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Spectrum of the Real Part of a Weighted Shift Operator
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by Stephen Crowley

January 21, 2024

1  Introduction

This document presents an overview of the spectrum of the real part of a
weighted shift operator and explains why it is equal to the closed
interval [-1,1]. The explanation is grounded in the principles of
functional analysis and operator theory.
2  Preliminaries

2.1  Weighted Shift Operator

A weighted shift operator, denoted as T, is a type of linear operator
acting on a Hilbert space H. It shifts the elements of a sequence or a
function space and multiplies each element by a corresponding weight.
The spectral properties of this operator are significantly influenced by
these weights.
2.2  Spectrum of an Operator

The spectrum of a linear operator T, denoted by σ(T), comprises the set
of complex numbers λ for which T-λ*I is not invertible, where I is the
identity operator. The spectrum includes eigenvalues and other values
where the operator is not invertible.
2.3  Real Part of an Operator

The real part of an operator T, denoted as ℜ(T), is given by
1/2*(T+T^∗), where T^∗ is the adjoint of T. This operator is
self-adjoint, even if T itself is not.
3  Spectrum of the Real Part of a Weighted Shift Operator

The statement in question is that the spectrum of the real part of a
weighted shift operator is the closed interval [-1,1]. This can be
understood through the following considerations:
•  The weights of the shift operator, bounded by 1 in absolute value,
limit the operator norms of T and T^∗ to 1.
•  The real part of T combines T and T^∗ and inherits their spectral
characteristics.
•  Consequently, the spectrum of the real part lies within [-1,1], as
the operator norms are bounded and the spectrum of a self-adjoint
operator is always within the interval defined by its norm.
4  Conclusion

The spectrum of the real part of a weighted shift operator being within
the interval [-1,1] is a result derived from the bounded nature of the
operator and its adjoint, as well as the spectral theorem for
self-adjoint operators. This theorem asserts that a self-adjoint
operator on a Hilbert space has a real spectrum, comprising eigenvalues
or continuous spectrum intervals, which in this case is the interval
[-1,1].[1]
Bibliography
[1]  J. DOMBROWSKI. Spectral properties of real parts of weighted shift
operators. Indiana University Mathematics Journal, 29(2):249–259, 1980.
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<doc-data|<doc-title|Spectrum of the Real Part of a Weighted Shift
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<section|Introduction>

This document presents an overview of the spectrum of the real part of a
weighted shift operator and explains why it is equal to the closed interval
<math|<around|[|-1,1|]>>. The explanation is grounded in the principles of
functional analysis and operator theory.

<section|Preliminaries>

<subsection|Weighted Shift Operator>

A weighted shift operator, denoted as <math|T>, is a type of linear
operator acting on a Hilbert space <math|H>. It shifts the elements of a
sequence or a function space and multiplies each element by a corresponding
weight. The spectral properties of this operator are significantly
influenced by these weights.

<subsection|Spectrum of an Operator>

The spectrum of a linear operator <math|T>, denoted by
<math|\<sigma\><around|(|T|)>>, comprises the set of complex numbers
<math|\<lambda\>> for which <math|T-\<lambda\>*I> is not invertible, where
<math|I> is the identity operator. The spectrum includes eigenvalues and
other values where the operator is not invertible.

<subsection|Real Part of an Operator>

The real part of an operator <math|T>, denoted as
<math|\<Re\><around|(|T|)>>, is given by
<math|<frac|1|2>*<around|(|T+T<rsup|\<ast\>>|)>>, where
<math|T<rsup|\<ast\>>> is the adjoint of <math|T>. This operator is
self-adjoint, even if <math|T> itself is not.

<section|Spectrum of the Real Part of a Weighted Shift Operator>

The statement in question is that the spectrum of the real part of a
weighted shift operator is the closed interval <math|<around|[|-1,1|]>>.
This can be understood through the following considerations:

<\itemize>
<item>The weights of the shift operator, bounded by 1 in absolute value,
limit the operator norms of <math|T> and <math|T<rsup|\<ast\>>> to 1.

<item>The real part of <math|T> combines <math|T> and
<math|T<rsup|\<ast\>>> and inherits their spectral characteristics.

<item>Consequently, the spectrum of the real part lies within
<math|<around|[|-1,1|]>>, as the operator norms are bounded and the
spectrum of a self-adjoint operator is always within the interval defined
by its norm.
</itemize>

<section|Conclusion>

The spectrum of the real part of a weighted shift operator being within the
interval <math|<around|[|-1,1|]>> is a result derived from the bounded
nature of the operator and its adjoint, as well as the spectral theorem for
self-adjoint operators. This theorem asserts that a self-adjoint operator
on a Hilbert space has a real spectrum, comprising eigenvalues or
continuous spectrum intervals, which in this case is the interval
<math|<around|[|-1,1|]>>.<cite|RealWeightedShiftOperatorSpectra>

<\bibliography|bib|tm-plain|refs>
<\bib-list|1>
<bibitem*|1><label|bib-RealWeightedShiftOperatorSpectra>J.<nbsp>DOMBROWSKI.
<newblock>Spectral properties of real parts of weighted shift
operators. <newblock><with|font-shape|italic|Indiana University
Mathematics Journal>, 29(2):249\U259, 1980.<newblock>
</bib-list>
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<vspace*|1fn><with|font-series|<quote|bold>|math-font-series|<quote|bold>|4<space|2spc>Conclusion>
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2 changes: 1 addition & 1 deletion docs/refs.bib
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lccn = {86010167},
url = {https://books.google.com/books?id=HaAZAQAAIAAJ},
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@article{c4864bb7-afee-3559-82e7-373ab33458a1,
@article{RealWeightedShiftOperatorSpectra,
ISSN = {00222518, 19435258},
URL = {http://www.jstor.org/stable/24892893},
author = {J. DOMBROWSKI},
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