scholarly journals SOLVABILITY CONDITIONS FOR SOME NON FREDHOLM OPERATORS IN HIGHER DIMENSIONS

2014 ◽  
Vol 7 (3) ◽  
Author(s):  
Vitali Vougalter
Keyword(s):  
Higher Dimensions ◽  
Fredholm Operators ◽  
Solvability Conditions ◽  
Non Fredholm Operators

scholarly journals Solvability conditions for some non-Fredholm operators

2010 ◽  
Vol 54 (1) ◽  
pp. 249-271 ◽  
Author(s):  
Vitali Vougalter ◽  
Vitaly Volpert
Keyword(s):  
Spectral Theory ◽  
Elliptic Equations ◽  
Scattering Theory ◽  
Adjoint Equation ◽  
Fredholm Operators ◽  
Solvability Conditions ◽  
Non Fredholm Operators ◽  
Schrödinger Type Operators

AbstractWe obtain solvability conditions for some elliptic equations involving non-Fredholm operators with the methods of spectral theory and scattering theory for Schrödinger-type operators. One of the main results of the paper concerns solvability conditions for the equation –Δu+V(x)u–au=fwhere a ≥ 0. The conditions are formulated in terms of orthogonality of the functionfto the solutions of the homogeneous adjoint equation.

scholarly journals Solvability conditions for elliptic problems with non-Fredholm operators

2002 ◽  
Vol 29 (2) ◽  
pp. 219-238 ◽  
Author(s):  
V. Volpert ◽  
B. Kaźmierczak ◽  
M. Massot ◽  
Z. Peradzyński
Keyword(s):  
Elliptic Problems ◽  
Fredholm Operators ◽  
Solvability Conditions ◽  
Non Fredholm Operators

scholarly journals Trace formulas for a class of non-Fredholm operators: A review

2016 ◽  
Vol 28 (10) ◽  
pp. 1630002 ◽  
Author(s):  
Alan Carey ◽  
Fritz Gesztesy ◽  
Harald Grosse ◽  
Galina Levitina ◽  
Denis Potapov ◽  
...  
Keyword(s):  
Essential Spectrum ◽  
Trace Formula ◽  
Differential Operators ◽  
Trace Class ◽  
Spectral Shift ◽  
General Situation ◽  
Spectral Flow ◽  
Fredholm Operators ◽  
Type Formula ◽  
Non Fredholm Operators

Take a one-parameter family of self-adjoint Fredholm operators [Formula: see text] on a Hilbert space [Formula: see text], joining endpoints [Formula: see text]. There is a long history of work on the question of whether the spectral flow along this path is given by the index of the operator [Formula: see text] acting in [Formula: see text], where [Formula: see text] denotes the multiplication operator [Formula: see text] for [Formula: see text]. Most results are about the case where the operators [Formula: see text] have compact resolvent. In this article, we review what is known when these operators have some essential spectrum and describe some new results. Using the operators [Formula: see text], [Formula: see text], an abstract trace formula for Fredholm operators with essential spectrum was proved in [23], extending a result of Pushnitski [35], although, still under strong hypotheses on [Formula: see text]: [Formula: see text] where [Formula: see text], [Formula: see text], [Formula: see text]. Associated to the pairs [Formula: see text] and [Formula: see text] are Krein spectral shift functions [Formula: see text] and [Formula: see text], respectively. From the trace formula, it was shown that there is a second, Pushnitski-type, formula: [Formula: see text] This can be employed to establish the desired equality, [Formula: see text] This equality was generalized to non-Fredholm operators in [14] in the form [Formula: see text] replacing the Fredholm index on the left-hand side by the Witten index of [Formula: see text] and [Formula: see text] on the right-hand side by an appropriate arithmetic mean (assuming [Formula: see text] is a right and left Lebesgue point for [Formula: see text] denoted by [Formula: see text] and [Formula: see text], respectively). But this applies only under the restrictive assumption that the endpoint [Formula: see text] is a relatively trace class perturbation of [Formula: see text] (ruling out general differential operators). In addition to reviewing this previous work, we describe in this article some extensions using a [Formula: see text]-dimensional setup, where [Formula: see text] are non-Fredholm differential operators. By a careful analysis we prove, for a class of examples, that the preceding trace formula still holds in this more general situation. Then we prove that the Pushnitski-type formula for spectral shift functions also holds and this then gives the equality of spectral shift functions in the form [Formula: see text] for the [Formula: see text]-dimensional model operator at hand. This shows that neither the relatively trace class perturbation assumption nor the Fredholm assumption are required if one works with spectral shift functions. The results support the view that the spectral shift function should be a replacement for the spectral flow in certain non-Fredholm situations and also point the way to the study of higher-dimensional cases. We discuss the connection with summability questions in Fredholm modules in an appendix.

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