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- From: palais@binah.cc.brandeis.edu
- Newsgroups: sci.physics,sci.math
- Subject: Re: Covariant vs. Lie Derivative in Gen. Rel.?
- Message-ID: <1992Nov17.174528.18418@news.cs.brandeis.edu>
- Date: 17 Nov 92 17:45:28 GMT
- References: <1992Nov11.062853.22717@galois.mit.edu> <1992Nov12.172748.16273@kakwa.ucs.ualberta.ca> <1992Nov13.213840.10075@galois.mit.edu> <1992Nov15.230139.24943@sbcs.sunysb.edu>,<phfrom.385@nyx.uni-konstanz.de>
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- Reply-To: palais@binah.cc.brandeis.edu
- Organization: Brandeis University
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-
- > rscott@libws3.ic.sunysb.edu (Robert Scott) writes:
-
- >>ISN'T IT EASY TO SHOW THAT THE LIE ALGEBRA OF SYMMETRIES OF AN
- >>AFFINE CONNECTION ON A CONNECTED FINITE-DIMENSIONAL MANIFOLD IS
- >>FINITE-DIMENSIONAL? THUS THE LIE ALGEBRA OF INFINITESIMAL
- >>SYMPLECTOMORPHISMS OF A SYMPLECTIC MANIFOLD IS FAR TOO BIG TO
- >>PRESERVE AN AFFINE CONNECTION.
-
- >You confuse me a bit :)
-
- >If I understand right, the covariant derivative must only preserve the
- >symplectic metric j with components
-
- > j_{ab} = j_{[ab]} = - j_{ba} ,
-
- >not the set of all symplectic transformations, to obtain a metricity
- >condition analogous to the Riemannian: There the Levi-Civita connection only
- >leaves (pseudo)-orthogonal g invariant, not all elements of the Lorentz
- >group. The symplectic metricity condition reads explicitely
-
- > 0 == - j_{ab;c} = - j_{ab,c} + j_{db} G^d_{ac} + j_{ad} G^d_{bc} .
- ^^^^^^
- = - j_{da}
-
- >The connection is then a 1-form with values in the symplectic Lie
- >algebra which is defined as the set of all generators of transformations
- >that leave j invariant, as the Riemannian is contained in the (local,
- >[pseudo]-orthogonal) invariance group of g. As I tried to line out in a
- >previous posting, I do not see a reasonable argument for uniquely fixing a
- >symplectic-metric connection, which happens to be possible for the
- >Riemannian by the demand of vanishing torsion, so that there remain
- >connection components independent of j.
-
- >BTW: The symplectic Lie algebra Sp(D,j) is of course finite-dimensional at
- > each point, and the j-metric connection is contained in it by def. It is
- > only infinite-dimensional (like the space of any scalar, vector, tensor,
- > spinor, or isotensor fields, i.e. the corresponding bundle) when viewed
- > non-locally, i.e. in some neighborhood, etc. Dimension of Sp(D,j) is
- > D*(D+1)/2 if D is the dimension of the manifold under consideration.
- --
- ===============
- There is great confusion going on here, and I hope the following will help
- clear it up, rather than increase the confusion!
-
- First, Robert Scott was replying to a remark of John Baez, saying that he did
- not believe that there was any way to construct canonically a connection (or
- covariant equivalently a covariant derivative) from a symplectic structure).
- Scott's answer (while not new) was exactly on target. His point was that if
- there was a canonical connection on a symplectic manifold (like the "Levi-Civita"
- connection on a Riemannian manifold) then just as an isometry of a Riemannian
- manifold preserves the Levi-Civita connection, any symplectomorphism of a
- symplectic manifold would preserve this canonical connection. But then he says
- it would follow that the group of syplectomorphisms would be isomorphic to
- a subgroup of the group of automorphisms of a connection---which is well-known
- to be finite dimensional (proof sketched below) while it is also well known that
- the group of symplectomorphisms is always infinite dimensional (the Lie algebra
- is isomorphic to the algebra of smooth functions (modulo constants) under Poisson
- bracket). (Of course the same argument applies to Riemannian manifolds and shows
-