8,213 research outputs found

    Third Order Trace Formula

    Full text link
    In (J. Funct. Anal. 257, 1092-1132 (2009)), Dykema and Skripka showed the existence of higher order spectral shift functions when the unperturbed self-adjoint operator is bounded and the perturbations is Hilbert-Schmidt. In this article, we give a different proof for the existence of spectral shift function for the third order when the unperturbed operator is self-adjoint (bounded or unbounded, but bounded below).Comment: 26 page

    Inner multipliers and Rudin type invariant subspaces

    Full text link
    Let E\mathcal{E} be a Hilbert space and HE2(D)H^2_{\mathcal{E}}(\mathbb{D}) be the E\mathcal{E}-valued Hardy space over the unit disc D\mathbb{D} in C\mathbb{C}. The well known Beurling-Lax-Halmos theorem states that every shift invariant subspace of HE2(D)H^2_{\mathcal{E}}(\mathbb{D}) other than {0}\{0\} has the form ΘHE2(D)\Theta H^2_{\mathcal{E}_*}(\mathbb{D}), where Θ\Theta is an operator-valued inner multiplier in HB(E,E)(D)H^\infty_{B(\mathcal{E}_*, \mathcal{E})}(\mathbb{D}) for some Hilbert space E\mathcal{E}_*. In this paper we identify H2(Dn)H^2(\mathbb{D}^n) with H2(Dn1)H^2(\mathbb{D}^{n-1})-valued Hardy space HH2(Dn1)2(D)H^2_{H^2(\mathbb{D}^{n-1})}(\mathbb{D}) and classify all such inner multiplier ΘHB(H2(Dn1))(D)\Theta \in H^\infty_{\mathcal{B}(H^2(\mathbb{D}^{n-1}))}(\mathbb{D}) for which ΘHH2(Dn1)2(D)\Theta H^2_{H^2(\mathbb{D}^{n-1})}(\mathbb{D}) is a Rudin type invariant subspace of H2(Dn)H^2(\mathbb{D}^n).Comment: 8 page
    corecore