Quantcast
  • Register
PhysicsOverflow is a next-generation academic platform for physicists and astronomers, including a community peer review system and a postgraduate-level discussion forum analogous to MathOverflow.

Welcome to PhysicsOverflow! PhysicsOverflow is an open platform for community peer review and graduate-level Physics discussion.

Please help promote PhysicsOverflow ads elsewhere if you like it.

News

PO is now at the Physics Department of Bielefeld University!

New printer friendly PO pages!

Migration to Bielefeld University was successful!

Please vote for this year's PhysicsOverflow ads!

Please do help out in categorising submissions. Submit a paper to PhysicsOverflow!

... see more

Tools for paper authors

Submit paper
Claim Paper Authorship

Tools for SE users

Search User
Reclaim SE Account
Request Account Merger
Nativise imported posts
Claim post (deleted users)
Import SE post

Users whose questions have been imported from Physics Stack Exchange, Theoretical Physics Stack Exchange, or any other Stack Exchange site are kindly requested to reclaim their account and not to register as a new user.

Public \(\beta\) tools

Report a bug with a feature
Request a new functionality
404 page design
Send feedback

Attributions

(propose a free ad)

Site Statistics

205 submissions , 163 unreviewed
5,082 questions , 2,232 unanswered
5,353 answers , 22,789 comments
1,470 users with positive rep
820 active unimported users
More ...

  The Tangent Bundle of the Space of CR Structures on S^(2n+1)

+ 4 like - 0 dislike
911 views

Let $M$ be a smooth compact $n$-manifold without boundary, $g$ some choice of Riemannian metric on $M$, and $\omega_g$ the volume form gotten from $g$. Say you're interested in finding extrema for quantities determined by a choice of Riemannian metric on $M$ . . . perhaps $\lambda_1(\int_M \omega_g)^{2/n}$, where $\lambda_1$ is the first nonzero eigenvalue of a Laplace-type operator, or maybe the zeta-regularized determinant of the conformal Laplacian.

The setting for this variational problem is the space of Riemannian metrics $\mathcal{M}$ on $M$. This is a tame Frechet manifold and is an open convex cone inside the tame Frechet space $\Gamma^\infty\!(S^2T^\ast\!M)$ of symmetric covariant 2-tensors on $M$ (Hamilton, 1982). These objects are standard in conformal geometry. In particular, if $M=S^{n}$, then $\Gamma^\infty\!(S^2T^\ast\!M)$ is the space of sections of a vector bundle associated to a representation of the conformal group of $M$, and variational problems can be addressed via the action of the conformal group (Møller & Ørsted, 2009).

My concern is whether there is an analogue of this picture for strongly pseudoconvex CR manifolds, in particular for $S^{2n+1}$ with its standard CR structure. What is the tangent bundle of the space of strongly pseudoconvex CR structures? What is the tangent bundle of the space of all CR structures? Is the space of strongly pseudoconvex CR structures on the sphere a tame Frechet manifold sitting as an open convex cone inside some tame Frechet space of sections of some vector bundle over $S^{2n+1}$? Is this vector bundle associated to a representation of a Lie group?

This post imported from StackExchange MathOverflow at 2014-09-20 22:39 (UCT), posted by SE-user user41626
asked Oct 21, 2013 in Mathematics by user41626 (20 points) [ no revision ]
retagged Nov 21, 2014 by dimension10

Your answer

Please use answers only to (at least partly) answer questions. To comment, discuss, or ask for clarification, leave a comment instead.
To mask links under text, please type your text, highlight it, and click the "link" button. You can then enter your link URL.
Please consult the FAQ for as to how to format your post.
This is the answer box; if you want to write a comment instead, please use the 'add comment' button.
Live preview (may slow down editor)   Preview
Your name to display (optional):
Privacy: Your email address will only be used for sending these notifications.
Anti-spam verification:
If you are a human please identify the position of the character covered by the symbol $\varnothing$ in the following word:
p$\hbar$ysicsO$\varnothing$erflow
Then drag the red bullet below over the corresponding character of our banner. When you drop it there, the bullet changes to green (on slow internet connections after a few seconds).
Please complete the anti-spam verification




user contributions licensed under cc by-sa 3.0 with attribution required

Your rights
...