R 65 ; Secondary 57 M 99 SYMPLECTIC 2 - HANDLES AND TRANSVERSE LINKS

نویسنده

  • DAVID T. GAY
چکیده

A standard convexity condition on the boundary of a symplectic manifold involves an induced positive contact form (and contact structure) on the boundary; the corresponding concavity condition involves an induced negative contact form. We present two methods of symplectically attaching 2-handles to convex boundaries of symplectic 4-manifolds along links transverse to the induced contact structures. One method results in concave boundaries and depends on a fibration of the link complement over S 1 ; in this case the handles can be attached with any framing larger than a lower bound determined by the fibration. The other method results in a weaker convexity condition on the new boundary (sufficient to imply tightness of the new contact structure), and in this case the handles can be attached with any framing less than a certain upper bound. These methods supplement methods developed by Weinstein and Eliashberg for attaching symplectic 2-handles along Legendrian knots. When constructing symplectic manifolds it is natural to wonder whether topo-logical techniques using handles can be made to work symplectically. Weinstein [6] and Eliashberg [2] have shown how to do this in certain cases; here we present two new symplectic " handle-by-handle " constructions in dimension four. In such constructions it is desirable to retain control of the symplectic form near the boundary; one form of control is the following: Given a symplectic manifold (X, ω) we say that ∂X is convex (respectively concave) if there exists a vector field V defined in a neighborhood of ∂X, satisfying the equation L V ω = ω (in other words, V is a symplectic dilation) and pointing out of (respectively into) X. This induces a contact form α = ı V ω| ∂X and a contact structure ξ = ker α on ∂X. Weinstein and Eliashberg show that, if (X, ω) is a symplectic 2n-manifold with ∂X convex, then one can attach k-handles to X, for 0 ≤ k ≤ n, and extend ω across the handles so that the new boundary is again convex. Conditions are imposed on the attaching spheres in relation to the contact structure ξ on ∂X and in particular, in dimension four, 2-handles must be attached along Legendrian knots (knots tangent to ξ). In this paper we show how to symplectically attach 2-handles along transverse knots (transverse to ξ) in the convex boundary of a symplectic 4-manifold so that the new boundary becomes concave. Along the way, …

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Symplectic 2-handles and Transverse Links

When constructing symplectic manifolds it is natural to wonder whether topological techniques using handles can be made to work symplectically. Weinstein [6] and Eliashberg [2] have shown how to do this in certain cases; here we present two new symplectic “handle-byhandle” constructions in dimension four. In such constructions it is desirable to retain control of the symplectic form near the bo...

متن کامل

Low-dimensional topology and geometry.

A t the core of low-dimensional topology has been the classification of knots and links in the 3-sphere and the classification of 3and 4-dimensional manifolds (see Wikipedia for the definitions of basic topological terms). Beginning with the introduction of hyperbolic geometry into knots and 3-manifolds by W. Thurston in the late 1970s, geometric tools have become vital to the subject. Next cam...

متن کامل

On Disk Embedding up to S-cobordism

The disk embedding lemma is a technique underlying the topological classification results in 4-manifold topology for good fundamental groups. The purpose of this paper is to develop new tools for disk embedding that work up to s-cobordism, without restrictions on the fundamental group. As an application we show that a surgery problem gives rise to a collection of capped gropes that fit in the f...

متن کامل

{ 2{ for Popular`supergravity' Models, M 1 and M 2 Unify at a Gut Scale, with M 1 M 2 =2 at the Electroweak Scale. Consequently, the Mass Diierence M = M E ? M E 0

II.1. Introduction: The theoretical strong points of super-symmetry (SUSY) have motivated many searches for super-symmetric particles. Many of these have been based on the canonical missing-energy signature caused by the escape of weakly-interacting LSP's (`lightest supersymmetric particles'). Other scenarios have also been investigated, widening the range of topologies and experimental signatu...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2001