Singular Integral Operators with Coefficients of a Special Structure Related to Operator Equalities.pdf
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Singular Integral Operators with Coefficients of a Special Structure Related to Operator Equalities
Compl. anal. oper. theory 2 (2008), 549–567
c? 2008 Birkha?user Verlag Basel/Switzerland
1661-8254/040549-19, published online July 15, 2008
DOI 10.1007/s11785-008-0066-x
Complex Analysis
and Operator Theory
Singular Integral Operators with Coefficients of a
Special Structure Related to Operator Equalities
Aleksandr Karelin
Abstract. In our previous works we have constructed operator equalities
which transform scalar singular integral operators with shift to matrix char-
acteristic singular integral operators without shift and found some of their
applications to problems with shift. In this article the operator equalities are
used for the study of matrix characteristic singular integral operators.
Conditions for the invertibility of the singular integral operators with
orientation preserving shift and coefficients with a special structure generated
by piecewise constant functions, t, t?1, were found.
Conditions for the invertibility of the matrix characteristic singular in-
tegral operators with four-valued piecewise constant coefficients of a special
structure were likewise obtained.
Mathematics Subject Classification (2000). Primary 47G10, 45E99, 54F15.
Keywords. Singular integral operator, matrix characteristic operator, piece-
wise constant coefficients, invertibility.
1. Introduction
We denote by [B1, B2] the set of all bounded linear operators mapping the Banach
space B1 into the Banach space B2, [B1] ≡ [B1, B1]. It is known [1, 2] that for
any operator A = X + ZY , where X,Y,Z ∈ [B1] and Z is an involutive operator,
Z2 = I, the Gohberg–Krupnik matrix equality is fulfilled:
H
[
A 0
0 A1
]
H?1 = D ,
where A1 is an additional associated operator, A1 = X ? ZY , and
H =
1√
2
[
I I
Z ?Z
]
, H?1 =
1√
2
[
I Z
I ?Z
]
, D =
[
X ZY Z
Y ZXZ
]
.
550 A. Karelin Comp.an.op.th.
We denote the Cauchy singular integral operator along a contour Γ by
(SΓ?)(t) =
1
πi
∫
Γ
?(τ)
τ ? tdτ
and the identity operator on Γ by (IΓ?)(t) = ?(t).
Suppose that
X = aIΓ + cSΓ , Y = (Zb)IΓ + (Zd)S
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