Download From Stein to Weinstein and Back: Symplectic Geometry of by Kai Cieliebak, Yakov Eliashberg PDF

By Kai Cieliebak, Yakov Eliashberg

This e-book is dedicated to the interaction among advanced and symplectic geometry in affine advanced manifolds. Affine advanced (a.k.a. Stein) manifolds have canonically equipped into them symplectic geometry that is answerable for many phenomena in complicated geometry and research. The objective of the publication is the exploration of this symplectic geometry (the highway from "Stein to Weinstein") and its purposes within the complicated geometric global of Stein manifolds (the highway "back"). this is often the 1st ebook which systematically explores this connection, therefore delivering a brand new method of the classical topic of Stein manifolds. It additionally includes the 1st designated research of Weinstein manifolds, the symplectic opposite numbers of Stein manifolds, which play a big position in symplectic and phone topology. Assuming just a basic heritage from differential topology, the e-book offers introductions to some of the concepts from the idea of capabilities of numerous advanced variables, symplectic geometry, h-principles, and Morse idea that input the proofs of the most effects. the most result of the ebook are unique result of the authors, and several other of those effects look right here for the 1st time. The booklet might be precious for all scholars and mathematicians drawn to geometric facets of complicated research, symplectic and make contact with topology, and the interconnections among those matters.

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This e-book via Jakob Nielsen (1890-1959) and Werner Fenchel (1905-1988) has had
a lengthy and intricate historical past. In 1938-39, Nielsen gave a sequence of lectures on
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World battle II - to jot down the 1st chapters of the ebook (in German). whilst Fenchel,
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When Nielsen moved to Copenhagen college in 1951 (where he stayed until eventually
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further writing of the manuscript was once left to Fenchel. The records of Fenchel now
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man containing Chapters I-II (

I -15), and a whole manuscript (manuscript I) in
English containing Chapters I-V (

1-27). The information additionally comprise a part of a corre-
spondence (first in German yet later in Danish) among Nielsen and Fenchel, the place
Nielsen makes precise reviews to Fenchel's writings of Chapters III-V. Fenchel,
who succeeded N. E. Nf/Jrlund at Copenhagen college in 1956 (and stayed there
until 1974), used to be a great deal concerned with a radical revision of the curriculum in al-
gebra and geometry, and focused his study within the idea of convexity, heading
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at Aarhus college) with the evidence examining of the TEX-manuscript (manuscript three)
against manuscript 2 in addition to with a common dialogue of the variation to the fashion
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we have indicated the start and finish of an explanation within the traditional variety of TEX.
With this TEX -manuscript I approached Walter de Gruyter in Berlin in 1992, and
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Studies in arithmetic. i'm so much thankful for this confident and speedy response. One
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figures that are an essential component of the presentation. Christian Siebeneicher had at
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We thought of including an entire checklist of references, yet determined opposed to it because of
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My ultimate and such a lot honest thank you visit Dr. Manfred Karbe from Walter de Gruyter
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Extra info for From Stein to Weinstein and Back: Symplectic Geometry of Affine Complex Manifolds

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This condition ensures that the boundary of the open cone Kp := {z ∈ Uj ∩ W | fp (z) > 0} in W is given by {z ∈ Uj ∩ W | fp (z) = 0} for all p ∈ Wj ∩ L. To see this, suppose by contradiction that there exists a point z = (u, v) ∈ K p ∩ ∂Uj . Then 2|v|2 − |u − p|2 = fp (z) ≥ 0 and the choice of W yield the contradiction dist(Wj , ∂Uj )2 ≤ |u − p|2 + |v|2 ≤ 3|v|2 < dist(Wj , ∂Uj )2 . Moreover, we can choose W so small that fp is J-convex on Kp for all p ∈ Wj ∩ W . Let φp := g ◦ fp , where g(t) = e−1/t for t > 0 and 0 for t ≤ 0.

A) Adding up ddC (βψ) = β ddC ψ + dβ ∧ dC ψ + dψ ∧ dC β + ψ ddC β and the corresponding equation for (1 − β)φ at any point x ∈ V , we find −ddC ϑ = −(1 − β) ddC φ − βddC ψ + dβ ∧ dC (φ − ψ) + d(φ − ψ) ∧ dC β + (φ − ψ)ddC β ≥ min (mφ , mψ ) − 2|dβ| |d(φ − ψ)| − |φ − ψ| |ddC β| > 0. (b) At the point x the terms φ − ψ and dφ − dψ vanish, so the computation in (a) shows −ddC ϑ = −(1−β) ddC φ−βddC ψ. Hence at the point x we have dϑ = dφ = dψ and the associated metrics satisfy gϑ = (1 − β)gφ + βgψ .

1) holds} is called the modulus of subharmonicity of the function φ. 1) for functions δ supported near z. 1), then choosing a sequence of functions δn converging to the Dirac measure of a point z ∈ U and integrating by parts shows ∆φ(z) ≥ m(z), so for a C 2 -function the two definitions agree and mφ = ∆φ. 1By “subharmonic” we will always mean “strictly subharmonic”. Non-strict subharmonicity will be referred to as “weak subharmonicity”. The same applies to plurisubharmonicity discussed below. 33 34 3.

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