5
Applied Mathematics Letters 25 (2012) 190–194 Contents lists available at SciVerse ScienceDirect Applied Mathematics Letters journal homepage: www.elsevier.com/locate/aml On Dresher’s inequalities for width-integrals Chang-Jian Zhao 1 Department of Mathematics, China Jiliang University, Hangzhou 310018, PR China article info Article history: Received 17 January 2011 Received in revised form 25 March 2011 Accepted 4 August 2011 Keywords: Dresher’s inequality Brunn–Minkowski inequality Convex body Mixed projection body abstract In the paper, we establish a reversed Dresher’s integral inequality, based on the Minkowski inequality and an inequality due to Radon. Further, we prove Dresher-type inequalities for width-integrals of convex bodies and mixed projection bodies, respectively. © 2011 Elsevier Ltd. All rights reserved. 1. Notations and preliminaries The setting for this paper is n-dimensional Euclidean space R n . Let K n denote the set of all convex bodies (compact, convex subsets with non-empty interiors) in R n . We reserve the letter u for unit vectors, and the letter B is reserved for the unit ball centered at the origin. The surface of B is S n1 . The volume of the unit n-ball is denoted by ω n . For u S n1 , let E u denote the hyperplane, through the origin, that is orthogonal to u. We use K u to denote the image of K under an orthogonal projection onto the hyperplane E u . If K 1 ,..., K n1 K n , we denote by v(K u 1 ,..., K u n1 ) the mixed volume of the figures K u 1 ,..., K u n1 in the space E u . If K 1 =···= K n1 = K , then we write v(K u ) for v(K u ,..., K u ). We use V (K ) for the n-dimensional volume of convex body K . Let h(K , ·) : S n1 R denote the support function of K K n ; i.e. for u S n1 h(K , u) = Max{u · x : x K }, where u · x denotes the usual inner product u and x in R n . Let δ denote the Hausdorff metric on K n , i.e. for K , L K n ,δ(K , L) =|h K h L | , where |·| denotes the sup-norm on the space of continuous functions C (S n1 ) ([1], also see [2]). 1.1. Width-integrals of convex bodies For u S n1 , b(K , u) =: 1 2 (h(K , u) + h(K , u)) is defined to be half the width of K in the direction u. Two convex bodies K and L are said to have similar width if there exists a constant λ> 0 such that b(K , u) = λb(L, u) for all u S n1 . Width- integrals were first considered by Blaschke (see [3]). The width-integral of index i is defined by Lutwak [4]. For K K n , i R B i (K ) = 1 n S n1 b(K , u) ni dS (u). (1.1) This definition implies that the width-integral of index i is non-negative and continuous. E-mail addresses: [email protected], [email protected]. 1 Research is supported by National Natural Science Foundation of China (10971205). 0893-9659/$ – see front matter © 2011 Elsevier Ltd. All rights reserved. doi:10.1016/j.aml.2011.08.013

On Dresher’s inequalities for width-integrals

Embed Size (px)

Citation preview

Applied Mathematics Letters 25 (2012) 190–194

Contents lists available at SciVerse ScienceDirect

Applied Mathematics Letters

journal homepage: www.elsevier.com/locate/aml

On Dresher’s inequalities for width-integralsChang-Jian Zhao 1

Department of Mathematics, China Jiliang University, Hangzhou 310018, PR China

a r t i c l e i n f o

Article history:Received 17 January 2011Received in revised form 25 March 2011Accepted 4 August 2011

Keywords:Dresher’s inequalityBrunn–Minkowski inequalityConvex bodyMixed projection body

a b s t r a c t

In the paper, we establish a reversed Dresher’s integral inequality, based on theMinkowskiinequality and an inequality due to Radon. Further, we prove Dresher-type inequalities forwidth-integrals of convex bodies and mixed projection bodies, respectively.

© 2011 Elsevier Ltd. All rights reserved.

1. Notations and preliminaries

The setting for this paper is n-dimensional Euclidean space Rn. Let Kn denote the set of all convex bodies (compact,convex subsets with non-empty interiors) in Rn. We reserve the letter u for unit vectors, and the letter B is reserved for theunit ball centered at the origin. The surface of B is Sn−1. The volume of the unit n-ball is denoted by ωn. For u ∈ Sn−1, let Eudenote the hyperplane, through the origin, that is orthogonal to u. We use K u to denote the image of K under an orthogonalprojection onto the hyperplane Eu. If K1, . . . , Kn−1 ∈ Kn, we denote by v(K u

1 , . . . , K un−1) the mixed volume of the figures

K u1 , . . . , K u

n−1 in the space Eu. If K1 = · · · = Kn−1 = K , then we write v(K u) for v(K u, . . . , K u).

We use V (K) for the n-dimensional volume of convex body K . Let h(K , ·) : Sn−1→ R denote the support function of

K ∈ Kn; i.e. for u ∈ Sn−1

h(K , u) = Max{u · x : x ∈ K},

where u · x denotes the usual inner product u and x in Rn.Let δ denote the Hausdorff metric on Kn, i.e. for K , L ∈ Kn, δ(K , L) = |hK − hL|∞, where | · |∞ denotes the sup-norm

on the space of continuous functions C(Sn−1) ([1], also see [2]).

1.1. Width-integrals of convex bodies

For u ∈ Sn−1, b(K , u) =:12 (h(K , u)+ h(K , −u)) is defined to be half the width of K in the direction u. Two convex bodies

K and L are said to have similar width if there exists a constant λ > 0 such that b(K , u) = λb(L, u) for all u ∈ Sn−1. Width-integralswere first considered by Blaschke (see [3]). Thewidth-integral of index i is defined by Lutwak [4]. ForK ∈ Kn, i ∈ R

Bi(K) =1n

∫Sn−1

b(K , u)n−idS(u). (1.1)

This definition implies that the width-integral of index i is non-negative and continuous.

E-mail addresses: [email protected], [email protected] Research is supported by National Natural Science Foundation of China (10971205).

0893-9659/$ – see front matter© 2011 Elsevier Ltd. All rights reserved.doi:10.1016/j.aml.2011.08.013

C.-J. Zhao / Applied Mathematics Letters 25 (2012) 190–194 191

The following results (see [4]) will be used laterb(K + L, u) = b(K , u) + b(L, u). (1.2)

B2n ≤ V (K p), (1.3)with equality if and only if K is centered with respect to p.

1.2. Polar mixed projection bodies

The projection body ΠK of a convex body K ∈ Kn, is defined as the convex body whose support function is given by(see [5])

h(ΠK , u) = v(K u), u ∈ Sn−1.

If K1, . . . , Kn−1 ∈ Kn, then Π(K1, . . . , Kn−1) denote the mixed projection body of K1, . . . , Kn−1. Support function ofΠ(K1, . . . , Kn−1) is defined by

h(Π(K1, . . . , Kn−1), u) = v(K u1 , . . . , K u

n−1).

It is easy to see that Π(K1, . . . , Kn−1) is centered.The following property (see [5]) will be used later. If K , L, K3, . . . , Kn ∈ Kn, λ, µ > 0 andM = (K3, . . . , Kn),

Π(λK + µL,M) = λΠ(K ,M) + µΠ(L,M). (1.4)If K is a convex body that contains the origin in its interior, the polar body of K , K ∗, is defined by

K ∗:= {x ∈ Rn

|x · y ≤ 1, y ∈ K}.

If K1, . . . , Kn−1 ∈ Kn, then polar of the mixed projection body Π(K1, . . . , Kn−1) is usually written as Π∗(K1, . . . , Kn−1).If K1 = K + L and M = (K3, . . . , Kn), then the polar mixed projection body Π∗(K1, K3 . . . , Kn) is written as Π∗(K + L,M).

2. Reversed Dresher’s inequality

The well-known inequality due to Beckenbach can be stated as follows ([6], p. 27).

Theorem 2.1. If 1 ≤ p ≤ 2, and f (x), g(x) > 0, then(f (x) + g(x))pdx

(f (x) + g(x))p−1dx≤

f (x)pdx

f (x)p−1dx+

g(x)pdx

g(x)p−1dx. (2.1)

An extension of the Beckenbach’s inequality was obtained by Dresher [7] by an ingenious method, using moment-space theory.

Theorem 2.2. If p ≥ 1 ≥ r ≥ 0, f (x), g(x) ≥ 0, and φ(x) is a distribution function, then(f + g)pdφ(f + g)rdφ

1/(p−r)

f pdφf rdφ

1/(p−r)

+

gpdφg rdφ

1/(p−r)

. (2.2)

In the following, an inverse of inequality (2.2) is established.

Theorem 2.3. If p ≤ 0 ≤ r ≤ 1, f (x), g(x) ≥ 0, and φ(x) is a distribution function, then(f + g)pdφ(f + g)rdφ

1/(p−r)

f pdφf rdφ

1/(p−r)

+

gpdφg rdφ

1/(p−r)

, (2.3)

with equality if and only if the functions f and g are proportional.

We need the following lemma to prove Theorem 2.3.

Lemma 2.4 ([8], p. 61, Radon’s Inequality). If a and b are positive and 0 < p < 1, then− ap

bp−1<

∑ap∑

bp−1 , (2.4)

unless (a) and (b) are proportional.

Proof. If α1 ≥ 0, α1 ≥ 0, β1 > 0, and β2 > 0, and −1 < λ < 0, then from Radon’s inequality, we have

αλ+11

βλ1

+αλ+12

βλ2

≤(α1 + α2)

λ+1

(β1 + β2)λ, (2.5)

with equality if and only if (α) and (β) are proportional. Let

192 C.-J. Zhao / Applied Mathematics Letters 25 (2012) 190–194

α1 =

∫f pdφ

1/p

, β1 =

∫f rdφ

1/r

, (2.6)

α2 =

∫gpdφ

1/p

, β2 =

∫g rdφ

1/r

, (2.7)

and let

λ =r

p − r. (2.8)

From (2.5)–(2.8), we obtain

αλ+11

βλ1

+αλ+12

βλ2

=

f pdφ

(λ+1)/pf rdφ

λ/r +

gpdφ

(λ+1)/pg rdφ

λ/r =

f pdφf rdφ

1/(p−r)

+

gpdφg rdφ

1/(p−r)

≤(α1 + α2)

λ+1

(β1 + β2)λ=

f pdφ

1/p+

gpdφ

1/pp/(p−r)

f rdφ

1/r+

g rdφ

1/rr/(p−r) . (2.9)

Since −1 < λ =r

p−r < 0, we may assume p < 0 < r , and by Minkowski inequality for p < 0 and 0 < r ≤ 1, we haverespectively∫

f pdφ1/p

+

∫gpdφ

1/pp

∫(f + g)pdφ, (2.10)

with equality if and only if f and g are proportional, and∫f rdφ

1/r

+

∫g rdφ

1/rr

∫(f + g)rdφ. (2.11)

with equality if and only if f and g are proportional.From equality conditions for (2.5), (2.10) and (2.11), it follows that the sign of equality in (2.3) holds if and only if f and

g are proportional.From (2.9)–(2.11), inequality (2.3) follows. �

3. Dresher’s inequalities for width-integrals

3.1. Dresher-type inequality for width-integrals of convex bodies

Theorem 3.1. If K , L ∈ Kn and let p ≤ 0 ≤ r ≤ 1 and p, r ∈ R, thenBn−p(K + L)Bn−r(K + L)

1/(p−r)

Bn−p(K)

Bn−r(K)

1/(p−r)

+

Bn−p(L)Bn−r(L)

1/(p−r)

, (3.1)

with equality if and only if K and L have similar width.The inequality is reversed for p ≥ 1 ≥ r ≥ 0.

Remark 3.2. Let p = n − i and r = n − j in (3.1), and in view of p ≤ 0 ≤ r ≤ 1 ⇒ i ≥ n ≥ j ≥ n − 1, we haveBi(K + L)Bj(K + L)

1/(j−i)

Bi(K)

Bj(K)

1/(j−i)

+

Bi(L)Bj(L)

1/(j−i)

, (3.2)

with equality if and only if K and L have similar width.Taking for j = n in (3.2) and in view of Bn(K) =

1n

Sn−1 dS(u) = nωn, a constant, we obtain

Bi(K + L)1/(n−i)≥ Bi(K)1/(n−i)

+ Bi(L)1/(n−i), i ≥ n,

with equality if and only if K and L have similar width. This was previously obtained by Lutwak [4] for i < n − 1.Taking for j = n and i = 2n in (3.2), we obtain

B2n(K + L)−1/n≥ B2n(K)−1/n

+ B2n(L)−1/n, (3.3)

with equality if and only if K and L have similar width.

C.-J. Zhao / Applied Mathematics Letters 25 (2012) 190–194 193

If K , L are centered at the origin so that K + L is centered, then from (1.3) and (3.3), we have

V ((K + L)∗)−1/n≥ V (K ∗)−1/n

+ V (L∗)−1/n,

with equality if and only if K and L have similar width.

Proof of Theorem 3.1. From (1.1) and (1.2), we have

Bn−p(K + L) =1n

∫Sn−1

b(K + L, u)pdS(u) =1n

∫Sn−1

(b(K , u) + b(L, u))pdS(u) (3.4)

and

Bn−r(K + L) =1n

∫Sn−1

(b(K , u) + b(L, u))rdS(u). (3.5)

From (3.4) and (3.5) and in view of inequality (2.3), we obtainBn−p(K + L)Bn−r(K + L)

1/(p−r)

=

Sn−1(b(K , u) + b(L, u))pdS(u)Sn−1(b(K , u) + b(L, u))rdS(u)

1/(p−r)

Sn−1 b(K , u)pdS(u)Sn−1 b(K , u)rdS(u)

1/(p−r)

+

Sn−1 b(L, u)pdS(u)Sn−1 b(L, u)rdS(u)

1/(p−r)

=

Bn−p(K)

Bn−r(K)

1/(p−r)

+

Bn−p(L)Bn−r(L)

1/(p−r)

,

with equality if and only if K and L have similar width. �

3.2. Dresher-type inequality for width-integrals of mixed projection bodies

Theorem 3.3. Let K , L, K3, . . . , Kn are convex bodies in Rn and M = (K3, . . . , Kn). If p ≤ 0 ≤ r ≤ 1 and p, r ∈ R, thenBn−p(Π(K + L,M))

Bn−r(Π(K + L,M))

1/(p−r)

Bn−p(Π(K ,M))

Bn−r(Π(K ,M))

1/(p−r)

+

Bn−p(Π(L,M))

Bn−r(Π(L,M))

1/(p−r)

, (3.6)

with equality if and only if Π(K ,M) and Π(L,M) have similar width.The inequality is reversed for p ≥ 1 ≥ r ≥ 0.

Remark 3.4. Let p = n − i and r = n − j in (3.6), in view of p ≤ 0 ≤ r ≤ 1 ⇒ i ≥ n ≥ j ≥ n − 1, we haveBi(Π(K + L,M))

Bj(Π(K + L,M))

1/(j−i)

Bi(Π(K ,M))

Bj(Π(K ,M))

1/(j−i)

+

Bi(Π(L,M))

Bj(Π(L,M))

1/(j−i)

, (3.7)

with equality if and only if Π(K ,M) and Π(L,M) have similar width.Taking for j = n and i = 2n in (3.7) we have

B2n(Π(K + L,M))−1/n≥ B2n(Π(K ,M))−1/n

+ B2n(Π(L,M))−1/n, (3.8)

with equality if and only if Π(K ,M) and Π(L,M) have similar width.From (1.3) and (3.8) and in view of the projection body centered at the origin, we have

V (Π∗(K + L,M))−1/n≥ V (Π∗(K ,M))−1/n

+ V (Π∗(L,M))−1/n,

with equality if and only if Π(K ,M) and Π(L,M) have similar width. This was contained in [9,10].

Proof of Theorem 3.3. From (1.1), (1.2) and (1.4), we have

Bn−p(Π(K + L,M)) =1n

∫Sn−1

(b(Π(K ,M), u) + b(Π(L,M), u))pdS(u) (3.9)

and

Bn−r(Π(K + L,M)) =1n

∫Sn−1

(b(Π(K ,M), u) + b(Π(L,M), u))rdS(u). (3.10)

194 C.-J. Zhao / Applied Mathematics Letters 25 (2012) 190–194

From (3.9) and (3.10) and in view of inequality (2.3), we obtainBn−p(Π(K + L,M))

Bn−r(Π(K + L,M))

1/(p−r)

=

Sn−1(b(Π(K ,M), u) + b(Π(L,M), u))pdS(u)Sn−1(b(Π(K ,M), u) + b(Π(L,M), u))rdS(u)

1/(p−r)

Sn−1 b(Π(K ,M), u)pdS(u)Sn−1 b(Π(K ,M), u)rdS(u)

1/(p−r)

+

Sn−1 b(Π(L,M), u)pdS(u)Sn−1 b(Π(L,M), u)rdS(u)

1/(p−r)

=

Bn−p(Π(K ,M))

Bn−r(Π(K ,M))

1/(p−r)

+

Bn−p(Π(L,M))

Bn−r(Π(L,M))

1/(p−r)

,

with equality if and only if Π(K ,M) and Π(L,M) have similar width. �

Acknowledgments

The author expresses his sincere thanks to the two referees for their many very valuable suggestions and comments.

References

[1] R.J. Gardner, Geometric Tomography, Cambridge Univ. Press, New York, 1996.[2] R. Schneider, Convex Bodies: The Brunn–Minkowski Theory, Cambridge Univ. Press, 1993.[3] W. Blaschck, Vorlesungen über Integralgeometrie, I, Chelsea Publishing, New York, 1949.[4] E. Lutwak, Width-integrals of convex bodies, Proc. Amer. Math. Soc. 53 (1975) 435–439.[5] E. Lutwak, Inequalities for mixed projection bodies, Trans. Amer. Math. Soc. 339 (1993) 901–916.[6] E.F. Bechenbach, R. Bellman, Inequalities, Springer-Verlag, Berlin-Göttingen, Heidelberg, 1961.[7] M. Dresher, Moment spaces and inequalities, Duke Math. J. 20 (1953) 261–271.[8] G.H. Hardy, J.E. Littlewood, G. Pólya, Inequalities, Cambridge Univ. Press, Cambridge, 1934.[9] C. Zhao, G. Leng, L. Debnath, Some new Brunn–Minkowski-type inequalities in convex bodies, Inter. J. Math. Math. Sci. 2005 (2005) 895–915.

[10] C. Zhao, G. Leng, On polars of mixed projection bodies, J. Math. Anal. Appl. 316 (2006) 664–678.