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Characterizing when divided differences are valid symbols for multiple operator integrals

Determine general, practically checkable conditions on a scalar function f that guarantee its n-th divided difference Dif_n f belongs to the symbol space S((E_0,...,E_n),(T_1,...,T_n);ψ) associated with multiple operator integrals J(·, (E_0,...,E_n), (T_1,...,T_n)) on a separable Hilbert space H. Concretely, for arbitrary tuples of spectral measures (E_0,...,E_n) and operator vectors (T_1,...,T_n) as defined in Definition 2.1, identify sufficient and ideally necessary regularity or integrability assumptions on f ensuring Dif_n f ∈ S((E_0,...,E_n),(T_1,...,T_n);ψ) so that the integral is well-defined, beyond the known sufficient condition that f^(n) has an integrable Fourier transform.

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Background

Multiple operator integrals (MOI) provide a functional calculus for several spectral measures and play a central role in non-commutative Taylor expansions and the construction of higher order spectral shift functions. The MOI J(φ, E, T) requires its symbol φ to belong to a symbol space S(E,T;ψ), characterized by an integral factorization against measurable kernels (Definition 2.1).

In applications, φ is typically the divided difference Dif_n f of a scalar function f. While the paper supplies a widely used sufficient condition—namely, that the n-th derivative fn has an integrable Fourier transform—this does not settle the broader question of finding general, accessible criteria on f that ensure Dif_n f lies in the symbol space for MOI with arbitrary spectral data.

The author notes that, despite considerable development of MOI theory, a general characterization remains out of reach, and points to Peller’s survey for further context. A resolution would streamline assumptions in perturbation theory and broaden the applicability of MOI beyond currently known function classes.

References

A classical question in the theory of multiple operator integrals is under which 'accessible' conditions on f the divided difference Dif_{n}f is a symbol in \mathcal{S}(\mathbf{E},\mathbf{T};\psi). It turns out, that it is surprisingly difficult to answer, and remains in its admittedly vaguely formulated generality unresolved to the knowledge of the author.

Higher order spectral shift of Euclidean Callias operators (2506.01647 - Fürst, 2 Jun 2025) in Section 2 (Construction of higher order spectral shift), paragraph following Lemma Genochi–Hermite (before Proposition on divided differences as symbols)