The Fubini-Study metric is the standard unitary-invariant Kähler metric on Complex projective space, induced from the unit sphere by the Hopf fibration. Its associated Kähler form is the Fubini-Study form; scaling conventions determine the area of a projective line.
The Fubini-Study form is the standard Kähler form on complex projective space. With the integral normalization, .
The two-form is associated with the Fubini-Study metric.
The form patches on Complex projective space. The dual tautological metric on identifies it with normalized Chern curvature, so . With the unnormalized convention , divide by to obtain this integral class.
The scalar circle group action on with the standard symplectic form has moment map in the convention . Reduction of the radius- sphere gives Complex projective space and the form . Its area on a complex projective line is . Thus yields the Fubini-Study form normalized to projective-line area , while yields half that form. The Hopf fibration identifies the quotient.
Normalize the Fubini-Study form so that a complex projective line has symplectic area . The displayed map takes the unit symplectic ball in diffeomorphically onto the complement of the last-coordinate hyperplane. Its lift to the unit sphere has last coordinate positive real, so that coordinate contributes zero to the pulled-back standard symplectic form. The map is therefore a symplectomorphism.
Two disjoint symplectic balls of radii embedding into the unit four-ball must satisfy the displayed inequality. Extend their transported standard complex structures on smaller concentric balls to a compatible almost complex structure on the projective plane. A degree-one J-holomorphic curve through both centres has area . The Monotonicity theorem for a J-holomorphic curve bounds its area in each smaller ball below by . Disjointness allows these bounds to be added; letting increase to proves the result.
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The Fubini–Study metric is a Riemannian metric defined on complex projective space, specifically on the projective Hilbert space \( \mathbb{CP}^n \). It is often used in the context of quantum mechanics and quantum information theory as it provides a way to measure distances and angles between quantum states represented as rays in complex projective space.