By Juan M. Delgado Sanchez, Tomas Dominguez Benavides

This quantity contains a suite of articles via prime researchers in mathematical research. It offers the reader with an in depth review of the present-day learn in numerous components of mathematical research (complex variable, harmonic research, actual research and useful research) that holds nice promise for present and destiny advancements. those overview articles are hugely valuable when you are looking to find out about those issues, as many effects scattered within the literature are mirrored in the course of the many separate papers featured herein.

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Blasco, M. Carro and A. Gillespie, Discretization versus transference for bilinear operators, (2008), to appear. 4. O. Blasco, M. Carro and A. Gillespie, Bilinear Hilbert transform on measure spaces, J. Fourier Anal. and Appl. 11 (2005), 459–470. 5. O. Blasco and F. Villarroya, Transference of bilinear multipliers on Lorentz spaces, Illinois J. Math. 47(4) (2005), 1327–1343. 6. R. R. Coifman and Y. Meyer, Fourier Analysis of multilinear convolution, Calder´ on theorem and analysis of Lipschitz curves, Euclidean Harmonic Analysis (Proc.

Hj−1 ) , (22) λj − λ where Xj is a polynomial. In particular, hj depends only on λ, a2 , . . , aj . hj = The formal power series linearizing f is not converging if its coefficients grow too fast. Thus, (22) links the radius of convergence of h to the behaviour of λj − λ: if the latter becomes too small, the series defining h does not converge. This is known as the small denominators problem in this context. It is then natural to introduce the following quantity: Ωλ (m) = min |λk − 1| 1≤k≤m 1 for λ ∈ S and m ≥ 1.

Write, for each v ∈ R, TK (f, g) = Sv−1 Sv R = Sv−1 R = Sv−1 R−u f Ru gK(u)du Sv (R−u f Ru g)K(u)du (Rv−u f )(Rv+u g)K(u)du R Hence p3 TK (f, g) p3 Lp3 (µ) ≤ (Rv−u f )(Rv+u g)K(u)du R . Lp3 (µ) Given N ∈ N, integrating over v ∈ [−N, N ], 2N TK (f, g) p3 Lp3 (µ) p3 N ≤ dm(v). (Rv−u f )(Rv+u g)K(u)du −N R Lp3 (µ) May 6, 2008 15:45 36 WSPC - Proceedings Trim Size: 9in x 6in ws-procs9x6 O. Blasco Therefore 2N TK (f, g) p3 Lp3 (µ) N A −N −A = p3 N ≤ −N Ω R p3 dv Rv−u f (w)Rv+u g(w)K(u)du Ω dµ(w) BK (Ru f (w)χ[−A−N,A+N ] , Ru g(w)χ[−A−N,A+N ])(v) = Ω dµ(w)dv Rv−u f (w)Rv+u g(w)K(u)du p3 dv R × dµ(w) = BK (Ru f (w)χ[−A−N,A+N ], Ru g(w)χ[−A−N,A+N ] ) Ω ≤ Np1 ,p2 (BK )p3 Ru f (w)χ[−A−N,A+N ] Ω × = Np1 ,p2 (BK ) p3 Ru g(w)χ[−A−N,A+N ] Ω Ru f p1 Lp1 (µ) = Np1 ,p2 (BK ) Ru g −(A+N ) p2 Lp2 (R) p3 /p2 dµ(w) du p2 Lp2 (µ) du p3 /p1 A+N f −(A+N ) p1 Lp1 (µ) p2 Lp2 (µ) g −(A+N ) ≤ Np1 ,p2 (BK )p3 (2(A + N )) f du p3 /p2 A+N × p3 /p1 dµ(w) p3 /p2 A+N × dµ(w) p3 /p1 A+N −(A+N ) p3 p1 Lp1 (R) p3 Lp3 (R) p3 Lp1 (µ) g du p3 Lp2 (µ) .