polynomials are :\theta_n(x;\alpha, \beta):= \fracL_n^(\beta x)=x^n y_n\left(\frac 1 x;\alpha,\beta\right). The explicit coefficients of the y_n(x;\alpha, \beta) polynomials are: :y_n(x;\alpha, \beta)= \sum_^n\binom(n+k+\alpha-2)^\left(\frac\right)^k. Consequently, the \theta_n(x;\alpha, \beta) polynomials can explicitly be written as follows: :\theta_n(x;\alpha, \beta)=\sum_^n\binom(2n-k+\alpha-2)^\frac. For the weighting function :\rho(x;\alpha,\beta):= \, _1F_1\left(1,\alpha-1,-\frac \beta x\right) they are orthogonal, for the relation :0= \oint_c\rho(x;\alpha,\beta)y_n(x;\alpha,\beta) y_m(x;\alpha,\beta)\mathrm d x holds for ''m'' ≠ ''n'' and ''c'' a curve surrounding the 0 point. They specialize to the Bessel polynomials for α = β = 2, in which situation ρ(''x'') = exp(−2 / ''x'').


Rodrigues formula for Bessel polynomials

The Rodrigues formula for the Bessel polynomials as particular solutions of the above differential equation is : :B_n^(x)=\frac \left(\frac\right)^n (x^ e^) where ''a'' are normalization coefficients.


Associated Bessel polynomials

According to this generalization we have the following generalized differential equation for associated Bessel polynomials: :x^2\frac + \alpha+2)x+\betafrac - \left n(\alpha+n+1) + \frac \rightB_^(x)=0 where 0\leq m\leq n. The solutions are, :B_^(x)=\frac \left(\frac\right)^ (x^ e^)


Zeros

If one denotes the zeros of y_n(x;\alpha,\beta) as \alpha_k^(\alpha,\beta), and that of the \theta_n(x;\alpha,\beta) by \beta_k^(\alpha,\beta), then the following estimates exist: :\frac\le\alpha_k^(\alpha,2)\le\frac, and :\frac\le\beta_k^(\alpha,2)\le\frac, for all \alpha\ge2. Moreover, all these zeros have negative real part. Sharper results can be said if one resorts to more powerful theorems regarding the estimates of zeros of polynomials (more concretely, the Parabola Theorem of Saff and Varga, or differential equations techniques). One result is the following: :\frac\le\alpha_k^(\alpha,2)\le\frac.


Particular values

The Bessel polynomials y_n(x) up to n=5 are : \begin y_0(x) & = 1 \\ y_1(x) & = x + 1 \\ y_2(x) & = 3x^2+ 3x + 1 \\ y_3(x) & = 15x^3+ 15x^2+ 6x + 1 \\ y_4(x) & = 105x^4+105x^3+ 45x^2+ 10x + 1 \\ y_5(x) & = 945x^5+945x^4+420x^3+105x^2+15x+1 \end No Bessel polynomial can be factored into lower degree polynomials with rational coefficients. The reverse Bessel polynomials are obtained by reversing the coefficients. Equivalently, \theta_k(x) = x^k y_k(1/x). This results in the following: : \begin \theta_0(x) & = 1 \\ \theta_1(x) & = x + 1 \\ \theta_2(x) & = x^ + 3 x + 3 \\ \theta_3(x) & = x^ + 6 x^ + 15 x + 15 \\ \theta_4(x) & = x^ + 10 x^ + 45 x^ + 105 x + 105 \\ \theta_5(x) & = x^ + 15 x^ + 105 x^ + 420 x^ + 945 x + 945 \\ \end


See also

*
Bessel function Bessel functions, first defined by the mathematician Daniel Bernoulli and then generalized by Friedrich Bessel, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary ...
* Neumann polynomial * Lommel polynomial *
Hankel transform In mathematics, the Hankel transform expresses any given function ''f''(''r'') as the weighted sum of an infinite number of Bessel functions of the first kind . The Bessel functions in the sum are all of the same order ν, but differ in a scalin ...
* Fourier–Bessel series


References

* * *


External links

* * {{MathWorld, title=Bessel Polynomial, urlname=BesselPolynomial Orthogonal polynomials Special hypergeometric functions