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INNER PRODUCT SPACES

A. H. ANSARI AND M. S. MOSLEHIAN

Received 8 February 2005 and in revised form 17 May 2005

Refining some results of Dragomir, several new reverses of the generalized triangle in- equality in inner product spaces are given. Among several results, we establish some re- verses for the Schwarz inequality. In particular, it is proved that ifais a unit vector in a real or complex inner product space (H;·,·),r,s >0, p(0,s], D= {xH,rx sap},x1,x2D− {0}, andαr,s=min{(r2xk2p2+s2)/2rsxk: 1k2}, then (x1x2Rex1,x2)/(x1+x2)2αr,s.

1. Introduction

It is interesting to know under which conditions the triangle inequality went the other way in a normed spaceX; in other words, we would like to know if there is a positive constantcwith the property thatcnk=1xkn

k=1xkfor any finite setx1,...,xnX. Nakai and Tada [7] proved that the normed spaces with this property are precisely those of finite dimensional.

The first authors investigating reverse of the triangle inequality in inner product spaces were Diaz and Metcalf [2] by establishing the following result as an extension of an in- equality given by Petrovich [8] for complex numbers.

Theorem1.1 (Diaz-Metcalf theorem). Letabe a unit vector in an inner product space (H;·,·). Suppose the vectorsxkH,k∈ {1,...,n}satisfy

0rRexk,a

xk , k∈ {1,...,n}. (1.1)

Then

rn

k=1

xk

n k=1

xk

, (1.2)

Copyright©2005 Hindawi Publishing Corporation

International Journal of Mathematics and Mathematical Sciences 2005:18 (2005) 2883–2893 DOI:10.1155/IJMMS.2005.2883

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where equality holds if and only if n k=1

xk=rn

k=1

xka. (1.3)

Inequalities related to the triangle inequality are of special interest (cf. [6, Chapter XVII]). They may be applied to get interesting inequalities in complex numbers or to study vector-valued integral inequalities [4,5].

Using several ideas and following the terminology of [4,5], we modify or refine some results of Dragomir and ours [1] and get some new reverses of triangle inequality. Among several results, we show that if ais a unit vector in a real or complex inner product space (H;·,·),xkH− {0}, 1kn,α=min{xk: 1kn}, p(0,α2+ 1), max{xka: 1kn} ≤p, andβ=min{(xk2p2+ 1)/2xk: 1kn}, then

n k=1

xk

n k=1

xk

1β

β Re n

k=1

xk,a

. (1.4)

We also examine some reverses for the celebrated Schwarz inequality. In particular, it is proved that ifais a unit vector in a real or complex inner product space (H;·,·),r,s >0, p(0,s],D= {xH,rxsap},x1,x2D− {0}, andαr,s=min{(r2xk2p2+ s2)/2rsxk: 1k2}, then

x1x2Rex1,x2

x1+x2

2 αr,s. (1.5)

Throughout the paper, (H;·,·) denotes a real or complex inner product space. We use repeatedly the Cauchy-Schwarz inequality without mentioning it. The reader is re- ferred to [3,9] for the terminology on inner product spaces.

2. Reverse of triangle inequality

We start this section by pointing out the following theorem of [1] which is a modification of [5, Theorem 3].

Theorem 2.1. Leta1,...,am be orthonormal vectors in the complex inner product space (H;·,·). Suppose that for1tm,rttR, and that the vectorsxkH,k∈ {1,...,n} satisfy

0rt2xkRexk,rtat

, 0ρ2txkImxktat

, 1tm. (2.1) Then

m

t=1

rt2+ρ2t

1/2n k=1

xk

n k=1

xk

(2.2)

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and the equality holds in (2.2) if and only if n

k=1

xk= n k=1

xkm

t=1

rt+t at. (2.3)

The following theorem is a strengthen of [5, Corollary 1] and a generalization of [1, Theorem 2].

Theorem2.2. Letabe a unit vector in the complex inner product space(H;·,·). Suppose that the vectorsxkH− {0},k∈ {1,...,n}satisfy

maxrxksa: 1knp, maxrxkisa: 1knq, (2.4) wherer,r,s,s>0and

p

()2+s2 1/2, q

(rα)2+s2 1/2,

α=minxk: 1kn. (2.5)

Let

αr,s=min

r2xk2p2+s2

2rsxk : 1kn

, βr,s=min

r2xk2q2+s2

2rsxk : 1kn

.

(2.6)

Then

α2r,s+β2r,s 1/2n

k=1

xk

n k=1

xk

(2.7)

and the equality holds if and only if n k=1

xk=

αr,s+r,s

n k=1

xka. (2.8)

Proof. From the first inequality above, we infer that rxksa,rxksap2,

r2xk2+s2p22 Rerxk,sa. (2.9) Then

r2xk2+s2p2

2rsxk xkRexk,a. (2.10) Similarly,

r2xk2q2+s2

2rsxk xkImxk,a, (2.11)

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consequently,

αr,sxkRexk,a,

βr,sxkImxk,a. (2.12) ApplyingTheorem 2.1form=1,r1=αr,s, andρ1=βr,s, we deduce the desired inequal-

ity.

The next result is an extension of [1, Corollary 3].

Corollary2.3. Letabe a unit vector in the complex inner product space(H;·,·). Sup- pose thatxkH,k∈ {1,...,n},max{rxksa: 1kn} ≤r,max{rxkisa: 1 kn} ≤s, wherer >0,s >0, andα=min{xk: 1kn}. Then

s2

n k=1

xk

n k=1

xk

. (2.13)

The equality holds if and only if n k=1

xk=(1 +i) 2s

n k=1

xka. (2.14)

Proof. ApplyTheorem 2.2withr=r,s=s,p=r,q=s. Note thatαr,s=rα/2s=βr,s. Theorem2.4. Letabe a unit vector in(H;·,·). Suppose that the vectorsxkH,k {1,...,n}satisfy

maxrxksa: 1knp <(rα)2+s2 1/2, (2.15) wherer >0,s >0and

α= min

1knxk. (2.16)

Let

αr,s=min

r2xk2p2+s2

2rsxk : 1kn

. (2.17)

Then

αr,s

n k=1

xk

n k=1

xk

. (2.18)

Moreover, the equality holds if and only if n k=1

xk=αr,s

n k=1

xka. (2.19)

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Proof. Proof is similar to that ofTheorem 2.2in which we useTheorem 2.1withm=1,

ρ1=0.

Theorem2.5. Letabe a unit vector in(H;·,·). Suppose thatr,s >0, and vectorsxk H− {0},k∈ {1,...,n}satisfy

n k=1

xk=0. (2.20)

Then

r2α2+s2maxrxksa: 1n, (2.21) where

α= min

1knxk. (2.22)

Proof. Letp=max{rxksa: 1kn}. Ifp <r2α2+s2, then, usingTheorem 2.4, we get

αr,s

n k=1

xk

n k=1

xk

=0. (2.23)

Henceαr,s=0. On the other hand, (p2s2)/r2< α2, so αr,s=min

r2xk2p2+s2

2rsxk : 1kn

>0 (2.24)

holds a contradiction.

Theorem 2.6. Leta1,...,am be orthonormal vectors in the complex inner product space (H;·,·),Mtmt>0,Ltt>0,1tm, andxkH− {0},k∈ {1,...,n}such that

ReMtatxk,xkmtat

0, ReLtiatxk,xktiat

0, (2.25) or equivalently

xkmt+Mt

2 at

Mtmt

2 ,

xkLt+t

2 iat

Ltt

2 , (2.26)

for all1knand1tm. Let

αmt,Mt=min xk2+mtMt

mt+Mt xk: 1kn

, 1tm, αt,Lt=min xk2+tLt

mt+Mt xk: 1kn

, 1tm,

(2.27)

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then

m

t=1

α2mt,Mt+α2t,Lt

1/2n k=1

xk

n k=1

xk

. (2.28)

The equality holds if and only if n k=1

xk= n

k=1

xkm

t=1

αmt,Mt+t,Lt at. (2.29)

Proof. Given 1tmand all 1kn, it follows fromxk((mt+Mt)/2)at(Mt mt)/2 that

xk2+mtMt

mt+Mt Rexk,at

. (2.30)

Then

xk2+mtMt

mt+Mt xkxkRexk,at

, (2.31)

and so

αmt,MtxkRexk,at

. (2.32)

Similarly, from the second inequality, we deduce that αt,LtxkImxk,at

. (2.33)

ApplyingTheorem 2.5forrt=αmt,Mt andρt=αt,Lt, we obtain the required inequality.

We will need [4, Theorem 7]. We mention it for the sake of completeness.

Theorem 2.7. Let abe a unit vector in(H;·,·), and xkH− {0},k∈ {1,...,n}. If rk0,k∈ {1,...,n}such that

xkRexk,ark, (2.34)

then

n k=1

xk

n k=1

xk

n

k=1

rk. (2.35)

The equality holds if and only if n k=1

xk n k=1

rk, n

k=1

xk= n

k=1

xkn

k=1

rk

a.

(2.36)

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Theorem2.8. Letabe a unit vector in(H;·,·), andxkH− {0},k∈ {1,...,n}. Let α=minxk: 1kn, p

0,α2+ 1 , maxxka: 1knp, β=minxk2p2+ 1

2xk : 1kn

.

(2.37) Then

n k=1

xk

n k=1

xk

1β

β Re n

k=1

xk,a

. (2.38)

The equality holds if and only if n k=1

xk1β β Re

n

k=1

xk,a

, n

k=1

xk= n

k=1

xk1β β Re

n

k=1

xk,a

a.

(2.39)

Proof. Since max{xka: 1kn} ≤p, we have

xka,xkap2, xk2+ 1p22 Rexk,a, xk2p2+ 1

2xk xkRexk,a, βxkRexk,a, xk1

βRexk,a,

(2.40)

for allk∈ {1,...,n}. Then

xkRexk,a1β

β Rexk,a, k∈ {1,...,n}. (2.41) ApplyingTheorem 2.7forrk=((1β)/β) Rexk,a,k∈ {1,...,n}, we deduce the desired

inequality.

As a corollary, we obtain a result similar to [4, Theorem 9].

Corollary2.9. Letabe a unit vector in(H;·,·), andxkH− {0},k∈ {1,...,n}. Let maxxka: 1kn1,

α=minxk: 1kn. (2.42)

Then

n k=1

xk

n k=1

xk

2α

α Re n

k=1

xk,a

. (2.43)

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The equality holds if and only if n k=1

xk2α α Re

n

k=1

xk,a

, n

k=1

xk= n

k=1

xk2α α Re

n

k=1

xk,a

a.

(2.44)

Proof. ApplyTheorem 2.8withβ=α/2.

Theorem2.10. Letabe a unit vector in(H;·,·),Mm >0, andxkH− {0},k {1,...,n}such that

ReMaxk,xkma0 (2.45)

or equivalently

xkm+M

2 aMm

2 . (2.46)

Let

αm,M=min xk2+mM

(m+M)xk: 1kn

. (2.47)

Then

n k=1

xk

n k=1

xk

1αm,M

αm,M Re n

k=1

xk,a

. (2.48)

The equality holds if and only if n k=1

xk1αm,M

αm,M Re n

k=1

xk,a

, n

k=1

xk= n

k=1

xk1αm,M

αm,M Re n

k=1

xk,a

a.

(2.49)

Proof. For each 1kn, it follows from the inequality xkm+M

2 aMm

2 (2.50)

that

xkm+M

2 a,xkm+M

2 aMm 2

2

. (2.51)

Hence

xk2+mM(m+M) Rexk,a. (2.52)

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So that

αm,MxkRexk,a, (2.53)

consequently

xkRexk,a1αm,M

αm,M Rexk,a. (2.54) Now applyTheorem 2.7forrk=((1αm,M)/αm,M) Rexk,a,k∈ {1,...,n}. 3. Reverses of Schwarz inequality

In this section, we provide some reverses of the Schwarz inequality. The first theorem is an extension of [4, Proposition 5.1].

Theorem3.1. Letabe a unit vector in(H;·,·). Suppose thatr,s >0,p(0,s], and D=

xH,rxsap. (3.1)

If0 =x1D,0 =x2D, then

x1x2Rex1,x2 x1+x2 2 1

2

1

r2x12p2+s2 2rsx1 2

(3.2) or

x1x2Rex1,x2

x1+x2

2 1

2

1r2x22p2+s2 2rsx2 2

. (3.3)

Proof. Putαr,s=min{(r2xk2p2+s2)/2rsxk: 1k2}. ByTheorem 2.4, we ob- tain

αr,sx1+x2 x1+x2. (3.4) Then

α2r,sx12+ 2x1x2+x22

x12+ 2 Rex1,x2

+x22. (3.5) Setα2r,s=1t2. Then

x1x2Rex1,x2

x1+x2

2 1

2t2, (3.6)

namely,

x1x2Rex1,x2

x1+x2 2 1

2

1α2r,s . (3.7)

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Corollary3.2. Letabe a unit vector in(H;·,·). Suppose thatr,s >0and D=

xH,rxsas. (3.8)

Ifx,yDand0<x<y, then xyRex,y

x+y 2 1 2

1 rx

2s 2

. (3.9)

Proof. In the notation of the proof ofTheorem 3.1, we get fromp=s,x1=x,x2=ythat

αr,s=rx/2s. Now applyTheorem 3.1.

Corollary3.3. Letabe a unit vector in(H;·,·),Mm >0, andxkH− {0},k=1, 2 such that

ReMaxk,xkma0 (3.10)

or equivalently

xkm+M

2 aMm

2 . (3.11)

Then

x1x2Rex1,x2 x1+x2 2 1

2

1 x12+mM (m+M)x12

(3.12) or

x1x2Rex1,x2

x1+x2

2 1

2

1 x22+mM (m+M)x22

. (3.13)

Proof. Putr=1,s=(m+M)/2,p=(Mm)/2,x=x1, andy=x2inTheorem 3.1.

Acknowledgment

The authors would like to thank the referees for their valuable suggestions.

References

[1] A. H. Ansari and M. S. Moslehian,Refinements of reverse triangle inequalities in inner product spaces, JIPAM. J. Inequal. Pure Appl. Math.6(2005), no. 3, article 64.

[2] J. B. Diaz and F. T. Metcalf,A complementary triangle inequality in Hilbert and Banach spaces, Proc. Amer. Math. Soc.17(1966), no. 1, 88–97.

[3] S. S. Dragomir,Discrete Inequalities of the Cauchy-Bunyakovsky-Schwarz Type, Nova Science, New York, 2004.

[4] ,Reverses of the triangle inequality in inner product spaces, Aust. J. Math. Anal. Appl.1 (2004), no. 2, 1–14, article 7.

[5] , Some reverses of the generalised triangle inequality in complex inner product spaces, Linear Algebra Appl.402(2005), 245–254.

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[6] D. S. Mitrinovi´c, J. E. Peˇcari´c, and A. M. Fink,Classical and New Inequalities in Analysis, Math- ematics and Its Applications (East European Series), vol. 61, Kluwer Academic, Dordrecht, 1993.

[7] M. Nakai and T. Tada,The reverse triangle inequality in normed spaces, New Zealand J. Math.

25(1996), no. 2, 181–193.

[8] M. Petrovich,Module d’une somme, L’Ensignement Math´ematique19(1917), no. 1/2, 53–56 (French).

[9] Th. M. Rassias (ed.),Inner Product Spaces and Applications, Pitman Research Notes in Mathe- matics Series, vol. 376, Longman, Harlow, 1997.

A. H. Ansari: Department of Mathematics, Ferdowsi University, P.O. Box 1159, Mashhad 91775, Iran

E-mail address:arsalan h [email protected]

M. S. Moslehian: Department of Mathematics, Ferdowsi University, P.O. Box 1159, Mashhad 91775, Iran

E-mail address:[email protected]

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Special Issue on

Modeling Experimental Nonlinear Dynamics and Chaotic Scenarios

Call for Papers

Thinking about nonlinearity in engineering areas, up to the 70s, was focused on intentionally built nonlinear parts in order to improve the operational characteristics of a device or system. Keying, saturation, hysteretic phenomena, and dead zones were added to existing devices increasing their behavior diversity and precision. In this context, an intrinsic nonlinearity was treated just as a linear approximation, around equilibrium points.

Inspired on the rediscovering of the richness of nonlinear and chaotic phenomena, engineers started using analytical tools from “Qualitative Theory of Differential Equations,”

allowing more precise analysis and synthesis, in order to produce new vital products and services. Bifurcation theory, dynamical systems and chaos started to be part of the mandatory set of tools for design engineers.

This proposed special edition of the Mathematical Prob- lems in Engineering aims to provide a picture of the impor- tance of the bifurcation theory, relating it with nonlinear and chaotic dynamics for natural and engineered systems.

Ideas of how this dynamics can be captured through precisely tailored real and numerical experiments and understanding by the combination of specific tools that associate dynamical system theory and geometric tools in a very clever, sophis- ticated, and at the same time simple and unique analytical environment are the subject of this issue, allowing new methods to design high-precision devices and equipment.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

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Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

José Roberto Castilho Piqueira,Telecommunication and Control Engineering Department, Polytechnic School, The University of São Paulo, 05508-970 São Paulo, Brazil;

[email protected]

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