Abstract
For operators on a compact manifold X with boundary ∂X, the basic zeta coefficient C 0(B, P 1,T ) is the regular value at s = 0 of the zeta function \({Tr(B P_{1,T}^{-s})}\) , where B = P + + G is a pseudodifferential boundary operator (in the Boutet de Monvel calculus)—for example the solution operator of a classical elliptic problem—and P 1,T is a realization of an elliptic differential operator P 1, having a ray free of eigenvalues. Relative formulas (e.g., for the difference between the constants with two different choices of P 1,T ) have been known for some time and are local. We here determine C 0(B, P 1,T ) itself (with even-order P 1), showing how it is put together of local residue-type integrals (generalizing the noncommutative residues of Wodzicki, Guillemin, Fedosov–Golse–Leichtnam–Schrohe) and global canonical trace-type integrals (generalizing the canonical trace of Kontsevich and Vishik, formed of Hadamard finite parts). Our formula generalizes a formula shown recently by Paycha and Scott for manifolds without boundary. It leads in particular to new definitions of noncommutative residues of expressions involving log P 1,T . Since the complex powers of P 1,T lie far outside the Boutet de Monvel calculus, the standard consideration of holomorphic families is not really useful here; instead we have developed a resolvent parametric method, where results from our calculus of parameter-dependent boundary operators can be used.
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Grubb, G. The local and global parts of the basic zeta coefficient for operators on manifolds with boundary. Math. Ann. 341, 735–788 (2008). https://doi.org/10.1007/s00208-008-0211-x
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DOI: https://doi.org/10.1007/s00208-008-0211-x