Chaotic Order of Indefinite Type
Takashi Sano vol. 8, iss. 3, art. 62, 2007
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ON CHAOTIC ORDER OF INDEFINITE TYPE
TAKASHI SANO
Department of Mathematical Sciences Faculty of Science, Yamagata University Yamagata 990-8560, Japan
EMail:sano@sci.kj.yamagata-u.ac.jp
Received: 02 June, 2006
Accepted: 27 April, 2007
Communicated by: F. Hansen 2000 AMS Sub. Class.: 47B50, 47A63.
Key words: Inner product space; Furuta inequality of indefinite type.
Abstract: LetA, BbeJ-selfadjoint matrices with positive eigenvalues andI=J A, I=J B.Then it is proved as an application of Furuta inequality of indefinite type that
LogA=J LogB
if and only if
Ar =J (Ar2BpAr2)p+rr for allp >0andr >0.
Chaotic Order of Indefinite Type
Takashi Sano vol. 8, iss. 3, art. 62, 2007
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In [2], T. Ando gave inequalities for matrices on an (indefinite) inner product space; for instance,
Proposition 1 ([2, Theorem 4]). LetA, BbeJ-selfadjoint matrices withσ(A), σ(B)j (α, β).Then
A=J B ⇒f(A)=J f(B) for any operator monotone functionf(t)on(α, β).
Since the principal branch Log x of the logarithm is operator monotone, as a corollary, we have
Corollary 2. For J-selfadjoint matrices A, B with positive eigenvalues and A =J B, we have
LogA=J LogB.
In this note, we give a characterization of this inequality relation, called a chaotic order, forJ-selfadjoint matricesA, B with positive eigenvalues andI =J A, I =J B.
Before giving our theorem, we recall basic facts about matrices on an (indefinite) inner product space. We refer the reader to [3].
LetMn(C)be the set of all complexn-square matrices acting onCnand leth·,·i be the standard inner product onCn;hx, yi := Pn
i=1xiyi forx = (xi), y = (yi) ∈ Cn. For a selfadjoint involutionJ ∈ Mn(C);J = J∗ andJ2 = I,we consider the (indefinite) inner product[·,·]onCngiven by
[x, y] :=hJ x, yi (x, y ∈Cn).
Chaotic Order of Indefinite Type
Takashi Sano vol. 8, iss. 3, art. 62, 2007
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TheJ-adjoint matrixA]ofA∈Mn(C)is defined as [Ax, y] = [x, A]y] (x, y ∈Cn).
In other words, A] = J A∗J. A matrix A ∈ Mn(C) is said to be J-selfadjoint if A] =AorJ A∗J =A.And forJ-selfadjoint matricesAandB,theJ-order, denoted asA=J B, is defined by
[Ax, x]=[Bx, x] (x∈Cn).
A matrixA∈Mn(C)is calledJ-positive ifA=J O,or [Ax, x]=0 (x∈Cn).
A matrixA∈Mn(C)is said to be aJ-contraction ifI =J A]Aor[x, x]=[Ax, Ax]
(x∈Cn).We remark thatI =J Aimplies that all eigenvalues ofAare real. Hence, for aJ-contractionAall eigenvalues ofA]Aare real. In fact, by a result of Potapov- Ginzburg (see [3, Chapter 2, Section 4]), all eigenvalues ofA]Aare non-negative.
We also recall facts in [6]:
Proposition 3 ([6, Theorem 2.6]). Let A, B be J-selfadjoint matrices with non- negative eigenvalues and0< α <1. If
I =J A=J B, thenJ-selfadjoint powersAα, Bα are well defined and
I =J Aα =J Bα.
Proposition 4 ([6, Lemma 3.1]). Let A, B be J-selfadjoint matrices with non- negative eigenvalues and I =J A, I =J B. Then the eigenvalues of ABA are non-negative and
I =J Aλ for allλ >0.
Chaotic Order of Indefinite Type
Takashi Sano vol. 8, iss. 3, art. 62, 2007
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We also have a generalization; Furuta inequality of indefinite type:
Proposition 5 ([6, Theorem 3.4]). Let A, B be J-selfadjoint matrices with non- negative eigenvalues andI =J A=J B.For eachr=0,
Ar2ApAr21q
=J Ar2BpAr21q holds for allp=0, q =1with(1 +r)q=p+r.
Remark 1. Let0< α <1.ForJ-selfadjoint matricesA, Bwith positive eigenvalues andA=J B, we have
Aα =J Bα,
by applying Proposition 1 to the operator monotone function xα whose principal branch is considered. Hence,
Aα−I
α =J Bα−I α .
We remark thatAαis given by the Dunford integral and that Aα−I
α = 1
2πi Z
C
ζα−1
α (ζI−A)−1dζ,
whereC is a closed rectifiable contour in the domain of ζα with positive direction surrounding all eigenvalues ofAin its interior. Since
ζα−1
α →Log ζ (α→0) uniformly forζ,we also have Corollary2.
Our theorem is as follows:
Chaotic Order of Indefinite Type
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Theorem 6. LetA, B beJ-selfadjoint matrices with positive eigenvalues andI =J A, I =J B.Then the following statements are equivalent:
(i) LogA =J LogB.
(ii) Ar =J (Ar2BpAr2)p+rr for allp > 0andr >0.
Here, principal branches of the functions are considered.
This theorem, as well as the corresponding result on a Hilbert space ([1,4,5,7]), can be obtained and the similar approach in [7] also works. But careful arguments are necessary, and this is the reason for the present note.
Proof. (ii)=⇒(i): Assume that
Ar =J Ar2BpAr2p+rr for allp >0andr >0.Then by Corollary2, we have
r(p+r)LogA=J rLog Ar2BpAr2 .
Dividing this inequality byr >0and takingp, rasp= 1, r→0,we have (i).
(i)=⇒(ii): Since
I =J A, B, by assumption, it follows from Corollary2that
O= LogI =J LogA,LogB.
Hence, forn∈N
I =J I + 1
n LogA=:A1, I+ 1
n LogB =:B1.
Chaotic Order of Indefinite Type
Takashi Sano vol. 8, iss. 3, art. 62, 2007
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For a sufficiently largen, all eigenvalues ofA1, B1 are positive. Applying Proposi- tion5toA1, B1andnp, nr,nr+npnr (resp.) asp, r, q(resp.), we get
(]) Anr1 =J
A
nr 2
1 B1npA
nr 2
1
np+nrnr
for allp >0, q >0.Recall that
n→∞lim
I+ A n
n
=eA
for any matrixAand thateLogX =Xfor any matrixXwith all eigenvalues positive.
Therefore, takingnasn → ∞in the inequality (]), we obtain the conclusion.
Chaotic Order of Indefinite Type
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References
[1] T. ANDO, On some operator inequalities, Math. Ann., 279 (1987), 157–159.
[2] T. ANDO, Löwner inequality of indefinite type, Linear Algebra Appl., 385 (2004), 73–80.
[3] T. Ya. AZIZOV AND I.S. IOKHVIDOV, Linear Operators in Spaces with an Indefinite Metric, Nauka, Moscow, 1986, English translation: Wiley, New York, 1989.
[4] M. FUJII, T. FURUTAAND E. KAMEI, Furuta’s inequality and its application to Ando’s theorem, Linear Algebra Appl., 179 (1993), 161–169.
[5] T. FURUTA, Applications of order preserving operator inequalities, Op. Theory Adv. Appl., 59 (1992), 180-190.
[6] T. SANO, Furuta inequality of indefinite type, Math. Inequal. Appl., 10 (2007), 381–387.
[7] M. UCHIYAMA, Some exponential operator inequalities, Math. Inequal. Appl., 2 (1999), 469–471.