Exact(1)
In Theorem 2.1, we have constructed the function (H x)), (x> 2 ), and used it to derive the main integral equation by the scattering data (3.13).
Similar(59)
We construct the function f ( z ) θ 3 ( z | τ ).
Inverse Problem 3 Given the Weyl function M , construct the function q ( x ).
Using the solution of the main equation, one can construct the function q ( x ).
Now, let us construct the function S ( x, λ ) by (3) and the function Ω ( x ) by (4).
Inverse Problem 2 Given the spectra { λ n } n ≥ 1, { μ n } n ≥ 0, construct the function q ( x ).
To construct the function f 1, it is sufficient to consider the sequences b = { 1 ( | m | + 1 ) ? 1 } m ?
Using this solution, we construct the function v ( x ) which will satisfy all the conditions of problem (17 - 18).
Using the data, we construct the function f(t) according to Eq. (7) and analyze it with the wavelet transform (Eq. 5).
In the case thatXdoes not have finite cotype we can construct the function with the additional property of being analytic, in the sense that its Fourier coefficients of negative frequency are null.
Using Definition 1, construct the function (Psi z)=psi (z -frac{z -frac{!}sigma_{n}) in such a way that the function Ψ is n-concave on ([delta_{1},c]) and n-convex on ([c,delta_{2}]).
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