Spectral Averaging and the Krein Spectral Shift
نویسنده
چکیده
We provide a new proof of a theorem of Birman and Solomyak that if A(s) = A0+ sB with B ≥ 0 trace class and dμs(·) = Tr(BEA(s)(·)B), then ∫ 1 0 [dμs(λ)] ds = ξ(λ)dλ where ξ is the Krein spectral shift from A(0) to A(1). Our main point is that this is a simple consequence of the formula: d ds Tr(f(A(s)) = Tr(Bf ′(A(s))). Let A and C = A+B be bounded self-adjoint operators and suppose that B ≥ 0 and B is trace class. Then it is a fundamental result of Krein [5, 6, 7] that there is an L function ξA,C(λ) so that for any C function f (and, in particular, for all f ∈ C∞ 0 (R )), Tr(f(C)− f(A)) = ∫ f ′(λ)ξA,C(λ)dλ. (1) ξ ≥ 0 and is uniquely determined by (1) and the condition that ξ is L. This ξ has compact support (if A,C are bounded). Moreover, if B is finite rank, then 0 ≤ ξA,C(λ) ≤ rank(B) (2) and lim s→∞ [ ξA,A+sB(λ)− ξA,A−sB(λ) ] = rank(B). (3) In 1971, Javrjan [3] proved a remarkable formula for rank(B) = 1: Let B = (φ, · )φ and define dμs(λ) by ∫ edμs(λ) = (φ, eφ) and dη(λ) = ∫ s1 s0 [dμs(·)] ds, the average of the spectral measures for A+ sB. Then, Javrjan’s formula is dη(λ) = ξA+s0B,A+s1B(λ)dλ. (4) ∗ This material is based upon work supported by the National Science Foundation under Grant No. DMS-9401491. The Government has certain rights in this material. To be submitted to Proc. Amer. Math. Soc.
منابع مشابه
Estimates for the spectral shift function of the polyharmonic operator
The Lifshits–Krein spectral shift function is considered for the pair of operators H0 = (−4)l, l > 0 and H = H0 + V in L2(R), d ≥ 1; here V is a multiplication operator. The estimates for this spectral shift function ξ(λ;H,H0) are obtained in terms of the spectral parameter λ > 0 and the integral norms of V . These estimates are in a good agreement with the ones predicted by the classical phase...
متن کاملAn Optimal L-bound on the Krein Spectral Shift Function
and |ξA,B(λ)| ≤ n if A −B is rank n (2) are well known; see, for example, [5] or [6]. The Krein spectral shift function can also be defined for unbounded self-adjoint operators A,B and enjoys the same properties as long as their difference is trace class. The results of this paper extend to general unbounded operators A and B (as long as their difference is trace class) but for simplicity, we w...
متن کاملLarge Amplitude Vibration Analysis of Graphene Sheets as Resonant Mass Sensors Using Mixed Pseudo-Spectral and Integral Quadrature Methods
The present paper investigates the potential application of graphene sheets with attached nanoparticles as resonant sensors by introducing a nonlocal shear deformation plate model. To take into account an elastic connection between the nanoplate and the attached nanoparticle, the nanoparticle is considered as a mass-spring system. Then, a combination of pseudo-spectral and integral quadrature m...
متن کاملAbstractAbstr GRAPH SUBSPACES AND THE SPECTRAL SHIFT FUNCTION
We extend the concept of Lifshits–Krein spectral shift function associated with a pair of self-adjoint operators to the case of pairs of (admissible) operators that are similar to self-adjoint operators. An operator H is called admissible if: (i) there is a bounded operator V with a bounded inverse such that H = V −1 HV for some self-adjoint operator H; (ii) the operators H and H are resolvent ...
متن کامل. SP ] 1 6 Ja n 20 09 HIGHER ORDER SPECTRAL SHIFT , II . UNBOUNDED CASE
Abstract. We construct higher order spectral shift functions, which represent the remainders of Taylor-type approximations for the value of a function at a perturbed self-adjoint operator by derivatives of the function at an initial unbounded operator. In the particular cases of the zero and the first order approximations, the corresponding spectral shift functions have been constructed by M. G...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 1996