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Gromov's inequality for complex projective space

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Optimal stable 2-systolic inequality

In Riemannian geometry, Gromov's optimal stable 2-systolic inequality is the inequality

s t s y s 2 n n ! v o l 2 n ( C P n ) {\displaystyle \mathrm {stsys} _{2}{}^{n}\leq n!\;\mathrm {vol} _{2n}(\mathbb {CP} ^{n})} ,

valid for an arbitrary Riemannian metric on the complex projective space, where the optimal bound is attained by the symmetric Fubini–Study metric, providing a natural geometrisation of quantum mechanics. Here s t s y s 2 {\displaystyle \operatorname {stsys_{2}} } is the stable 2-systole, which in this case can be defined as the infimum of the areas of rational 2-cycles representing the class of the complex projective line C P 1 C P n {\displaystyle \mathbb {CP} ^{1}\subset \mathbb {CP} ^{n}} in 2-dimensional homology.

The inequality first appeared in Gromov (1981) as Theorem 4.36.

The proof of Gromov's inequality relies on the Wirtinger inequality for exterior 2-forms.

Projective planes over division algebras R , C , H {\displaystyle \mathbb {R,C,H} }

In the special case n=2, Gromov's inequality becomes s t s y s 2 2 2 v o l 4 ( C P 2 ) {\displaystyle \mathrm {stsys} _{2}{}^{2}\leq 2\mathrm {vol} _{4}(\mathbb {CP} ^{2})} . This inequality can be thought of as an analog of Pu's inequality for the real projective plane R P 2 {\displaystyle \mathbb {RP} ^{2}} . In both cases, the boundary case of equality is attained by the symmetric metric of the projective plane. Meanwhile, in the quaternionic case, the symmetric metric on H P 2 {\displaystyle \mathbb {HP} ^{2}} is not its systolically optimal metric. In other words, the manifold H P 2 {\displaystyle \mathbb {HP} ^{2}} admits Riemannian metrics with higher systolic ratio s t s y s 4 2 / v o l 8 {\displaystyle \mathrm {stsys} _{4}{}^{2}/\mathrm {vol} _{8}} than for its symmetric metric (Bangert et al. 2009).

See also

References

Systolic geometry
1-systoles of surfaces
1-systoles of manifolds
Higher systoles


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