The Xi Operator and its Relation to Krein's Spectral Shift Function

Abstract

We explore connections between Krein's spectral shift function $ξ(λ,H_0,H)$ associated with the pair of self-adjoint operators $(H_0,H)$, $H=H_0+V$ in a Hilbert space $\calH$ and the recently introduced concept of a spectral shift operator $Ξ(J+K^*(H_0-λ-i0)^{-1}K)$ associated with the operator-valued Herglotz function $J+K^*(H_0-z)^{-1}K$, $\Im(z)>0$ in $\calH$, where $V=KJK^*$ and $J=\sgn(V)$. Our principal results include a new representation for $ξ(λ,H_0,H)$ in terms of an averaged index for the Fredholm pair of self-adjoint spectral projections $(E_{J+A(λ)+tB(λ)}((-\infty,0)),E_J((-\infty,0)))$, $t\in\bbR$, where $A(λ)=\Re(K^*(H_0-λ-i0)^{-1}K)$, $B(λ)=\Im(K^*(H_0-λ-i0)^{-1}K)$ a.e. Moreover, introducing the new concept of a trindex for a pair of operators $(A,P)$ in $\calH$, where $A$ is bounded and $P$ is an orthogonal projection, we prove that $ξ(λ,H_0,H)$ coincides with the trindex associated with the pair $(Ξ(J+K^*(H_0-λ-i0)^{-1}K),Ξ(J))$. In addition, we discuss a variant of the Birman-Krein formula relating the trindex of a pair of $Ξ$-operators and the Fredholm determinant of the abstract scattering matrix. We also provide a generalization of the classical Birman-Schwinger principle, replacing the traditional eigenvalue counting functions by appropriate spectral shift functions.