Infinitesimal form of Brunn-Minkowski type inequalities

Size: px
Start display at page:

Download "Infinitesimal form of Brunn-Minkowski type inequalities"

Transcription

1 Andrea Colesanti Università di Firenze Infinitesimal form of Brunn-Minkowski type inequalities Convex and Discrete Geometry Vienna, 4-8 July, 2016 Dedicated to professor Peter Gruber on the occasion of his 75th birthday

2 At this point of the conference it is difficult to add any word to what has been said about the relevance as a mathematician, the generosity, and the quality to be a gentlemen in any circumstance, of Peter Gruber. I simply associate myself to the previous speakers, and express my gratitude to Peter Gruber and wish him a hundred of days like this!

3 The results presented in this communication are obtained in collaboration with Galyna Livshyts and Arnaud Marsiglietti.

4 The Brunn-Minkowski inequality

5 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure.

6 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure. V n ((1 t)k + tl) 1/n (1 t)v n (K) 1/n + tv n (L) 1/n, (BM) for every K, L K n and t [0, 1].

7 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure. V n ((1 t)k + tl) 1/n (1 t)v n (K) 1/n + tv n (L) 1/n, (BM) for every K, L K n and t [0, 1]. Equivalently, the functional is concave in K n. G : K n R, K G(K) = V n (K) 1/n

8 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure. V n ((1 t)k + tl) 1/n (1 t)v n (K) 1/n + tv n (L) 1/n, (BM) for every K, L K n and t [0, 1]. Equivalently, the functional G : K n R, K G(K) = V n (K) 1/n is concave in K n. Hence (heuristically): D 2 G(K) 0, K K n, (IBM)

9 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure. V n ((1 t)k + tl) 1/n (1 t)v n (K) 1/n + tv n (L) 1/n, (BM) for every K, L K n and t [0, 1]. Equivalently, the functional G : K n R, K G(K) = V n (K) 1/n is concave in K n. Hence (heuristically): D 2 G(K) 0, K K n, (IBM) where D 2 G denotes the second variation of G.

10 The Brunn-Minkowski inequality K n = {convex bodies in R n }; V n = Lebesgue measure. V n ((1 t)k + tl) 1/n (1 t)v n (K) 1/n + tv n (L) 1/n, (BM) for every K, L K n and t [0, 1]. Equivalently, the functional G : K n R, K G(K) = V n (K) 1/n is concave in K n. Hence (heuristically): D 2 G(K) 0, K K n, (IBM) where D 2 G denotes the second variation of G. (IBM) is what we call the infinitesimal form of (BM).

11 What is the second variation of a functional?

12 What is the second variation of a functional? Let G : K n R (sufficiently smooth).

13 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function.

14 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function).

15 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function). For s [ ɛ, ɛ], and ɛ small enough, h s = h + sφ

16 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function). For s [ ɛ, ɛ], and ɛ small enough, h s = h + sφ = support function of a convex body K s C 2,+.

17 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function). For s [ ɛ, ɛ], and ɛ small enough, h s = h + sφ = support function of a convex body K s C 2,+. We set d 2 ds 2 G(K s) s=0

18 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function). For s [ ɛ, ɛ], and ɛ small enough, h s = h + sφ = support function of a convex body K s C 2,+. We set d 2 ds 2 G(K s) = (D 2 G(K) φ, φ). s=0

19 What is the second variation of a functional? Let G : K n R (sufficiently smooth). Fix a convex body K, of class C 2,+, and let h be its support function. Let φ C (S n 1 ) (test function). For s [ ɛ, ɛ], and ɛ small enough, h s = h + sφ = support function of a convex body K s C 2,+. We set d 2 ds 2 G(K s) = (D 2 G(K) φ, φ). s=0 D 2 G(K) is a quadratic form acting on test functions.

20 (BM) (IBM)

21 (BM) (IBM) Let G = V 1/n n.

22 (BM) (IBM) Let G = V 1/n n. Proposition. The (BM) inequality is equivalent to the condition (D 2 G(K) φ, φ) 0, K C 2,+, φ C (S n 1 ). (IBM)

23 (BM) (IBM) Let G = V 1/n n. Proposition. The (BM) inequality is equivalent to the condition (D 2 G(K) φ, φ) 0, K C 2,+, φ C (S n 1 ). (IBM) All in all, (BM) turns out to be equivalent to a whole class of functional inequalities.

24 (BM) (IBM) Let G = V 1/n n. Proposition. The (BM) inequality is equivalent to the condition (D 2 G(K) φ, φ) 0, K C 2,+, φ C (S n 1 ). (IBM) All in all, (BM) turns out to be equivalent to a whole class of functional inequalities. These are inequalities of Poincaré type on S n 1.

25 The standard Poincare inequality on Sn 1

26 The standard Poincaré inequality on S n 1 S n 1 φ 2 dx 1 n 1 S n 1 φ 2 dx,

27 The standard Poincaré inequality on S n 1 φ 2 dx 1 φ 2 dx, S n 1 n 1 S n 1 φ C (S n 1 ) : φdx = 0. S n 1

28 The standard Poincaré inequality on S n 1 φ 2 dx 1 φ 2 dx, S n 1 n 1 S n 1 φ C (S n 1 ) : φdx = 0. S n 1 1 The constant n 1 is sharp (equality is obtained for restriction of linear functions to S n 1 ).

29 The standard Poincaré inequality on S n 1 φ 2 dx 1 φ 2 dx, S n 1 n 1 S n 1 φ C (S n 1 ) : φdx = 0. S n 1 1 The constant n 1 is sharp (equality is obtained for restriction of linear functions to S n 1 ). An equivalent formulation is S n 1 φ 2 dx 1 S n 1 ( S n 1 φdx ) 2 1 n 1 S n 1 φ 2 dx.

30 More general Poincaré inequalities

31 More general Poincaré inequalities ( ) 2 Aφ 2 dx Bφdx S n 1 S n 1 n 1 S n 1 i,j=1 C ij φ i φ j dx.

32 More general Poincaré inequalities Here: ( ) 2 Aφ 2 dx Bφdx S n 1 S n 1 n 1 S n 1 i,j=1 C ij φ i φ j dx. φ i, i = 1,..., n 1, are the first covariant derivatives of φ.

33 More general Poincaré inequalities Here: ( ) 2 Aφ 2 dx Bφdx S n 1 S n 1 n 1 S n 1 i,j=1 C ij φ i φ j dx. φ i, i = 1,..., n 1, are the first covariant derivatives of φ. A, B are positive (smooth) functions on S n 1.

34 More general Poincaré inequalities Here: ( ) 2 Aφ 2 dx Bφdx S n 1 S n 1 n 1 S n 1 i,j=1 C ij φ i φ j dx. φ i, i = 1,..., n 1, are the first covariant derivatives of φ. A, B are positive (smooth) functions on S n 1. The matrix is positive definite. (C ij ) i,j=1...,n,

35 How (BM) is related to the Poincaré inequality?

36 How (BM) is related to the Poincaré inequality? n = 2;

37 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+,

38 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+, h = support function of K, defined on S 1 [0, 2π).

39 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+, h = support function of K, defined on S 1 [0, 2π). V 2 (K) = 1 2 2π 0 h(h + h )dt.

40 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+, h = support function of K, defined on S 1 [0, 2π). φ C ([0, 2π)); V 2 (K) = 1 2 2π 0 h(h + h )dt.

41 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+, h = support function of K, defined on S 1 [0, 2π). V 2 (K) = 1 2 2π 0 h(h + h )dt. φ C ([0, 2π)); K s K 2 such that its support function is h s := h + sφ (for small s ).

42 How (BM) is related to the Poincaré inequality? n = 2; K K 2 of class C 2,+, h = support function of K, defined on S 1 [0, 2π). V 2 (K) = 1 2 2π 0 h(h + h )dt. φ C ([0, 2π)); K s K 2 such that its support function is h s := h + sφ (for small s ). V 2 (K s ) = 1 2 2π 0 (h + sφ)(h + sφ + (h + sφ ))dt.

43 ( ) D 2 V 1/2 2 (K)φ, φ = d 2 V2 ds 2 (K s ) 0 s=0 (IBM)

44 ( ) D 2 V 1/2 2 (K)φ, φ = d 2 V2 ds 2 (K s ) 0 s=0 d 2 ds 2 2π (h + sφ)(h + sφ + (h + sφ ))dt 0. 0 s=0 (IBM)

45 ( ) D 2 V 1/2 2 (K)φ, φ = d 2 V2 ds 2 (K s ) 0 s=0 d 2 ds 2 After computations: [ 1 [V 2 (K)] 3/2 2 V 2 (K) 2π (h + sφ)(h + sφ + (h + sφ ))dt 0. 0 s=0 2π 0 (IBM) ( 2π ) 2 ] φ(φ + φ)dt φ(h + h )dt 0, 0

46 ( ) D 2 V 1/2 2 (K)φ, φ = d 2 V2 ds 2 (K s ) 0 s=0 d 2 ds 2 After computations: [ 1 [V 2 (K)] 3/2 2 V 2 (K) 2π (h + sφ)(h + sφ + (h + sφ ))dt 0. 0 s=0 2π whence (with an integration by parts) 2π 0 φ 2 dt 0 (IBM) ( 2π ) 2 ] φ(φ + φ)dt φ(h + h )dt 0, 0 ( 1 2π 2 φ(h + h )dx) 2V 2 (K) 0 2π 0 (φ ) 2 dt.

47 Infinitesimal (BM) in dimension 2

48 Infinitesimal (BM) in dimension 2 (D 2 V 1/2 2 (K) φ, φ) 0, φ

49 Infinitesimal (BM) in dimension 2 (D 2 V 1/2 2 (K) φ, φ) 0, φ 2π 0 ( φ 2 1 2π 2 dt φ(h + h )dx) 2V 2 (K) 0 2π 0 (φ ) 2 dt, φ.

50 Infinitesimal (BM) in dimension 2 (D 2 V 1/2 2 (K) φ, φ) 0, φ 2π 0 ( φ 2 1 2π 2 dt φ(h + h )dx) 2V 2 (K) 0 2π 0 (φ ) 2 dt, φ. When K is the unit ball, i.e. h 1, we get precisely the standard Poincaré inequality on S 1 : 2π 0 φ 2 dt 1 ( 2π 2 φdx) 2π 0 2π 0 (φ ) 2 dt.

51 Infinitesimal (BM) in general dimension

52 Infinitesimal (BM) in general dimension Thm. [C. 2008] Let K K n be of class C 2,+. The condition ( ) D 2 Vn 1/n φ, φ 0, φ C (S n 1 ), (IBM)

53 Infinitesimal (BM) in general dimension Thm. [C. 2008] Let K K n be of class C 2,+. The condition ( ) D 2 Vn 1/n φ, φ 0, φ C (S n 1 ), (IBM) is equivalent to tr (c ij )φ 2 dx 1 ( φ det(h ij + hδ ij )dx S n 1 V n (K) S n 1 n 1 c ij φ i φ j dx, φ C (S n 1 ). S n 1 i,j=1 ) 2

54 Infinitesimal (BM) in general dimension Thm. [C. 2008] Let K K n be of class C 2,+. The condition ( ) D 2 Vn 1/n φ, φ 0, φ C (S n 1 ), (IBM) is equivalent to tr (c ij )φ 2 dx 1 ( φ det(h ij + hδ ij )dx S n 1 V n (K) S n 1 n 1 c ij φ i φ j dx, φ C (S n 1 ). S n 1 i,j=1 Here: h ij = second covariant derivatives of h; δ ij= Kronecker symbols; (c ij ) = cofactor matrix of (h ij + hδ ij ). ) 2

55 Infinitesimal (BM) in general dimension Thm. [C. 2008] Let K K n be of class C 2,+. The condition ( ) D 2 Vn 1/n φ, φ 0, φ C (S n 1 ), (IBM) is equivalent to tr (c ij )φ 2 dx 1 ( φ det(h ij + hδ ij )dx S n 1 V n (K) S n 1 n 1 c ij φ i φ j dx, φ C (S n 1 ). S n 1 i,j=1 Here: h ij = second covariant derivatives of h; δ ij= Kronecker symbols; (c ij ) = cofactor matrix of (h ij + hδ ij ). For h 1 (K = unit ball), this is the standard Poincaré inequality on S n 1. ) 2

56 What we did

57 What we did Together with G. Livshyts and A. Marsiglietti, we studied the infinitesimal form of some conjectured inequalities of (BM) type; namely:

58 What we did Together with G. Livshyts and A. Marsiglietti, we studied the infinitesimal form of some conjectured inequalities of (BM) type; namely: the dimensional Brunn-Minkowski inequality for the Gauss measure;

59 What we did Together with G. Livshyts and A. Marsiglietti, we studied the infinitesimal form of some conjectured inequalities of (BM) type; namely: the dimensional Brunn-Minkowski inequality for the Gauss measure; the log-brunn-minkowski inequality.

60 The dimensional (BM) inequality for the Gauss measure

61 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n.

62 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n. Thm. For every K, L K n and for every t [0, 1]: γ n ((1 t)k + tl) γ n (K) 1 t γ n (L) t. (1)

63 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n. Thm. For every K, L K n and for every t [0, 1]: γ n ((1 t)k + tl) γ n (K) 1 t γ n (L) t. (1) Conjecture (Gardner-Zvavitch). For every K, L K n, centrally symmetric, [γ n ((1 t)k + tl)] 1/n (1 t)[γ n (K)] 1/n + t[γ n (L)] 1/n. (2)

64 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n. Thm. For every K, L K n and for every t [0, 1]: γ n ((1 t)k + tl) γ n (K) 1 t γ n (L) t. (1) Conjecture (Gardner-Zvavitch). For every K, L K n, centrally symmetric, [γ n ((1 t)k + tl)] 1/n (1 t)[γ n (K)] 1/n + t[γ n (L)] 1/n. (2) Remarks. (2) is stronger that (1).

65 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n. Thm. For every K, L K n and for every t [0, 1]: γ n ((1 t)k + tl) γ n (K) 1 t γ n (L) t. (1) Conjecture (Gardner-Zvavitch). For every K, L K n, centrally symmetric, [γ n ((1 t)k + tl)] 1/n (1 t)[γ n (K)] 1/n + t[γ n (L)] 1/n. (2) Remarks. (2) is stronger that (1). (2) is false without central symmetry, even if K and L contains the origin (Nayar and Tkocz, 2013).

66 The dimensional (BM) inequality for the Gauss measure Let γ n be the Gauss probability measure in R n. Thm. For every K, L K n and for every t [0, 1]: γ n ((1 t)k + tl) γ n (K) 1 t γ n (L) t. (1) Conjecture (Gardner-Zvavitch). For every K, L K n, centrally symmetric, [γ n ((1 t)k + tl)] 1/n (1 t)[γ n (K)] 1/n + t[γ n (L)] 1/n. (2) Remarks. (2) is stronger that (1). (2) is false without central symmetry, even if K and L contains the origin (Nayar and Tkocz, 2013). Gardner and Zvavitch proved (2) for rectangular boxes. Livshyts, Marsiglietti, Nayar and Zvavitch (2015) proved it in dimension 2, and in general dimension for unconditional convex bodies.

67 The infinitesimal form

68 The infinitesimal form We computed, for an arbitrary K K n of class C 2,+, ( ) D 2 γn 1/n (K)φ, φ, φ C (S n 1 ).

69 The infinitesimal form We computed, for an arbitrary K K n of class C 2,+, ( ) D 2 γn 1/n (K)φ, φ, φ C (S n 1 ). In particular we could prove the following statement. Thm. ( D 2 γ 1/n n ) (B)φ, φ 0, φ C (S n 1 ). where B is any ball centered at the origin.

70 The infinitesimal form We computed, for an arbitrary K K n of class C 2,+, ( ) D 2 γn 1/n (K)φ, φ, φ C (S n 1 ). In particular we could prove the following statement. Thm. ( D 2 γ 1/n n ) (B)φ, φ 0, φ C (S n 1 ). where B is any ball centered at the origin. Note: the perturbation φ does not need to be even.

71 The infinitesimal form We computed, for an arbitrary K K n of class C 2,+, ( ) D 2 γn 1/n (K)φ, φ, φ C (S n 1 ). In particular we could prove the following statement. Thm. ( D 2 γ 1/n n ) (B)φ, φ 0, φ C (S n 1 ). where B is any ball centered at the origin. Note: the perturbation φ does not need to be even. This indicates that the dimensional (BM) inequality for γ n is true close to the unit ball (in an appropriate sense).

72 The log-brunn-minkowski inequality (shortly)

73 The log-brunn-minkowski inequality (shortly) The log-brunn-minkowski inequality was conjectured by Böröczky, Lutwak, Yang and Zhang, who proved it in the two-dimensional case.

74 The log-brunn-minkowski inequality (shortly) The log-brunn-minkowski inequality was conjectured by Böröczky, Lutwak, Yang and Zhang, who proved it in the two-dimensional case. Subsequently, Saroglou established this inequality for unconditional convex bodies in R n.

75 The log-brunn-minkowski inequality (shortly) The log-brunn-minkowski inequality was conjectured by Böröczky, Lutwak, Yang and Zhang, who proved it in the two-dimensional case. Subsequently, Saroglou established this inequality for unconditional convex bodies in R n. As in the previous case, we computed the second variation of the relevant functional at any K K n of class C 2,+,

76 The log-brunn-minkowski inequality (shortly) The log-brunn-minkowski inequality was conjectured by Böröczky, Lutwak, Yang and Zhang, who proved it in the two-dimensional case. Subsequently, Saroglou established this inequality for unconditional convex bodies in R n. As in the previous case, we computed the second variation of the relevant functional at any K K n of class C 2,+, and we checked that it has the right sign (i.e. confirming the conjecture) when K is a ball centered at the origin.

77 The message

78 The message Various (BM) type inequalities are equivalent (or at least related) to a class of Poincaré inequalities on S n 1, which represent their infinitesimal version. This provides, in principle, a way to prove (or confute) them.

79 The message Various (BM) type inequalities are equivalent (or at least related) to a class of Poincaré inequalities on S n 1, which represent their infinitesimal version. This provides, in principle, a way to prove (or confute) them. Nevertheless, it is complicated, in general, to establish the validity of these Poincaré inequalities, and very few cases (typically, corresponding to centered balls) are accessible.

80 The message Various (BM) type inequalities are equivalent (or at least related) to a class of Poincaré inequalities on S n 1, which represent their infinitesimal version. This provides, in principle, a way to prove (or confute) them. Nevertheless, it is complicated, in general, to establish the validity of these Poincaré inequalities, and very few cases (typically, corresponding to centered balls) are accessible. Never-the-nevertheless, very recent results of E. Milman and Kolesnikov, concerning Brunn-Minkowski inequalities on Riemannian manifolds, show that in some cases this approach can be successful.

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

Around the Brunn-Minkowski inequality

Around the Brunn-Minkowski inequality Around the Brunn-Minkowski inequality Andrea Colesanti Technische Universität Berlin - Institut für Mathematik January 28, 2015 Summary Summary The Brunn-Minkowski inequality Summary The Brunn-Minkowski

More information

On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric-type inequalities

On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric-type inequalities On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric-type inequalities Galyna Livshyts, Arnaud Marsiglietti, Piotr Nayar, Artem Zvavitch June 8, 2015 Abstract In

More information

On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric type-inequalities

On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric type-inequalities On the Brunn-Minkowski inequality for general measures with applications to new isoperimetric type-inequalities Galyna Livshyts, Arnaud Marsiglietti, Piotr Nayar, Artem Zvavitch April 24, 215 Abstract

More information

RESEARCH STATEMENT GALYNA V. LIVSHYTS

RESEARCH STATEMENT GALYNA V. LIVSHYTS RESEARCH STATEMENT GALYNA V. LIVSHYTS Introduction My research is devoted to exploring the geometry of convex bodies in high dimensions, using methods and ideas from probability, harmonic analysis, differential

More information

BORELL S GENERALIZED PRÉKOPA-LEINDLER INEQUALITY: A SIMPLE PROOF. Arnaud Marsiglietti. IMA Preprint Series #2461. (December 2015)

BORELL S GENERALIZED PRÉKOPA-LEINDLER INEQUALITY: A SIMPLE PROOF. Arnaud Marsiglietti. IMA Preprint Series #2461. (December 2015) BORELL S GENERALIZED PRÉKOPA-LEINDLER INEQUALITY: A SIMPLE PROOF By Arnaud Marsiglietti IMA Preprint Series #2461 December 215 INSTITUTE FOR MATHEMATICS AND ITS APPLICATIONS UNIVERSITY OF MINNESOTA 4 Lind

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

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

arxiv: v3 [math.mg] 15 Apr 2017

arxiv: v3 [math.mg] 15 Apr 2017 ON THE TABILITY OF BRUNN-MINKOWKI TYPE INEQUALITIE ANDREA COLEANTI, GALYNA LIVHYT, ARNAUD MARIGLIETTI arxiv:66.6586v3 [math.mg] 5 Apr 27 ABTRACT. We establish the stability near a Euclidean ball of two

More information

Murat Akman. The Brunn-Minkowski Inequality and a Minkowski Problem for Nonlinear Capacities. March 10

Murat Akman. The Brunn-Minkowski Inequality and a Minkowski Problem for Nonlinear Capacities. March 10 The Brunn-Minkowski Inequality and a Minkowski Problem for Nonlinear Capacities Murat Akman March 10 Postdoc in HA Group and Postdoc at the University of Connecticut Minkowski Addition of Sets Let E 1

More information

Abstracts. Analytic and Probabilistic Techniques in Modern Convex Geometry November 7-9, 2015 University of Missouri-Columbia

Abstracts. Analytic and Probabilistic Techniques in Modern Convex Geometry November 7-9, 2015 University of Missouri-Columbia Abstracts Analytic and Probabilistic Techniques in Modern Convex Geometry November 7-9, 2015 University of Missouri-Columbia Rotations of shadows of convex bodies: Positive Results and Counterexamples

More information

Moment Measures. Bo az Klartag. Tel Aviv University. Talk at the asymptotic geometric analysis seminar. Tel Aviv, May 2013

Moment Measures. Bo az Klartag. Tel Aviv University. Talk at the asymptotic geometric analysis seminar. Tel Aviv, May 2013 Tel Aviv University Talk at the asymptotic geometric analysis seminar Tel Aviv, May 2013 Joint work with Dario Cordero-Erausquin. A bijection We present a correspondence between convex functions and Borel

More information

Citation for the original published paper (version of record):

Citation for the original published paper (version of record): http://www.diva-portal.org Preprint This is the submitted version of a paper published in Advances in Mathematics. Citation for the original published paper (version of record): Colesanti, A., Nyström,

More information

1 First and second variational formulas for area

1 First and second variational formulas for area 1 First and second variational formulas for area In this chapter, we will derive the first and second variational formulas for the area of a submanifold. This will be useful in our later discussion on

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

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

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

Information Theoretic Inequalities for Contoured Probability Distributions

Information Theoretic Inequalities for Contoured Probability Distributions 1 Information Theoretic Inequalities for Contoured Probability Distributions Onur G. Guleryuz, Erwin Lutwak, Deane Yang, Gaoyong Zhang O. G. Guleryuz (onur@vision.poly.edu) is with the Department of Electrical

More information

Irrational constructions in Convex Geometry

Irrational constructions in Convex Geometry Irrational constructions in Convex Geometry Vitali Milman and Liran Rotem 1 Introduction We begin by quickly recalling some basic definitions from convex geometry. We refer the reader to [0] for more information.

More information

Eigenvalues of Collapsing Domains and Drift Laplacian

Eigenvalues of Collapsing Domains and Drift Laplacian Eigenvalues of Collapsing Domains and Drift Laplacian Zhiqin Lu Dedicate to Professor Peter Li on his 60th Birthday Department of Mathematics, UC Irvine, Irvine CA 92697 January 17, 2012 Zhiqin Lu, Dept.

More information

ANALYTIC DEFINITIONS FOR HYPERBOLIC OBJECTS. 0. Introduction

ANALYTIC DEFINITIONS FOR HYPERBOLIC OBJECTS. 0. Introduction Trends in Mathematics Information Center for Mathematical Sciences Volume 5, Number 1,June 00, Pages 11 15 ANALYTIC DEFINITIONS FOR HYPERBOLIC OBJECTS YUNHI CHO AND HYUK KIM Abstract We can extend the

More information

Brunn Minkowski Theory in Minkowski space-times. François Fillastre Université de Cergy Pontoise France

Brunn Minkowski Theory in Minkowski space-times. François Fillastre Université de Cergy Pontoise France Brunn Minkowski Theory in Minkowski space-times François Fillastre Université de Cergy Pontoise France Convex bodies A convex body is a (non empty) compact convex set of R d+1 Convex bodies A convex body

More information

Calderón-Zygmund inequality on noncompact Riem. manifolds

Calderón-Zygmund inequality on noncompact Riem. manifolds The Calderón-Zygmund inequality on noncompact Riemannian manifolds Institut für Mathematik Humboldt-Universität zu Berlin Geometric Structures and Spectral Invariants Berlin, May 16, 2014 This talk is

More information

Heat kernels of some Schrödinger operators

Heat kernels of some Schrödinger operators Heat kernels of some Schrödinger operators Alexander Grigor yan Tsinghua University 28 September 2016 Consider an elliptic Schrödinger operator H = Δ + Φ, where Δ = n 2 i=1 is the Laplace operator in R

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

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

Super-Gaussian directions of random vectors

Super-Gaussian directions of random vectors Super-Gaussian directions of random vectors Bo az Klartag Abstract We establish the following universality property in high dimensions: Let be a random vector with density in R n. The density function

More information

Analogs of Hodge Riemann relations

Analogs of Hodge Riemann relations Analogs of Hodge Riemann relations in algebraic geometry, convex geometry and linear algebra V. Timorin State University of New York at Stony Brook March 28, 2006 Hodge Riemann form Let X be a compact

More information

An introduction to Birkhoff normal form

An introduction to Birkhoff normal form An introduction to Birkhoff normal form Dario Bambusi Dipartimento di Matematica, Universitá di Milano via Saldini 50, 0133 Milano (Italy) 19.11.14 1 Introduction The aim of this note is to present an

More information

Transport Continuity Property

Transport Continuity Property On Riemannian manifolds satisfying the Transport Continuity Property Université de Nice - Sophia Antipolis (Joint work with A. Figalli and C. Villani) I. Statement of the problem Optimal transport on Riemannian

More information

On the analogue of the concavity of entropy power in the Brunn-Minkowski theory

On the analogue of the concavity of entropy power in the Brunn-Minkowski theory On the analogue of the concavity of entropy power in the Brunn-Minkowski theory Matthieu Fradelizi and Arnaud Marsiglietti Université Paris-Est, LAMA (UMR 8050), UPEMLV, UPEC, CNRS, F-77454, Marne-la-Vallée,

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

ON A DISCRETE BRUNN-MINKOWSKI TYPE INEQUALITY

ON A DISCRETE BRUNN-MINKOWSKI TYPE INEQUALITY ON DISCRETE BRUNN-MINKOWSKI TYPE INEQULITY MRÍ. HERNÁNDEZ CIFRE, DVID IGLESIS, ND JESÚS YEPES NICOLÁS bstract. The Brunn-Minkowski inequality states that the volume of compact sets K, L R n satisfies volk

More information

On the analogue of the concavity of entropy power in the Brunn-Minkowski theory

On the analogue of the concavity of entropy power in the Brunn-Minkowski theory On the analogue of the concavity of entropy power in the Brunn-Minkowski theory Matthieu Fradelizi and Arnaud Marsiglietti Laboratoire d Analyse et de Mathématiques Appliquées, Université Paris-Est Marne-la-Vallée,

More information

Approximately Gaussian marginals and the hyperplane conjecture

Approximately Gaussian marginals and the hyperplane conjecture Approximately Gaussian marginals and the hyperplane conjecture Tel-Aviv University Conference on Asymptotic Geometric Analysis, Euler Institute, St. Petersburg, July 2010 Lecture based on a joint work

More information

Super-Gaussian directions of random vectors

Super-Gaussian directions of random vectors Weizmann Institute & Tel Aviv University IMU-INdAM Conference in Analysis, Tel Aviv, June 2017 Gaussian approximation Many distributions in R n, for large n, have approximately Gaussian marginals. Classical

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

Convex inequalities, isoperimetry and spectral gap III

Convex inequalities, isoperimetry and spectral gap III Convex inequalities, isoperimetry and spectral gap III Jesús Bastero (Universidad de Zaragoza) CIDAMA Antequera, September 11, 2014 Part III. K-L-S spectral gap conjecture KLS estimate, through Milman's

More information

On the cosmic no-hair conjecture in the Einstein-Vlasov setting

On the cosmic no-hair conjecture in the Einstein-Vlasov setting On the cosmic no-hair conjecture in the Einstein-Vlasov setting KTH, Royal Institute of Technology, Stockholm Recent Advances in Mathematical General Relativity Institut Henri Poincaré, Paris September

More information

On isotropicity with respect to a measure

On isotropicity with respect to a measure On isotropicity with respect to a measure Liran Rotem Abstract A body is said to be isoptropic with respect to a measure µ if the function θ x, θ dµ(x) is constant on the unit sphere. In this note, we

More information

Shape optimization problems for variational functionals under geometric constraints

Shape optimization problems for variational functionals under geometric constraints Shape optimization problems for variational functionals under geometric constraints Ilaria Fragalà 2 nd Italian-Japanese Workshop Cortona, June 20-24, 2011 The variational functionals The first Dirichlet

More information

On the distance between homotopy classes of maps between spheres

On the distance between homotopy classes of maps between spheres On the distance between homotopy classes of maps between spheres Shay Levi and Itai Shafrir February 18, 214 Department of Mathematics, Technion - I.I.T., 32 Haifa, ISRAEL Dedicated with great respect

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

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

Quantum field theory and the Ricci flow

Quantum field theory and the Ricci flow Quantum field theory and the Ricci flow Daniel Friedan Department of Physics & Astronomy Rutgers the State University of New Jersey, USA Natural Science Institute, University of Iceland Mathematics Colloquium

More information

Randomized isoperimetric inequalities

Randomized isoperimetric inequalities Randomized isoperimetric inequalities Grigoris Paouris Peter Pivovarov May 6, 2016 Abstract We discuss isoperimetric inequalities for convex sets. These include the classical isoperimetric inequality and

More information

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true 3 ohn Nirenberg inequality, Part I A function ϕ L () belongs to the space BMO() if sup ϕ(s) ϕ I I I < for all subintervals I If the same is true for the dyadic subintervals I D only, we will write ϕ BMO

More information

Poincaré Inequalities and Moment Maps

Poincaré Inequalities and Moment Maps Tel-Aviv University Analysis Seminar at the Technion, Haifa, March 2012 Poincaré-type inequalities Poincaré-type inequalities (in this lecture): Bounds for the variance of a function in terms of the gradient.

More information

THE DOUBLE COVER RELATIVE TO A CONVEX DOMAIN AND THE RELATIVE ISOPERIMETRIC INEQUALITY

THE DOUBLE COVER RELATIVE TO A CONVEX DOMAIN AND THE RELATIVE ISOPERIMETRIC INEQUALITY J. Aust. Math. Soc. 80 (2006), 375 382 THE DOUBLE COVER RELATIVE TO A CONVEX DOMAIN AND THE RELATIVE ISOPERIMETRIC INEQUALITY JAIGYOUNG CHOE (Received 18 March 2004; revised 16 February 2005) Communicated

More information

High-dimensional distributions with convexity properties

High-dimensional distributions with convexity properties High-dimensional distributions with convexity properties Bo az Klartag Tel-Aviv University A conference in honor of Charles Fefferman, Princeton, May 2009 High-Dimensional Distributions We are concerned

More information

A Lower Bound on the Differential Entropy of Log-Concave Random Vectors with Applications

A Lower Bound on the Differential Entropy of Log-Concave Random Vectors with Applications entropy Article A Lower Bound on the Differential Entropy of Log-Concave Random Vectors with Applications Arnaud Marsiglietti, * and Victoria Kostina Center for the Mathematics of Information, California

More information

MATH 426, TOPOLOGY. p 1.

MATH 426, TOPOLOGY. p 1. MATH 426, TOPOLOGY THE p-norms In this document we assume an extended real line, where is an element greater than all real numbers; the interval notation [1, ] will be used to mean [1, ) { }. 1. THE p

More information

Characterization of Self-Polar Convex Functions

Characterization of Self-Polar Convex Functions Characterization of Self-Polar Convex Functions Liran Rotem School of Mathematical Sciences, Tel-Aviv University, Tel-Aviv 69978, Israel Abstract In a work by Artstein-Avidan and Milman the concept of

More information

Logarithmic Sobolev Inequalities

Logarithmic Sobolev Inequalities Logarithmic Sobolev Inequalities M. Ledoux Institut de Mathématiques de Toulouse, France logarithmic Sobolev inequalities what they are, some history analytic, geometric, optimal transportation proofs

More information

Christoffel Symbols. 1 In General Topologies. Joshua Albert. September 28, W. First we say W : λ n = x µ (λ) so that the world

Christoffel Symbols. 1 In General Topologies. Joshua Albert. September 28, W. First we say W : λ n = x µ (λ) so that the world Christoffel Symbols Joshua Albert September 28, 22 In General Topoloies We have a metric tensor nm defined by, Note by some handy theorem that for almost any continuous function F (L), equation 2 still

More information

Adiabatic Paths and Pseudoholomorphic Curves

Adiabatic Paths and Pseudoholomorphic Curves ESI The Erwin Schrödinger International Boltzmanngasse 9 Institute for Mathematical Physics A-1090 Wien, Austria Adiabatic Paths and Pseudoholomorphic Curves A.G. Sergeev Vienna, Preprint ESI 1676 (2005)

More information

Spectral Gap and Concentration for Some Spherically Symmetric Probability Measures

Spectral Gap and Concentration for Some Spherically Symmetric Probability Measures Spectral Gap and Concentration for Some Spherically Symmetric Probability Measures S.G. Bobkov School of Mathematics, University of Minnesota, 127 Vincent Hall, 26 Church St. S.E., Minneapolis, MN 55455,

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

The Log-Convex Density Conjecture and tangential surface area in R n {0}

The Log-Convex Density Conjecture and tangential surface area in R n {0} The Log-Convex Density Conjecture and tangential surface area in R n {0} (or vertical surface area in warped products). arxiv:1107.4402 Sean Howe (seanpkh@gmail.com) Universiteit Leiden and Université

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

8.324 Relativistic Quantum Field Theory II

8.324 Relativistic Quantum Field Theory II 8.3 Relativistic Quantum Field Theory II MIT OpenCourseWare Lecture Notes Hong Liu, Fall 010 Lecture Firstly, we will summarize our previous results. We start with a bare Lagrangian, L [ 0, ϕ] = g (0)

More information

PROD. TYPE: COM ARTICLE IN PRESS. Andrea Colesanti. Received 4 August 2003; accepted 8 June 2004 Communicated by Michael Hopkins

PROD. TYPE: COM ARTICLE IN PRESS. Andrea Colesanti. Received 4 August 2003; accepted 8 June 2004 Communicated by Michael Hopkins YAIMA28.0. pp: - (col.fig.: nil) PROD. TYPE: COM ED: Suraina PAGN: Vidya -- SCAN: Girish Advances in Mathematics ( ) www.elsevier.com/locate/aim 2 2 Brunn Minkowski inequalities for variational functionals

More information

VARIATIONS OF A CLASS OF MONGE-AMPÈRE TYPE FUNCTIONALS AND THEIR APPLICATIONS. 1. Introduction

VARIATIONS OF A CLASS OF MONGE-AMPÈRE TYPE FUNCTIONALS AND THEIR APPLICATIONS. 1. Introduction VARIATIONS OF A CLASS OF MONGE-AMPÈRE TYPE FUNCTIONALS AND THEIR APPLICATIONS HAODI CHEN, SHIBING CHEN, AND QI-RUI LI Abstract. In this paper, we study a class of Monge-Ampère type functionals arising

More information

Lecture 2: Isoperimetric methods for the curve-shortening flow and for the Ricci flow on surfaces

Lecture 2: Isoperimetric methods for the curve-shortening flow and for the Ricci flow on surfaces Lecture 2: Isoperimetric methods for the curve-shortening flow and for the Ricci flow on surfaces Ben Andrews Mathematical Sciences Institute, Australian National University Winter School of Geometric

More information

Probabilistic Methods in Asymptotic Geometric Analysis.

Probabilistic Methods in Asymptotic Geometric Analysis. Probabilistic Methods in Asymptotic Geometric Analysis. C. Hugo Jiménez PUC-RIO, Brazil September 21st, 2016. Colmea. RJ 1 Origin 2 Normed Spaces 3 Distribution of volume of high dimensional convex bodies

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

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

An Introduction to Riemann-Finsler Geometry

An Introduction to Riemann-Finsler Geometry D. Bao S.-S. Chern Z. Shen An Introduction to Riemann-Finsler Geometry With 20 Illustrations Springer Contents Preface Acknowledgments vn xiii PART ONE Finsler Manifolds and Their Curvature CHAPTER 1 Finsler

More information

Quadratic forms. Here. Thus symmetric matrices are diagonalizable, and the diagonalization can be performed by means of an orthogonal matrix.

Quadratic forms. Here. Thus symmetric matrices are diagonalizable, and the diagonalization can be performed by means of an orthogonal matrix. Quadratic forms 1. Symmetric matrices An n n matrix (a ij ) n ij=1 with entries on R is called symmetric if A T, that is, if a ij = a ji for all 1 i, j n. We denote by S n (R) the set of all n n symmetric

More information

Some problems involving fractional order operators

Some problems involving fractional order operators Some problems involving fractional order operators Universitat Politècnica de Catalunya December 9th, 2009 Definition ( ) γ Infinitesimal generator of a Levy process Pseudo-differential operator, principal

More information

A GEODESIC EQUATION IN THE SPACE OF SASAKIAN METRICS. Dedicated to Professor S.T. Yau on the occasion of his 60th birthday

A GEODESIC EQUATION IN THE SPACE OF SASAKIAN METRICS. Dedicated to Professor S.T. Yau on the occasion of his 60th birthday A GEODESIC EQUATION IN THE SPACE OF SASAKIAN ETRICS PENGFEI GUAN AND XI ZHANG Dedicated to Professor S.T. Yau on the occasion of his 60th birthday This paper is to draw attention to a geodesic equation

More information

Decouplings and applications

Decouplings and applications April 27, 2018 Let Ξ be a collection of frequency points ξ on some curved, compact manifold S of diameter 1 in R n (e.g. the unit sphere S n 1 ) Let B R = B(c, R) be a ball with radius R 1. Let also a

More information

Simplices. Rolf Schneider

Simplices. Rolf Schneider Simplices Rolf Schneider These two lectures are about extremal properties of simplices in the affine geometry of convex bodies. I begin with the well-known fact that the space of affine equivalence classes

More information

DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17

DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17 DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17 6. Geodesics A parametrized line γ : [a, b] R n in R n is straight (and the parametrization is uniform) if the vector γ (t) does not depend on t. Thus,

More information

Manifolds in Fluid Dynamics

Manifolds in Fluid Dynamics Manifolds in Fluid Dynamics Justin Ryan 25 April 2011 1 Preliminary Remarks In studying fluid dynamics it is useful to employ two different perspectives of a fluid flowing through a domain D. The Eulerian

More information

Needle decompositions and Ricci curvature

Needle decompositions and Ricci curvature Tel Aviv University CMC conference: Analysis, Geometry, and Optimal Transport KIAS, Seoul, June 2016. A trailer (like in the movies) In this lecture we will not discuss the following: Let K 1, K 2 R n

More information

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011 LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS S. G. Bobkov and F. L. Nazarov September 25, 20 Abstract We study large deviations of linear functionals on an isotropic

More information

LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS

LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS 1. The Bishop-Gromov Volume Comparison Theorem Recall that the Riemannian volume density is defined, in an open chart, to be

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

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

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

31st Jerusalem Winter School in Theoretical Physics: Problem Set 2

31st Jerusalem Winter School in Theoretical Physics: Problem Set 2 31st Jerusalem Winter School in Theoretical Physics: Problem Set Contents Frank Verstraete: Quantum Information and Quantum Matter : 3 : Solution to Problem 9 7 Daniel Harlow: Black Holes and Quantum Information

More information

Geometric Functional Analysis College Station July Titles/Abstracts. Sourav Chatterjee. Nonlinear large deviations

Geometric Functional Analysis College Station July Titles/Abstracts. Sourav Chatterjee. Nonlinear large deviations Geometric Functional Analysis College Station 25-29 July 2016 Titles/Abstracts 1 Mini-courses Sourav Chatterjee Nonlinear large deviations I will talk about a general technique for computing large deviations

More information

Iterations of the projection body operator and a remark on Petty s conjectured projection inequality

Iterations of the projection body operator and a remark on Petty s conjectured projection inequality Iterations of the projection body operator and a remar on Petty s conjectured projection inequality C. Saroglou and A. Zvavitch November 10, 015 Abstract We prove that if a convex body has absolutely continuous

More information

Fisher information and Stam inequality on a finite group

Fisher information and Stam inequality on a finite group Fisher information and Stam inequality on a finite group Paolo Gibilisco and Tommaso Isola February, 2008 Abstract We prove a discrete version of Stam inequality for random variables taking values on a

More information

Characterisation of Accumulation Points. Convergence in Metric Spaces. Characterisation of Closed Sets. Characterisation of Closed Sets

Characterisation of Accumulation Points. Convergence in Metric Spaces. Characterisation of Closed Sets. Characterisation of Closed Sets Convergence in Metric Spaces Functional Analysis Lecture 3: Convergence and Continuity in Metric Spaces Bengt Ove Turesson September 4, 2016 Suppose that (X, d) is a metric space. A sequence (x n ) X is

More information

Mixed volumes and mixed integrals

Mixed volumes and mixed integrals Snapshots of modern mathematics from Oberwolfach xx/xxxx Mixed volumes and mixed integrals Liran Rotem In recent years, analytic and probabilistic tools proved themselves to be very useful in the study

More information

Geometry of log-concave Ensembles of random matrices

Geometry of log-concave Ensembles of random matrices Geometry of log-concave Ensembles of random matrices Nicole Tomczak-Jaegermann Joint work with Radosław Adamczak, Rafał Latała, Alexander Litvak, Alain Pajor Cortona, June 2011 Nicole Tomczak-Jaegermann

More information

Discrete Ricci curvature: Open problems

Discrete Ricci curvature: Open problems Discrete Ricci curvature: Open problems Yann Ollivier, May 2008 Abstract This document lists some open problems related to the notion of discrete Ricci curvature defined in [Oll09, Oll07]. Do not hesitate

More information

Stronger versions of the Orlicz-Petty projection inequality

Stronger versions of the Orlicz-Petty projection inequality Stronger versions of the Orlicz-Petty projection inequality Károly J. Böröczky arxiv:1105.3251v3 [math.mg] 24 Jul 2013 June 9, 2018 Abstract We verify a conjecture of Lutwak, Yang, Zhang about the equality

More information

Multiple integrals: Sufficient conditions for a local minimum, Jacobi and Weierstrass-type conditions

Multiple integrals: Sufficient conditions for a local minimum, Jacobi and Weierstrass-type conditions Multiple integrals: Sufficient conditions for a local minimum, Jacobi and Weierstrass-type conditions March 6, 2013 Contents 1 Wea second variation 2 1.1 Formulas for variation........................

More information

Brunn-Minkowski inequalities for two functionals involving the p-laplace operator

Brunn-Minkowski inequalities for two functionals involving the p-laplace operator Brunn-Minkowski inequalities for two functionals involving the p-laplace operator Andrea Colesanti Paola Cuoghi Paolo Salani Abstract In the family of n-dimensional convex bodies, we prove a Brunn-Minkowski

More information

A Sharpened Hausdorff-Young Inequality

A Sharpened Hausdorff-Young Inequality A Sharpened Hausdorff-Young Inequality Michael Christ University of California, Berkeley IPAM Workshop Kakeya Problem, Restriction Problem, Sum-Product Theory and perhaps more May 5, 2014 Hausdorff-Young

More information

Vectors, metric and the connection

Vectors, metric and the connection Vectors, metric and the connection 1 Contravariant and covariant vectors 1.1 Contravariant vectors Imagine a particle moving along some path in the 2-dimensional flat x y plane. Let its trajectory be given

More information

William P. Thurston. The Geometry and Topology of Three-Manifolds

William P. Thurston. The Geometry and Topology of Three-Manifolds William P. Thurston The Geometry and Topology of Three-Manifolds Electronic version 1.1 - March 00 http://www.msri.org/publications/books/gt3m/ This is an electronic edition of the 1980 notes distributed

More information

On the distribution of the ψ 2 -norm of linear functionals on isotropic convex bodies

On the distribution of the ψ 2 -norm of linear functionals on isotropic convex bodies On the distribution of the ψ 2 -norm of linear functionals on isotropic convex bodies Joint work with G. Paouris and P. Valettas Cortona 2011 June 16, 2011 (Cortona 2011) Distribution of the ψ 2 -norm

More information

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by

L p Functions. Given a measure space (X, µ) and a real number p [1, ), recall that the L p -norm of a measurable function f : X R is defined by L p Functions Given a measure space (, µ) and a real number p [, ), recall that the L p -norm of a measurable function f : R is defined by f p = ( ) /p f p dµ Note that the L p -norm of a function f may

More information

Estimates for the resolvent and spectral gaps for non self-adjoint operators. University Bordeaux

Estimates for the resolvent and spectral gaps for non self-adjoint operators. University Bordeaux for the resolvent and spectral gaps for non self-adjoint operators 1 / 29 Estimates for the resolvent and spectral gaps for non self-adjoint operators Vesselin Petkov University Bordeaux Mathematics Days

More information

ON A LINEAR REFINEMENT OF THE PRÉKOPA-LEINDLER INEQUALITY

ON A LINEAR REFINEMENT OF THE PRÉKOPA-LEINDLER INEQUALITY ON A LINEAR REFINEMENT OF TE PRÉKOPA-LEINDLER INEQUALITY A. COLESANTI, E. SAORÍN GÓMEZ, AND J. YEPES NICOLÁS Abstract. If f, g : R n R 0 are non-negative measurable functions, then the Prékopa-Leindler

More information