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STABILITY ESTIMATES IN INVERSE SCATTERING
 ACTA APPL.MATH.
, 1992
"... An algorithm is given for calculating the solution to the 3D inverse scattering problem with noisy discrete fixed energy data. The error estimates for the calculated solution are derived. The methods developed are of general nature and can be used in many applications: in nondestructive evaluation a ..."
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Cited by 35 (23 self)
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An algorithm is given for calculating the solution to the 3D inverse scattering problem with noisy discrete fixed energy data. The error estimates for the calculated solution are derived. The methods developed are of general nature and can be used in many applications: in nondestructive evaluation and remote sensing, in geophysical exploration, medical diagnostics and technology.
Stability of the solution to inverse obstacle scattering problem. J. Inverse and Illposed Problems V.2
 J. CHENG, Y. C. HON, AND M. YAMAMOTO
, 1994
"... ..."
Numerical Method for Solving 3D Inverse Problems of Geophysics
, 1988
"... A numerical method is given to invert surface data for the refraction coefficient. ..."
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Cited by 5 (5 self)
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A numerical method is given to invert surface data for the refraction coefficient.
Fixedenergy inverse scattering
, 2008
"... The author’s method for solving inverse scattering problem with fixedenergy data is described. Its comparison with the method based on the DN map is given. A new inversion procedure is formulated. ..."
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Cited by 1 (0 self)
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The author’s method for solving inverse scattering problem with fixedenergy data is described. Its comparison with the method based on the DN map is given. A new inversion procedure is formulated.
325.tex J.Inverse and IllPosed problems 2,N3,(1994),269275. STABILITY OF THE SOLUTION TO INVERSE OBSTACLE SCATTERING PROBLEM
, 2000
"... Abstract. It is proved that if the scattering amplitudes for two obstacles (from a large class of obstacles) differ a little, then the obstacles differ a little, and the rate of convergence is given. An analytical formula for calculating the characteristic function of the obstacle is obtained, given ..."
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Abstract. It is proved that if the scattering amplitudes for two obstacles (from a large class of obstacles) differ a little, then the obstacles differ a little, and the rate of convergence is given. An analytical formula for calculating the characteristic function of the obstacle is obtained, given the scattering amplitude at a fixed frequency. Introduction. Let D ⊂ R 3 be a bounded domain with a smooth boundary Γ, ( ∇ 2 + k 2)u = 0 in D ′: = R 3 \ D, k = const> 0; u = 0 on Γ (1) u = exp(ikα · x) + A(α ′ , α, k)r −1 exp(ikr) + o(r −1), r: = x  → ∞, α ′: = xr −1. (2) Here α ∈ S 2 is a given unit vector, S 2 is the unit sphere in R 3, the function A(α ′ , α, k) is called the
Acta Appl.Math. 28, N1,(1992), 142. STABILITY ESTIMATES IN INVERSE SCATTERING
"... Abstract: An algorithm is given for calculating the solution to the 3D inverse scattering problem with noisy discrete fixed energy data. The error estimates for the calculated solution are derived. The methods developed are of general nature and can be used in many applications: in nondestructive ev ..."
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Abstract: An algorithm is given for calculating the solution to the 3D inverse scattering problem with noisy discrete fixed energy data. The error estimates for the calculated solution are derived. The methods developed are of general nature and can be used in many applications: in nondestructive evaluation and remote sensing, in geophysical exploration, medical diagnostics and technology.
Random Fields Estimation Theory
, 2006
"... This book presents analytic theory of random fields estimation optimal by the criterion of minimum of the variance of the error of the estimate. This theory is a generalization of the classical Wiener theory. Wiener’s theory has been developed for optimal estimation of stationary random processes, t ..."
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This book presents analytic theory of random fields estimation optimal by the criterion of minimum of the variance of the error of the estimate. This theory is a generalization of the classical Wiener theory. Wiener’s theory has been developed for optimal estimation of stationary random processes, that is, random functions of one variable. Random fields are random functions of several variables. Wiener’s theory was based on the analytical solution of the basic integral equation of estimation theory. This equation for estimation of stationary random processes was WienerHopftype of equation, originally on a positive semiaxis. About 25 years later the theory of such equations has been developed for the case of finite intervals. The assumption of stationarity of the processes was vital for the theory. Analytical formulas for optimal estimates (filters) have been obtained under the assumption that the spectral density of the stationary process is a positive rational function. We generalize Wiener’s theory in several directions. First, estimation theory of random fields and not only random processes
Multidimensional Inverse Scattering with FixedEnergy Data
"... In this lecture the author reviews his results on multidimensional inverse scattering. References to the works of other authors can be found in [20]. Five topics are briefly discussed: property C with constraints and new type of the uniqueness theorems ..."
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In this lecture the author reviews his results on multidimensional inverse scattering. References to the works of other authors can be found in [20]. Five topics are briefly discussed: property C with constraints and new type of the uniqueness theorems
Necessary and Sufficient Condition for 2 to Have Property C
, 1989
"... Let Y =x;, z. a, 8 ’ be a formal differential operator with constant coefficients in R”, n 3 2, j is a multiindex. We say that Y has property C iff, for any bounded domain D c R”, the set of products {urr} t(u,w~N,(Y): = {u:Zu=O in D, UEH~(D)} is complete in L’(D). Here H”‘(D) is the Sobolev space. ..."
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Let Y =x;, z. a, 8 ’ be a formal differential operator with constant coefficients in R”, n 3 2, j is a multiindex. We say that Y has property C iff, for any bounded domain D c R”, the set of products {urr} t(u,w~N,(Y): = {u:Zu=O in D, UEH~(D)} is complete in L’(D). Here H”‘(D) is the Sobolev space. A necessary and sutficient condition is given for 4p to have property C. 0 1991 Acadenuc Press, Inc. I.