Pseudoholomorphic curves
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== Linearisation == | == Linearisation == | ||
− | <wikitex>; One can think of $\bar{\partial}_J$ as a section of a Banach bundle. Explicitly, let $\mathcal{B}$ denote the $W^{1,p}$-completion of the space of maps $\Sigma\to X$ and let $\mathcal{J}$ denote the space of $\omega$-compatible almost complex structures. Define the Banach bundle $\mathcal{E}$ over $\mathcal{B}\times\mathcal{J}$ whose fibre over $(u,J)$ is the $L^p$-completion of the space $$\Omega^{0,1}(\Sigma,u^*TX)$$ of $(0,1)$-forms on $\Sigma$ with values in $u^*TX$. Here $(0,1)$ refers to the complex structures $j$ on $T\Sigma$ and $J$ on $u^*TX$. By definition, $\bar{\partial}\colon(u,J)\to\bar{\partial}_J(u)$ is a section of this bundle over the smooth locus and it extends naturally to the Sobolev completions. {{beginthm|Definition|Linearised Cauchy-Riemann operator}} The linearisation of $\bar{\partial}$ at a $J$-holomorphic curve $u$ is the operator $$D\bar{\partial}\colon W^{1,p}(\Sigma,u^*TX)\to L^p\Omega^{0,1}(\Sigma,u^*TX)$$ given (in local complex coordinates $a+ib$ on $\Sigma$) by $$D\bar{\partial}(\xi)(\partial_a)=\partial_a+J\partial_b+\frac{\partial J}{\partial\xi}du(\partial_a)$$ | + | <wikitex>; |
+ | One can think of $\bar{\partial}_J$ as a section of a Banach bundle. Explicitly, let $\mathcal{B}$ denote the $W^{1,p}$-completion of the space of maps $\Sigma\to X$ and let $\mathcal{J}$ denote the space of $\omega$-compatible almost complex structures. Define the Banach bundle $\mathcal{E}$ over $\mathcal{B}\times\mathcal{J}$ whose fibre over $(u,J)$ is the $L^p$-completion of the space $$\Omega^{0,1}(\Sigma,u^*TX)$$ of $(0,1)$-forms on $\Sigma$ with values in $u^*TX$. Here $(0,1)$ refers to the complex structures $j$ on $T\Sigma$ and $J$ on $u^*TX$. By definition, $\bar{\partial}\colon(u,J)\to\bar{\partial}_J(u)$ is a section of this bundle over the smooth locus and it extends naturally to the Sobolev completions. {{beginthm|Definition|Linearised Cauchy-Riemann operator}} The linearisation of $\bar{\partial}$ at a $J$-holomorphic curve $u$ is the operator $$D\bar{\partial}\colon W^{1,p}(\Sigma,u^*TX)\to L^p\Omega^{0,1}(\Sigma,u^*TX)$$ given (in local complex coordinates $a+ib$ on $\Sigma$) by $$D\bar{\partial}(\xi)(\partial_a)=\partial_a+J\partial_b+\frac{\partial J}{\partial\xi}du(\partial_a)$$ | ||
Here we think of $J$ as a section of $\mathrm{End}(TX)$ and $dJ$ as a map $TX\to T\mathrm{End}(TX)$ so $\frac{\partial J}{\partial\xi}$ means the pushforward of $\xi$ along $dJ$. The linearisation measures to first order the change in $\bar{\partial}_J(u)$ when $u$ is deformed along a vector field $\xi$. One can also allow $j$ to vary in the space of complex structures on $\Sigma$ or $J$ to vary in a family of almost complex structures by adding corresponding terms to the linearisation. | Here we think of $J$ as a section of $\mathrm{End}(TX)$ and $dJ$ as a map $TX\to T\mathrm{End}(TX)$ so $\frac{\partial J}{\partial\xi}$ means the pushforward of $\xi$ along $dJ$. The linearisation measures to first order the change in $\bar{\partial}_J(u)$ when $u$ is deformed along a vector field $\xi$. One can also allow $j$ to vary in the space of complex structures on $\Sigma$ or $J$ to vary in a family of almost complex structures by adding corresponding terms to the linearisation. | ||
{{endthm}} | {{endthm}} | ||
− | {{beginthm|Theorem|Ellipticity} | + | {{beginthm|Theorem|Ellipticity}} |
The linearised Cauchy-Riemann operator of a holomorphic curve is a Fredholm operator. | The linearised Cauchy-Riemann operator of a holomorphic curve is a Fredholm operator. | ||
{{endthm}} | {{endthm}} |
Revision as of 16:24, 19 February 2012
This page has not been refereed. The information given here might be incomplete or provisional. |
Contents |
1 Introduction
In this article, will denote an almost complex manifold of dimension .
Definition 1.1 (-holomorphic curve). Let be a Riemann surface with complex structure . A -holomorphic curve
is a smooth map satisfying
or equivalently
A -holomorphic map is called simple if it cannot be factored as where is a -holomorphic branched cover of degree strictly greater than 1. We will usually omit from the notation and speak of -holomorphic curves. The term pseudoholomorphic curve will be used to describe a -holomorphic curve when we do not want to specify .
Pseudoholomorphic curves provide a useful tool for studying symplectic manifolds.
2 Taming J
Pseudoholomorphic curves in a general almost complex manifold can be quite wild (EXAMPLE?). Better behaviour can be ensured by the existence of a symplectic taming , that is the quadratic form
is positive-definite. This gives us topological control on the energy of a -holomorphic curve
(here the norm and volume form are taken with respect to the metric ) thanks to the identity
Lemma 2.1 (Energy identity). If is a -holomorphic curve and is tamed by then
If moreover we require the metric to be -invariant () then we say that is -compatible and we have the identity
so that the -holomorphic curves are the absolute minima of the energy functional on the space of maps .
3 Linearisation
Here we think of as a section of and as a map so means the pushforward of along . The linearisation measures to first order the change in when is deformed along a vector field . One can also allow to vary in the space of complex structures on or to vary in a family of almost complex structures by adding corresponding terms to the linearisation.
Theorem 3.2 Ellipticity. The linearised Cauchy-Riemann operator of a holomorphic curve is a Fredholm operator.
4 Moduli spaces
Simple -holomorphic curves form nice moduli spaces
Theorem 4.1 Transversality for simple curves. Fix a homology class and a Riemann surface . There is a subset of the second-category such that the space
is a finite-dimensional manifold of dimension
If one allows to vary then this dimension formula gains an extra if or if .
These almost complex structures are the regular almost complex structures, for which the linearised problem has vanishing cokernel. Transversality is achieved by making small perturbations of the almost complex structure in regions through which the pseudoholomorphic curve has to pass.
It is harder to achieve transversality for curves which are multiple covers.
5 Compactness
While the -control on the derivatives of given by the energy identity 2.1 is not enough to ensure a priori compactness of moduli spaces, there is a natural compactification by adding in strata of stable maps.
Definition 5.1 (Stable map). Let be a nodal Riemann surface (i.e. a connected, compact reduced complex curve with at worst ordinary double points) and a collection of distinct non-nodal marked points on . A stable map is a -holomorphic map such that any irreducible component of which is mapped down to a point has either
- arithmetic genus 0 and at least three points which are either marked or nodal,
- arithmetic genus 1 and at least one point which is either marked or nodal,
- arithmetic genus 2 or more.
This is equivalent to the requirement that the group of holomorphic automorphisms of fixing the marked points and satisfying is finite. A reparametrisation of a stable map is a holomorphic automorphism of the domain which does not necessarily leave invariant and we usually only consider stable maps up to reparametrisation.
There is a notion of convergence for stable maps up to reparametrisation, called Gromov convergence, which allows us to define a topology of the moduli space of stable maps.
Theorem 5.2 (Gromov compactness). The moduli space of stable maps (modulo reparametrisations) with the topology of Gromov convergence is both compact and Hausdorff.