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June 2, 2006

Mathai on T-Duality, II: T-dual K-classes by Fourier-Mukai

Posted by Urs Schreiber

The first part of my transcript of V. Mathai’s talk.

To start with, consider first spacetimes XX which are trivial circle bundles

(1)X=M×T. X = M \times \mathbf{T} \,.

Let T^\hat \mathbf{T} denote the dual torus, dual to T\mathbf{T}. Technically (since there is no metric in this topological game) this means that we take T^\hat \mathbf{T} to be the space of characters (\to) of T\mathbf{T}, when the latter is regarded as an abelian group.

What governs T-duality is something known as the Poincaré line bundle (\to) on the correspondence space (\to)

(2)M×T×T^ p 2 M×T^ p 1 M×T. \array{ M \times \mathbf{T} \times \hat \mathbf{T} &\overset{p_2}{\to}& M \times \hat \mathbf{T} \\ p_1 \downarrow \;\; \\ M \times \mathbf{T} } \,.

For the present purpose, the Poincaré line bundle on T×T^\mathbf{T}\times \hat \mathbf{T} is defined as the quotient of ×T^×\mathbb{R}\times \hat \mathbf{T} \times \mathbb{C} by \mathbb{Z}, where \mathbb{Z} acts as

(3)×T^× n ×T^× (r,ρ,z) (rn,ρ,ρ(n)z), \array{ \mathbb{R}\times \hat \mathbf{T} \times \mathbb{C} &\overset{n \in \mathbb{Z}}{\to} & \mathbb{R}\times \hat \mathbf{T} \times \mathbb{C} \\ (r,\rho,z) &\mapsto& (r\cdot n, \rho, \rho(n)\cdot z) } \,,

such that

(4)P=(×T^×)/ T×T^. \array{ P = (\mathbb{R}\times \hat \mathbf{T} \times \mathbb{C} )/\mathbb{Z} \\ \downarrow \\ \mathbf{T}\times \hat \mathbf{T} \,. }

The curvature of this bundle is

(5)F=dθdθ^. F = d\theta \wedge d\hat \theta \,.

So PP is flat when restricted to either T\mathbf{T} or T^\hat \mathbf{T}, but is nontrivial on all of T×T^\mathbf{T} \times \hat \mathbf{T}.

Let

(6)GΩ (M×T) G \in \Omega^\bullet(M\times \mathbf{T})

be the total RR-field strength, i.e.

(7)GΩ even(M×T) G \in \Omega^\mathrm{even}(M \times \mathbf{T})

for type IIA and

(8)GΩ odd(M×T) G \in \Omega^\mathrm{odd}(M \times \mathbf{T})

for type IIB. The the Buscher rules describing the transformation of the RR fields under T-duality read

(9)T *G:= Te FG. T_* G := \int_\mathbf{T}\; e^{F\wedge} G \,.

Notice that e Fe^F is the Chern character of the Poincaré line bundle

(10)e F=ch(P) e^F = \mathrm{ch}(P)

and note that GG is a closed form if and only if its T-dual T *GT_* G is a closed form. This means that the above Buscher rule(s) may be interpreted as an isomorphism of the deRham cohomology of the T-dual spacetimes M×TM \times \mathbf{T} and M×T^M \times \hat \mathbf{T}

(11)T *:H (M×T)H (M×T^). T_* : H^\bullet(M \times \mathbf{T}) \simeq H^\bullet(M \times \hat \mathbf{T}) \,.

What we are after is actually a T-duality induced isomorphism of the K-theory of one background with that (possibly up to a shift in degree) of the corresponding T-dual background.

Given any map

(12)XfY X \overset{f}{\to} Y

there is an obvious way to pull back a class in K(Y)K(Y) to a class in K(X)K(X), simply by pulling back any representative bundle. There is not really a general way to push forward a bundle along ff, of course. But there is such an operation on K-theory classes. This push forward at the level of K-theory, which can be denoted by f *f_*, is often written f !f_!.

Whenever we have a notion of pulling back and of pushing forward for some kind of object, then we can use correspondences like

(13)P M×T×T^ p^ M×T^ p M×T \array{ P \\ \downarrow \\ M \times \mathbf{T} \times \hat \mathbf{T} &\overset{\hat p}{\to}& M \times \hat \mathbf{T} \\ p \downarrow \;\; \\ M \times \mathbf{T} }

to induce maps on the space of these objects (\to).

This is how T-duality acts on K-theory classes: we pull them back along pp, tensor them fiberwise with PP and then push the result forward along p^\hat p:

(14)T !:K (M×T) K +1(M×T^) E p^ *((p *E)P). \array{ T_! : K^\bullet(M\times \mathbf{T}) &\simeq& K^{\bullet + 1}(M\times \hat \mathbf{T}) \\ E &\mapsto& \hat p_*((p^* E) \otimes P) } \,.

Up to the extra factor of MM, this is nothing but the Fourier-Mukai transformation, something which may be regarded as a categorified version of ordinary Fourier transformation (\to).

Notice that so far no background HH-flux was considered. So the above transformation exchanges IIA with IIB data without changing the topology (which is that of M×TM\times \mathbf{T}).

By way of the Chern character the isomorphism of K-theories and that of deRham cohomology is naturally related, in that this diagram commutes

(15)K (M×T) T ! K +1(M×T^) ch ch H (M×T) T * H +1(M×T^). \array{ K^\bullet(M\times \mathbf{T}) &\overset{T_!}{\to}& K^{\bullet + 1}(M \times \hat \mathbf{T}) \\ \mathrm{ch}\downarrow \;\; && \;\; \downarrow \mathrm{ch} \\ H^\bullet(M\times \mathbf{T}) &\overset{T_*}{\to}& H^{\bullet + 1}(M \times \hat \mathbf{T}) } \,.
Posted at June 2, 2006 12:58 PM UTC

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