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Power Quasi Binormal Operator

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Volume 8, Number 2, 2022, Pages 337-342 https://doi.org/10.34198/ejms.8222.337342

Received: December 24, 2021; Accepted: February 12, 2022 2010 Mathematics Subject Classification: 47B20.

Keywords and phrases: normal operator, quasi normal operator, binormal operator, Hilbert space.

-Power Quasi Binormal Operator

Alaa Hussein Mohammed

Department of Mathematics, College of Education, University of Al-Qadisiyah, Diwaniya, Iraq e-mail: [email protected]

Abstract

In this paper we introduce a new class of operators on Hilbert space called -power quasi binormal operator. We study this operator and give some properties of it.

Introduction

Consider ( ) be the algebra of all bounded linear operators on Hilbert space . An operator is called normal if = . Quasi normal operator was introduced by Brown in 1953 [1]. In [3] Campbell introduced the class binormal of operator which is defined as = ∗ ∗ .

In [5] Sid Ahmed generalize quasi normal operator to -power quasi normal operator. In this paper we define a new class of operators on Hilbert space as ( ) = ( ∗ ∗ ) called q-power quasi binormal operator and study some properties of it.

1. Main Results

Definition 1.1. Let be bounded operator. Then is called q-power quasi binormal operator if and only if ( ) = ( ∗ ∗ ) , where is a nonnegative integer.

Proposition 1.2. If S is a self adjoint and q-power quasi binormal operator, then is a q-power quasi binormal operator.

Proof. Since is -power quasi binormal operator, ( ) = ( ∗ ∗ ) .

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Let

( ) (( )∗ ∗ ∗( )) = ( ) ( ∗ ∗ ), since is a self adjoint

= ( ), since is -power quasi binormal

= ( ∗ ∗ ) , since is a self adjoint

= ( ( )( )∗ ∗)( ) . Hence, is -power quasi binormal operator.

Proposition 1.3. If S is a q-power quasi binormal operator, and if exist, then is a q-power quasi binormal operator.

Proof. Since is -power quasi binormal operator, ( ) = ( ∗ ∗ ) . Let

( ) ( ) ( )) = ( ) ( ) ( ) )

= ( ) ( ) ( ) )

= ( ) ( )( )

= ( ) , since is binormal

= ( ∗ ∗ ) ,

since is a -power quasi binormal,

= ( ) , since is binormal

= ( ∗ ∗ )

= ( ∗ ∗ ) ( )

= ( ) ( ) ( )

= ( ) ( ) ( )

= ( )( ) ( ) . Hence, is -power quasi binormal operator.

Definition 1.4 [4]. If , are bounded operator on Hilbert space . Then , are unitary equivalent if there is an isomorphism : → such that = .

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Proposition 1.5. If S is q-power quasi binormal operator and if ∈ ( ) is unitary equivalent to S, then R is q-power quasi binormal operator.

Proof. Since is unitary equivalent to , = , ( ) = and since is -power quasi binormal operator, ( ) = ( ∗ ∗ ) .

Let

( ) = ( ) ( )( )( )( )

= ( ) ( ∗ ∗) ( )( )( ∗ ∗)

= ( ) ,since is -power quasi binormal operator

= ( ∗ ∗ )

= ( )( ∗ ∗)( ∗ ∗)( ) ( ) = ( ∗ ∗ ) . Hence is -power quasi binormal operator.

Theorem 1.6. The set of all q-power quasi binormal operators on H is a closed subset of ( ) under scalar multiplication.

Proof. Let

( ) = ∈ ( ): is -power quasi binormal operator on for some nonnegative integer

Let ∈ ( ), then we have is -power quasi binormal operator and thus ( ) = ( ∗ ∗ ) .

Let ! be a scalar, hence

"! # (! )(! )(! )(! ) = ! !̅ (! )(! ))!̅

= ! !̅!!!% ( )

= ! !̅!!!% ( ∗ ∗ )

= (! )(! )(! )(! ) "! # . Thus ! ∈ ( ).

Let & be a sequence in ( ) and converge to , then we can get that

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‖ ( ) − ( ∗ ∗ ) ‖

= ) ( ) − &( & & & &) + ( & &

&

&) & − ( ∗ ∗ ) )

≤ ) ( ) − &( & & & &)) + )( & &

&

&) & − ( ∗ ∗ ) ) → 0 as / →.

Hence, ( ) = ( ∗ ∗ ) .

Therefore ∈ ( ). Then, ( ) is closed subset.

Theorem 1.7. If 0 and are normal, -power quasi binormal operators on , and let commute with 0, then ( 0) is -power quasi binormal operator on .

Proof. Since T and S are -power quasi binormal operators ( ) = ( ∗ ∗ ) and 0 (0000) = (0000)0 ,

( 0) (( 0)( 0)( 0)( 0)) = (0 ) (0∗ ∗)( 0)( 0)(0∗ ∗)

= (0 ) 0∗ ∗ 0 0 0∗ ∗

= (0 ) 0 0 00

= (0 ) 0∗ ∗0 0∗ ∗0

= (0 ) 00 0 0

= (0 ) 00∗ ∗ 0∗ ∗ 0

= 0 00∗ ∗ 0∗ ∗ 0

= 0 00∗ ∗ 0∗ ∗ 0

= 0 0 0∗ ∗ 0∗ ∗ 0

= 00 0∗ ∗ 0∗ ∗ 0

= ( 0)(0∗ ∗)(0∗ ∗)( 0) (0 )

= (( 0)( 0)( 0)( 0))( 0) . Then ( 0) is -power quasi binormal operator.

Theorem 1.8. Let 0 , 02, … , 0& are q-power quasi binormal operators on H. Then the direct sum ( 0 ⨁02⨁ … ⨁0&) is q-power quasi binormal operator on .

Proof. Since every operator of 0 , 02, … , 0& is -power quasi binormal,

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05 (050505 )

= (05050505)05 for all 6 = 1,2, … , /

= (0 ⨁02⨁ … ⨁0&) (0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)

× (0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)

= ( 0 ⨁02 ⨁ … ⨁0& ) ( 0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)

× (0 ⨁02⨁ … ⨁0&)( 0 ⨁02⨁ … ⨁0&)

= 0 (00 0 0)⨁02 (02020202)⨁ … ⨁0& (0&0&0&0&)

= (0 000 )0 ⨁(02020202)02 ⨁ … ⨁(0&0&0&0&)0&

= (0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)(0 ⨁02⨁ … ⨁0&)

× (0 ⨁02⨁ … ⨁0&)

Thus, (0 ⨁02⨁ … ⨁0&) is -power quasi binormal operator on .

Theorem 1.9. Let 0 , 02, … , 0& are -power quasi binormal operators on . Then the tenser product ( 0 ⨂02⨂ … ⨂0&) is -power quasi binormal operator on .

Proof. Since every operator of , 2, … , & is a -power quasi binormal, 05 (050505 )

= (05050505)05 for all 6 = 1,2, … , /

= (0 ⨂02⨂ … ⨂0&) (0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&)

× (0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&) (;<⨂;=⨂ … ⨂;>)

= ( 0 ⨂02 ⨂ … ⨂0& ) ( 0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&)

× (0 ⨂02⨂ … ⨂0&)( 0 ⨂02⨂ … ⨂0&) (;<⨂;=⨂ … ⨂;>)

= 0 (00 0 0);<⨂02 (02020202);=⨂ … ⨂ 0& (0&0&0&0&);>

= 0 (0 0 0 0 ) ;<⨂ (02020202)02 ;=⨂ … ⨂ (0&0&0&0&)0& ;>

= (0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&)(0 ⨂02⨂ … ⨂0&)

× (0 ⨂02⨂ … ⨂0&) (;<⨂;=⨂ … ⨂;>).

Thus (0 ⨂02⨂ … ⨂0&) is -power quasi binormal operator.

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References

[1] A. Brown, On a class of operators, Proc. Amer. Math. Soc. 4 (1953), 723-728.

https://doi.org/10.1090/S0002-9939-1953-0059483-2

[2] S. K. Berberian, Introduction to Hilbert Space, 2nd ed., Chelsea Publishing Co., New York, 1976.

[3] Stephen L. Campbell, Linear operators for which 00 and 00commute, Proc. Amer.

Math. Soc. 34 (1972), 177-180. https://doi.org/10.2307/2037922

[4] J. B. Conway, A course in functional analysis, Graduate Texts in Mathematics, 96, Springer-Verlag, New York, 1985. https://doi.org/10.1007/978-1-4757-3828-5

[5] Ould Ahmed Mahmoud Sid Ahmed, On the class of n-power quasi-normal operators on Hilbert space, Bull. Math. Anal. Appl. 3(2) (2011), 213-228.

This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted, use, distribution and reproduction in any medium, or format for any purpose, even commercially provided the work is properly cited.

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