29.1 Non-degenerate bilinear forms

Concept links · terms present in this machine draft; source roles are unverified: vector space · complex inner product · orthogonal group · complexification

In the case of , the dual phase space, the Poisson bracket determines an antisymmetric bilinear form on , which, for a basis and two vectors

is given explicitly by

Matrices such that

make up the group and preserve Ω, satisfying

This choice of Ω is much less arbitrary than it looks. One can show that given any non-degenerate antisymmetric bilinear form on a basis can be found with respect to which it will be the Ω given here (for a proof, see [8]). This is also true if one complexifies , using the same formula for Ω, which is now a bilinear form on . In the real case the group that preserves Ω is called , in the complex case

To get a fermionic analog of this, all one needs to do is replace “nondegenerate antisymmetric bilinear form with “non-degenerate symmetric bilinear form . Such a symmetric bilinear form is actually something much more familiar from geometry than the antisymmetric case analog: it is just a notion of inner product. Two things are diferent in the symmetric case:

• The underlying vector space does not have to be even dimensional, one can take for any including n odd. To get a detailed analog of the bosonic case though, we will need to consider the even case

• For a given dimension , there is not just one possible choice of up to change of basis, but one possible choice for each pair of non-negative integers , such that . Given , any choice of can be put

in the form

For a proof by Gram-Schmidt orthogonalization, see [8].

We can thus extend our definition of the orthogonal group as the group of transformations g preserving an inner product

to the case arbitrary by:

Definition (Orthogonal group $O ( r , s , { \bf R } )

)O ( r , s , \mathbf { R } )r + sr + sg$ that satisfy

is the subgroup of matrices of determinant +1.

If one complexifies, taking components of vectors to be in , using the same formula for , one can change basis by multiplying the s basis elements by a factor of and in this new basis all basis vectors satisfy One thus sees that on , as in the symplectic case, up to change of basis there is only one non-degenerate symmetric bilinear form. The group preserving this is called . Note that on is not the Hermitian inner product (which is antilinear on the first variable), and it is not positive definite.

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原书 PDF · 印刷页 318、319、320、321、322、323、324、325

来源版本:2025-10-20

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