By Abul Hasan Siddiqi

Consultant covers the most up-tp-date analytical and numerical tools in infinite-dimensional areas, introducing fresh ends up in wavelet research as utilized in partial differential equations and sign and photo processing. For researchers and practitioners. comprises index and references.

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H d . h . PI P2 III t e secon term gIve t e equatIOn 36(n - 2j)(n - 2j + l)bj + 4(3j + 8 + 2)(3n + 12(n - 2j)aj = 0, 3j + 301 + 6 + l)bi +I (4) h-Harmonic Polynomials, h-Hankel Transform, ... 41 where 0:::; j :::; [(n-1)/2]. We set 8 = -1 in (3) and (4). "( n _ 2J. b. (n-2j+1)! 4 of [371]. "( n + l)n-i _ 2J. ')' b. (n-2j+1)! ' and this gives the h-harmonic polynomial P3n+5(Z) = Z2 r3n+3C::t: (cos 9) - zr 3nH C::+ I(cos 39) = z2c~~il,a)(z3), n ~ -1, (6) of degree 3n + 5. The conjugates of the polynomials (5) and (6) are also h-harmonic.

The operators Tt. We can consider on h-harmonic polynomials the scalar product of the space ,r}(sn-I, h 2 dw). Therefore, we have the operator T;* which is adjoint to the operator T i . Since Tif)f C f)f+1 then T;* f)f C f)f-1. The aim of this section is to prove the formula Ttp(x) = (n + 2r + 21') [XiP(X) - (n + 2r + 21' - 2)-1 IxI2TiP(X)] , where P E f)~ and l' P E f)~, = 0'1 + ... + am. To prove this formula we first show that for + 2TiP(X), (2) 2)-1IxI 2Tip(X) E f)~+I. (3) ~h(XiP(X)) = Xi~hP(X) XiP(X) - (n By the product rules for ~ ~ + 2r + 21' - and \7 we have ~h(XiP(X)) = Xi~p(X) apeX) + 2~ .

Ft + (VFt, VF2 ))dx, (2) n where F I ,F2 E C 2 (n). (hh) n + (V(hh), V(fz h))] dx. (3) Chapter 1. 22 If Fl = h 1 ,F2 = fthh in (2), then we get j fth ~~ hdp, = an j [fd2hflh + (V(Jd2h), Vh)]dx. (4) n Subtracting equation (4) from equation (3) after some transformations we obtain the relation j h ~ h 2dp, = an j[hh(fl(fth) - ftflh) + h2(Vft, Vfz)]dx n which leads to formula (1). Lemma is proved. Theorem 1. If PI E f)~'P2 E f)~ and r j f:. k, then pl(X)p2(X)h(x)2dw = o. (5) S,",-1 Proof By using formula (1), the fact that the operator Dh is symmetric, and the formula 1 en j f(x)dx = j r,,-ldr j B 0 f(rx)dw(x), sn-l we obtain (degpl - degp2) j PIP2h2dw = en j(P2LhPl - PILhP2)h2dx B sn-l = en j (P2DhPl - PI DhP2)h 2dx = O.