Integral Operators in Potential Theory

Author(s):  
Josef Král
2010 ◽  
Vol 33 (14) ◽  
pp. 1685-1691 ◽  
Author(s):  
Oleg F. Gerus ◽  
Vladimir N. Kutrunov ◽  
Michael Shapiro

1986 ◽  
Vol 29 (3) ◽  
pp. 405-411 ◽  
Author(s):  
John F. Ahner

In [7] Plemelj established some fundamental results in two- and three-dimensional potential theory about the eigenvalues of both the double layer potential operator and its adjoint, the normal derivative of the single layer potential operator. In [3] Blumenfeld and Mayer established some additional results concerning the eigenvalues of these integral operators in the case of ℝ2. The spectral properties established by Plemelj [7] and by Blumenfeld and Mayer [3] have had a profound effect in the area of integral equation methods in scattering and potential theory in both ℝ2 and ℝ3.


1992 ◽  
Vol 43 (4) ◽  
pp. 387-407 ◽  
Author(s):  
J. M. Anderson ◽  
D. Khavinson ◽  
V. Lomonosov

1993 ◽  
Vol 64 (6) ◽  
pp. 1297-1313 ◽  
Author(s):  
N. V. Grachev ◽  
V. G. Maz'ya

2018 ◽  
Vol 60 (3) ◽  
pp. 610-629
Author(s):  
G. A. Karapetyan ◽  
H. A. Petrosyan
Keyword(s):  

Author(s):  
Brian Street

This chapter turns to a general theory which generalizes and unifies all of the examples in the preceding chapters. A main issue is that the first definition from the trichotomy does not generalize to the multi-parameter situation. To deal with this, strengthened cancellation conditions are introduced. This is done in two different ways, resulting in four total definitions for singular integral operators (the first two use the strengthened cancellation conditions, while the later two are generalizations of the later two parts of the trichotomy). Thus, we obtain four classes of singular integral operators, denoted by A1, A2, A3, and A4. The main theorem of the chapter is A1 = A2 = A3 = A4; i.e., all four of these definitions are equivalent. This leads to many nice properties of these singular integral operators.


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