Download PDF by Alexander G. Ramm (Eds.): Dynamical Systems Method for Solving Operator Equations

By Alexander G. Ramm (Eds.)

ISBN-10: 0444527958

ISBN-13: 9780444527950

The booklet is of curiosity to graduate scholars in practical research, numerical research, and ill-posed and inverse difficulties in particular. The ebook offers a normal technique for fixing operator equations, specially nonlinear and ill-posed. It calls for a reasonably modest historical past and is basically self-contained. the entire effects are proved within the ebook, and a few of the history fabric is additionally incorporated. the implications provided are as a rule acquired via the writer. - includes a systematic improvement of a unique normal strategy, the dynamical structures approach, DSM for fixing operator equations, specifically nonlinear and ill-posed - Self-contained, appropriate for extensive viewers - can be utilized for varied classes for graduate scholars and partially for undergraduates (especially for RUE sessions)

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Extra info for Dynamical Systems Method for Solving Operator Equations

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Aδ is known, ||Aδ − A|| ≤ δ, and A is unknown. 1. 45) 2. ILL-POSED PROBLEMS 40 where Ta,δ := A∗δ Aδ + aI. 47) solves the equation (Tδ + aI)ua,δ = A∗δ fδ . 48) We have ||Tδ − T || ≤ ||(A∗δ − A∗ )Aδ || + ||A∗ (Aδ − A)|| ≤ 2δ(||A|| + δ). 48) can be written as ua,δ = Ta−1 A∗ +Ta−1 (A∗δ −A∗ )fδ +Ta−1 A∗ (fδ −f )+Ta−1 (A∗ A−A∗δ Aδ )ua,δ . 50) We have ||Ta−1 (A∗ A − A∗δ Aδ )|| ≤ 2δ(||A|| + δ) . 51) Assume that a(δ) satisfies the conditions δ = 0, δ→0 a(δ) lim lim a(δ) = 0. 53) where c is an upper bound of the norm of the operator [I −(A∗ A−A∗δ Aδ )]−1 .

Also a stable estimate of a q ∈ Qa is obtained in [R44] when the noisy data Aδ (α , α) are given, sup |Aδ (α , α) − A(α , α)| ≤ δ. 28) α,α ∈S 2 Recently ([R65]) the author has formulated and solved the following inverse scattering-type problem with fixed k = k0 > 0 and fixed α = α0 data A(β) := A(β, α0 , k0 ), known for all β ∈ S 2 . The problem consists in finding a potential q ∈ L2 (D), such that the corresponding scattering amplitude Aq (β, α0 , k0 ) := A(β) would approximate an arbitrary given function f (β) ∈ L2 (S 2 ) with arbitrary accuracy: ||f (β) − A(β)||L2 (S 2 ) < , where > 0 is an a priori given, arbitrarily small, fixed number.

One has F(ua,δ ) ≤ F(u). 6) Indeed, one can check that F(ua,δ ) ≤ F(ua,δ + v) ∀v ∈ H, and the equation sign is attained if and only if v = 0. Let us choose a = a(δ) so that uδ := ua(δ),δ would satisfy the relation: lim ||uδ − y|| = 0. 7) δ→0 To do so, we estimate: ||Ta−1 A∗ fδ − y|| ≤ ||Ta−1 A∗ (fδ − f )|| + ||Ta−1 A∗ f − y|| := J1 + J2 . 8) Note that 1 ||Ta−1 A∗ || ≤ √ . 9) one uses the commutation formula ∗ Ta−1 A∗ = A∗ Q−1 a , Q := AA . 10) by Qa from the right and by Ta from the left and get an obvious relation: A∗ (AA∗ + aI) = (A∗ A + aI)A∗ .

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Dynamical Systems Method for Solving Operator Equations by Alexander G. Ramm (Eds.)

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