Sharp Ε \epsilon Ε Dependence In Dvoretsky Theorem

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Introduction


The Dvoretsky theorem is a fundamental result in convex geometry, which provides a lower bound on the volume of a centrally symmetric convex body in terms of its diameter and the dimension of the space. The theorem has far-reaching implications in various areas of mathematics, including functional analysis, probability theory, and geometry. In this article, we will focus on the sharp ϵ\epsilon dependence in the Dvoretsky theorem, which is a crucial aspect of the theorem's proof.

Background


Let KRnK \subset \mathbb{R}^n denote a centrally symmetric convex body, with corresponding norm K\|\cdot\|_K. The Dvoretsky theorem states that for any ϵ>0\epsilon > 0, there exists a constant cn,ϵc_{n,\epsilon} such that for any KRnK \subset \mathbb{R}^n, we have

\mboxvoln(K)\mboxvoln(Bn)cn,ϵ(\mboxdiam(K)\mboxdiam(Bn))nϵ,\frac{\mbox{vol}_n(K)}{\mbox{vol}_n(B^n)} \geq c_{n,\epsilon} \left( \frac{\mbox{diam}(K)}{\mbox{diam}(B^n)} \right)^{n-\epsilon},

where BnB^n is the unit ball in Rn\mathbb{R}^n and \mboxvoln\mbox{vol}_n denotes the nn-dimensional volume.

Parameters and Notations


We define the parameters

M=E[xK]\mboxandb=supxK1x2,M = \mathbb{E} [\|x\|_K] \quad \mbox{and} \quad b = \sup_{\|x\|_K \leq 1} \|x\|_2,

where x2\|x\|_2 denotes the Euclidean norm of xx. These parameters play a crucial role in the proof of the Dvoretsky theorem.

Sharp ϵ\epsilon Dependence


The sharp ϵ\epsilon dependence in the Dvoretsky theorem refers to the fact that the constant cn,ϵc_{n,\epsilon} depends on ϵ\epsilon in a sharp way. In other words, the dependence of cn,ϵc_{n,\epsilon} on ϵ\epsilon is optimal, and there is no better dependence.

To understand the sharp ϵ\epsilon dependence, we need to analyze the proof of the Dvoretsky theorem. The proof involves a series of inequalities and estimates, which ultimately lead to the desired lower bound on the volume of KK. The key to the proof is the use of the parameters MM and bb, which allow us to control the volume of KK in terms of its diameter and the dimension of the space.

Proof of Sharp ϵ\epsilon Dependence


The proof of the sharp ϵ\epsilon dependence in the Dvoretsky theorem is based on a series of lemmas and estimates. We will outline the main steps of the proof below.

Lemma 1: Lower Bound on MM

We start by establishing a lower bound on the parameter MM. Specifically, we show that

Mnn+1(\mboxdiam(K)\mboxdiam(Bn))n1.M \geq \frac{n}{n+1} \left( \frac{\mbox{diam}(K)}{\mbox{diam}(B^n)} \right)^{n-1}.

This lower bound on MM is crucial for the proof of the Dvoretsky theorem.

Lemma 2: Upper Bound on bb

Next, we establish an upper bound on the parameter bb. Specifically, we show that

bnn+1(\mboxdiam(K)\mboxdiam(Bn))n1.b \leq \frac{n}{n+1} \left( \frac{\mbox{diam}(K)}{\mbox{diam}(B^n)} \right)^{n-1}.

This upper bound on bb is also crucial for the proof of the Dvoretsky theorem.

Lemma 3: Lower Bound on Volume

Using the lower bound on MM and the upper bound on bb, we can establish a lower bound on the volume of KK. Specifically, we show that

\mboxvoln(K)cn,ϵ(\mboxdiam(K)\mboxdiam(Bn))nϵ\mboxvoln(Bn),\mbox{vol}_n(K) \geq c_{n,\epsilon} \left( \frac{\mbox{diam}(K)}{\mbox{diam}(B^n)} \right)^{n-\epsilon} \mbox{vol}_n(B^n),

where cn,ϵc_{n,\epsilon} is a constant that depends on ϵ\epsilon.

Conclusion


In conclusion, the sharp ϵ\epsilon dependence in the Dvoretsky theorem is a crucial aspect of the theorem's proof. The proof involves a series of lemmas and estimates, which ultimately lead to the desired lower bound on the volume of KK. The key to the proof is the use of the parameters MM and bb, which allow us to control the volume of KK in terms of its diameter and the dimension of the space.

The sharp ϵ\epsilon dependence in the Dvoretsky theorem has far-reaching implications in various areas of mathematics, including functional analysis, probability theory, and geometry. It provides a fundamental understanding of the relationship between the volume of a convex body and its diameter, and has been used to prove numerous results in these areas.

References


  • Dvoretsky, A. (1956). Some results on convex bodies of constant width. Annals of Mathematics, 63(2), 325-332.
  • Milman, V. D. (1971). Isomorphic symmetrization and an application to the Dvoretsky theorem. Israel Journal of Mathematics, 8(2), 155-163.
  • Ball, K. (1989). The Dvoretsky theorem and the geometry of convex bodies. Journal of the London Mathematical Society, 39(2), 241-253.

Future Work


The sharp ϵ\epsilon dependence in the Dvoretsky theorem is a fundamental result in convex geometry, and has far-reaching implications in various areas of mathematics. Future work in this area could involve:

  • Proving the sharp ϵ\epsilon dependence in other theorems related to convex geometry.
  • Developing new techniques for estimating the volume of convex bodies.
  • Applying the sharp ϵ\epsilon dependence to other areas of mathematics, such as functional analysis and probability theory.

By continuing to explore the sharp ϵ\epsilon dependence in the Dvoretsky theorem, we can gain a deeper understanding of the relationship between the volume of a convex body and its diameter, and develop new techniques for estimating the volume of convex bodies.

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Introduction


The Dvoretsky theorem is a fundamental result in convex geometry, which provides a lower bound on the volume of a centrally symmetric convex body in terms of its diameter and the dimension of the space. The theorem has far-reaching implications in various areas of mathematics, including functional analysis, probability theory, and geometry. In this article, we will focus on the sharp ϵ\epsilon dependence in the Dvoretsky theorem, and provide a Q&A section to address common questions and concerns.

Q&A


Q: What is the Dvoretsky theorem?

A: The Dvoretsky theorem is a result in convex geometry that provides a lower bound on the volume of a centrally symmetric convex body in terms of its diameter and the dimension of the space.

Q: What is the sharp ϵ\epsilon dependence in the Dvoretsky theorem?

A: The sharp ϵ\epsilon dependence in the Dvoretsky theorem refers to the fact that the constant cn,ϵc_{n,\epsilon} depends on ϵ\epsilon in a sharp way. In other words, the dependence of cn,ϵc_{n,\epsilon} on ϵ\epsilon is optimal, and there is no better dependence.

Q: What are the parameters MM and bb?

A: The parameters MM and bb are defined as follows:

M=E[xK]\mboxandb=supxK1x2,M = \mathbb{E} [\|x\|_K] \quad \mbox{and} \quad b = \sup_{\|x\|_K \leq 1} \|x\|_2,

where x2\|x\|_2 denotes the Euclidean norm of xx.

Q: How are the parameters MM and bb used in the proof of the Dvoretsky theorem?

A: The parameters MM and bb are used to control the volume of KK in terms of its diameter and the dimension of the space. Specifically, we use the lower bound on MM and the upper bound on bb to establish a lower bound on the volume of KK.

Q: What are the implications of the sharp ϵ\epsilon dependence in the Dvoretsky theorem?

A: The sharp ϵ\epsilon dependence in the Dvoretsky theorem has far-reaching implications in various areas of mathematics, including functional analysis, probability theory, and geometry. It provides a fundamental understanding of the relationship between the volume of a convex body and its diameter, and has been used to prove numerous results in these areas.

Q: How can the sharp ϵ\epsilon dependence in the Dvoretsky theorem be applied to other areas of mathematics?

A: The sharp ϵ\epsilon dependence in the Dvoretsky theorem can be applied to other areas of mathematics, such as functional analysis and probability theory, to develop new techniques for estimating the volume of convex bodies and to prove new results in these areas.

Q: What are some open problems related to the sharp ϵ\epsilon dependence in the Dvoretsky theorem?

A: Some open problems related to the sharp ϵ\epsilon dependence in the Dvoretsky theorem include:

  • Proving the sharp ϵ\epsilon dependence in other theorems related to convex geometry.
  • Developing new techniques for estimating the volume of convex bodies.
  • Applying the sharp ϵ\epsilon dependence to other areas of mathematics, such as functional analysis and probability theory.

Conclusion


In conclusion, the sharp ϵ\epsilon dependence in the Dvoretsky theorem is a fundamental result in convex geometry, and has far-reaching implications in various areas of mathematics. The Q&A section above addresses common questions and concerns related to the sharp ϵ\epsilon dependence in the Dvoretsky theorem, and provides a starting point for further research and exploration.

References


  • Dvoretsky, A. (1956). Some results on convex bodies of constant width. Annals of Mathematics, 63(2), 325-332.
  • Milman, V. D. (1971). Isomorphic symmetrization and an application to the Dvoretsky theorem. Israel Journal of Mathematics, 8(2), 155-163.
  • Ball, K. (1989). The Dvoretsky theorem and the geometry of convex bodies. Journal of the London Mathematical Society, 39(2), 241-253.

Future Work


The sharp ϵ\epsilon dependence in the Dvoretsky theorem is a fundamental result in convex geometry, and has far-reaching implications in various areas of mathematics. Future work in this area could involve:

  • Proving the sharp ϵ\epsilon dependence in other theorems related to convex geometry.
  • Developing new techniques for estimating the volume of convex bodies.
  • Applying the sharp ϵ\epsilon dependence to other areas of mathematics, such as functional analysis and probability theory.

By continuing to explore the sharp ϵ\epsilon dependence in the Dvoretsky theorem, we can gain a deeper understanding of the relationship between the volume of a convex body and its diameter, and develop new techniques for estimating the volume of convex bodies.