dilations, models, scattering and spectral problems of 1d discrete hamiltonian systems
نویسندگان
چکیده
in this paper, the maximal dissipative extensions of a symmetric singular 1d discrete hamiltonian operator with maximal deficiency indices (2,2) (in limit-circle cases at ±∞) and acting in the hilbert space ℓ_{ω}²(z;c²) (z:={0,±1,±2,...}) are considered. we consider two classes dissipative operators with separated boundary conditions both at -∞ and ∞. for each of these cases we establish a selfadjoint dilation of the dissipative operator and construct the incoming and outgoing spectral representations that makes it possible to determine the scattering function (matrix) of the dilation. further a functional model of the dissipative operator and its characteristic function in terms of the weyl function of a selfadjoint operator are constructed. finally we show that the system of root vectors of the dissipative operators are complete in the hilbert space ℓ_{ω}²(z;c²).
منابع مشابه
Dilations, models, scattering and spectral problems of 1D discrete Hamiltonian systems
In this paper, the maximal dissipative extensions of a symmetric singular 1D discrete Hamiltonian operator with maximal deficiency indices (2,2) (in limit-circle cases at ±∞) and acting in the Hilbert space ℓ_{Ω}²(Z;C²) (Z:={0,±1,±2,...}) are considered. We consider two classes dissipative operators with separated boundary conditions both at -∞ and ∞. For each of these cases we establish a self...
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Proof. It would be easy to obtain these properties from the matrix form of U constructed in Sec. I.5.2, but we prefer to give a direct proof, independent of the particular realization of U . Part (i): To prove that L and L∗ are wandering subspaces, it suffices to show that UL0 ⊥L0 and UL0 ⊥ L0 for n = 1,2, . . .; by reason of symmetry it even suffices to consider one of these cases, say that of...
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Proof. It would be easy to obtain these properties from the matrix form of U constructed in Sec. I.5.2, but we prefer to give a direct proof, independent of the particular realization of U . Part (i): To prove that L and L∗ are wandering subspaces, it suffices to show that UL0 ⊥L0 and UL0 ⊥ L0 for n = 1,2, . . .; by reason of symmetry it even suffices to consider one of these cases, say that of...
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Proof. It would be easy to obtain these properties from the matrix form of U constructed in Sec. I.5.2, but we prefer to give a direct proof, independent of the particular realization of U . Part (i): To prove that L and L∗ are wandering subspaces, it suffices to show that UL0 ⊥L0 and UL0 ⊥ L0 for n = 1,2, . . .; by reason of symmetry it even suffices to consider one of these cases, say that of...
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عنوان ژورنال:
bulletin of the iranian mathematical societyجلد ۴۰، شماره ۶، صفحات ۱۵۵۳-۱۵۷۱
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