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In this paper, it is proved that every s-sparse vector xRn can be exactly recovered from the measurement vector z=AxRm via some ?q-minimization with 0<q?1, as soon as each s-sparse vector xRn is uniquely determined by the measurement z. Moreover it is shown that the exponent q in the ?q-minimization can be so chosen to be about 0.6796×(1?δ2s(A)), where δ2s(A) is the restricted isometry constant of order 2s for the measurement matrix A.  相似文献   

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This paper considers optimal solutions of general interval linear programming problems. Necessary and sufficient conditions of (A,b)(A,b)-strong and (A,b,c)(A,b,c)-strong optimal solutions to the interval linear programming with inequality constraints are proposed. The features of the proposed methods are illustrated by some examples.  相似文献   

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We construct an example of a finitely generated ideal I of R[X], where R is a one-dimensional domain, whose leading terms ideal is not finitely generated. This gives a negative answer to the open question of whether if R is a domain with Krull dimension ≤1, then for any finitely generated ideal I of R[X], the leading terms ideal of I is also finitely generated. Moreover, as a positive part of our answer, we prove that for any one-dimensional domain R and any a,bR, the ideal of R[X] generated by the leading terms of 1+aX,b is finitely generated.  相似文献   

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M. Gurtin has proved that the Beltrami representation, S=rotrotA, of a smooth, divergence-free stress tensor in a smooth domain, is verified if and only if S is self-equilibrated. Here, Gurtin's conditions are extended to the case of a bounded domain with a Lipschitz-continuous boundary, for a tensor field SL2(Ω;Msym3). We apply this result to obtain an extension of the Saint Venant's equations of compatibility to non necessarily simply-connected domains. To cite this article: G. Geymonat, F. Krasucki, C. R. Acad. Sci. Paris, Ser. I 342 (2006).  相似文献   

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An original approach of the singular complement method for Maxwell's equations in bounded polygonal domains is presented. A splitting of the electric field à la Moussaoui is proposed: E=ER+λxP, where ERH1(ω)2, λ depends on the data and domain and xP is known explicitly. The same splitting can be used for the magnetic field. No cut-off function is needed and improved error estimates are derived. To cite this article: E. Jamelot, C. R. Acad. Sci. Paris, Ser. I 339 (2004).  相似文献   

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