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Singular perturbations of abstract wave equations

机译:抽象波动方程的奇摄动

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Given, on the Hilbert space H-0, the self-adjoint operator B and the skew-adjoint operators C-1 and C-2, we consider, on the Hilbert space H similar or equal to D(B) circle plus H-0, the skew-adjoint operator[GRAPHICS]corresponding to the abstract wave equation phi - (C-1 + C-2)phi = - (B-2 + C1C2)phi. Given then an auxiliary Hilbert space h and a linear map tau : D(B-2) -> h with a kernel H dense in H-0, we explicitly construct skew-adjoint operators W-Theta on a Hilbert space H-Theta similar or equal to D(B) circle plus H-0 circle plus h which coincide with W on N similar or equal to K circle plus D D(B). The extension parameter Theta ranges over the set of positive, bounded and injective self-adjoint operators on h.In the case C-1 = C-2 = 0 our construction allows a natural definition of negative (strongly) singular perturbations A(Theta) of A := -B-2 such that the diagram[GRAPHICS]is commutative. (c) 2005 Elsevier Inc. All rights reserved.
机译:给定,在希尔伯特空间H-0上,自伴算子B和斜伴随算子C-1和C-2,我们考虑在希尔伯特空间H上等于或等于D(B)圆加H- 0,对应于抽象波动方程phi-(C-1 + C-2)phi =-(B-2 + C1C2)phi的偏伴随算子[GRAPHICS]。给定一个辅助希尔伯特空间h和一个线性映射tau:D(B-2)-> h,其核H在H-0中密集,我们在希尔伯特空间H-Theta上类似地构造偏向伴随算子W-Theta等于D(B)圈加H-0圈加h,它与N上的W重合,类似于或等于K圈加DD(B)。扩展参数Theta的范围是h上的正,有界和内射自伴随算子集。在C-1 = C-2 = 0的情况下,我们的构造允许自然地定义负(强烈)奇异摄动A(Theta) A:= -B-2的等式使得图[GRAPHICS]是可交换的。 (c)2005 Elsevier Inc.保留所有权利。

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