Romanovski polynomials
In mathematics, the Romanovski polynomials are one of three finite subsets of real orthogonal polynomials discovered by Vsevolod Romanovsky^{[1]} (Romanovski in French transcription) within the context of probability distribution functions in statistics. They form an orthogonal subset of a more general family of littleknown Routh polynomials introduced by Edward John Routh^{[2]} in 1884. The term Romanovski polynomials was put forward by Raposo,^{[3]} with reference to the socalled 'pseudoJacobi polynomials in Lesky's classification scheme.^{[4]} It seems more consistent to refer to them as Romanovski–Routh polynomials, by analogy with the terms Romanovski–Bessel and Romanovski–Jacobi used by Lesky for two other sets of orthogonal polynomials.
In some contrast to the standard classical orthogonal polynomials, the polynomials under consideration differ, in so far as for arbitrary parameters only a finite number of them are orthogonal, as discussed in more detail below.
Contents
The differential equation for the Romanovski polynomialsEdit
The Romanovski polynomials solve the following version of the hypergeometric differential equation

(1)
Curiously, they have been omitted from the standard textbooks on special functions in mathematical physics^{[5]}^{[6]} and in mathematics^{[7]}^{[8]} and have only a relatively scarce presence elsewhere in the mathematical literature.^{[9]}^{[10]}^{[11]}
The weight functions are

(2)
they solve Pearson's differential equation

(3)
that assures the selfadjointness of the differential operator of the hypergeometric ordinary differential equation.
For α = 0 and β < 0, the weight function of the Romanovski polynomials takes the shape of the Cauchy distribution, whence the associated polynomials are also denoted as Cauchy polynomials^{[12]} in their applications in random matrix theory.^{[13]}
The Rodrigues formula specifies the polynomial R^{(α,β)}
_{n}(x) as

(4)
where N_{n} is a normalization constant. This constant is related to the coefficient c_{n} of the term of degree n in the polynomial R^{(α,β)}
_{n}(x) by the expression

(5)
which holds for n ≥ 1.
Relationship between the polynomials of Romanovski and JacobiEdit
As shown by Askey this finite sequence of real orthogonal polynomials can be expressed in terms of Jacobi polynomials of imaginary argument and thereby is frequently referred to as complexified Jacobi polynomials.^{[14]} Namely, the Romanovski equation (1) can be formally obtained from the Jacobi equation,^{[15]}

(6)
via the replacements, for real x,

(7)
in which case one finds

(8)
(with suitably chosen normalization constants for the Jacobi polynomials). However, this alternative expression is not useful when considering the orthogonality properties. The issue is that the orthogonality integrals of the complex Jacobi polynomials depend on the integration contour. In Kuijlaars et al. (2003)^{[16]} an orthogonality relation for Jacobi polynomials along the imaginary axis has been given, as required by the replacements in (7), but only for a limited case of real, not integer, parameters.
Notice the invertibility of (8) according to

(9)
where, now, P^{(α,β)}
_{n}(x) is a real Jacobi polynomial and
would be a complex Romanovski polynomial.
Properties of Romanovski polynomialsEdit
Explicit constructionEdit
For real α, β and n = 0, 1, 2, ..., a function R^{(α,β)}
_{n}(x) can be defined
by the Rodrigues formula in Equation (4) as

(10)
where w^{(α,β)} is the same weight function as in (2), and s(x) = 1 + x^{2} is the coefficient of the second derivative of the hypergeometric differential equation as in (1).
Note that we have chosen the normalization constants N_{n} = 1, which is equivalent to making a choice of the coefficient of highest degree in the polynomial, as given by equation (5). It takes the form

(11)
Also note that the coefficient c_{n} does not depend on the parameter α, but only on β and, for particular values of β, c_{n} vanishes (i.e., for all the values
where k = 0, ..., n − 1). This observation poses a problem addressed below.
For later reference, we write explicitly the polynomials of degree 0, 1, and 2,
which derive from the Rodrigues formula (10) in conjunction with Pearson's ODE (3).
OrthogonalityEdit
The two polynomials, R^{(α,β)}
_{m}(x) and R^{(α,β)}
_{n}(x) with m ≠ n, are orthogonal,^{[3]}

(12)
if and only if,

(13)
In other words, for arbitrary parameters, only a finite number of Romanovski polynomials are orthogonal. This property is referred to as finite orthogonality. However, for some special cases in which the parameters depend in a particular way on the polynomial degree infinite orthogonality can be achieved.
This is the case of a version of equation (1) that has been independently encountered anew within the context of the exact solubility of the quantum mechanical problem of the trigonometric Rosen–Morse potential and reported in Compean & Kirchbach (2006).^{[17]} There, the polynomial parameters α and β are no longer arbitrary but are expressed in terms of the potential parameters, a and b, and the degree n of the polynomial according to the relations,

(14)
Correspondingly, λ_{n} emerges as λ_{n} = −n(2a + n − 1), while the weight function takes the shape
Finally, the onedimensional variable, x, in Compean & Kirchbach (2006)^{[17]} has been taken as
where r is the radial distance, while is an appropriate length parameter. In Compean & Kirchbach^{[17]} it has been shown that the family of Romanovski polynomials corresponding to the infinite sequence of parameter pairs,

(15)
is orthogonal.
Generating functionEdit
In Weber (2007)^{[18]} polynomials Q^{(αn, βn + n)}
_{ν}(x), with β_{n} + n = −a, and complementary to R^{(αn, βn)}
_{n}(x) have been studied, generated in the following way:

(16)
In taking into account the relation,

(17)
Equation (16) becomes equivalent to

(18)
and thus links the complementary to the principal Romanovski polynomials.
The main attraction of the complementary polynomials is that their generating function can be calculated in closed form.^{[19]} Such a generating function, written for the Romanovski polynomials based on Equation (18) with the parameters in (14) and therefore referring to infinite orthogonality, has been introduced as

(19)
The notational differences between Weber^{[18]} and those used here are summarized as follows:
 G^{(αn, βn)}(x,y) here versus Q(x,y;α,−a) there, α there in place of α_{n} here,
 a = −β_{n} − n, and
 Q^{(α,−a)}
_{ν}(x) in Equation (15) in Weber^{[18]} corresponding to R^{(αn, βn + n − ν)}
_{ν}(x) here.
The generating function under discussion obtained in Weber^{[18]} now reads:

(20)
Recurrence relationsEdit
Recurrence relations between the infinite orthogonal series of Romanovski polynomials with the parameters in the above equations (14) follow from the generating function,^{[18]}

(21)
and

(22)
as Equations (10) and (23) of Weber (2007)^{[18]} respectively.
See alsoEdit
ReferencesEdit
This article lacks ISBNs for the books listed in it. (December 2017) 
 ^ Romanovski, V. (1929). "Sur quelques classes nouvelles de polynomes orthogonaux". C. R. Acad. Sci. Paris (in French). 188: 1023.
 ^ Routh, E. J. (1884). "On some properties of certain solutions of a differential equation of second order". Proc. London Math. Soc. 16: 245. doi:10.1112/plms/s116.1.245.
 ^ ^{a} ^{b} Raposo, A. P.; Weber, H. J.; Álvarez Castillo, D. E.; Kirchbach, M. (2007). "Romanovski polynomials in selected physics problems". Cent. Eur. J. Phys. 5 (3): 253–284. arXiv:0706.3897. Bibcode:2007CEJPh...5..253R. doi:10.2478/s1153400700185.
 ^ Lesky, P. A. (1996). "Endliche und unendliche Systeme von kontinuierlichen klassischen Orthogonalpolynomen". Z. Angew. Math. Mech. (in German). 76 (3): 181. Bibcode:1996ZaMM...76..181L. doi:10.1002/zamm.19960760317.
 ^ Abramowitz, M.; Stegun, I. (1972). Handbook of Mathematical Functions with Formulas, Graphs and Mathematical Tables (2nd ed.). New York, NY: Dover. ISBN 9780486612720.
 ^ Nikiforov, A. F.; Uvarov, V. B. (1988). Special Functions of Mathematical Physics. Basel: Birkhäuser Verlag.
 ^ Szego, G. (1939). Orthogonal Polynomials. 23. Providence, RI: American Mathematical Society.
 ^ Ismail, M. E. H. (2005). Classical and Quantum Orthogonal Polynomials in One Variable. Cambridge University Press.
 ^ Askey, R. (1987). "An integral of Ramanujan and orthogonal polynomials". J. Indian Math. Soc. 51: 27.
 ^ Askey, R. (1987). "Beta integrals and the associated orthogonal polynomials". Number Theory. Lecture Notes in Math. 1395. Madras/Berlin: Springer. p. 84.
 ^ Zarzo Altarejos, A. (1995). Differential Equations of the Hypergeometric Type (PhD) (in Spanish). Faculty of Science, University of Granada.
 ^ Witte, N. S.; Forrester, P. J. (2000). "Gap probabilities in finite and scaled Cauchy random matrix ensembles". Nonlinearity. 13 (6): 13–1986. arXiv:mathph/0009022. Bibcode:2000Nonli..13.1965W. doi:10.1088/09517715/13/6/305.
 ^ Forrester, P. J. (2010). LogGases and Random Matrices. London Mathematical Society Monographs. Princeton University Press.
 ^ Cotfas, N. (2004). "Systems of orthogonal polynomials defined by hypergeometric type equations with application to quantum mechanics". Cent. Eur. J. Phys. 2 (3): 456–466. arXiv:mathph/0602037. Bibcode:2004CEJPh...2..456C. doi:10.2478/bf02476425.
 ^ Weisstein, Eric W. "Jacobi Differential Equation". MathWorld.
 ^ Kuijlaars, A. B. J.; MartinezFinkelshtein, A.; Orive, R. (2005). "Orthogonality of Jacobi polynomials with general parameters". Electron. Trans. Num. Anal. 19: 1–17. arXiv:math/0301037. Bibcode:2003math......1037K.
 ^ ^{a} ^{b} ^{c} Compean, C. B.; Kirchbach, M. (2006). "The trigonometric Rosen–Morse potential in supersymmetric quantum mechanics and its exact solutions". J. Phys. A: Math. Gen. 39 (3): 547–558. arXiv:quantph/0509055. Bibcode:2006JPhA...39..547C. doi:10.1088/03054470/39/3/007.
 ^ ^{a} ^{b} ^{c} ^{d} ^{e} ^{f} Weber, H. J. (2007). "Connection between Romanovski polynomials and other polynomials". Central European Journal of Mathematics. 5 (3): 581. arXiv:0706.3153. doi:10.2478/s1153300700144.
 ^ Weber, H. J. (2007). "Connections between real polynomial solutions of hypergeometrictype differential equations with Rodrigues formula". Central European Journal of Mathematics. 5 (2): 415–427. arXiv:0706.3003. doi:10.2478/s1153300700046.