Journal of Inequalities in Pure and Applied Mathematics http://jipam.vu.edu.au/ Volume 6, Issue 3, Article 79, 2005 ON AN ε-BIRKHOFF ORTHOGONALITY JACEK CHMIELIŃSKI I NSTYTUT M ATEMATYKI , A KADEMIA P EDAGOGICZNA W K RAKOWIE P ODCHOR A̧ ŻYCH 2, 30-084 K RAKÓW, P OLAND jacek@ap.krakow.pl Received 18 February, 2005; accepted 28 July, 2005 Communicated by S.S. Dragomir A BSTRACT. We define an approximate Birkhoff orthogonality relation in a normed space. We compare it with the one given by S.S. Dragomir and establish some properties of it. In particular, we show that in smooth spaces it is equivalent to the approximate orthogonality stemming from the semi-inner-product. Key words and phrases: Birkhoff (Birkhoff-James) orthogonality, Approximate orthogonality, Semi-inner-product. 2000 Mathematics Subject Classification. 46B20, 46C50. 1. I NTRODUCTION In an inner product space, with the standard orthogonality relation ⊥, one can consider the approximate orthogonality defined by: x⊥ε y ⇔ | hx|yi | ≤ ε kxk kyk . ( | cos(x, y)| ≤ ε for x, y 6= 0). The notion of orthogonality in an arbitrary normed space, with the norm not necessarily coming from an inner product, may be introduced in various ways. One of the possibilities is the following definition introduced by Birkhoff [1] (cf. also James [6]). Let X be a normed space over the field K ∈ {R, C}; then for x, y ∈ X x⊥B y ⇐⇒ ∀ λ ∈ K : kx + λyk ≥ kxk . We call the relation ⊥B , a Birkhoff orthogonality (often called a Birkhoff-James orthogonality). Our aim is to define an approximate Birkhoff orthogonality generalizing the ⊥ε one. Such a definition was given in [3]: x⊥ B y ⇐⇒ ∀λ ∈ K : kx + λyk ≥ (1 − ε) kxk . ε We are going to give another definition of this concept. (1.1) ISSN (electronic): 1443-5756 c 2005 Victoria University. All rights reserved. The paper has been completed during author’s stay at the Silesian University in Katowice. 043-05 2 JACEK C HMIELI ŃSKI 2. B IRKHOFF A PPROXIMATE O RTHOGONALITY Let us define an approximate Birkhoff orthogonality. For ε ∈ [0, 1): (2.1) x⊥εB y ⇐⇒ ∀λ ∈ K : kx + λyk2 ≥ kxk2 − 2ε kxk kλyk . If the above holds, we say that x is ε-Birkhoff orthogonal to y. Note, that the relation ⊥εB is homogeneous, i.e., x⊥εB y implies αx⊥εB βy (for arbitrary α, β ∈ K). Indeed, for any λ ∈ K we have (excluding the obvious case α = 0) 2 β kαx + λβyk2 = |α|2 x + λ y α β 2 2 ≥ |α| kxk − 2ε kxk λ y α = kαxk2 − 2εkαxkkλβyk. Proposition 2.1. If X is an inner product space then, for arbitrary ε ∈ [0, 1), x⊥ε y ⇐⇒ x⊥εB y. We omit the proof – a more general result will be proved later (Theorem 3.3). As a corollary, for ε = 0, we obtain the well known fact: x⊥B y ⇔ x⊥y (in an inner product space). √ Let us modify slightly the definition of Dragomir (1.1). Replacing 1 − ε by 1 − ε2 we obtain: √ x⊥εD y ⇐⇒ ∀ λ ∈ K : kx + λyk ≥ 1 − ε2 kxk . √ Thus x⊥εD y ⇔ x⊥ y with ρ = ρ(ε) = 1 − 1 − ε2 . B ρ Then, for inner product spaces we have: x⊥εD y ⇐⇒ x⊥ε y (see [3, Proposition 1]). T. Szostok [10], considering a generalization of the sine function introduced, for a real normed space X, the mapping: inf λ∈R kx+λyk , for x ∈ X \ {0}; kxk s(x, y) = 1, for x = 0. It is easily seen that x⊥B y ⇔ps(x, y) = 1. It is also apparent that x⊥εD y ⇔ s(x, y) ≥ √ 1 − ε2 . Defining c(x, y) := ± 1 − s2 (x, y) (generalized cosine) one gets x⊥εD y ⇔ |c(x, y)| ≤ ε. Let us compare the approximate orthogonalities ⊥εD and ⊥εB . In an inner product space both of them are equal to ε-orthogonality ⊥ε . Thus one may ask if they are equal in an arbitrary normed space. This is not true. Moreover, neither ⊥εB ⊂ ⊥εD nor ⊥εD ⊂ ⊥εB holds generally (i.e., for an arbitrary normed space and all ε ∈ [0, 1)). For, consider X = R2 (over R) equipped with 1 1 the maximum norm k(x1 , x2 )k := max{|x1 |, |x2 |}. Now, let x = (1, 0), y = 2 , 1 , ε = 2 . One 2 can verify that x⊥εB y (i.e., that max 1 + λ2 , |λ| ≥ 1 − |λ| holds for each λ ∈ R) but not 2 ε ε ε x⊥D y (take λ = − 3 ). Thus ⊥B 6⊂ ⊥D . √ 2 On the other hand, for x = 1, 12 , y = (1, 0), ε = 23 we have max{|1 + λ|, 21 } ≥ √ 2 √ 1 − 23 , i.e., x⊥εD y but not x⊥εB y (consider, for example, λ = 23 − 1). Thus ⊥εD 6⊂ ⊥εB . See also Remark 4.1 for further comparison of ⊥εB and ⊥εD . J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/ O N AN ε-B IRKHOFF O RTHOGONALITY 3 3. S EMI – INNER – PRODUCT ( APPROXIMATE ) O RTHOGONALITY Let X be a normed space over K ∈ {R, C}. The norm in X need not come from an inner product. However, (cf. G. Lumer [7] and J.R. Giles [5]) there exists a mapping [·|·] : X × X → K satisfying the following properties: (s1) [λx + µy|z] = λ [x|z] + µ [y|z] , x, y, z ∈ X, λ, µ ∈ K; (s2) [x|λy] = λ [x|y] , x, y ∈ X, λ ∈ K; (s3) [x|x] = kxk2 , x ∈ X; (s4) | [x|y] | ≤ kxk · kyk , x, y ∈ X. (Cf. also [4].) We will call each mapping [·|·] satisfying (s1)–(s4) a semi-inner-product (s.i.p.) in a normed space X. Let us stress that we assume that a s.i.p. generates the given norm in X (i.e., (s3) is satisfied). Note, that there may exist infinitely many different semi-inner-products in X. There is a unique s.i.p. in X if and only if X is smooth (i.e., there is a unique supporting hyperplane at each point of the unit sphere S or, equivalently, the norm is Gâteaux differentiable on S – cf. [2, 4]). If X is an inner product space, the only s.i.p. on X is the inner-product itself ([7, Theorem 3]). We say that s.i.p. is continuous iff Re [y|x + λy] → Re [y|x] as R 3 λ → 0 for all x, y ∈ S. The continuity of s.i.p is equivalent to the smoothness of X (cf. [5, Theorem 3] or [4]). It follows also in that case (see the proof of Theorem 3 in [5]): (3.1) lim λ→0 λ∈R kx + λyk − 1 = Re [y|x] , x, y ∈ S. λ Extending previous notations we define semi-orthogonality and approximate semi-orthogonality: x⊥s y ⇔ [y|x] = 0; x⊥εs y ⇔ | [y|x] | ≤ ε kxk · kyk , for x, y ∈ X and 0 ≤ ε < 1. Obviously, for an inner–product space: ⊥s = ⊥ and ⊥εs = ⊥ε . Proposition 3.1. For x, y ∈ X, if x⊥εs y, then x⊥εB y (i.e., ⊥εs ⊂ ⊥εB ). Proof. Suppose that x⊥εs y, i.e., | [y|x] | ≤ ε kxk · kyk. Then, for some θ ∈ [0, 1] and for some ϕ ∈ [−π, π] we have: [y|x] = θε kxk · kyk · eiϕ . For arbitrary λ ∈ K we have: kx + λyk · kxk ≥ | [x + λy|x] | = kxk2 + λ [y|x] = kxk2 + θε kxk · kyk · λ · eiϕ whence kx + λyk ≥ kxk + θε kyk · λ · eiϕ = kxk + θε kyk Re λeiϕ + iθε kyk Im λeiϕ . J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/ 4 JACEK C HMIELI ŃSKI Therefore kx + λyk2 ≥ kxk + θε kyk Re λeiϕ 2 + θε kyk Im λeiϕ iϕ 2 = kxk2 + 2θε kxk kyk Re λe 2 2 2 iϕ 2 iϕ 2 + Im λe + θ ε kyk Re λe = kxk2 + 2θε kxk kyk Re λeiϕ + θ2 ε2 kλyk2 ≥ kxk2 + 2θε kxk kyk Re λeiϕ ≥ kxk2 + 2θε kxk kyk − λeiϕ = kxk2 − 2θε kxk kλyk ≥ kxk2 − 2ε kxk kλyk , i.e., x⊥εB y. Since | [y|x] | ≤ kxk kyk, i.e., x⊥1s y for arbitrary x, y, the above result gives also x⊥1B y for all x, y. That is the reason we restrict ε to the interval [0, 1). Proposition 3.2. If X is a continuous s.i.p. space and ε ∈ [0, 1), then ⊥εB ⊂ ⊥εs . Proof. Suppose that x⊥εB y. Because of the homogeneity of relations ⊥εB and ⊥εs we may assume, without loss of generality, that x, y ∈ S. Then, for arbitrary λ ∈ K we have: 0 ≤ kx + λyk2 − 1 + 2ε |λ| = [x|x + λy] + [λy|x + λy] − 1 + 2ε |λ| . Therefore 0 ≤ Re [x|x + λy] + Re [λy|x + λy] − 1 + 2ε |λ| ≤ |[x|x + λy]| + Re [λy|x + λy] − 1 + 2ε |λ| ≤ kx + λyk + Re [λy|x + λy] − 1 + 2ε |λ| whence (3.2) Re [λy|x + λy] + kx + λyk − 1 ≥ −2ε |λ| , for all λ ∈ K. Let λ0 ∈ K \ {0}, n ∈ N and λ = λn0 . Then from (3.2) we have λ0 λ0 λ0 |λ0 | Re y|x + y + x + y − 1 ≥ −2ε ; n n n n |λ0 | λ0 x + n |λ0 | y − 1 λ0 |λ0 | λ0 ≥ −2ε. Re y|x + y + |λ0 | |λ0 | n |λ0 | n Putting y 0 := inequality λ0 y |λ0 | ∈ S, ξn := |λ0 | n ∈ R (ξn → 0 as n → ∞) we obtain from the above kx + ξn y 0 k − 1 ≥ −2ε. ξn Letting n → ∞, using continuity of the s.i.p. and (3.1) Re [y 0 |x + ξn y 0 ] + Re [y 0 |x] + Re [y 0 |x] ≥ −2ε whence Re [λ0 y|x] ≥ −ε|λ0 |. Putting −λ0 in the place of λ0 we obtain Re [λ0 y|x] ≤ ε|λ0 | whence |Re [λ0 y|x]| ≤ ε|λ0 | for arbitrary λ0 ∈ K. J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/ O N AN ε-B IRKHOFF O RTHOGONALITY 5 Now, taking λ0 = [y|x] we get h i Re [y|x]y|x ≤ ε| [y|x] | whence | [y|x] |2 ≤ ε| [y|x] | and finally | [y|x] | ≤ ε, i.e., x⊥εs y. Without the additional continuity assumption, the inclusion ⊥εB ⊂ ⊥εs need not hold. P 1 Example 3.1. Consider the space l1 (with the norm kxk = ∞ i=1 |xi | for x = (x1 , x2 , . . .) ∈ l ). Define ∞ X xi yi [x|y] := kyk , x, y ∈ l1 |y | i i=1 1 — a semi-inner-product in l . Let ε ∈ [0, Then, for an arbitrary λ ∈ K: √ yi 6=0 2 − 1) and let x = (1, 0, 0, . . .), y = (1, 1, ε, 0, . . .). kx + λyk2 − kxk2 + 2ε kxk kλyk = (|1 + λ| + |λ| + |λε|)2 − 1 + 2ε(2 + ε) |λ| ≥ (1 + |λ| ε)2 − 1 + 2ε(2 + ε) |λ| = 2ε(3 + ε) |λ| + |λ|2 ε2 ≥ 0, i.e., x⊥εB y (in fact, x⊥B y). On the other hand, 1 [y|x] = 1 = kxk kyk > ε kxk kyk 2+ε whence ¬(x⊥εs y). In particular, for ε = 0, this shows that ⊥B 6⊂ ⊥s (cf. [4, 8, 9]). From the last two propositions we have: Theorem 3.3. If X is a continuous s.i.p. space, then ⊥εB = ⊥εs . Moreover we obtain, for ε = 0, (cf. [5, Theorem 2]) Corollary 3.4. If X is a continuous s.i.p. space, then ⊥B = ⊥s . Conversely, ⊥B ⊂ ⊥s implies continuity of s.i.p. (smoothness) – cf. [4] and [8]. 4. S OME R EMARKS Remark 4.1. Dragomir [3, Definition 5] introduces the following concept: The s.i.p. [·|·] is of (APP)-type if there exists a mapping η : [0, 1) → [0, 1) such that η(ε) = 0 ⇔ ε = 0 and η(ε) x⊥D y implies x⊥εs y for all ε ∈ [0, 1). It follows from Proposition 3.1 that in that case we have also (4.1) η(ε) x⊥D y ⇒ x⊥εB y for all ε ∈ [0, 1). It follows from [3, Lemma 1] that for a closed, proper linear subspace G of a normed space ε X and for an arbitrary ε ∈ (0, 1), the set G⊥D of all vectors ⊥εD -orthogonal to G is nonzero. Using (4.1) we get η(ε) (4.2) ε G⊥D ⊂ G⊥B . Therefore, we have J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/ 6 JACEK C HMIELI ŃSKI Lemma 4.2. If X is a normed space with the s.i.p. [·|·] of the (APP)-type, then for an arbitrary ε proper and closed linear subspace G and an arbitrary ε ∈ [0, 1) the set G⊥B of all vectors ε-Birkhoff orthogonal to G is nonzero. We have also Theorem 4.3. If X is a normed space with the s.i.p. [·|·] of the (APP)-type, then for an arbitrary closed linear subspace G and an arbitrary ε ∈ [0, 1) the following decomposition holds: ε X = G + G⊥B . Proof. Fix G and ε ∈ [0, 1). It follows from [3, Theorem 3] that η(ε) X = G + G⊥D . Using (4.2) we get the assertion. The final example shows that the set of all ε-orthogonal vectors may be equal to the set of all orthogonal ones. Example 4.1. Consider again the space l1 with the s.i.p. defined above. Let e = (1, 0, . . .). Observe that vectors ε-orthogonal to e are, in fact, orthogonal to e: x⊥εB e ⇒ x⊥B e. (4.3) Indeed, let ε ∈ [0, 1) be fixed and let x = (x1 , x2 , . . .) ∈ l1 satisfy x⊥εB e. Because of the homogeneity of ⊥εB we may assume, without loss of generality, that kxk = 1 and x1 ≥ 0. Thus we have ∀λ ∈ K : kx + λek2 ≥ 1 − 2ε |λ| . Therefore ∀ λ ∈ K : (|x1 + λ| + 1 − x1 )2 ≥ 1 − 2ε |λ| . Suppose that x1 > 0. Take λ ∈ R such that λ < 0, λ > −x1 and λ > −2(1 − ε). Then we have (x1 + λ + 1 − x1 )2 ≥ 1 + 2ελ, which leads to λ ≤ −2(1 − ε) – a contradiction. Thus x1 = 0, i.e, x = (0, x2 , x3 , . . .) and |x2 | + |x3 | + · · · = 1. This yields, for arbitrary λ ∈ K, kx + λek = |λ| + 1 ≥ 1 = kxk , i.e., x⊥B e. It follows from (4.3) that for G := lin e we have ε G⊥B = G⊥B . Note, that the implication e⊥εB x ⇒ e⊥B x is not true. Take for example x = 3 kek 4 Then [x|e] = λ = − 53 one has 3 4 3 4 3 1 , , 0, . . . 4 4 . kxk, i.e, e⊥s x, whence (Proposition 3.1) e⊥B x. On the other hand, for ke + λxk = 2 < 1 = kek, 3 i.e., ¬(e⊥B x). J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/ O N AN ε-B IRKHOFF O RTHOGONALITY 7 R EFERENCES [1] G. 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SZOSTOK, On a generalization of the sine function, Glasnik Matematički, 38 (2003), 29–44. J. Inequal. Pure and Appl. Math., 6(3) Art. 79, 2005 http://jipam.vu.edu.au/