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Mahler volume

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In convex geometry, the Mahler volume of a centrally symmetric convex body is a dimensionless quantity that is associated with the body and is invariant under linear transformations. It is named after German-English mathematician Kurt Mahler. It is known that the shapes with the largest possible Mahler volume are the balls and solid ellipsoids; this is now known as the Blaschke–Santaló inequality. The still-unsolved Mahler conjecture states that the minimum possible Mahler volume is attained by a hypercube.

Definition

A convex body in Euclidean space is defined as a compact convex set with non-empty interior. If B is a centrally symmetric convex body in n-dimensional Euclidean space, the polar body Bo is another centrally symmetric body in the same space, defined as the set

The Mahler volume of B is the product of the volumes of B and Bo.[1]

If T is an invertible linear transformation, then ; thus applying T to B changes its volume by and changes the volume of Bo by . Thus the overall Mahler volume of B is preserved by linear transformations.

Examples

The polar body of an n-dimensional unit sphere is itself another unit sphere. Thus, its Mahler volume is just the square of its volume,

Here Γ represents the Gamma function. By affine invariance, any ellipsoid has the same Mahler volume.[1]

The polar body of a polyhedron or polytope is its dual polyhedron or dual polytope. In particular, the polar body of a cube or hypercube is an octahedron or cross polytope. Its Mahler volume can be calculated as[1]

The Mahler volume of the sphere is larger than the Mahler volume of the hypercube by a factor of approximately .[1]

Extreme shapes

The Blaschke–Santaló inequality states that the shapes with maximum Mahler volume are the spheres and ellipsoids. The three-dimensional case of this result was proven by Wilhelm Blaschke; the full result was proven much later by Luis Santaló (1949) using a technique known as Steiner symmetrization by which any centrally symmetric convex body can be replaced with a more sphere-like body without decreasing its Mahler volume.[1]

The shapes with the minimum known Mahler volume are hypercubes, cross polytopes, and more generally the Hanner polytopes which include these two types of shapes, as well as their affine transformations. The Mahler conjecture states that the Mahler volume of these shapes is the smallest of any n-dimensional symmetric convex body; it remains unsolved. As Terry Tao writes:[1]

The main reason why this conjecture is so difficult is that unlike the upper bound, in which there is essentially only one extremiser up to affine transformations (namely the ball), there are many distinct extremisers for the lower bound - not only the cube and the octahedron, but also products of cubes and octahedra, polar bodies of products of cubes and octahedra, products of polar bodies of… well, you get the idea. It is really difficult to conceive of any sort of flow or optimisation procedure which would converge to exactly these bodies and no others; a radically different type of argument might be needed.

Bourgain & Milman (1987) prove that the Mahler volume is bounded below by cn times the volume of a sphere for some absolute constant c > 0, matching the scaling behavior of the hypercube volume but with a smaller constant. A result of this type is known as a reverse Santaló inequality.

Notes

  1. ^ a b c d e f Tao (2007).

References

  • Bourgain, J.; Milman, V. D. (1987), "New volume ratio properties for convex symmetric bodies in Rn", Inventiones Mathematicae, 88 (2): 319–340, doi:10.1007/BF01388911, MR 0880954.
  • Santaló, L. A. (1949), "An affine invariant for convex bodies of n-dimensional space", Portugaliae Math., 8: 155–161, MR 0039293 {{citation}}: |format= requires |url= (help).
  • Tao, Terence (March 8, 2007), Open question: the Mahler conjecture on convex bodies. Revised and reprinted in Tao, Terence (2009), "3.8 Mahler's conjecture for convex bodies", Structure and Randomness: Pages from Year One of a Mathematical Blog, American Mathematical Society, pp. 216–219, ISBN 978-0-8218-4695-7.