Fourier–Mukai transform

Definition

Let X and Y be smooth projective varieties, K ∈ Db(X×Y) an object in the derived category of coherent sheaves on their product. Denote by q the projection X×Y→X, by p the projection X×Y→Y. Then the Fourier-Mukai transform Φ**K is a functor Db(X)→Db(Y) given by :\mathcal{F} \mapsto \mathrm{R}p_\left(q^\mathcal{F} \otimes^{L} K\right) where R*p** is the derived direct image functor and \otimes^L is the derived tensor product.

Fourier-Mukai transforms always have left and right adjoints, both of which are also kernel transformations. Given two kernels K1 ∈ Db(X×Y) and K2 ∈ Db(Y×Z), the composed functor Φ**K2 \circ Φ**K1 is also a Fourier-Mukai transform.

The structure sheaf of the diagonal \mathcal{O}_{\Delta} \in \mathrm{D}^b(X \times X), taken as a kernel, produces the identity functor on Db(X). For a morphism f:X→Y, the structure sheaf of the graph Γf produces a pushforward when viewed as an object in Db(X×Y), or a pullback when viewed as an object in Db(Y×X).

On abelian varieties

Let X be an abelian variety and \hat X be its dual variety. The Poincaré bundle \mathcal P on X \times \hat X, normalized to be trivial on the fiber at zero, can be used as a Fourier-Mukai kernel. Let p and \hat p be the canonical projections. The corresponding Fourier–Mukai functor with kernel \mathcal P is then :R\mathcal S: \mathcal F \in D(X) \mapsto R\hat p_\ast (p^\ast \mathcal F \otimes \mathcal P) \in D(\hat X)

There is a similar functor

:R\widehat{\mathcal S} : D(\hat X) \to D(X). ,

If the canonical class of a variety is ample or anti-ample, then the derived category of coherent sheaves determines the variety. In general, an abelian variety is not isomorphic to its dual, so this Fourier–Mukai transform gives examples of different varieties (with trivial canonical bundles) that have equivalent derived categories.

Let g denote the dimension of X. The Fourier–Mukai transformation is nearly involutive : :R\mathcal S \circ R\widehat{\mathcal S} = (-1)^\ast [-g]

It interchanges Pontrjagin product and tensor product. :R\mathcal S(\mathcal F \ast \mathcal G) = R\mathcal S(\mathcal F) \otimes R\mathcal S(\mathcal G) :R\mathcal S(\mathcal F \otimes \mathcal G) = R\mathcal S(\mathcal F) \ast R\mathcal S(\mathcal G)[g]

have used the Fourier-Mukai transform to prove the Künneth decomposition for the Chow motives of abelian varieties.

Applications in string theory

In string theory, T-duality (short for target space duality), which relates two quantum field theories or string theories with different spacetime geometries, is closely related with the Fourier-Mukai transformation.

References

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References

1. (2001). "Reconstruction of a variety from the derived category and groups of autoequivalences". Compositio Mathematica.
2. (2000). "From special Lagrangian to Hermitian-Yang-Mills via Fourier-Mukai transform". Advances in Theoretical and Mathematical Physics.
3. (2014). "Defects, non-abelian t-duality, and the Fourier-Mukai transform of the Ramond-Ramond fields". Journal of High Energy Physics.