Valuations and Surface Area Measures

Size: px
Start display at page:

Download "Valuations and Surface Area Measures"

Transcription

1 Valuations and Surface Area Measures Christoph Haberl and Lukas Parapatits Abstract We consider valuations defined on polytopes containing the origin which have measures on the sphere as values. We show that the classical surface area measure is essentially the only such valuation which is SL(n) contravariant of degree one. Moreover, for all real p, an L p version of the above result is established for GL(n) contravariant valuations of degree p. This provides a characterization of the L p surface area measures from the L p Brunn-Minkowski theory. Mathematics Subject Classification: 52B45, 28A0 Introduction A valuation is a map µ : Q n A, + defined on a set Q n of subsets of R n with values in an abelian semigroup such that µ(p Q) + µ(p Q) = µ(p ) + µ(q) whenever the sets P, Q, P Q, P Q are contained in Q n. Valuations were the critical ingredient in Dehn s solution of Hilbert s Third Problem and played a prominent role in geometry thereafter. Especially over recent years the theory of valuations witnessed an explosive growth (see e.g. [2 6, 9, 3 5, 20 25, 34, 39 4]). For example, it turned out that basic objects in convex geometric analysis can be characterized as valuations which are compatible with a subgroup of the affine group. Moreover, new geometric insights gained from such classification results led to strengthenings of various affine isoperimetric and Sobolev inequalities (see [8, 7, 8, 28, 30]). In this paper we classify measure valued valuations which are compatible with the general linear group. We will show that the only non-trivial examples of such valuations are surface area measures and their L p analogs. Surface area measures are a fundamental concept in the theory of convex bodies, i.e. nonempty compact convex subsets of R n. Given a convex polytope P R n, its surface area measure S(P, ) is the Borel measure on the Euclidean unit sphere S n R n

2 which is given by () S(P, ) = u N (P ) V n (F u )δ u. Here, N (P ) denotes the set of all unit facet normals of P, V n (F u ) stands for the (n )-dimensional volume of the facet corresponding to u, and δ u is the Dirac probability measure supported at u. Surface area measures can actually be associated with arbitrary convex bodies. We write K n for the space of convex bodies in R n equipped with Hausdorff distance. For a body K K n, its surface area measure S(K, ) is simply the weak limit of the measures S(P k, ), where P k is some sequence of polytopes converging to K. Surface area measures are the central object of a cornerstone of the classical Brunn- Minkowski theory: The Minkowski problem. It asks which measures on the Euclidean unit sphere are surface area measures of convex bodies. The answer to this question had a huge impact on convex geometry, geometric tomography, differential geometry, and elliptic partial differential equations (see e.g. [, 35, 38]). The first main result of this paper is a characterization of the surface area measure. We will consider valuations which are defined on polytopes containing the origin and which have measures on the sphere as values. We show that the surface area measure is essentially the only such valuation with a certain compability with the special linear group. What we mean by compatibility is contained in the following definition. Let G be a subgroup of the general linear group GL(n) and denote by M(S n ) the space of finite positive Borel measures on S n. Suppose that p R. A map µ : Q n M(S n ) defined on Q n K n is called G contravariant of degree p if f dµ(φp, ) = det φ f φ t dµ(p, ) S n S n for every map φ G, each P Q n with φp Q n, and every continuous p-homogeneous function f : R n \{o} R. Here, φ t denotes the transpose of the inverse of φ GL(n). We remark that the concept of G contravariance is simply the behavior of mixed volumes (and their L p analogs) under the action of the general linear group (see Section 2). We are now in a position to state our first main result. Throughout this article we work in R n with n 3. Convex polytopes in R n which contain the origin are denoted by Po n. Theorem. A map µ : P n o M(S n ) is an SL(n) contravariant valuation of degree if and only if there exist constants c, c 2, c 3, c 4 R with c, c 2 0 and c + c 3 0, c 2 + c 4 0 such that µ(p, ) = c S(P, ) + c 2 S( P, ) + c 3 S (P, ) + c 4 S ( P, ) 2

3 for every P P n o. The measure S (P, ) is defined similarly to the surface area measure of P but the summation in () ranges only over those facets in N (P ) which do not contain the origin. An immediate consequence of the above result is the following classification of measure valued valuations defined on all convex bodies. Corollary 2. A map µ : K n M(S n ) is a weakly continuous, translation invariant, and SL(n) contravariant valuation of degree if and only if there exist nonnegative constants c, c 2 R such that for every K K n. µ(k, ) = c S(K, ) + c 2 S( K, ) Schneider [37] previously obtained a classification of rotation contravariant valuations of degree under the additional assumption that they are defined locally. As explained before, surface area measures lie at the very core of the Brunn- Minkowski theory. Based on Firey s L p addition for convex bodies, Lutwak [26, 27] showed that the classical Brunn-Minkowski theory can be extended to an L p Brunn- Minkowski theory. The importance of this new L p theory is reflected for example in the fact that L p inequalities almost invariably turn out to be stronger than their classical counterparts. Since Lutwak s seminal work, this L p Brunn-Minkowski theory evolved enormously (see e.g. [7, 0, 7, 8, 22, 25, 28, 29, 36, 42 45]). Let p R. The analog of the surface area measure in the L p Brunn-Minkowski theory is defined as follows. For a convex polytope P Po n, the L p surface area measure S p (P, ) M(S n ) is given by S p (P, ) = h(p, u) p V n (F u )δ u, u N (P ) where N (P ) denotes the set of unit facet normals of P corresponding to facets which do not contain the origin and h(p, ) is the support function of P (see Section 2 for the precise definition). Finding necessary and sufficient conditions for a measure to be the L p surface area measure of a convex body is one of the major problems in modern convex geometric analysis. Consequently, this L p analog of the Minkowski problem has been studied intensively (see e.g. [7,6,26,43]). Solutions to the L p Minkowski problem were crucial for the proofs of affine versions of the Pólya-Szegö principle and new affine Sobolev inequalities (see [8, 7, 8, 28, 30]). The following theorem provides a characterization of L p surface area measures for all p. 3

4 Theorem 3. Let p R\{}. A map µ : Po n M(S n ) is a GL(n) contravariant valuation of degree p if and only if there exist nonnegative constants c, c 2 R such that µ(p, ) = c S p (P, ) + c 2 S p ( P, ) for every P P n o. Since the L p Brunn Minkowski theory is based on an addition which makes sense only for p, most of the L p concepts are restricted to such p s. However, the above theorem reveals that the concept of L p surface area measures is independent of p in a very natural way. For positive p, we will actually prove a stronger version of Theorem 3. It will be shown in Theorem 7 that for such p s the L p surface area measure can actually be characterized as an SL(n) contravariant valuation. Moreover, Theorem 4 will show that L p surface area measures are characterized as valuations which are SL(n) contravariant of degree p for all p R provided that their images are discrete. Recently, the next step in the evolution of the Brunn-Minkowski theory towards an Orlicz Brunn-Minkowski theory has been made (see e.g. [6, 25, 3, 32]). Whereas some elements of the L p Brunn-Minkowski theory have been generalized to an Orlicz setting, the Orlicz analog of the surface area measure is still unknown. This question actually motivated the axiomatic characterization of L p surface area measures obtained in this article. Since characterizing properties of L p surface area measures are now identified, they can possibly lead to the correct notion of Orlicz surface area measures. 2 Notation and Preliminaries In this section we collect the necessary definitions and facts about convex bodies. Excellent references for the theory of convex bodies are the books by Gardner [], Gruber [2], and Schneider [38]. We write R + for the set of positive real numbers. Given two vectors x, y R n we write x y for their standard Euclidean product. The Euclidean length of a vector x R n is denoted by x. If x R n is not equal to the zero vector, then we set x = x x. The canonical basis vectors of R n are denoted by e,..., e n. The standard simplex T n R n is the convex hull of the origin and the canonical basis vectors e,..., e n. We denote by T the intersection T n e where e stands for the hyperplane through the origin orthogonal to e. If p is positive, then we write C p + (R n ) for the space of nonnegative, continuous, p-homogeneous functions from R n to R. 4

5 For the definition of L p surface area measures we already used the notion of support functions. The precise definition is as follows. Given a convex body K K n, its support function is defined as h(k, x) = max{x y : y K}, x R n. It follows from the inclusion-exclusion principle that a valuation µ : P n o M(S n ) is uniquely determined by its values on n-dimensional simplices having one vertex at the origin and its value on {o} (see [33] for a short proof). If µ is in addition SL(n) contravariant of degree p, then the uniqueness part of Riesz s representation theorem implies that beside its behavior at the origin µ is uniquely determined by its values on the simplices st n with s > 0. We summarize this in the following lemma. Lemma 4. Let p R. A valuation µ : P n o M(S n ) which is SL(n) contravariant of degree p is uniquely determined by its values on positive multiples of the standard simplex T n and its value on {o}. A measure µ M(S n ) is called continuous if singletons have µ-measure zero. We call it discrete, if there exists a countable set N S n such that µ(s n \N) = 0. The set of all discrete members of M(S n ) is denoted by M d (S n ). Note that for µ, ν M d (S n ) we have (2) µ = ν µ(x) = ν(x) for all x S n. Here we used the convention µ(x) := µ({x}) for x S n. For every µ M(S n ) there exists a unique pair consisting of a continuous measure µ c and a discrete measure µ d such that (3) µ = µ c + µ d. Let µ : Po n M(S n ) be given. If µ is a valuation, so is µ d. Indeed, since the valuation property has to be checked only for points by (2), the assertion directly follows from the decomposition (3). Note that if µ is SL(n) contravariant of degree p, then by the uniqueness part of Riesz s representation theorem and the transformation behavior of image measures we have fdµ(φp, ) = S n f φ t dµ(p, ) S n for all p-homogeneous extensions of bounded Borel measurable functions f : S n R. In particular, the last relation holds for indicator functions of points. This yields (4) µ(φp, x ) x p = µ(p, φ t x ) φ t x p 5

6 for all P P n o, x R n \{o}, and all φ SL(n). Note that this together with (3) implies the SL(n) contravariance of degree p of µ d provided that µ is SL(n) contravariant of degree p. Surface area measures and their L p analogs were already defined in the introduction. It will be convenient for us to write S p (P, x) = S p (P, x ) x p for x R n \{o}. Similar conventions will apply to the measures S (P, ) and S o (P, ) := S(P, ) S (P, ). The following lemma guarantees that surface area measures and their L p analogs are GL(n) contravariant valuations. Lemma 5. The measures S, S, S o and the L p surface area measures S p for p are GL(n) contravariant valuations of degree p on P n o. Proof. First, assume that p. Given a p-homogeneous function f : R n \{o} R, define for v S n, { f 0 t 0, (t, v) = t p f(v) t > 0. It was shown in [33] that for such functions f : R S n R the expression Z f P = V n (F (P, v))f (h(p, v), v) v N (P ) is a real-valued valuation. Here, F (P, v) denotes the facet of P with outer unit normal vector v. Let ω be a Borel set on S n and take f(x) = I ω (x/ x ) x p, where I ω denotes the indicator function of ω. Then we have S p (P, ω) = Z f P and we see that S p is a measure valued valuation. For φ GL(n) and v S n we clearly have as well as v N (P ) φ t v N (φp ) V n (F (φp, φ t v )) = φ t v det φ V n (F (P, v)). The transformation behavior of the support function with respect to the general linear group and the homogeneity of f yield f (h(φp, φ t v ), φ t v ) = f (h(p, φ t φ t v ), φ t v ) Therefore we obtain that = f ( φ t v h(p, v), φ t v φ t v) = φ t v f (h(p, v), φ t v). V n (F (φp, φ t v ))f (h(φp, φ t v ), φ t v ) = det φ V n (F (P, v))f (h(p, v), φ t v). 6

7 This immediately implies the GL(n) contravariance of degree p of S p. For p =, the same proof yields the desired properties for S. By changing the definition of f to { f 0 t < 0, (t, v) = f(v) t 0 we obtain these properties for the surface area measure S. Therefore we also have them for S o = S S. For p > 0, the L p cosine transform of a signed finite Borel measure µ on S n is defined by C p µ(u) = u v p dµ(v), u S n. S n We need the following injectivity result: For a finite signed Borel measure µ on S n (5) C µ = 0 = µ(ω) = µ( ω), for each Borel set ω on S n. In the proof of our classification results for positive p we will make use of known characterizations of function valued valuations. Therefore, we need a translation of SL(n) contravariance to such valuations. For positive p, a function Z : Po n C p + (R n ) is called SL(n) contravariant if Z(φP )(x) = Z P (φ x) for all P Po n, each φ SL(n), and all x R n. The next two results were established in [3] and [33], respectively. Theorem 6. If Z : P n o C + (Rn ), + is an even SL(n) contravariant valuation, then there exist constants c, c 2 R such that for every P P n o. Z P = C (c S(P, ) + c 2 S (P, )) Theorem 7. Let p R + \{}. If Z : P n o C + p (R n ), + is an even SL(n) contravariant valuation, then there exists a constant c R such that for every P P n o. Z P = C p (cs p (P, )) As announced in the introduction, we briefly describe where the notion of G contravariance comes from. The basis of the L p Brunn-Minkowski theory is the following addition for convex bodies. Let p and suppose that P, Q Po n contain the origin in their interiors. For ε > 0 there exists a unique convex body P + p ε Q such that h(p + p ε Q, ) p = h(p, ) p + εh(q, ) p. 7

8 Using this addition, Lutwak [26] extended the classical case p = in order to prove that for the volume V and all p, V (P + p ε Q) V (P ) lim = h(q, u) p ds p (P, u). ε 0 + ε p S n This limit is called the L p mixed volume of P and Q and is an important notion of the L p Brunn-Minkowski theory. The L p mixed volume is denoted by V p (P, Q). Clearly we have V p (φp, Q) = det φ V p (P, φ Q) for all φ GL(n). The above integral representation and the fact that h(φ Q, u) = h(q, φ t u) imply that h(q, u) p ds p (φp, u) = det φ h(q, φ t u) p ds p (P, u). S n S n Note that pth powers of support functions are homogeneous of degree p. Moreover, Kiderlen [9] showed that differences of pth powers of support functions are dense in the space of continuous functions on S n. So the last equation immediately implies that L p surface area measures are GL(n) contravariant of degree p. 3 Functional equations Let λ (0, ) and p R. We define two families of linear maps on R n by and φ λ e = e, φ λ e 2 = ( λ)e + λe 2, φ λ e k = e k for 3 k n, ψ λ e = ( λ)e + λe 2, ψ λ e 2 = e 2, ψ λ e k = e k for 3 k n. The following functional equation for f : R + R n \{o} R will play a key role: ) ( ) (6) f(s, x) = λ p n f (sλ n, φ t λ x + ( λ) p n f s( λ) n, ψ t λ x. The next result proves that a function which satisfies (6) at certain points is homogeneous in its first argument. Lemma 8. Let p R and suppose that a function f : R + R n \{o} R satisfies (6). If x R n \{o} is a fixed point of φ t λ and ψt λ and f(, x) is bounded from below on some open interval then f(s, x) = s n p f(, x) for every s > 0. 8

9 Proof. From (6) we see that (7) f(s n, x) = λ p n f(s n λ n, x) + ( λ) p n f(s n ( λ) n, x) for every s > 0 and λ (0, ). Define a function g : R + R by g(s) = f(s n, x). Then, for every s > 0 and λ (0, ), equation (7) reads as (8) g(s) = λ p n g(sλ) + ( λ) p n g(s( λ)). Let a and b be arbitrary positive real numbers. Set s = a + b and λ = a(a + b). If we insert these particular values of s and λ in (8), then we have for all a, b > 0, (a + b) p n g(a + b) = a p n g(a) + b p n g(b). Thus the function t t p/n g(t) solves Cauchy s functional equation on R + and, by assumption, it is bounded from below on some open interval. It is well known (see e.g. [, Corollary 9]) that this implies that t p n g(t) = tg() and hence g(t) = t p n g(). Finally, the definition of g immediately yields f(s, x) = g(s n ) = s n p g() = s n p f(, x). Next, we are going to show that special solutions of (6) are determined by their values on a small set. Lemma 9. Let p R and suppose that f : R + R n \{o} R has the following properties: (i) f satisfies (6). (ii) f is positively homogeneous of degree p in the second argument. (iii) For every s R + the function f(s, ) has countable support if restricted to S n. (iv) For every x R n \{o} the function f(, x) is bounded from below on some open interval. 9

10 (v) For each π SL(n) which is induced by a permutation matrix and all (s, x) R + R n \{o} (9) f(s, πx) = f(s, x). If then f(s, x) = 0 for every (s, x) R + {±e }, f(s, x) = 0 for every (s, x) R + R n \ lin{e + + e n }. Proof. Note that (6) gives for all (s, x) R + R n \{o} and each λ (0, ), (0) f(s, ψ t λ x) = λ p n f(sλ n, φ t λ ψ t λ x) + ( λ) p n f(s( λ) n, x), () f(s, φ t λ x) = λ p p n f(sλ n, x) + ( λ) n f(s( λ) n, ψ t λ φ t λ x). For j n we use induction on the number j of non-vanishing coordinates to prove that f(s, x) = 0 for all s > 0 and every x with j non-vanishing coordinates. Let j =. Since we can always find a permutation matrix π SL(n) with e i = πe, we have f(s, ±e i ) = f(s, ±πe ) = f(s, ±e ) = 0. Since f is positively homogeneous in the second argument we infer that f(s, x) = 0 for every x with one non-vanishing coordinate. Let j < n and suppose that f(s, x) = 0 for every s > 0 and every x o with at most j non-vanishing coordinates. By (9) it is enough to prove f(s, x) = 0 for x = x e + +x j+ e j+ with x,..., x j+ 0. Suppose that 0 < x < x 2 or x 2 < x < 0 and set λ = x /x 2. Then ψ t λ x = x 2e 2 + x 3 e x j+ e j+, φ t λ ψ t λ x = x e 2 + x 3 e x j+ e j+. Relation (0) and the induction hypothesis show f(s( λ) n, x) = 0 for every s R +, and hence f(s, x) = 0 for every s R +. If 0 < x 2 < x or x < x 2 < 0, then set λ = (x x 2 )/x. Thus φ t λ x = x e + x 3 e x j+ e j+, ψλ t φ t λ x = x 2e + x 3 e x j+ e j+. Relation () and the induction hypothesis show f(sλ n, x) = 0 for every s R +, and hence f(s, x) = 0 for every s R +. 0

11 If sgn(x ) sgn(x 2 ), set λ = x /(x x 2 ). Then φ t λ x = x e + x 3 e x j+ e j+, ψ t λ x = x 2e 2 + x 3 e x j+ e j+. It follows directly from (6) that f(s, x) = 0 for every s R +. In conclusion, we proved that for x = x e + +x j+ e j+ with x,..., x j+ 0 and x x 2 we have f(s, x) = 0 for every s R +. This and (9) actually show that f(s, x) = 0 for every s R + and each x = x e + + x j+ e j+ where at least two coordinates are different. It remains to prove that f(s, x) = 0 for every s R + and x = x e + + x e j+ with x 0. By the homogeneity of f in its second argument it suffices to prove that f(s, x) = 0 for every s R + and x = e + + e j+ or x = e e j+. We consider only the case x = e + + e j+ ; the other one is treated similarly. Let 0 < λ < and set y = λe + e e j+2. Note that ψ t λ y = e 2 + e e j+2, φ t λ ψ t λ y = λe 2 + e e j+2. By what we have already shown, relation (9), and (0) we arrive at f(s, ψ t λ y) = ( λ) p n f(s( λ) n, y). From (9) and Lemma 8 we infer that f(, ψ t λ y) is positively homogeneous of degree n p, and hence ( λ) f(, ψ t λ y) = f(, y) for all 0 < λ <. If f(, ψ t λ y) = f(, e 2 + e e j+2 ) were nonzero, then f(, y) = f(, λe + e e j+2 ) would therefore be nonzero for all 0 < λ <. But since f is positively homogeneous in the second argument, this would contradict the assumption that f(, ) has countable support on S n. By homogeneity, for each s R +, we have f(s, ψ t λ y) = 0 and hence (9) gives f(s, e + + e j+ ) = 0. This concludes the induction. We showed that f(s, x) = 0 for s R + and points x with at most n nonvanishing coordinates. As in the first part of the induction we see that also f(s, x) = 0 for s R + and points x with n non-vanishing coordinates provided that at least two of them are different. 4 The case p = Lemma 0. Suppose that µ : P n o M d (S n ) is SL(n) contravariant of degree. Then there exists a constant a R + such that µ(st, ) = as n (δ e + δ e )

12 for every s R + and µ({o}, ) = 0, where T denotes the (n )-dimensional standard simplex in e. Proof. First, we show that µ(p, ) is supported at ±e k provided that P e k. So let P e k and set f(p, x) = µ(p, x ) x for x R n \{o}. Suppose that x R n is given with x j 0 for some j k. For t R define φ SL(n) by Since φp = P we get from (4) that φe k = e k + te j, φe i = e i, i {,..., n}\{k}. f(p, x) = f(φp, x) = f(p, φ t x) = f(p, (x,..., x k, x k + tx j, x k+,..., x n )). If f(p, x) 0, then f(p, (x,..., x k, x k + tx j, x k+,..., x n )) 0 for all t R. Since these correspond to uncountably many points on S n and f(p, ) restricted to S n has countable support, f(p, x) has to be zero. Consequently, f(p, ) is supported only at ±e k. In particular, the measure µ({o}, ) has to be supported at ±e as well as ±e 2. Therefore, it has to be zero. It remains to prove the formula for µ(st, ). We already know that f(st, ) is supported only at ±e. Thus Define ψ SL(n) by f(st, x) = a (s)δ e ( x ) x + a 2 (s)δ e ( x ) x. ψe = e, ψe 2 = e 3, ψe 3 = e 2, ψe i = e i, 4 i n. Then by (4) and the relation st = ψ(st ) we have f(st, e ) = f(st, e ) and therefore a (s) = a 2 (s). Finally, define τ SL(n) by τe = s n e, τe i = se i, 2 i n. Then st = τt and relation (4) again show that f(st, e ) = s n f(t, e ), which proves a (s) = s n a(). Now set a = a(). Now, we are in a position to prove Theorem. For the reader s convenience we will repeat its statement. 2

13 Theorem. A map µ : P n o M(S n ) is an SL(n) contravariant valuation of degree if and only if there exist constants c, c 2, c 3, c 4 R with c, c 2 0 and c + c 3 0, c 2 + c 4 0 such that (2) µ(p, ) = c S(P, ) + c 2 S( P, ) + c 3 S (P, ) + c 4 S ( P, ) for every P P n o. Proof. Set f(p, x) = µ d (P, x ) x, x R n \{o}, and define constants By Lemma 0 we have Hence, the function d = (n )!(f(t, e ) f(t n, e )), d 2 = (n )!f(t n, e ). f(st, x) = f(t, e )s n (δ e ( x ) + δ e ( x )) x. g(p, x) = f(p, x) d S o (P, x) d 2 S o ( P, x) is a valuation which vanishes on st. For λ (0, ) let H λ be the hyperplane through o with normal vector λe ( λ)e 2. Note that (st n ) H + λ = sφ λt n, (st n ) H λ = sψ λt n and (st n ) H λ = sφ λ T. So the valuation property of g implies that for all (s, x) R + R n \{o}, g(st n, x) + g(sφ λ T, x) = g(sφ λ T n, x) + g(sψ λ T n, x). By (4) we have g(sφ λ T, x) = λ /n g(sλ /n T, φ t λ x), g(sφ λt n, x) = λ /n g(sλ /n T n, φ t λ x), and g(sψ λ T n, x) = ( λ) /n g(s( λ) /n T n, ψλ t x). This and the fact that g vanishes on multiples of T proves (3) g(st n, x) = λ n g(sλ n T n, φ t λ x) + ( λ) n g(s( λ) n T n, ψ t λ x). Consequently, the map (s, x) g(st n, x) satisfies (6). By Lemma 8 we know that g(st n, e 3 ) = s n g(t n, e 3 ) for all positive s. But g(st n, e ) = g(st n, e 3 ) and g(t n, e ) = 0 by definition. Thus g(st n, e ) = 0 for all s R +. For x = x e + x 2 e 2 with x > 0 and x 2 < 0 set λ = x x x 2. Evaluating (3) for this x and λ, Lemma 8 together with the homogeneity of g of degree in the second argument, the equality g(st n, e ) = 0 and the definition of λ show that g(st n, x) = λ n g(sλ n T n, x e ) + ( λ) n g(s( λ) n T n, x 2 e 2 ) = λ g(st n, e ) + λ g(st n, e 2 ) x x 2 = g(st n, e 2 ). x x 2 3

14 Since g(st n, e 2 ) = g(st n, e ) and g(st n, ) has at most countable support if restricted to S n, we obtain from the last lines that also g(st n, e ) = 0. From Lemma 9 we further deduce that g(st n, ) is supported only at ± e + +e n. Define constants d 3 = g(t n, e + + e n ) S (T n, e + + e n ), d 4 = g(t n, e + + e n ) S ( T n, e + + e n ). Thus, by Lemma 8, we have g(st n, x) = d 3 S (st n, x) + d 4 S ( st n, x) and consequently µ d (st n, x) = d S(sT n, x)+d 2 S( st n, x)+(d 3 d )S (st n, x)+(d 4 d 2 )S ( st n, x). By Lemma 4 this proves (2) for the discrete part µ d. Note that P C µ(p, ) is a function from Po n to C + (Rn ) which is an even SL(n) contravariant valuation. The linearity of the cosine transform gives C µ(p, ) = C µ c (P, ) + C µ d (P, ). From Theorem 6 we know that C µ(p, ) = C (d 5 S(P, ) + d 6 S (P, )). By the discrete case we just established we know that and hence also C µ d (P, ) = C (d 7 S(P, ) + d 8 S (P, )), C µ c (P, ) = C (d 9 S(P, ) + d 0 S (P, )). In particular, we have C µ c (st, ) = d 9 C S(sT, ). By the injectivity property (5) we know that µ c (st, e ) + µ c (st, e ) = 2s n d 9 /(n )!. But since µ c (st, ) is continuous we have d 9 = 0. Thus C µ c (st n, )(e i e j ) = d 0 C S (st n, )(e i e j ) = 0 for i j n. So µ c (st n, ) has to be concentrated on each hyperplane {x i = x j }, and consequently it is concentrated at the two points ± e + + e n. The continuity of µ c (st n, ) therefore implies µ c (st n, ) = 0. So by the discrete case we have µ(st n, ) = µ d (st n, ) = c S(sT n, ) + c 2 S( st n, ) + c 3 S (st n, ) + c 4 S ( st n, ). for some constants c,..., c 4 R. Next, we want to prove that µ({o}, ) = 0. For s > 0 define φ SL(n) by φe = s e, φe 2 = se 2, φe k = e k, 3 k n. 4

15 Since φ{o} = {o} the SL(n) contravariance of µ implies µ({o}, S n ) = x dµ(φ{o}, x) S n = (s 2 x 2 + s 2 x x x 2 n) 2 dµ({o}, x). S n Take the limit s in the above equation. Then Fatou s lemma implies µ({o}, S n ) µ({o}, {x 0}). Since µ({o}, ) is finite, µ({o}, ) is supported at {x = 0}. Similarly, one shows that µ({o}, ) is supported at {x j = 0} for j = 2,..., n. This immediately implies that µ({o}, ) = 0. Lemma 4 and the fact that S(P, ) = S o (P, ) + S (P, ) therefore prove µ(p, ) = c S(P, ) + c 2 S( P, ) + c 3 S (P, ) + c 4 S ( P, ) = c S o (P, ) + c 2 S o ( P, ) + (c + c 3 )S (P, ) + (c 2 + c 4 )S ( P, ) for every P P n o. In particular as well as 0 µ(t n, e ) = c 2 /(n )! and 0 µ(t n, e ) = c /(n )!, 0 µ(t n, e + + e n ) = n(c + c 3 )/(n )!, 0 µ(t n, e + + e n ) = n(c 2 + c 4 )/(n )!, which proves the asserted relations for the constants. 5 The case p We begin by studying SL(n) contravariant valuations on lower dimensional polytopes. Lemma 2. Suppose that p and µ : Po n M(S n ) is an SL(n) contravariant valuation of degree p which vanishes on polytopes of dimension less than n. Let s R +. If µ(st, ) is supported only at the two points ±e, then µ(st, ) = 0. Proof. For λ (0, ) let H λ denote the hyperplane containing the origin with normal vector λe 2 ( λ)e 3. The valuation property of µ yields (4) µ(st, ) + µ(st H λ, ) = µ(st H + λ, ) + µ(st H λ, ). 5

16 Define maps σ, τ SL(n) by and Since σe = λ e, σe 2 = e 2, σe 3 = ( λ)e 2 + λe 3, σe k = e k, 4 k n, τe = λ e, τe 2 = ( λ)e 2 + λe 3, τe k = e k, 3 k n. st H + λ = σ(st ) and st H λ = τ(st ) and since µ vanishes on st H λ, we have Thus by (4) we obtain µ(st, ) = µ(σ(st ), ) + µ(τ(st ), ). µ(st, ±e ) = µ(σ(st ), ±e ) + µ(τ(st ), ±e ) Since p, we get µ(st, ±e ) = The discrete case = µ(st, ± σ t e ) σ t e p + µ(st, ± τ t e ) τ t e p = (λ p + ( λ) p )µ(st, ±e ). The next result concerns simplicity for valuations with discrete images. Lemma 3. Let p and suppose that µ : Po n M d (S n ) is SL(n) contravariant of degree p. Then µ(st, ) = 0 for every s R + and µ({o}, ) = 0. Proof. By Lemma 2 it is enough to show that µ(p, ) is supported at ±e k provided that P e k. So let P e k and set f(p, x) = µ(p, x ) x p for x R n \{o}. Suppose that x R n is given with x j 0 for some j k. For t R define φ SL(n) by Since φp = P, we get from (4) that φe k = e k + te j, φe i = e i, i {,..., n}\{k}. f(p, x) = f(φp, x) = f(p, φ t x) = f(p, (x,..., x k, x k + tx j, x k+,..., x n )). If f(p, x) 0, then f(p, (x,..., x k, x k + tx j, x k+,..., x n )) 0 for all t R. Since these correspond to uncountably many points on S n and f(p, ) restricted to S n has countable support, f(p, x) has to be zero. Consequently, f(p, ) is supported only at ±e k. 6

17 The main result of this section is the following classification of SL(n) contravariant valuations of degree p with discrete images. Theorem 4. Let p R\{}. A map µ : P n o M d (S n ) is an SL(n) contravariant valuation of degree p if and only if there exist nonnegative constants c, c 2 R such that µ(p, ) = c S p (P, ) + c 2 S p ( P, ) for every P P n o. By Lemmas 4 and 3, this theorem will be an immediate consequence of the following Lemma 5. Let p and µ : Po n M(S n ) be an SL(n) contravariant valuation of degree p. If, for all s > 0, µ(st, ) = 0 and µ(st n, ) is discrete, then there exist constants c, c 2 0 such that for all s > 0 µ(st n, ) = c S p (st n, ) + c 2 S p ( st n, ). Proof. For λ (0, ) let H λ be the hyperplane through o with normal vector λe ( λ)e 2. Note that (st n ) H + λ = sφ λt n, (st n ) H λ = sψ λt n, and (st n ) H λ = sφ λ T. Set f(p, x) = µ(p, x ) x p. (s, x) R + R n \{o}, Then the valuation property of µ implies that for all f(st n, x) + f(sφ λ T, x) = f(sφ λ T n, x) + f(sψ λ T n, x). From (4) and the assumption that µ vanishes on multiples of T we deduce that f(st n, x) = λ p n f(sλ n T n, φ t λ x) + ( λ) p n f(s( λ) n T n, ψ t λ x). Consequently, the map (s, x) f(st n, x) satisfies (6). Evaluating this equality at the first canonical basis vector e proves (5) f(s, e ) = λ p n f(sλ n, e + ( λ)e 2 ) + ( λ) p n f(s( λ) n, ( λ)e ). But e 3 is a fixpoint of φ t λ and ψt λ and f(s, e 3) = f(s, e ) for all positive s, hence by Lemma 8 we get f(s, e ) = s n p f(, e ) for all s > 0. Thus we obtain from (5) that ( ( λ) p )f(s, e ) = λ p n f(sλ n, e + ( λ)e 2 ). 7

18 This shows in particular that f(sλ n, e + ( λ)e 2 ) = s n p f(λ n, e + ( λ)e 2 ) for all s > 0 and each λ (0, ). Consequently and hence f(sλ n, e + ( λ)e 2 ) = s n p λ p n f(, e + ( λ)e 2 ) ( ( λ) p )λ f(s, e ) = f(s, e + ( λ)e 2 ). Since p and for fixed s the function f(s, ) has countable support if restricted to S n, we see that f(s, e ) = 0 for all s > 0. Similarly, by looking at e instead of e in the above argument, we infer f(s, e ) = 0 for all s > 0. From Lemma 9 we deduce that f(s, ) is supported only at ± e + + e n. Define constants c = f(, e + + e n ) S p (T n, e + + e n ) and c 2 = f(, e + + e n ) S p ( T n, e + + e n ). Since ± e + + e n are fixpoints of φ t λ and ψt λ, we therefore have by Lemma 8 that f(s, x) = c S p (st n, x) + c 2 S p ( st n, x) for all s > 0 and all x S n. Now, relation (2) concludes the proof. 5.2 The case p > 0 Lemma 6. Let p R + \{}. If µ : P n o M(S n ) is an SL(n) contravariant valuation of degree p, then µ(st, ) = 0 for every s > 0 and µ({o}, ) = 0. Proof. By Lemma 2 it is enough to show that µ(p, ) is supported at ±e k provided that P e k. So let P e k. For t R and j k define φ SL(n) by φe k = e k + te j, φe i = e i, i {,..., n}\{k}. Note that φp = P. Therefore the SL(n) contravariance of µ implies µ(p, S n ) = µ(φp, S n ) = x p dµ(φp, x) S n ( = x x 2 k + (x k tx j ) 2 + x 2 k+ + + x2 n S n ) p 2 dµ(p, x) If µ(p, {x j 0}) 0, then Fatou s lemma shows that the last integral goes to infinity as t tends to infinity. But this would contradict the finiteness of µ(p, ). Thus µ(p, {x j 0}) = 0, which immediately implies that µ(p, ) is supported only at ±e k. 8

19 Now, we establish the characterization of L p surface area measures for positive p which was already announced in the introduction. We emphasize again that for positive p no homogeneity assumptions are needed. It suffices to assume SL(n) contravariance instead of GL(n) contravariance. Theorem 7. Let p R + \{}. A map µ : P n o M(S n ) is an SL(n) contravariant valuation of degree p if and only if there exist nonnegative constants c, c 2 R such that µ(p, ) = c S p (P, ) + c 2 S p ( P, ) for every P P n o. Proof. Note that C p µ(p, ) : Po n Thus, by Theorem 7, we have C + p (R n ) is an even SL(n) contravariant valuation. C p µ(st n, )(e i e j ) = c C p S p (st n, )(e i e j ) = 0. for i j n. So µ(st n, ) has to be concentrated on each hyperplane {x i = x j }, and consequently it is concentrated at the two points ± e + + e n. By Lemmas 5 and 6 there exist nonnegative constants c and c 2 such that µ(st n, x) = c S p (st n, x) + c 2 S p ( st n, x) for all s > 0 and x S n. Thus, Lemma 4 concludes the proof. 5.3 The case p 0 Next, we prove the GL(n) contravariant case for non-positive p. We start with the simplicity in this case. Lemma 8. Let p 0 and µ : Po n M(S n ) be a GL(n) contravariant map of degree p. Then µ is simple, i.e. it vanishes on polytopes of dimension less than n. Proof. Without loss of generality we assume that P e. For s > 0 define φ GL(n) by φe = se, φe k = e k, 2 k n. Since φp = P, the GL(n) contravariance of µ yields µ(p, S n ) = µ(φp, S n ) = x p dµ(φp, x) S n ( ) x 2 p = s S n s 2 + x x 2 2 n µ(p, x). 9

20 Note that the integrand of the last integral is equal to ( + x 2 (/s2 ) ) p/2. Clearly, this function is greater than or equal to ( + /s 2 ) p/2 and hence µ(p, S n ) µ(p, S n )s ( + s ) p 2. 2 Now take the limit s and use the fact that µ(p, ) is a finite measure in order to arrive at µ(p, S n ) = 0. Hence µ(p, ) = 0. We are now in a position to prove Theorem 3 for non-positive p. Lemma 9. Let p 0. A map µ : P n o M(S n ) is a GL(n) contravariant valuation of degree p if and only if there exist nonnegative constants c, c 2 R such that for every P P n o. µ(p, ) = c S p (P, ) + c 2 S p ( P, ) Proof. For λ (0, ) let H λ be the hyperplane through o with normal vector λe ( λ)e 2. Recall that T n H + λ = φ λt n, T n H λ = ψ λt n and T n H λ = φ λ T. The valuation property, the simplicity derived in Lemma 8, and the GL(n) contravariance of µ yield f dµ(t n, ) = λ S n f φ t λ dµ(t n, ) + ( λ) S n f ψ t λ dµ(t n, ). S n Thus, for every continuous p-homogeneous f : R n \{o} R, we have (6) 0 = f φ t λ dµ(t n t ( λ)(f ψλ, ) + ) f dµ(t n, ). S n S n λ First, assume p < 0. Define f p (x) = ( (x x 2 ) 2 + x x2 n) p/2 for x R n \{o}. Note that f p is strictly positive and p-homogeneous. Set g p (λ, x) = f p ψ t λ = An elementary calculation shows that ( (x ) x x x 2 n λ ) p 2. (7) λ ( λ)g p(λ, x) = g p (λ, x) + p g p (λ, x) 2 (x x p 2 ) 2 ( λ) 2, 20

21 and hence ( λ)(f p ψ t λ lim ) f p (8) λ 0 + λ = λ ( λ)g p(λ, x) λ=0 = f p (x) + pf p (x) 2 p (x x 2 ) 2. Clearly we have lim λ 0 +(f p φ t λ )(x) = lim λ 0 + ( (x x 2 λ = I {x =x 2 }(x)f p (x). ) 2 ( ) x2 x x + x x 2 n λ If we take the limit λ 0 + in (6) and are allowed to interchange limit and integrals, then ( 0 = f p (x) I {x =x 2 }(x) + pf p (x) 2 p (x x 2 ) 2) dµ(t n, x). S n Since the last integrand is less than or equal to zero and equal to zero precisely for points x with x = x 2, we deduce that µ(t n, ) is concentrated on {x = x 2 }. Since by the GL(n) contravariance µ(t n, ) is invariant with respect to coordinate changes we get that µ(t n, ) is concentrated at the points ± e + + e n. In particular, µ(t n, ) is discrete. We still have to prove that we are actually allowed to interchange limit and integrals in the above argument. Since g p (λ, x) is obviously bounded on (0, /2] S n, equations (7) and (8), the mean value theorem, and the dominated convergence theorem show that we can interchange limit and integration in the second integral. In order to apply the dominated convergence theorem for the first integral it is enough to prove that the function f p φ t λ is bounded from above on (0, ) Sn. Recall that ( (x ) f p φ t λ (x) = x 2 ( 2 + x + x ) ) p 2 x x x 2 n. λ λ Define a set U = {x S n : (x x 2 ) 2 /25 or x x 2 n /25}. By the negativity of p, the function f p φ t λ is obviously bounded on (0, ) U. So suppose that x S n \U, i.e. (x x 2 ) 2 < /25 and x x2 n < /25. From these two inequalities and the fact that (x x 2 ) 2 + 2x x 2 + x x2 n = we get 2x x 2 > 2/25 = 23/25. Since x 2 we further obtain (9) x > ) p 2

22 Assume that there exists a λ (0, ) such that ( x x 2 Then we obviously must have λ ) 2 ( + x + x ) 2 x 2 + x x 2 n < λ 25. (20) as well as (2) ( x x 2 λ ) 2 < 25 ( x + x ) 2 x 2 < λ 25. But by the reverse triangle inequality, (9), and (20) we obtain x + x 2 x λ x x 2 x λ > 5, which contradicts (2). Consequently, f p φ t λ is bounded also on (0, ) S n \U, which immediately gives the desired result. For the case p = 0 set h(x) = x 3 f (x), x R n \{o}. Note that h is a nonnegative continuous 0-homogeneous function. Thus 0 = = h φ t λ dµ(t n t ( λ)(h ψλ, ) + ) h dµ(t n, ) S n S n λ x 3 (f φ t λ ) dµ(t n, ) + x 3 ( λ)(f t ψλ ) f dµ(t n, ) S n S n λ As before, we can take the limit λ 0 + in this equation and interchange limit and integration in order to arrive at 0 = x 3 f (x) ( I {x =x 2 }(x) f (x) 2 (x x 2 ) 2) dµ(t n, ). S n Thus µ(t n, ) has to be concentrated on {x 3 = 0} {x = x 2 }. Since µ(t n, ) is invariant under coordinate changes, µ(t n, ) has to be supported at { {xi = 0} {x j = x k } : i, j, k n with distinct i, j, k }. Suppose that x S n is a point in this intersection. Then either all coordinates of x are equal, or at least two are different, say x and x 2. But then all other coordinates 22

23 have to be zero. At least one of x and x 2 has to be nonzero, say x. Since x {x = 0} {x 2 = x 3 }, we have x 2 = 0 and thus x = ±. This implies that µ(t n, ) is concentrated at the points ±e i and ± e + + e n. So also in this case µ(t n, ) is discrete. By Lemmas 5 and 8 we infer that there exist constants c, c 2 0 such that for all s > 0 µ(st n, ) = c S p (st n, ) + c 2 S p ( st n, ). By the simplicity of µ we also have µ({o}, ) = 0. Lemma 4 therefore concludes the proof. Acknowledgments The work of the authors was supported by Austrian Science Fund (FWF) Project P23639-N8. References [] J. Aczél and J. Dhombres. Functional equations in several variables, volume 3 of Encyclopedia of Mathematics and its Applications. Cambridge University Press, Cambridge, 989. With applications to mathematics, information theory and to the natural and social sciences. [2] S. Alesker. Continuous rotation invariant valuations on convex sets. Ann. of Math. (2) 49 (999), [3] S. Alesker. Description of translation invariant valuations on convex sets with solution of P. McMullen s conjecture. Geom. Funct. Anal. (200), [4] S. Alesker, A. Bernig and F. Schuster. Harmonic analysis of translation invariant valuations. Geom. Funct. Anal. 2 (20), [5] A. Bernig. A Hadwiger-type theorem for the special unitary group. Geom. Funct. Anal. 9 (2009), [6] A. Bernig and J. H. G. Fu. Hermitian integral geometry. Ann. of Math (2) 73 (20), [7] K.-S. Chou and X.-J. Wang. The L p -Minkowski problem and the Minkowski problem in centroaffine geometry. Adv. Math. 205 (2006),

24 [8] A. Cianchi, E. Lutwak, D. Yang and G. Zhang. Affine Moser-Trudinger and Morrey-Sobolev inequalities. Calc. Var. Partial Differential Equations 36 (2009), [9] J. Fu. Structure of the unitary valuation algebra. J. Differential Geom. 72 (2006)(3), [0] R. Gardner and A. Giannopoulos. p-cross-section bodies. Indiana Univ. Math. J. 48 (999), [] R. J. Gardner. Geometric tomography, volume 58 of Encyclopedia of Mathematics and its Applications. Cambridge University Press, New York, second edition, [2] P. Gruber. Convex and Discrete Geometry. Springer, Berlin, [3] C. Haberl. Minkowski valuations intertwining the special linear group. J. Eur. Math. Soc., in press. [4] C. Haberl. Blaschke valuations. Amer. J. Math. 33 (20), [5] C. Haberl and M. Ludwig. A characterization of L p intersection bodies. Int. Math. Res. Not. (2006), Article ID 0548, 29 pages. [6] C. Haberl, E. Lutwak, D. Yang and G. Zhang. The even Orlicz Minkowski problem. Adv. Math 224 (200), [7] C. Haberl and F. Schuster. Asymmetric affine L p Sobolev inequalities. J. Funct. Anal. 257 (2009), [8] C. Haberl and F. Schuster. General L p affine isoperimetric inequalities. J. Differential Geom. 83 (2009), 26. [9] M. Kiderlen. Stability results for convex bodies in geometric tomography. Indiana Univ. Math. J. 57 (2008), [20] D. A. Klain. Invariant valuations on star-shaped sets. Adv. Math. 25 (997), [2] M. Ludwig. Ellipsoids and matrix valued valuations. Duke Math. J. 9 (2003), [22] M. Ludwig. Minkowski valuations. Trans. Amer. Math. Soc. 357 (2005), [23] M. Ludwig. Minkowski areas and valuations. J. Differential. Geom. 86 (200),

25 [24] M. Ludwig. Fisher information and matrix valued valuations. Adv. Math. 226 (20), [25] M. Ludwig and M. Reitzner. A classification of SL(n) invariant valuations. Ann. Math. (2) 72 (200), [26] E. Lutwak. The Brunn-Minkowski-Firey theory. I. Mixed volumes and the Minkowski problem. J. Differential Geom. 38 (993), [27] E. Lutwak. The Brunn-Minkowski-Firey theory. II: Affine and geominimal surface areas. Adv. Math. 8 (996), [28] E. Lutwak, D. Yang and G. Zhang. L p affine isoperimetric inequalities. J. Differential Geom. 56 (2000), 32. [29] E. Lutwak, D. Yang and G. Zhang. A new ellipsoid associated with convex bodies. Duke Math. J. 04 (2000), [30] E. Lutwak, D. Yang and G. Zhang. Sharp affine L p Sobolev inequalities. J. Differential Geom. 62 (2002), [3] E. Lutwak, D. Yang and G. Zhang. Orlicz centroid bodies. J. Differential Geom. 84 (200), [32] E. Lutwak, D. Yang and G. Zhang. Orlicz projection bodies. Adv. Math. 223 (200), [33] L. Parapatits. SL(n)-contravariant L p -Minkowski valuations. Trans. Amer. Math. Soc., in press. [34] L. Parapatits and F. Schuster. The Steiner Formula for Minkowski Valuations. Adv. Math., in press. [35] A. V. Pogorelov. The Minkowski Multidimensional Problem. V. H. Winston & Sons, Washington, D. C., 978. [36] D. Ryabogin and A. Zvavitch. The Fourier transform and Firey projections of convex bodies. Indiana Univ. Math. J. 53 (2004)(3), [37] R. Schneider. Kinematische Berührmaße für konvexe Körper. Abh. Math. Sem. Univ. Hamburg 44 (975), [38] R. Schneider. Convex bodies: the Brunn Minkowski theory. Cambridge Univ. Press, Cambridge,

26 [39] F. Schuster. Valuations and Busemann-Petty type problems. Adv. Math. 29 (2008), [40] F. Schuster. Crofton measures and Minkowski valuations. Duke Math. J. 54 (200), 30. [4] F. Schuster and T. Wannerer. GL(n) contravariant Minkwoski valuations. Trans. Amer. Math. Soc., in press. [42] C. Schütt and E. Werner. Surface bodies and p-affine surface area. Adv. Math. 87 (2004), [43] A. Stancu. On the number of solutions to the discrete two-dimensional L 0 - Minkowski problem. Adv. Math. 80 (2003), [44] E. Werner and D. Ye. Inequalities for mixed p-affine surface area. Math. Ann. 347 (200), [45] V. Yaskin and M. Yaskina. Centroid bodies and comparison of volumes. Indiana Univ. Math. J. 55 (2006), Christoph Haberl, Lukas Parapatits University of Salzburg Hellbrunnerstraße 34, 5020 Salzburg, Austria christoph.haberl@sbg.ac.at, lukas.parapatits@sbg.ac.at 26

Minkowski Valuations

Minkowski Valuations Minkowski Valuations Monika Ludwig Abstract Centroid and difference bodies define SL(n) equivariant operators on convex bodies and these operators are valuations with respect to Minkowski addition. We

More information

Valuations on Polytopes containing the Origin in their Interiors

Valuations on Polytopes containing the Origin in their Interiors Valuations on Polytopes containing the Origin in their Interiors Monika Ludwig Abteilung für Analysis, Technische Universität Wien Wiedner Hauptstraße 8-10/1142, 1040 Wien, Austria E-mail: monika.ludwig@tuwien.ac.at

More information

Brunn-Minkowski type inequalities for L p Blaschke- Minkowski homomorphisms

Brunn-Minkowski type inequalities for L p Blaschke- Minkowski homomorphisms Available online at www.tjnsa.com J. Nonlinear Sci. Appl. 9 (206), 6034 6040 Research Article Brunn-Minkowski type inequalities for L p Blaschke- Minkowski homomorphisms Feixiang Chen a,b,, Gangsong Leng

More information

MINKOWSKI AREAS AND VALUATIONS. Monika Ludwig. Abstract

MINKOWSKI AREAS AND VALUATIONS. Monika Ludwig. Abstract MINKOWSKI AREAS AND VALUATIONS Monika Ludwig Abstract All continuous GL(n) covariant valuations that map convex bodies to convex bodies are completely classified. This establishes a characterization of

More information

A Characterization of L p Intersection Bodies

A Characterization of L p Intersection Bodies A Characterization of L p Intersection Bodies Christoph Haberl and Monika Ludwig Dedicated to Prof. Peter M. Gruber on the occasion of his sixty-fifth birthday Abstract All GL(n) covariant L p radial valuations

More information

General Affine Surface Areas

General Affine Surface Areas General Affine Surface Areas Monika Ludwig Abstract Two families of general affine surface areas are introduced. Basic properties and affine isoperimetric inequalities for these new affine surface areas

More information

Quotient for radial Blaschke-Minkowski homomorphisms by Chang-Jian Zhao (1), Wing-Sum Cheung (2)

Quotient for radial Blaschke-Minkowski homomorphisms by Chang-Jian Zhao (1), Wing-Sum Cheung (2) Bull. Math. Soc. Sci. Math. Roumanie Tome 60 108) No. 2 2017 147 157 Quotient for radial Blaschke-Minkowski homomorphisms by Chang-Jian Zhao 1) Wing-Sum Cheung 2) Abstract Some new inequalities for quotient

More information

MINKOWSKI PROBLEM FOR POLYTOPES. α i u i = 0.

MINKOWSKI PROBLEM FOR POLYTOPES. α i u i = 0. ON THE L p MINKOWSKI PROBLEM FOR POLYTOPES DANIEL HUG, ERWIN LUTWAK, DEANE YANG, AND GAOYONG ZHANG Abstract. Two new approaches are presented to establish the existence of polytopal solutions to the discrete-data

More information

Affine surface area and convex bodies of elliptic type

Affine surface area and convex bodies of elliptic type Affine surface area and convex bodies of elliptic type Rolf Schneider Abstract If a convex body K in R n is contained in a convex body L of elliptic type (a curvature image), then it is known that the

More information

Valuations on Function Spaces

Valuations on Function Spaces Valuations on Function Spaces Monika Ludwig Dedicated to Peter M. Gruber on the occasion of his 70th birthday Abstract A short survey is given on classification results for valuations on function spaces.

More information

Crofton Measures and Minkowski Valuations

Crofton Measures and Minkowski Valuations Crofton Measures and Minkowski Valuations Franz E. Schuster Abstract. A description of continuous rigid motion compatible Minkowski valuations is established. As an application we present a Brunn Minkowski

More information

Rotation Invariant Minkowski Classes of Convex Bodies

Rotation Invariant Minkowski Classes of Convex Bodies Rotation Invariant Minkowski Classes of Convex Bodies Rolf Schneider and Franz E. Schuster Abstract A Minkowski class is a closed subset of the space of convex bodies in Euclidean space R n which is closed

More information

A VOLUME INEQUALITY FOR POLAR BODIES. Erwin Lutwak, Deane Yang and Gaoyong Zhang. Abstract

A VOLUME INEQUALITY FOR POLAR BODIES. Erwin Lutwak, Deane Yang and Gaoyong Zhang. Abstract A VOLUME INEQUALITY FOR POLAR BODIES Erwin Lutwak, Deane Yang and Gaoyong Zhang Abstract A sharp affine isoperimetric inequality is established which gives a sharp lower bound for the volume of the polar

More information

Minkowski Valuations on Convex Functions

Minkowski Valuations on Convex Functions Minkowski Valuations on Convex Functions Andrea Colesanti, Monika Ludwig and Fabian Mussnig Abstract A classification of SL(n) contravariant Minkowski valuations on convex functions and a characterization

More information

A sharp Rogers Shephard type inequality for Orlicz-difference body of planar convex bodies

A sharp Rogers Shephard type inequality for Orlicz-difference body of planar convex bodies Proc. Indian Acad. Sci. (Math. Sci. Vol. 124, No. 4, November 2014, pp. 573 580. c Indian Academy of Sciences A sharp Rogers Shephard type inequality for Orlicz-difference body of planar convex bodies

More information

GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. 2π) n

GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. 2π) n GAUSSIAN MEASURE OF SECTIONS OF DILATES AND TRANSLATIONS OF CONVEX BODIES. A. ZVAVITCH Abstract. In this paper we give a solution for the Gaussian version of the Busemann-Petty problem with additional

More information

A NEW ELLIPSOID ASSOCIATED WITH CONVEX BODIES

A NEW ELLIPSOID ASSOCIATED WITH CONVEX BODIES A NEW ELLIPSOID ASSOCIATED WITH CONVEX BODIES Erwin Lutwak, Deane Yang, and Gaoyong Zhang Department of Mathematics Polytechnic University Brooklyn, NY 11201 Abstract. It is shown that corresponding to

More information

Star bodies with completely symmetric sections

Star bodies with completely symmetric sections Star bodies with completely symmetric sections Sergii Myroshnychenko, Dmitry Ryabogin, and Christos Saroglou Abstract We say that a star body is completely symmetric if it has centroid at the origin and

More information

Gaussian Measure of Sections of convex bodies

Gaussian Measure of Sections of convex bodies Gaussian Measure of Sections of convex bodies A. Zvavitch Department of Mathematics, University of Missouri, Columbia, MO 652, USA Abstract In this paper we study properties of sections of convex bodies

More information

Christoph Haberl & Franz E. Schuster. Abstract

Christoph Haberl & Franz E. Schuster. Abstract j. differential geometry 83 2009) 1-26 GENERAL L p AFFINE ISOPERIMETRIC INEQUALITIES Christoph Haberl & Franz E. Schuster Abstract Sharp L p affine isoperimetric inequalities are established for the entire

More information

L p -Width-Integrals and Affine Surface Areas

L p -Width-Integrals and Affine Surface Areas LIBERTAS MATHEMATICA, vol XXX (2010) L p -Width-Integrals and Affine Surface Areas Chang-jian ZHAO and Mihály BENCZE Abstract. The main purposes of this paper are to establish some new Brunn- Minkowski

More information

ON THE DISCRETE LOGARITHMIC MINKOWSKI PROBLEM

ON THE DISCRETE LOGARITHMIC MINKOWSKI PROBLEM ON THE DISCRETE LOGARITHMIC MINKOWSKI PROBLEM Abstract. A new sufficient condition for the existence of a solution for the logarithmic Minkowski problem is established. This new condition contains the

More information

%HZ1EXLRS. CONVEXITY OF L p -INTERSECTION BODIES

%HZ1EXLRS. CONVEXITY OF L p -INTERSECTION BODIES %HZ1EXLRS CONVEXITY OF L p -INTERSECTION BODIES GAUTIER BERCK Abstract We extend the classical Brunn theorem to symmetric moments of convex bodies and use it to prove the convexity of the L p -intersection

More information

Banach Journal of Mathematical Analysis ISSN: (electronic)

Banach Journal of Mathematical Analysis ISSN: (electronic) Banach J. Math. Anal. 2 (2008), no., 70 77 Banach Journal of Mathematical Analysis ISSN: 735-8787 (electronic) http://www.math-analysis.org WIDTH-INTEGRALS AND AFFINE SURFACE AREA OF CONVEX BODIES WING-SUM

More information

On a Generalization of the Busemann Petty Problem

On a Generalization of the Busemann Petty Problem Convex Geometric Analysis MSRI Publications Volume 34, 1998 On a Generalization of the Busemann Petty Problem JEAN BOURGAIN AND GAOYONG ZHANG Abstract. The generalized Busemann Petty problem asks: If K

More information

Valuations on Sobolev Spaces

Valuations on Sobolev Spaces Valuations on Sobolev Spaces Monika Ludwig Abstract All affinely covariant convex-body-valued valuations on the Sobolev space W 1,1 pr n q are completely classified. It is shown that there is a unique

More information

GENERAL MIXED CHORD-INTEGRALS OF STAR BODIES

GENERAL MIXED CHORD-INTEGRALS OF STAR BODIES ROCKY MOUNTAIN JOURNAL OF MATHEMATICS Volume 46, Number 5, 206 GENERAL MIXED CHORD-INTEGRALS OF STAR BODIES YIBIN FENG AND WEIDONG WANG ABSTRACT. Mixed chord-integrals of star bodies were first defined

More information

Bulletin of the. Iranian Mathematical Society

Bulletin of the. Iranian Mathematical Society ISSN: 1017-060X (Print) ISSN: 1735-8515 (Online) Bulletin of the Iranian Mathematical Society Vol. 41 (2015), No. 3, pp. 581 590. Title: Volume difference inequalities for the projection and intersection

More information

On L p -affine surface areas

On L p -affine surface areas On L p -affine surface areas Elisabeth M. Werner Abstract Let K be a convex body in R n with centroid at 0 and B be the Euclidean unit ball in R n centered at 0. We show that lim t 0 K K t = O pk O p B,

More information

Estimates for the affine and dual affine quermassintegrals of convex bodies

Estimates for the affine and dual affine quermassintegrals of convex bodies Estimates for the affine and dual affine quermassintegrals of convex bodies Nikos Dafnis and Grigoris Paouris Abstract We provide estimates for suitable normalizations of the affine and dual affine quermassintegrals

More information

A Brunn Minkowski theory for coconvex sets of finite volume

A Brunn Minkowski theory for coconvex sets of finite volume A Brunn Minkowski theory for coconvex sets of finite volume Rolf Schneider Abstract Let C be a closed convex cone in R n, pointed and with interior points. We consider sets of the form A = C \ K, where

More information

Upper semicontinuous valuations on the space of convex discs

Upper semicontinuous valuations on the space of convex discs Upper semicontinuous valuations on the space of convex discs Monika Ludwig Abstract We show that every rigid motion invariant and upper semicontinuous valuation on the space of convex discs is a linear

More information

From the Brunn-Minkowski inequality to a class of Poincaré type inequalities

From the Brunn-Minkowski inequality to a class of Poincaré type inequalities arxiv:math/0703584v1 [math.fa] 20 Mar 2007 From the Brunn-Minkowski inequality to a class of Poincaré type inequalities Andrea Colesanti Abstract We present an argument which leads from the Brunn-Minkowski

More information

On the cells in a stationary Poisson hyperplane mosaic

On the cells in a stationary Poisson hyperplane mosaic On the cells in a stationary Poisson hyperplane mosaic Matthias Reitzner and Rolf Schneider Abstract Let X be the mosaic generated by a stationary Poisson hyperplane process X in R d. Under some mild conditions

More information

Stability results for some geometric inequalities and their functional versions

Stability results for some geometric inequalities and their functional versions Stability results for some geometric inequalities and their functional versions Umut Caglar and Elisabeth M Werner Abstract The Blaschke Santaló inequality and the L p affine isoperimetric inequalities

More information

THE LOGARITHMIC MINKOWSKI PROBLEM

THE LOGARITHMIC MINKOWSKI PROBLEM THE LOGARITHMIC MINKOWSKI PROBLEM Abstract. In analogy with the classical Minkowski problem, necessary and sufficient conditions are given to assure that a given measure on the unit sphere is the cone-volume

More information

Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian

Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian M. Novaga, B. Ruffini January 13, 2014 Abstract We prove that that the 1-Riesz capacity satisfies a Brunn-Minkowski

More information

AFFINE ISOPERIMETRIC INEQUALITIES. Erwin Lutwak, Deane Yang, and Gaoyong Zhang. Department of Mathematics Polytechnic University Brooklyn, NY 11201

AFFINE ISOPERIMETRIC INEQUALITIES. Erwin Lutwak, Deane Yang, and Gaoyong Zhang. Department of Mathematics Polytechnic University Brooklyn, NY 11201 L p AFFINE ISOPERIMETRIC INEQUALITIES Erwin Lutwak, Deane Yang, and Gaoyong Zhang Department of Mathematics Polytechnic University Brooklyn, NY 11201 Affine isoperimetric inequalities compare functionals,

More information

ON SUCCESSIVE RADII AND p-sums OF CONVEX BODIES

ON SUCCESSIVE RADII AND p-sums OF CONVEX BODIES ON SUCCESSIVE RADII AND p-sums OF CONVEX BODIES BERNARDO GONZÁLEZ AND MARÍA A. HERNÁNDEZ CIFRE Abstract. We study the behavior of the so called successive inner and outer radii with respect to the p-sums

More information

AFFINE INTEGRAL GEOMETRY FROM A DIFFERENTIABLE VIEWPOINT

AFFINE INTEGRAL GEOMETRY FROM A DIFFERENTIABLE VIEWPOINT AFFINE INTEGRAL GEOMETRY FROM A DIFFERENTIABLE VIEWPOINT DEANE YANG I dedicate this to the sixtieth birthday of Shing Tung Yau Abstract. The notion of a homogeneous contour integral is introduced and used

More information

Ginés López 1, Miguel Martín 1 2, and Javier Merí 1

Ginés López 1, Miguel Martín 1 2, and Javier Merí 1 NUMERICAL INDEX OF BANACH SPACES OF WEAKLY OR WEAKLY-STAR CONTINUOUS FUNCTIONS Ginés López 1, Miguel Martín 1 2, and Javier Merí 1 Departamento de Análisis Matemático Facultad de Ciencias Universidad de

More information

SPACES ENDOWED WITH A GRAPH AND APPLICATIONS. Mina Dinarvand. 1. Introduction

SPACES ENDOWED WITH A GRAPH AND APPLICATIONS. Mina Dinarvand. 1. Introduction MATEMATIČKI VESNIK MATEMATIQKI VESNIK 69, 1 (2017), 23 38 March 2017 research paper originalni nauqni rad FIXED POINT RESULTS FOR (ϕ, ψ)-contractions IN METRIC SPACES ENDOWED WITH A GRAPH AND APPLICATIONS

More information

NAKAJIMA S PROBLEM FOR GENERAL CONVEX BODIES

NAKAJIMA S PROBLEM FOR GENERAL CONVEX BODIES NAKAJIMA S PROBLEM FOR GENERAL CONVEX BODIES DANIEL HUG ABSTRACT. For a convex body K R n, the kth projection function of K assigns to any k-dimensional linear subspace of R n the k-volume of the orthogonal

More information

OPERATIONS BETWEEN SETS IN GEOMETRY RICHARD J. GARDNER, DANIEL HUG, AND WOLFGANG WEIL

OPERATIONS BETWEEN SETS IN GEOMETRY RICHARD J. GARDNER, DANIEL HUG, AND WOLFGANG WEIL OPERATIONS BETWEEN SETS IN GEOMETRY January 4, 2013 RICHARD J. GARDNER, DANIEL HUG, AND WOLFGANG WEIL Abstract. An investigation is launched into the fundamental characteristics of operations on and between

More information

GENERAL L p AFFINE ISOPERIMETRIC INEQUALITIES

GENERAL L p AFFINE ISOPERIMETRIC INEQUALITIES GENERAL L AFFINE ISOPERIMETRIC INEQUALITIES CHRISTOPH HABERL AND FRANZ E. SCHUSTER Abstract. Shar L affine isoerimetric inequalities are established for the entire class of L rojection bodies and the entire

More information

Chapter 1. Measure Spaces. 1.1 Algebras and σ algebras of sets Notation and preliminaries

Chapter 1. Measure Spaces. 1.1 Algebras and σ algebras of sets Notation and preliminaries Chapter 1 Measure Spaces 1.1 Algebras and σ algebras of sets 1.1.1 Notation and preliminaries We shall denote by X a nonempty set, by P(X) the set of all parts (i.e., subsets) of X, and by the empty set.

More information

SHORTEST PERIODIC BILLIARD TRAJECTORIES IN CONVEX BODIES

SHORTEST PERIODIC BILLIARD TRAJECTORIES IN CONVEX BODIES SHORTEST PERIODIC BILLIARD TRAJECTORIES IN CONVEX BODIES MOHAMMAD GHOMI Abstract. We show that the length of any periodic billiard trajectory in any convex body K R n is always at least 4 times the inradius

More information

On the approximation of a polytope by its dual L p -centroid bodies

On the approximation of a polytope by its dual L p -centroid bodies On the aroximation of a olytoe by its dual L -centroid bodies Grigoris Paouris and Elisabeth M. Werner Abstract We show that the rate of convergence on the aroximation of volumes of a convex symmetric

More information

Volumes of projection bodies of some classes of convex bodies

Volumes of projection bodies of some classes of convex bodies Volumes of projection bodies of some classes of convex bodies Christos Saroglou University of Crete Department of Mathematics Abstract Schneider posed the problem of determining the maximal value of the

More information

ORLICZ MIXED INTERSECTION BODIES

ORLICZ MIXED INTERSECTION BODIES Vol. 37 ( 07 No. 3 J. of Math. (PRC ORICZ MIXED INTERSECTION BODIES GUO Yuan-yuan, MA Tong-yi, GAO i (.School of Mathematics and Statistics, Northwest Normal University, anzhou 730070, China (.School of

More information

NAKAJIMA S PROBLEM: CONVEX BODIES OF CONSTANT WIDTH AND CONSTANT BRIGHTNESS

NAKAJIMA S PROBLEM: CONVEX BODIES OF CONSTANT WIDTH AND CONSTANT BRIGHTNESS NAKAJIMA S PROBLEM: CONVEX BODIES OF CONSTANT WIDTH AND CONSTANT BRIGHTNESS RALPH HOWARD AND DANIEL HUG Dedicated to Rolf Schneider on the occasion of his 65th birthday ABSTRACT. For a convex body K R

More information

Reflections of planar convex bodies

Reflections of planar convex bodies Reflections of planar convex bodies Rolf Schneider Abstract. It is proved that every convex body in the plane has a point such that the union of the body and its image under reflection in the point is

More information

Valuations on Convex Functions

Valuations on Convex Functions Valuations on Convex Functions Andrea Colesanti, Monika Ludwig and Fabian Mussnig Abstract All continuous, SLn) and translation invariant valuations on the space of convex functions on R n are completely

More information

Integrals of Smooth and Analytic Functions over Minkowski s Sums of Convex Sets

Integrals of Smooth and Analytic Functions over Minkowski s Sums of Convex Sets Convex Geometric Analysis MSRI Publications Volume 34, 1998 Integrals of Smooth and Analytic Functions over Minkowski s Sums of Convex Sets SEMYON ALESKER 1. Introduction and Statement of Main Results

More information

Math 530 Lecture Notes. Xi Chen

Math 530 Lecture Notes. Xi Chen Math 530 Lecture Notes Xi Chen 632 Central Academic Building, University of Alberta, Edmonton, Alberta T6G 2G1, CANADA E-mail address: xichen@math.ualberta.ca 1991 Mathematics Subject Classification. Primary

More information

Extreme points of compact convex sets

Extreme points of compact convex sets Extreme points of compact convex sets In this chapter, we are going to show that compact convex sets are determined by a proper subset, the set of its extreme points. Let us start with the main definition.

More information

STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY

STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY STABILITY RESULTS FOR THE BRUNN-MINKOWSKI INEQUALITY ALESSIO FIGALLI 1. Introduction The Brunn-Miknowski inequality gives a lower bound on the Lebesgue measure of a sumset in terms of the measures of the

More information

DAVIS WIELANDT SHELLS OF NORMAL OPERATORS

DAVIS WIELANDT SHELLS OF NORMAL OPERATORS DAVIS WIELANDT SHELLS OF NORMAL OPERATORS CHI-KWONG LI AND YIU-TUNG POON Dedicated to Professor Hans Schneider for his 80th birthday. Abstract. For a finite-dimensional operator A with spectrum σ(a), the

More information

ALEXANDER KOLDOBSKY AND ALAIN PAJOR. Abstract. We prove that there exists an absolute constant C so that µ(k) C p max. ξ S n 1 µ(k ξ ) K 1/n

ALEXANDER KOLDOBSKY AND ALAIN PAJOR. Abstract. We prove that there exists an absolute constant C so that µ(k) C p max. ξ S n 1 µ(k ξ ) K 1/n A REMARK ON MEASURES OF SECTIONS OF L p -BALLS arxiv:1601.02441v1 [math.mg] 11 Jan 2016 ALEXANDER KOLDOBSKY AND ALAIN PAJOR Abstract. We prove that there exists an absolute constant C so that µ(k) C p

More information

Convex Geometry. Otto-von-Guericke Universität Magdeburg. Applications of the Brascamp-Lieb and Barthe inequalities. Exercise 12.

Convex Geometry. Otto-von-Guericke Universität Magdeburg. Applications of the Brascamp-Lieb and Barthe inequalities. Exercise 12. Applications of the Brascamp-Lieb and Barthe inequalities Exercise 12.1 Show that if m Ker M i {0} then both BL-I) and B-I) hold trivially. Exercise 12.2 Let λ 0, 1) and let f, g, h : R 0 R 0 be measurable

More information

Exercises: Brunn, Minkowski and convex pie

Exercises: Brunn, Minkowski and convex pie Lecture 1 Exercises: Brunn, Minkowski and convex pie Consider the following problem: 1.1 Playing a convex pie Consider the following game with two players - you and me. I am cooking a pie, which should

More information

THE DUAL BRUNN-MINKOWSKI THEORY FOR BOUNDED BOREL SETS: DUAL AFFINE QUERMASSINTEGRALS AND INEQUALITIES

THE DUAL BRUNN-MINKOWSKI THEORY FOR BOUNDED BOREL SETS: DUAL AFFINE QUERMASSINTEGRALS AND INEQUALITIES June 22, 2007 THE DUAL BRUNN-MINKOWSKI THEORY FOR BOUNDED BOREL SETS: DUAL AFFINE QUERMASSINTEGRALS AND INEQUALITIES R. J. GARDNER Abstract. This paper develops a significant extension of E. Lutwak s dual

More information

The Measure Problem. Louis de Branges Department of Mathematics Purdue University West Lafayette, IN , USA

The Measure Problem. Louis de Branges Department of Mathematics Purdue University West Lafayette, IN , USA The Measure Problem Louis de Branges Department of Mathematics Purdue University West Lafayette, IN 47907-2067, USA A problem of Banach is to determine the structure of a nonnegative (countably additive)

More information

A VERY BRIEF REVIEW OF MEASURE THEORY

A VERY BRIEF REVIEW OF MEASURE THEORY A VERY BRIEF REVIEW OF MEASURE THEORY A brief philosophical discussion. Measure theory, as much as any branch of mathematics, is an area where it is important to be acquainted with the basic notions and

More information

On mixed discriminants of positively definite matrix

On mixed discriminants of positively definite matrix Also available at http://amc-journal.eu ISSN 1855-3966 printed edn., ISSN 1855-3974 electronic edn. ARS MATHEMATICA CONTEMPORANEA 9 2015 261 266 On mixed discriminants of positively definite matrix Chang-Jian

More information

RECONSTRUCTION OF CONVEX BODIES OF REVOLUTION FROM THE AREAS OF THEIR SHADOWS

RECONSTRUCTION OF CONVEX BODIES OF REVOLUTION FROM THE AREAS OF THEIR SHADOWS RECONSTRUCTION OF CONVEX BODIES OF REVOLUTION FROM THE AREAS OF THEIR SHADOWS D. RYABOGIN AND A. ZVAVITCH Abstract. In this note we reconstruct a convex body of revolution from the areas of its shadows

More information

Week 3: Faces of convex sets

Week 3: Faces of convex sets Week 3: Faces of convex sets Conic Optimisation MATH515 Semester 018 Vera Roshchina School of Mathematics and Statistics, UNSW August 9, 018 Contents 1. Faces of convex sets 1. Minkowski theorem 3 3. Minimal

More information

INEQUALITIES FOR DUAL AFFINE QUERMASSINTEGRALS

INEQUALITIES FOR DUAL AFFINE QUERMASSINTEGRALS INEQUALITIES FOR DUAL AFFINE QUERMASSINTEGRALS YUAN JUN AND LENG GANGSONG Received 18 April 2005; Revised 2 November 2005; Accepted 8 November 2005 For star bodies, the dual affine quermassintegrals were

More information

PAOLO DULIO, RICHARD J. GARDNER, AND CARLA PERI

PAOLO DULIO, RICHARD J. GARDNER, AND CARLA PERI January 31, 2015 CHARACTERIZING THE DUAL MIXED VOLUME VIA ADDITIVE FUNCTIONALS PAOLO DULIO, RICHARD J. GARDNER, AND CARLA PERI Abstract. Integral representations are obtained of positive additive functionals

More information

MINKOWSKI PROBLEM FOR POLYTOPES

MINKOWSKI PROBLEM FOR POLYTOPES ON THE L MINKOWSKI PROBLEM FOR POLYTOPES DANIEL HUG, ERWIN LUTWAK, DEANE YANG, AND GAOYONG ZHANG Abstract. Two new aroaches are resented to establish the existence of olytoal solutions to the discrete-data

More information

ON THE UNIQUENESS PROPERTY FOR PRODUCTS OF SYMMETRIC INVARIANT PROBABILITY MEASURES

ON THE UNIQUENESS PROPERTY FOR PRODUCTS OF SYMMETRIC INVARIANT PROBABILITY MEASURES Georgian Mathematical Journal Volume 9 (2002), Number 1, 75 82 ON THE UNIQUENESS PROPERTY FOR PRODUCTS OF SYMMETRIC INVARIANT PROBABILITY MEASURES A. KHARAZISHVILI Abstract. Two symmetric invariant probability

More information

Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian

Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian M. Novaga, B. Ruffini Abstract We prove that that the 1-Riesz capacity satisfies a Brunn-Minkowski inequality,

More information

DAR S CONJECTURE AND THE LOG-BRUNN-MINKOSKI INEQUALITY

DAR S CONJECTURE AND THE LOG-BRUNN-MINKOSKI INEQUALITY DAR S CONJECTURE AND THE LOG-BRUNN-MINKOSKI INEQUALITY DONGMENG XI AND GANGSONG LENG Abstract. In 999, Dar conjectured if there is a stronger version of the celebrated Brunn-Minkowski inequality. However,

More information

Introduction to Real Analysis Alternative Chapter 1

Introduction to Real Analysis Alternative Chapter 1 Christopher Heil Introduction to Real Analysis Alternative Chapter 1 A Primer on Norms and Banach Spaces Last Updated: March 10, 2018 c 2018 by Christopher Heil Chapter 1 A Primer on Norms and Banach Spaces

More information

Topological vectorspaces

Topological vectorspaces (July 25, 2011) Topological vectorspaces Paul Garrett garrett@math.umn.edu http://www.math.umn.edu/ garrett/ Natural non-fréchet spaces Topological vector spaces Quotients and linear maps More topological

More information

THE LOG-BRUNN-MINKOWSKI INEQUALITY

THE LOG-BRUNN-MINKOWSKI INEQUALITY THE LOG-BRUNN-MINKOWSKI INEQUALITY Abstract. For origin-symmetric convex bodies (i.e., the unit balls of finite dimensional Banach saces) it is conjectured that there exist a family of inequalities each

More information

On stable inversion of the attenuated Radon transform with half data Jan Boman. We shall consider weighted Radon transforms of the form

On stable inversion of the attenuated Radon transform with half data Jan Boman. We shall consider weighted Radon transforms of the form On stable inversion of the attenuated Radon transform with half data Jan Boman We shall consider weighted Radon transforms of the form R ρ f(l) = f(x)ρ(x, L)ds, L where ρ is a given smooth, positive weight

More information

The Canonical Gaussian Measure on R

The Canonical Gaussian Measure on R The Canonical Gaussian Measure on R 1. Introduction The main goal of this course is to study Gaussian measures. The simplest example of a Gaussian measure is the canonical Gaussian measure P on R where

More information

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability... Functional Analysis Franck Sueur 2018-2019 Contents 1 Metric spaces 1 1.1 Definitions........................................ 1 1.2 Completeness...................................... 3 1.3 Compactness......................................

More information

THE CONE VOLUME MEASURE OF ANTIPODAL POINTS

THE CONE VOLUME MEASURE OF ANTIPODAL POINTS THE CONE VOLUME MEASURE OF ANTIPODAL POINTS KÁROLY J BÖRÖCZKY AND PÁL HEGEDŰS Abstract The optimal condition of the cone volume measure of a pair of antipodal points is proved and analyzed Introduction

More information

On John type ellipsoids

On John type ellipsoids On John type ellipsoids B. Klartag Tel Aviv University Abstract Given an arbitrary convex symmetric body K R n, we construct a natural and non-trivial continuous map u K which associates ellipsoids to

More information

arxiv: v1 [math.mg] 26 Jul 2016

arxiv: v1 [math.mg] 26 Jul 2016 Extension of the first mixed volume to nonconvex sets Emmanuel Tsukerman University of California, Berkeley arxiv:1607.0780v1 [math.mg] 6 Jul 016 July 7, 016 Abstract We study the first mixed volume for

More information

BRUNN-MINKOWSKI INEQUALITY FOR L p -MIXED INTERSECTION BODIES

BRUNN-MINKOWSKI INEQUALITY FOR L p -MIXED INTERSECTION BODIES Miskolc Mathematical Notes HU e-issn 1787-2413 Vol. 18 (2017), No. 1, pp. 507 514 DOI: 10.18514/MMN.2017.416 BRUNN-MINKOWSKI INEQUALITY FOR L p -MIXED INTERSECTION BODIES CHANG-JIAN HAO AND MIHÁLY BENCE

More information

Isometry-Invariant Valuations on Hyperbolic Space

Isometry-Invariant Valuations on Hyperbolic Space Discrete Comput Geom OF1 OF21 (2006) DOI: 10.1007/s00454-006-1251-6 Discrete & Computational Geometry 2006 Springer Science+Business Media, Inc. Isometry-Invariant Valuations on Hyperbolic Space Daniel

More information

FURTHER STUDIES OF STRONGLY AMENABLE -REPRESENTATIONS OF LAU -ALGEBRAS

FURTHER STUDIES OF STRONGLY AMENABLE -REPRESENTATIONS OF LAU -ALGEBRAS FURTHER STUDIES OF STRONGLY AMENABLE -REPRESENTATIONS OF LAU -ALGEBRAS FATEMEH AKHTARI and RASOUL NASR-ISFAHANI Communicated by Dan Timotin The new notion of strong amenability for a -representation of

More information

GENERAL VOLUMES IN THE ORLICZ-BRUNN-MINKOWSKI THEORY AND A RELATED MINKOWSKI PROBLEM I

GENERAL VOLUMES IN THE ORLICZ-BRUNN-MINKOWSKI THEORY AND A RELATED MINKOWSKI PROBLEM I GENERAL VOLUMES IN THE ORLICZ-BRUNN-MINKOWSKI THEORY AND A RELATED MINKOWSKI PROBLEM I RICHARD J. GARDNER, DANIEL HUG, WOLFGANG WEIL, SUDAN XING, AND DEPING YE Abstract. The general volume of a star body,

More information

B. Appendix B. Topological vector spaces

B. Appendix B. Topological vector spaces B.1 B. Appendix B. Topological vector spaces B.1. Fréchet spaces. In this appendix we go through the definition of Fréchet spaces and their inductive limits, such as they are used for definitions of function

More information

POLARS AND DUAL CONES

POLARS AND DUAL CONES POLARS AND DUAL CONES VERA ROSHCHINA Abstract. The goal of this note is to remind the basic definitions of convex sets and their polars. For more details see the classic references [1, 2] and [3] for polytopes.

More information

Deviation Measures and Normals of Convex Bodies

Deviation Measures and Normals of Convex Bodies Beiträge zur Algebra und Geometrie Contributions to Algebra Geometry Volume 45 (2004), No. 1, 155-167. Deviation Measures Normals of Convex Bodies Dedicated to Professor August Florian on the occasion

More information

NONSINGULAR CURVES BRIAN OSSERMAN

NONSINGULAR CURVES BRIAN OSSERMAN NONSINGULAR CURVES BRIAN OSSERMAN The primary goal of this note is to prove that every abstract nonsingular curve can be realized as an open subset of a (unique) nonsingular projective curve. Note that

More information

Math 341: Convex Geometry. Xi Chen

Math 341: Convex Geometry. Xi Chen Math 341: Convex Geometry Xi Chen 479 Central Academic Building, University of Alberta, Edmonton, Alberta T6G 2G1, CANADA E-mail address: xichen@math.ualberta.ca CHAPTER 1 Basics 1. Euclidean Geometry

More information

1 Lesson 1: Brunn Minkowski Inequality

1 Lesson 1: Brunn Minkowski Inequality 1 Lesson 1: Brunn Minkowski Inequality A set A R n is called convex if (1 λ)x + λy A for any x, y A and any λ [0, 1]. The Minkowski sum of two sets A, B R n is defined by A + B := {a + b : a A, b B}. One

More information

Centrally Symmetric Convex Sets

Centrally Symmetric Convex Sets Journal of Convex Analysis Volume 14 (2007), No. 2, 345 351 Centrally Symmetric Convex Sets V. G. Boltyanski CIMAT, A.P. 402, 36000 Guanajuato, Gto., Mexico boltian@cimat.mx J. Jerónimo Castro CIMAT, A.P.

More information

BEST APPROXIMATIONS AND ORTHOGONALITIES IN 2k-INNER PRODUCT SPACES. Seong Sik Kim* and Mircea Crâşmăreanu. 1. Introduction

BEST APPROXIMATIONS AND ORTHOGONALITIES IN 2k-INNER PRODUCT SPACES. Seong Sik Kim* and Mircea Crâşmăreanu. 1. Introduction Bull Korean Math Soc 43 (2006), No 2, pp 377 387 BEST APPROXIMATIONS AND ORTHOGONALITIES IN -INNER PRODUCT SPACES Seong Sik Kim* and Mircea Crâşmăreanu Abstract In this paper, some characterizations of

More information

ON COHERENCE OF GRAPH PRODUCTS AND COXETER GROUPS

ON COHERENCE OF GRAPH PRODUCTS AND COXETER GROUPS ON COHERENCE OF GRAPH PRODUCTS AND COXETER GROUPS OLGA VARGHESE Abstract. Graph products and Coxeter groups are defined via vertex-edge-labeled graphs. We show that if the graph has a special shape, then

More information

A LOCALIZATION PROPERTY AT THE BOUNDARY FOR MONGE-AMPERE EQUATION

A LOCALIZATION PROPERTY AT THE BOUNDARY FOR MONGE-AMPERE EQUATION A LOCALIZATION PROPERTY AT THE BOUNDARY FOR MONGE-AMPERE EQUATION O. SAVIN. Introduction In this paper we study the geometry of the sections for solutions to the Monge- Ampere equation det D 2 u = f, u

More information

Lebesgue Measure on R n

Lebesgue Measure on R n 8 CHAPTER 2 Lebesgue Measure on R n Our goal is to construct a notion of the volume, or Lebesgue measure, of rather general subsets of R n that reduces to the usual volume of elementary geometrical sets

More information

THEOREMS, ETC., FOR MATH 515

THEOREMS, ETC., FOR MATH 515 THEOREMS, ETC., FOR MATH 515 Proposition 1 (=comment on page 17). If A is an algebra, then any finite union or finite intersection of sets in A is also in A. Proposition 2 (=Proposition 1.1). For every

More information

The small ball property in Banach spaces (quantitative results)

The small ball property in Banach spaces (quantitative results) The small ball property in Banach spaces (quantitative results) Ehrhard Behrends Abstract A metric space (M, d) is said to have the small ball property (sbp) if for every ε 0 > 0 there exists a sequence

More information

Weighted floating bodies and polytopal approximation

Weighted floating bodies and polytopal approximation Weighted floating bodies and polytopal approximation Florian Besau, Monika Ludwig and Elisabeth M. Werner Abstract Asymptotic results for weighted floating bodies are established and used to obtain new

More information