Stiefel manifold

Stiefel manifold

In mathematics, the Stiefel manifold "V""k"(R"n") is the set of all orthonormal "k"-frames in R"n". That is, it is the set of ordered "k"-tuples of orthonormal vectors in R"n". Likewise one can define the complex Stiefel manifold "V""k"(C"n") of orthonormal "k"-frames in C"n" and the quaternionic Stiefel manifold "V""k"(H"n") of orthonormal "k"-frames in H"n". More generally, the construction applies to any real, complex, or quaternionic inner product space.

In some contexts, a non-compact Stiefel manifold is defined as the set of all linearly independent "k"-frames in R"n", C"n", or H"n".

Topology

Let F stand for R, C, or H. The Stiefel manifold "V""k"(F"n") can be thought of as a set of "n" × "k" matrices by writing a "k"-frame as a matrix of "k" column vectors in F"n". The orthonormality condition is expressed by "A"*"A" = 1 where "A"* denotes the conjugate transpose of "A" and 1 denotes the "k" × "k" identity matrix. We then have:V_k(mathbb F^n) = left{A in mathbb F^{n imes k} : A^{ast}A = 1 ight}.

The topology on "V""k"(F"n") is the subspace topology inherited from F"n"×"k". With this topology "V""k"(F"n") is a compact manifold whose dimension is given by

:dim V_k(mathbb R^n) = nk - frac{1}{2}k(k+1):dim V_k(mathbb C^n) = 2nk - k^2:dim V_k(mathbb H^n) = 4nk - k(2k-1).

As a homogeneous space

Each of the Stiefel manifolds "V""k"(F"n") can be viewed as a homogeneous space for the action of a classical group in a natural manner.

Every orthogonal transformation of a "k"-frame in R"n" results in another "k"-frame, and any two "k"-frames are related by some orthogonal transformation. In other words, the orthogonal group O("n") acts transitively on "V""k"(R"n"). The stabilizer subgroup of a given frame is the subgroup isomorphic to O("n"−"k") which acts nontrivially on the orthogonal complement of the space spanned by that frame.

Likewise the unitary group U("n") acts transitively on "V""k"(C"n") with stabilizer subgroup U("n"−"k") and the symplectic group Sp("n") acts transitively on "V""k"(H"n") with stabilizer subgroup Sp("n"−"k").

In each case "V""k"(F"n") can be viewed as a homogeneous space:

:egin{align}V_k(mathbb R^n) &cong mbox{O}(n)/mbox{O}(n-k)\V_k(mathbb C^n) &cong mbox{U}(n)/mbox{U}(n-k)\V_k(mathbb H^n) &cong mbox{Sp}(n)/mbox{Sp}(n-k).end{align}

When "k" = "n", the corresponding action is free so that the Stiefel manifold "V""n"(F"n") is a principal homogeneous space for the corresponding classical group.

When "k" is strictly less than "n" then the special orthogonal group SO("n") also acts transitively on "V""k"(R"n") with stabilizer subgroup isomorphic to SO("n"−"k") so that:V_k(mathbb R^n) cong mbox{SO}(n)/mbox{SO}(n-k)qquadmbox{for } k < n.The same holds for the action of the special unitary group on "V""k"(C"n"):V_k(mathbb C^n) cong mbox{SU}(n)/mbox{SU}(n-k)qquadmbox{for } k < n.

pecial cases

A 1-frame in F"n" is nothing but a unit vector, so the Stiefel manifold "V"1(F"n") is just the unit sphere in F"n".

Given a 2-frame in R"n", let the first vector define a point in "S""n"−1 and the second a unit tangent vector to the sphere at that point. In this way, the Stiefel manifold "V"2(R"n") may be identified with the unit tangent bundle to "S""n"−1.

When "k" = "n" or "n"−1 we saw in the previous section that "V""k"(F"n") is a principal homogeneous space, and therefore diffeomorphic to the corresponding classical group. These are listed in the table at the right.

As a principal bundle

There is a natural projection:p: V_k(mathbb F^n) o G_k(mathbb F^n)from the Stiefel manifold "V""k"(F"n") to the Grassmannian of "k"-planes in F"n" which sends a "k"-frame to the subspace spanned by that frame. The fiber over a given point "P" in "G""k"(F"n") is the set of all orthonormal "k"-frames contained in the space "P".

This projection has the structure of a principal "G"-bundle where "G" is the associated classical group of degree "k". Take the real case for concreteness. There is a natural right action of O("k") on "V""k"(R"n") which rotates a "k"-frame in the space it spans. This action is free but not transitive. The orbits of this action are precisely the orthonormal "k"-frames spanning a given "k"-dimensional subspace; that is, they are the fibers of the map "p". Similar arguments hold in the complex and quaternionic cases.

We then have a sequence of principal bundles::egin{align}mathrm O(k) & o V_k(mathbb R^n) o G_k(mathbb R^n)\mathrm U(k) & o V_k(mathbb C^n) o G_k(mathbb C^n)\mathrm{Sp}(k) & o V_k(mathbb H^n) o G_k(mathbb H^n).end{align}

The vector bundles associated to these principal bundles via the natural action of "G" on F"k" are just the tautological bundles over the Grassmannians. In other words, the Stiefel manifold "V""k"(F"n") is the orthogonal, unitary, or symplectic frame bundle associated to the tautological bundle on a Grassmannian.

When one passes to the "n" &rarr; &infin; limit, these bundles become the universal bundles for the classical groups.

Homotopy

The Stiefel manifolds fit into a family of fibrations V_{k-1}(Bbb R^{n-1}) o V_k(Bbb R^n) o S^{n-1}, thus the first non-trivial homotopy group of the space V_k(Bbb R^n) is in dimension n-k. Moreover, pi_{n-k} V_k(Bbb R^n) simeq Bbb Z if n-k in 2 Bbb Z or if k=1. pi_{n-k} V_k(Bbb R^n) simeq Bbb Z_2 if n-k is odd and k>1. This result is used in the obstruction-theoretic definition of Stiefel-Whitney classes.

ee also

*Flag manifold

References

*cite book | first = Allen | last = Hatcher | authorlink = Allen Hatcher | year = 2002 | title = Algebraic Topology | publisher = Cambridge University Press | id = ISBN 0-521-79540-0 | url = http://www.math.cornell.edu/~hatcher/AT/ATpage.html
*cite book | first = Dale | last = Husemoller | year = 1994 | title = Fibre Bundles | edition = (3rd ed.) | publisher = Springer-Verlag | location = New York | id = ISBN 0-387-94087-1


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