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Bounds for the volume ratio of convex bodies DANIEL GALICER (Joint - PowerPoint PPT Presentation

The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Bounds for the volume ratio of convex bodies DANIEL GALICER (Joint work with Mariano Merzbacher and Dami an Pinasco) University of Buenos Aires and


  1. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Remarks If L = B n 2 we recover the standard notion of volume ratio. That is, vr( K , B n 2 ) = vr( K ) . The volume ratio is affinely invariant: vr( K , L ) = vr( T ( K ) , S ( L )) , for every affine transformation T , S .

  2. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Remarks If L = B n 2 we recover the standard notion of volume ratio. That is, vr( K , B n 2 ) = vr( K ) . The volume ratio is affinely invariant: vr( K , L ) = vr( T ( K ) , S ( L )) , for every affine transformation T , S . vr( K , L ) ≤ vr( K , Z )vr( Z , L ).

  3. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Remarks If L = B n 2 we recover the standard notion of volume ratio. That is, vr( K , B n 2 ) = vr( K ) . The volume ratio is affinely invariant: vr( K , L ) = vr( T ( K ) , S ( L )) , for every affine transformation T , S . vr( K , L ) ≤ vr( K , Z )vr( Z , L ). vr( K , L ) ≈ vr( L ◦ , K ◦ ) .

  4. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work General upper bounds for the volume ratio Giannopoulos-Hartzoulaki (2002) For every pair of convex bodies K , L ⊂ R n vr( K , L ) ≤ C √ n log( n ) . [GH02] A Giannopoulos, M Hartzoulaki On the volume ratio of two convex bodies. Bulletin of the London Mathematical Society 34.6 (2002): 703-707.

  5. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Lower bounds Khrabrov (2001) Given a convex body K there is Z such that n � vr( K , Z ) ≥ C log log( n ) . [Khr01] Alexander Igorevich Khrabrov. Generalized volume ratios and the Banach–Mazur distance. Mathematical Notes , 2001.

  6. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work The largest volume ratio Given a convex body K ⊂ R n we define its largest volume ratio as lvr( K ) := sup L ⊂ R n vr ( K , L ) . Remarks For every convex body K we have: log log( n ) � lvr( K ) � √ n log( n ) . � n

  7. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work The largest volume ratio Given a convex body K ⊂ R n we define its largest volume ratio as lvr( K ) := sup L ⊂ R n vr ( K , L ) . Remarks For every convex body K we have: log log( n ) � lvr( K ) � √ n log( n ) . � n For many bodies K ⊂ R n , lvr( K ) ≈ √ n .

  8. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Question: Can we improve the general bounds?

  9. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Question: Can we improve the general bounds? Question: Can we show sharp asymptotic estimates for certain classes of convex bodies?

  10. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Lower estimates...

  11. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Recall... For every convex body K , the best known general bounds for the largest volume ratio are log log( n ) � lvr( K ) � √ n log( n ) � n

  12. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Recall... For every convex body K , the best known general bounds for the largest volume ratio are log log( n ) � lvr( K ) � √ n log( n ) � n G., Merzbacher, Pinasco, 2019+ For every convex body K we have: √ n � lvr( K )

  13. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Reduction to the symmetric case Rogers-Shephard Inequality Given a convex body K , 1 1 n ≤ 4 vol ( K ) n . vol ( K − K )

  14. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Reduction to the symmetric case Rogers-Shephard Inequality Given a convex body K , 1 1 n ≤ 4 vol ( K ) n . vol ( K − K ) A body which contains the origin can be approximated by outside by a symmetric body with essentially the same volume. vr( K − K , K ) ≤ 4 . Then, vr( K − K , Z ) ≤ vr( K − K , K )vr( K , Z ) ≤ 4vr( K , Z ) .

  15. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Assumption Since there is always a reduction (considering either K − K or K ∩ − K depending on the case) we will assume for simplicity that all bodies involved are centrally symmetric.

  16. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work If K and Z are centrally symmetric 1 vr( K , Z ) = vol ( K ) n · inf {� T : X Z → X K � : det( T ) = 1 } 1 vol ( Z ) n

  17. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work If K and Z are centrally symmetric 1 vr( K , Z ) = vol ( K ) n · inf {� T : X Z → X K � : det( T ) = 1 } 1 vol ( Z ) n Idea: Given a fixed centrally symmetric body K ⊂ R n , find Z such that for every T ∈ SL n ( R ) the norm � T : X Z → X K � is big, 1 n is small. the measure vol ( Z ) But how???

  18. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How? The probabilistic method... ... is a nonconstructive method for proving the existence of a prescribed kind of mathematical object.

  19. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How? The probabilistic method... ... is a nonconstructive method for proving the existence of a prescribed kind of mathematical object. It works by showing that if one randomly chooses objects from a specified class, the probability that the result is of the prescribed kind is strictly greater than zero.

  20. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Random polytopes on the sphere (Gluskin’s polytopes) Given m ∈ N , we consider the set A m := { absconv { e 1 . . . e n , f 1 . . . , f m } : f k ∈ S n − 1 } .

  21. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Random polytopes on the sphere (Gluskin’s polytopes) Given m ∈ N , we consider the set A m := { absconv { e 1 . . . e n , f 1 . . . , f m } : f k ∈ S n − 1 } . Note that we have the following mapping S n − 1 × · · · × S n − 1 → A m , given by ( f 1 , . . . , f m ) �→ absconv { e 1 . . . e n , f 1 . . . , f m } .

  22. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Random polytopes on the sphere (Gluskin’s polytopes) Given m ∈ N , we consider the set A m := { absconv { e 1 . . . e n , f 1 . . . , f m } : f k ∈ S n − 1 } . Note that we have the following mapping S n − 1 × · · · × S n − 1 → A m , given by ( f 1 , . . . , f m ) �→ absconv { e 1 . . . e n , f 1 . . . , f m } . This induces a measure ν in A m : the push-forward of the product measure µ n × µ n × · · · × µ n , where µ n is the probability surface measure on S n − 1 .

  23. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Carl/Pajor - Gluskin: If Z ∈ A m , then � log( m / n ) 1 n � vol ( Z ) . n

  24. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Carl/Pajor - Gluskin: If Z ∈ A m , then � log( m / n ) 1 n � vol ( Z ) . n 1 n � 1 In particular, if m ∼ n then vol ( Z ) n .

  25. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work β B m = { Z ∈ A m : ∃ T ∈ SL n ( R ) with � T : X Z → X K � ≤ } . √ nvol ( K ) 1 n

  26. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work β B m = { Z ∈ A m : ∃ T ∈ SL n ( R ) with � T : X Z → X K � ≤ } . √ nvol ( K ) 1 n G., Merzbacher, Pinasco: refinement of Khrabrov’s result Let K ⊂ R n be a centrally symmetric body. Then, 2 → X K �√ nvol ( K ) ν ( B m ) ≤ C n 2 ( � id : ℓ n 1 n ) n 2 β mn .

  27. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work β B m = { Z ∈ A m : ∃ T ∈ SL n ( R ) with � T : X Z → X K � ≤ } . √ nvol ( K ) 1 n G., Merzbacher, Pinasco: refinement of Khrabrov’s result Let K ⊂ R n be a centrally symmetric body. Then, 2 → X K �√ nvol ( K ) ν ( B m ) ≤ C n 2 ( � id : ℓ n 1 n ) n 2 β mn . Suppose that for a given convex body K we have that 2 → X K �√ nvol ( K ) 1 ρ ( K ) := � id : ℓ n n is bounded by an absolute constant. Thus, ν ( B m ) ≤ D n 2 β mn ... By picking m ∼ n and β small enough we have ν ( B m ) < 1 .

  28. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work β B m = { Z ∈ A m : ∃ T ∈ SL n ( R ) with � T : X Z → X K � ≤ } . √ nvol ( K ) 1 n G., Merzbacher, Pinasco: refinement of Khrabrov’s result Let K ⊂ R n be a centrally symmetric body. Then, 2 → X K �√ nvol ( K ) ν ( B m ) ≤ C n 2 ( � id : ℓ n 1 n ) n 2 β mn . Suppose that for a given convex body K we have that 2 → X K �√ nvol ( K ) 1 ρ ( K ) := � id : ℓ n n is bounded by an absolute constant. Thus, ν ( B m ) ≤ D n 2 β mn ... By picking m ∼ n and β small enough we have ν ( B m ) < 1 . Therefore, the complement is non-empty.

  29. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work 1 n ∼ 1 Thus, there is some Z ∈ A cn (in particular vol ( Z ) n ) that is not in B cn . Note that in that case for every T ∈ SL n ( R ) we have β � T : X Z → X K � ≥ . √ nvol ( K ) 1 n

  30. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work 1 n ∼ 1 Thus, there is some Z ∈ A cn (in particular vol ( Z ) n ) that is not in B cn . Note that in that case for every T ∈ SL n ( R ) we have β � T : X Z → X K � ≥ . √ nvol ( K ) 1 n Then, 1 vr( K , Z ) = vol ( K ) n · inf {� T : X Z → X K � : det( T ) = 1 } 1 vol ( Z ) n ≈ √ n β 1 n · ≥ nvol ( K ) √ nvol ( K ) 1 n

  31. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work G., Merzbacher, Pinasco: refinement of Khrabrov’s result Let K ⊂ R n be a centrally symmetric body. Then, 2 → X K �√ nvol ( K ) 1 ν ( B m ) ≤ C n 2 ( � id : ℓ n n ) n 2 β mn . 2 → X K �√ nvol ( K ) 1 How to proceed in general if ρ ( K ) := � id : ℓ n n is not bounded by an absolute constant? Approximate the body K with a one that fulfills this hypothesis, without losing volume (the theory of isotropic convex bodies is involved).

  32. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How to approximate the body with a one with bounded ρ Given a centrally symmetric body K ⊂ R n there is W such that vr( W , K ) ≤ C 1 and 2 → X W �√ nvol ( W ) 1 ρ ( W ) = � id : ℓ n n ≤ C 2

  33. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How to approximate the body with a one with bounded ρ Given a centrally symmetric body K ⊂ R n there is W such that vr( W , K ) ≤ C 1 and 2 → X W �√ nvol ( W ) 1 ρ ( W ) = � id : ℓ n n ≤ C 2 Suppose that K ◦ is in isotropic position (so it has volume one).

  34. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How to approximate the body with a one with bounded ρ Given a centrally symmetric body K ⊂ R n there is W such that vr( W , K ) ≤ C 1 and 2 → X W �√ nvol ( W ) 1 ρ ( W ) = � id : ℓ n n ≤ C 2 Suppose that K ◦ is in isotropic position (so it has volume one). By a deep result of Paouris (2006) most of the mass of K ◦ concentrates inside √ nB n 2 .

  35. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How to approximate the body with a one with bounded ρ Given a centrally symmetric body K ⊂ R n there is W such that vr( W , K ) ≤ C 1 and 2 → X W �√ nvol ( W ) 1 ρ ( W ) = � id : ℓ n n ≤ C 2 Suppose that K ◦ is in isotropic position (so it has volume one). By a deep result of Paouris (2006) most of the mass of K ◦ concentrates inside √ nB n 2 . Take W ◦ := K ◦ ∩ √ nB n 1 2 . Observe that vol ( W ◦ ) n ∼ 1 so, 1 n ∼ 1 vol ( W ) n . On the other hand, vr( W , K ) ∼ vr( K ◦ , W ◦ ) ≤ C .

  36. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work How to approximate the body with a one with bounded ρ Given a centrally symmetric body K ⊂ R n there is W such that vr( W , K ) ≤ C 1 and 2 → X W �√ nvol ( W ) 1 ρ ( W ) = � id : ℓ n n ≤ C 2 Suppose that K ◦ is in isotropic position (so it has volume one). By a deep result of Paouris (2006) most of the mass of K ◦ concentrates inside √ nB n 2 . Take W ◦ := K ◦ ∩ √ nB n 1 2 . Observe that vol ( W ◦ ) n ∼ 1 so, 1 n ∼ 1 vol ( W ) n . On the other hand, vr( W , K ) ∼ vr( K ◦ , W ◦ ) ≤ C . By construction, W ◦ ⊂ √ nB n 2 ⊂ √ nW (which 2 then B n 2 → X W � ≤ √ n ). implies that � id : ℓ n

  37. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Upper estimates...

  38. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Lemma (Dvoretzky-Rogers) Let L ⊂ R n be a convex body in John’s position, there are y 1 . . . y n ∈ Bd ( B n 2 ) ∩ Bd ( L ) such that � 1 � n − i + 1 2 � P span { y 1 ... y i − 1 } ⊥ ( y i ) � ≥ . n

  39. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Lemma (Dvoretzky-Rogers) Let L ⊂ R n be a convex body in John’s position, there are y 1 . . . y n ∈ Bd ( B n 2 ) ∩ Bd ( L ) such that � 1 � n − i + 1 2 � P span { y 1 ... y i − 1 } ⊥ ( y i ) � ≥ . n � n n � 1 det | y 1 . . . y n | = � y 1 � � n i =2 � P span { y 1 ... y i − 1 } ⊥ ( y i ) � ≥ 2 n !

  40. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube

  41. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. y 1 0 y 2

  42. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 − y 1 y 2

  43. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 P = ∩ n i =1 {� x , y i � ≤ 1 } − y 1 y 2 P

  44. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 P = ∩ n i =1 {� x , y i � ≤ 1 } − y 1 y 2 2 n det | y 1 ... y n | ≤ C n vol( P ) = P

  45. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 P = ∩ n i =1 {� x , y i � ≤ 1 } − y 1 y 2 2 n det | y 1 ... y n | ≤ C n vol( P ) = n ≤ √ n . 1 1 vol ( P ) n ≤ vol ( P ) n n 1 1 vol ( B n vol ( L ) 2 ) P

  46. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 P = ∩ n i =1 {� x , y i � ≤ 1 } − y 1 y 2 2 n det | y 1 ... y n | ≤ C n vol( P ) = n ≤ √ n . 1 1 vol ( P ) n ≤ vol ( P ) n n 1 1 vol ( B n vol ( L ) 2 ) P

  47. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio for the cube Consider the points y 1 , . . . , y n given by D-R. L is symmetric, so − y 2 y 1 − y 1 , . . . , − y n ∈ Bd ( L ) 0 P = ∩ n i =1 {� x , y i � ≤ 1 } − y 1 y 2 2 n det | y 1 ... y n | ≤ C n vol( P ) = n ≤ √ n . 1 1 vol ( P ) n ≤ vol ( P ) n n 1 1 vol ( B n vol ( L ) 2 ) P ∞ ) ∼ √ n . lvr( B n

  48. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Unconditional bodies Definition A convex body K ⊂ R n is unconditional if ( x 1 , x 2 , . . . , x n ) ∈ L then ( ε 1 x 1 , ε 2 x 2 , . . . , ε n x n ) ∈ L for all ε i ∈ {− 1 , 1 } .

  49. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Unconditional bodies Definition A convex body K ⊂ R n is unconditional if ( x 1 , x 2 , . . . , x n ) ∈ L then ( ε 1 x 1 , ε 2 x 2 , . . . , ε n x n ) ∈ L for all ε i ∈ {− 1 , 1 } . Example unconditional: B n p for all 1 ≤ p ≤ ∞ , 2 ) ⊂ R n 2 . not unconditional: B L ( ℓ n

  50. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Unconditional bodies Definition A convex body K ⊂ R n is unconditional if ( x 1 , x 2 , . . . , x n ) ∈ L then ( ε 1 x 1 , ε 2 x 2 , . . . , ε n x n ) ∈ L for all ε i ∈ {− 1 , 1 } . Bobkov-Nazarov (2003) There is a constant c > 0 (independent of the dimension) such that for every unconditional isotropic convex body K ⊂ R n then [ − c , c ] n ⊂ K Sergey G Bobkov and Fedor L Nazarov. On convex bodies and log-concave probability measures with unconditional basis. In Geometric aspects of functional analysis , 2003.

  51. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Unconditional bodies Definition A convex body K ⊂ R n is unconditional if ( x 1 , x 2 , . . . , x n ) ∈ L then ( ε 1 x 1 , ε 2 x 2 , . . . , ε n x n ) ∈ L for all ε i ∈ {− 1 , 1 } . Bobkov-Nazarov (2003) There is a constant c > 0 (independent of the dimension) such that for every unconditional isotropic convex body K ⊂ R n then [ − c , c ] n ⊂ K Sergey G Bobkov and Fedor L Nazarov. On convex bodies and log-concave probability measures with unconditional basis. In Geometric aspects of functional analysis , 2003. vr( K , B n ∞ ) ≤ C .

  52. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work If K ⊂ R n is unconditional lvr( K ) ∼ √ n .

  53. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work If K ⊂ R n is unconditional lvr( K ) ∼ √ n . Indeed, ∞ , L ) ≤ C √ n . vr( K , L ) ≤ vr( K , B n ∞ )vr( B n

  54. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio of the simplex The unit cube, C = [0 , 1] n .

  55. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio of the simplex The unit cube, C = [0 , 1] n . C ⊂ S = co { 0 , ne 1 , . . . , ne n }

  56. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio of the simplex The unit cube, C = [0 , 1] n . C ⊂ S = co { 0 , ne 1 , . . . , ne n } vol( C ) = 1 vol( S ) = n n n !

  57. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio of the simplex The unit cube, C = [0 , 1] n . C ⊂ S = co { 0 , ne 1 , . . . , ne n } vol( C ) = 1 vol( S ) = n n n ! Applying Stirling’s formula: vr( S , B n ∞ ) = vr( S , C ) ≤ � vol ( S ) � 1 n ≈ 1 vol ( C )

  58. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Largest volume ratio of the simplex The unit cube, C = [0 , 1] n . C ⊂ S = co { 0 , ne 1 , . . . , ne n } vol( C ) = 1 vol( S ) = n n n ! Applying Stirling’s formula: vr( S , B n ∞ ) = vr( S , C ) ≤ � vol ( S ) � 1 n ≈ 1 vol ( C ) Therefore lvr( S ) ∼ √ n .

  59. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Schatten Classes Given A ∈ M d ( R ), consider s ( A ) = ( s 1 ( A ) , . . . , s d ( A )) the 1 sequence of eigenvalues of ( AA ∗ ) 2 . We define the p -Schatten norm on R d 2 as p = ( tr | A | p ) 1 / p , σ p ( A ) = � S ( A ) � ℓ d that is the ℓ p -norm of the singular values of A .

  60. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Schatten Classes Given A ∈ M d ( R ), consider s ( A ) = ( s 1 ( A ) , . . . , s d ( A )) the 1 sequence of eigenvalues of ( AA ∗ ) 2 . We define the p -Schatten norm on R d 2 as p = ( tr | A | p ) 1 / p , σ p ( A ) = � S ( A ) � ℓ d that is the ℓ p -norm of the singular values of A . p unit ball of the p -Schatten class in R d 2 . We denote B S d

  61. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work G., Merzbacher, Pinasco For every 1 ≤ p ≤ ∞ , the largest volume ratio of the unit ball of the p -Schatten class (which is a set in R d 2 ) behaves as lvr( B S d p ) ∼ d .

  62. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work G., Merzbacher, Pinasco For every 1 ≤ p ≤ ∞ , the largest volume ratio of the unit ball of the p -Schatten class (which is a set in R d 2 ) behaves as lvr( B S d p ) ∼ d . How?

  63. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work G., Merzbacher, Pinasco For every 1 ≤ p ≤ ∞ , the largest volume ratio of the unit ball of the p -Schatten class (which is a set in R d 2 ) behaves as lvr( B S d p ) ∼ d . How? We give a very careful look at the proofs of the general upper inequalities.

  64. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work G., Merzbacher, Pinasco For every 1 ≤ p ≤ ∞ , the largest volume ratio of the unit ball of the p -Schatten class (which is a set in R d 2 ) behaves as lvr( B S d p ) ∼ d . How? We give a very careful look at the proofs of the general upper inequalities. Again, all relies on the probabilistic method!!!!!!

  65. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Given T : X L → X K we have T ( L ) ⊂ � T � K and so 1 � T � vol ( K ) n vr( K , L ) ≤ . 1 1 n vol ( L ) (det T ) n

  66. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Given T : X L → X K we have T ( L ) ⊂ � T � K and so 1 � T � vol ( K ) n vr( K , L ) ≤ . 1 1 n vol ( L ) (det T ) n Chevet’s inequality If we denote O ( n ) the orthogonal group endowed with the Haar probability measure, then E � T : X L → X K � ≤ C √ n ( ℓ ( K ) � id : L → ℓ n 2 � 2 → X K � ℓ ( L ◦ )) . + � id : ℓ n

  67. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Given T : X L → X K we have T ( L ) ⊂ � T � K and so 1 � T � vol ( K ) n vr( K , L ) ≤ . 1 1 n vol ( L ) (det T ) n Chevet’s inequality If we denote O ( n ) the orthogonal group endowed with the Haar probability measure, then E � T : X L → X K � ≤ C √ n ( ℓ ( K ) � id : L → ℓ n 2 � 2 → X K � ℓ ( L ◦ )) . + � id : ℓ n We denote the right hand side of the inequality as α ( K , L ).

  68. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Given T : X L → X K we have T ( L ) ⊂ � T � K and so 1 � T � vol ( K ) n vr( K , L ) ≤ . 1 1 n vol ( L ) (det T ) n Chevet’s inequality If we denote O ( n ) the orthogonal group endowed with the Haar probability measure, then E � T : X L → X K � ≤ C √ n ( ℓ ( K ) � id : L → ℓ n 2 � 2 → X K � ℓ ( L ◦ )) . + � id : ℓ n We denote the right hand side of the inequality as α ( K , L ). 1 vr( K , L ) ≤ α ( K , L ) vol ( K ) n . 1 vol ( L ) n

  69. The volume ratio Lower estimates Upper bounds: some particular cases Future/Recent work Idea: Since the volume ratio is affinely invariant we look for a position of L such that � id : L → ℓ n 2 � and ℓ ( L ◦ ) are “not so big”. 1 n is “not so small”. vol ( L ) Proposition: For every centrally symmetric convex body K ⊂ R n , 1 lvr( K ) ≤ C � id : ℓ n n n log( n ) . 2 → X K � vol ( K )

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