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On index theory for non‐Fredholm operators: A (1 + 1)‐dimensional example
Authors:Alan Carey  Fritz Gesztesy  Galina Levitina  Denis Potapov  Fedor Sukochev  Dima Zanin
Affiliation:1. Mathematical Sciences Institute, Australian National University, Kingsley St., Canberra, ACT 0200, Australia and School of Mathematics and Applied Statistics, University of Wollongong, NSW, Australia;2. Department of Mathematics, University of Missouri, Columbia, MO, USA;3. School of Mathematics and Statistics, UNSW, Kensington, NSW, Australia
Abstract:Using the general formalism of 12 , a study of index theory for non‐Fredholm operators was initiated in 9 . Natural examples arise from (1 + 1)‐dimensional differential operators using the model operator urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0001 in urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0002 of the type urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0003, where urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0004, and the family of self‐adjoint operators urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0005 in urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0006 studied here is explicitly given by urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0007 Here urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0008 has to be integrable on urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0009 and urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0010 tends to zero as urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0011 and to 1 as urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0012 (both functions are subject to additional hypotheses). In particular, urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0013, urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0014, has asymptotes (in the norm resolvent sense) urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0015 as urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0016, respectively. The interesting feature is that urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0017 violates the relative trace class condition introduced in 9 , Hypothesis 2.1 urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0018]. A new approach adapted to differential operators of this kind is given here using an approximation technique. The approximants do fit the framework of 9 enabling the following results to be obtained. Introducing urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0019, urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0020, we recall that the resolvent regularized Witten index of urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0021, denoted by urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0022, is defined by urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0023 whenever this limit exists. In the concrete example at hand, we prove urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0024 Here urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0025 denotes the spectral shift operator for the pair of self‐adjoint operators urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0026, and we employ the normalization, urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0027, urn:x-wiley:0025584X:media:mana201500065:mana201500065-math-0028.
Keywords:Fredholm and Witten index  spectral shift function  Primary: 47A53  58J30  Secondary: 47A10  47A40
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