亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Additive Maps Preserving the Star Partial Order onB(H)

        2015-02-13 06:59:50XICUIANDJIGUoXING

        XI CUI AND JI GUo-XING

        (College of Mathematics and Information Science,Shaanxi Normal University,Xi’an,710062)

        Communicated by Ji You-qing

        Additive Maps Preserving the Star Partial Order onB(H)

        XI CUI AND JI GUo-XING*

        (College of Mathematics and Information Science,Shaanxi Normal University,Xi’an,710062)

        Communicated by Ji You-qing

        LetB(H)be theC?-algebra of all bounded linear operators on a complex Hilbert spaceH.It is proved that an additive surjective mapφonB(H)preserving the star partial order in both directions if and only if one of the following assertions holds.(1)There exist a nonzero complex numberαand two unitary operatorsUandVonHsuch thatφ(X)=αUXVorφ(X)=αUX?Vfor allX∈B(H).(2) There exist a nonzeroαand two anti-unitary operatorsUandVonHsuch thatφ(X)=αUXVorφ(X)=αUX?Vfor allX∈B(H).

        linear operator,star partial order,additive map

        1 Introduction

        In the last few decades,many researchers have studied properties of various partial orders on matrix algebras,or operator algebras acting on a complex infnite dimensional Hilbert space,such as minus partial order,star partial order,left and right star partial order and so on(see[1-6]).One of the orders on the algebraMnof alln×ncomplex matrices is the star partial orderdefned by Drazin in[5].LetA,B∈Mn.Then we say thatandWe note that this defnition can be extended to aC?-algebra by the same way.In particular,it can be extended to theC?-algebraB(H)of all bounded linear operators on a complex Hilbert spaceH.For example,motivated byˇSemrl’s approach presented in[7]for minus partial order,Dolinar and Marovt[4]gave an equivalentdefnition(see Defnition 2 in[4])of the star partial order and considered some properties of this partial order.We can refer[1,4]to see more interesting properties.

        On the other hand,as partially ordered algebraic structures onMnandB(H),what are the automorphisms ofMnandB(H)with respect to those partial orders?These topics have been studied and some interesting results have been obtained.ˇSemrl[7]described the structure of corresponding automorphisms for the minus partial order.For the star partial order,Guterman[8]characterized linear bijective maps onMnpreserving the star partial order and Legiˇsa[9]considered automorphisms ofMnwith respect to the star partial order. Recently,several authors consider the automorphisms of certain subspaces ofB(H)with respect to the star partial order whenHis infnite dimensional.Dolinar and Guterman[10]studied the automorphisms of the algebraK(H)of compact operators on a separable complex Hilbert spaceHand they characterized the bijective,additive,continuous maps onK(H) which preserve the star partial order in both directions.On the other hand,characterizations of certain continuous bijections on the normal elements of a von Neumann algebra preserving the star partial order in both directions are obtained by Bohata and Hamhalter[11].In this paper,we consider additive surjective maps preserving the star partial order in both directions onB(H)and characterizations of those maps are given.In particular,we improve the main result in[10].

        LetHbe a complex Hilbert space and denote by dimHthe dimension ofH.Let C and Q denote the complex feld and the rational number feld,respectively.LetB(H),K(H) andF(H)be the algebras of all bounded linear operators,the compact operators and the fnite rank operators onH,respectively.For every pair of vectorsx,y∈H,〈x,y〉denotes the inner product ofxandy,andx?ystands for the rank-1 linear operator onHdefned by(x?y)z=〈z,y〉xfor anyz∈H.Ifxis a unit vector,thenx?xis a rank-1 projection.σ(A)is the spectrum ofAfor anyA∈B(H).For a subsetSofH,[S]denotes the closed subspace ofHspanned bySandPMdenotes the orthogonal projection onMfor a closed subspaceMofH.We denote byR(T)andN(T)the range and the kernel of a linear mapTbetween two linear spaces.Throughout this paper,we generally denote byIthe identity operator on a Hilbert space.

        2 Additive Maps Preserving the Star Partial Order

        Letφbe an additive map onB(H).We say thatφpreserves the star partial order iffor anyA,B∈B(H)such thatWe say thatφpreserves the star partial order in both directions ifif and only iffor anyA,B∈B(H). We frstly give the following lemma which generalizes Lemma 10 in[10].

        LetT∈B(H).We denote by

        respectively.Then

        and

        with respect to the orthogonal decompositions(2.1),whereT0∈B(H1,K1)is an injective operator with dense range.

        Lemma 2.1LetT∈B(H)be a nonzero operator.ThenTis of rank-1if and only if for any operatorSwithwe haveS=0orS=T.

        PutU1=U|E(Δ)H1,A1=E(Δ)A,U2=U|(I-E(Δ))H1andA2=(I-E(Δ))AonH1, respectively.Then

        according to(2.3).Let

        Theorem 2.1Let φ be an additive surjective map on B(H).Then φ preserves the star partial order in both directions if and only if one of the following assertions hold:

        (1)There exist a nonzero α∈Cand two unitary operatorsUandVon H such that φ(X)=αUXVor φ(X)=αUX?Vfor allX∈B(H);

        (2)There exist a nonzero α∈Cand two anti-unitary operatorsUandVon H such that φ(X)=αUXVor φ(X)=αUX?Vfor allX∈B(H).

        Proof.The sufciency is clear.We only need prove the necessity.It is clear thatφis injective.Thenφ-1preserves the star partial order too.We complete the proof by several steps.

        Step 1.φpreserves rank-noperators in both directions.

        LetAbe a rank-1 operator andφ(A)=B.Suppose that rankB≥2.Then there is a nonzeroB1∈B(H)such thatB1?≤BandB1/=Bby Lemma 2.1.PutA1=φ-1(B1).

        ThusBis of rank-1.It follows thatφpreserves rank-1 operators in both directions.Since a rank-noperator is the sum ofnrank-1 operators,it is elementary thatφpreserves rank-noperators in both directions.

        Step 2.Letf,g∈Handφ(f?g)=u?v.Then

        In fact,for anyx∈{f}⊥,y∈{g}⊥,we have

        Letφ(x?y)=ξ?η.Then

        which implies that

        The converse is the same sinceφpreserves the star partial order in both directions.

        Step 3.For any unit vectorsMoreover,iff⊥g, then

        LetandBy Step 2,ξ1⊥ξ2andη1⊥η2. Without loss of generality,we may assume that

        PutUandVbe two unitary operators onHsuch that

        Letψ=UφV?.Thenψpreserves the star partial order in both directions such that

        and

        Thenψpreserves rank-1 operators in both directions.LetNote that bothandare of rank-1.Then eitherf(resp.g)andξ3orf(resp.g)andη3are linearly dependent.We assume that

        We thus have

        Put

        ThenE(r)is a projection and

        Of course,

        It follows that

        Then

        Thus

        If dimH=2,then for any unit vectorx∈Hwe have

        Thus we haveψ(x?x)is a projection and

        Assume that dimH>2.For any unit vectorsfandg,take any unit vectoThen

        We next assume that‖φ(f?f)‖=1 for any unit vectorf∈Hwithout loss of generality.

        Step 4.Let{eλ:λ∈Λ}be an orthonormal basis ofH.Then there are two orthonormal bases{fλ:λ∈Λ}and{gλ:λ∈Λ}such that

        If(2.4)holds,then both{fλ:λ∈Λ}and{gλ:λ∈Λ}are orthonormal families ofH.If there is a unit vectorf∈Hsuch thatf⊥fλfor allλ∈Λ,thenφ-1(f?gλ0)=x0?y0is a rank-1 operator.By Step 2,eλ∈{x0}⊥.This is a contradiction.Thus both{fλ:λ∈Λ}and{gλ:λ∈Λ}are bases ofH.

        Step 5.φis linear or conjugate linear onF(H).

        As in Step 4,let{eλ:λ∈Λ}be an orthonormal basis ofH.LetUandVbe two unitary operators onHsuch thatU1fλ=eλandV1gλ=eλfor anyλ∈Λ.Put

        Thenφ1preserves the star partial order in both directions such that

        For anyn∈N+and{eλi:1≤i≤n}?{eλ:λ∈Λ},denote

        We conclude that

        by the similar way as Step 4 of[10].In fact,it easily follows thatφ1(Q)=Q,whereQis the projection onto{eλ:λ∈S}for any subsetS?Λ.For anyA∈PnB(H)Pn,we know that

        Then

        It follows thatby a simple calculation.PnB(H)Pncan be identifed withMn.Socan be considered as a bijective,additive map onMn,which preserves the star partial order in both directions.It follows from Theorem 3.1 in[12] thatis linear or conjugate linear.We note that ifis linear(resp. conjugate linear)for somek≥2,thenis also linear(resp.conjugate linear)for anyn.This implies that ifis linear(resp.conjugate linear)for somek≥2,thenis linear(resp.conjugate linear)for anyn.We now assume thatis linear for somek≥2.LetLetMbe the subspace generated by

        ThenMis fnite dimensional with an orthonormal basis{hj:1≤j≤m}containingIt now follows thatis linear by preceding proof since

        Thusφis linear onF(H).

        Ifis conjugate linear for somek≥2,thenφis conjugate linear onF(H).

        We now next assume thatφis linear onF(H).Thenφis a rank preserving linear bijection onF(H).It follows from Theorem 2.1.6 in[13]that the following statements hold.

        (1)There exist two linear mapsAandConHsuch that for allx,y∈H,

        (2)There exist two conjugate linear mapsAandConH,such that for allx,y∈H,

        Note that bothAandCare invertible sinceφis bijective onF(H).Assume that(1) holds.Then for any unit vectorse,f∈Hsuch that〈e,f〉=0,we have that

        by Step 2.Note that(e+f)⊥(e-f).It follows that

        If dimH=2,then for any unit vectorx∈H,we havex=αe+βffor some constantsα,β∈C with|α|2+|β|2=1.We easily have that

        by an elementary calculus.If dimH>2,then for any unit vectorsx,y∈H,there is a unit vectorz∈{x,y}⊥.It now follows that

        Put

        Then?is an additive bijection onB(H)preserving the star partial order in both directions such that

        Now letP∈B(H)be any projection.Then for any fnite rank projectionQ,ifQ≤P,we have

        Then

        Noting that{λQ:Q≤P}is a?-increasing net and?-bounded from above such that

        in strong operator topology,by Proposition 3.5 in[1],we have

        We note that the?-increasing and?-bounded sequences are considered in this proposition. However,the proposition still holds if we replaces a sequence by a net.By considering?-1, we have

        Then?(X)=Xfor allX∈B(H)sinceXis a linear combination of fnitely many projections from Theorem 3 in[14].Thus

        If(2)holds,then there are two anti-unitary operatorsUandVsuch that

        Ifφis conjugate linear onF(H),then we similarly have two unitary operatorsUandVonHsuch that

        or two anti-unitary operatorsUandVonHsuch that

        The proof is completed.

        The following corollary is a generalization of the main result in[10].

        Corollary 2.1Let φ be an additive surjective map on K(H).Then φ preserves the star partial order in both directions if and only if one of the following holds:

        (1)There exist a nonzero α∈Cand two unitary operatorsUandVon H such that

        or

        (2)There exist a nonzero α∈Cand two anti-unitary operatorsUandVon H such that

        or

        [1]Antezana J,Cano C,Mosconi I,StojanofD.A note on the star order in Hilbert spaces.Linear Multilinear Algebra,2010,58(8):1037-1051.

        [2]Baksalary J K,Mitra S K.Left-star and right-star partial orderings.Linear Algebra Appl., 1991,149:73-89.

        [3]Baksalary J K,Pukelsheim F.On the L¨owner,minus and star partial ordering of nonnegative defnite matrices and their squares.Linear Algebra Appl.,1991,151:135-141.

        [4]Dolinar G,Marovt J.Star partial order onB(H).Linear Algebra Appl.,2011,434:319-326.

        [5]Drazin M P.Natural structures on semigroups with involution.Bull.Amer.Math.Soc.,1987,84:139-141.

        [6]Hartwig R E,Drazin M P.Lattice properties of the?-order for complex matrices.J.Math. Anal.Appl.,1982,86(2):539-578.

        [7]ˇSemrl P.Automorphisms ofB(H)with respect to minus partial order.J.Math.Anal.Appl., 2010,369(1):205-213.

        [8]Guterman A.Linear preservers for Drazin star partial order.Comm.Algebra,2001,29(9): 3905-3917.

        [9]Legiˇsa P.Automorphisms ofMn,Partially ordered by the star order.Linear Multilinear Algebra,2006,54(3):157-188.

        [10]Dolinar G,Guterman A.Marovt J.Automorphisms ofK(H)with respect to the star partial order.Oper.Matrices,2013,7(1):225-239.

        [11]Bohata M,Hamhalter J.Nonlinear maps on von Neumann algebras preserving the star order.Linear Multilinear Algebra,doi:10.1080/03081087.2012.721363,to appear.

        [12]Guterman A.Monotone additive matrix transformations.Math.Notes,2007,81(5/6):609-619.

        [13]Hou J,Cui J.Introduction to the Linear Maps on Operator Algebras(in Chinese).Beijing: Science Press,2002:22.

        [14]Pearcy C,Topping D.Sums of small numbers of idempotents.Michigan Math.J.,1967,14(4): 453-465.

        A

        1674-5647(2015)01-0089-08

        10.13447/j.1674-5647.2015.01.10

        Received date:July 11,2013.

        Foundation item:The NSF(11371233)of China and the Fundamental Research Funds(GK201301007)for the Central Universities.

        *

        .

        E-mail address:xicui@snnu.edu.cn(Xi C),gxji@snnu.edu.cn(Ji G X).

        2010 MR subject classifcation:47B49,47B47

        8090成人午夜精品无码| 中文字幕久久熟女蜜桃 | 成 人片 黄 色 大 片| 人妻精品动漫h无码网站| 精品国产AⅤ一区二区三区4区 | 国产一区在线视频不卡| 天天综合网网欲色| 国产成人乱色伦区| 不卡国产视频| 街拍丝袜美腿美女一区| 国产成人av一区二区三区在线观看| 中文字幕无码不卡一区二区三区 | 国产成人啪精品| 又爽又猛又大又湿的视频| 3亚洲日韩在线精品区| 男女深夜视频网站入口| 国产极品女主播国产区| 亚洲另类精品无码专区| 人妻少妇精品无码系列| 日日麻批免费高清视频| 欧美人牲交| 中文字幕在线亚洲一区二区三区| 一区二区亚洲 av免费| 二区三区三区视频在线观看| 中文字幕天天躁日日躁狠狠躁免费| 亚洲av日韩av综合aⅴxxx| 日韩精品一区二区在线视| 奇米影视色777四色在线首页 | 成人av在线免费播放| 亚洲乱码无人区卡1卡2卡3| 在线观看国产成人av片| 两个人免费视频大全毛片| 天天色天天操天天日天天射| 国产精品18久久久| 国产激情久久99久久| 亚洲免费福利视频网站| 少妇被爽到高潮喷水久久欧美精品| 亚洲免费观看在线视频| 中文字幕五月久久婷热| 娇小女人被黑人插免费视频| 影音先锋色小姐|