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Contractibility of unit sphere in Hilbert space

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In topology, it is a surprising fact that the unit sphere in (infinite-dimensional) Hilbert space is a contractible space, since no finite-dimensional spheres are contractible.

This can be demonstrated in several different ways.

Contents

[edit] Topological proof

First, one can use a purely topological argument, appealing to the Whitehead theorem. This proof proceeds as follows: Let H denote the Hilbert space, and S the unit sphere in H. Consider the k-th homotopy group πk(S). Any element in this group is represented by a map \gamma:S^k \to S where Sk is the standard k-sphere. Since Sk is compact, so is its image under γ. Hence the image is contained in some n-dimensional subspace of H. Since the intersection of this subspace with S is an n-sphere, by choosing n large enough (i.e. larger than k), one sees that the map γ is null-homotopic when considered as a map S^k \to S^n, hence it is also null-homotopic as a map S^k \to S. Thus, all of the homotopy groups πk(S) vanish. Furthermore, since the inclusion \lbrace point \rbrace \to S induces isomorphisms on all homotopy groups, and all spaces under consideration are connected CW-complexes, the conditions of the Whitehead theorem apply and we can conclude that S is homotopy-equivalent to a point, i.e. contractible.

[edit] Constructive proof via shift operator

Let H be a separable, infinite-dimensional Hilbert space. One can assume H = l2(N), the space of square-summable complex sequences. Let S be the unit ball in H.

The topological proof given in the preceding section is non-constructive. It is possible to prove the contractibility of S by explicitly showing that S deformation retracts to a single point, that is, writing down a homotopy between the identity map on S and a constant map

e( (z_i)_{i \geq 1} ) = (1,0,0,\cdots)

on S. This can be done in two stages. First we show that the identity map on S is homotopic to the shift operator T restricted to S. Second, we show that T restricted to S is homotopic to e. The desired result then follows from the transitivity of homotopy equivalence.

The shift operator T on H is defined by

T (z_1, z_2, ...) = (0, z_1, z_2, ...). \,

T is an isometry (which is not the case if H were finite dimensional), and therefore leaves S invariant. The image T(S) is the equator of S, which is homeomorphic to the sphere S itself (which clearly does not hold in the finite-dimensional case).

Consider the line segment γ from xS to TxS:

\gamma_x (t) = (1-t)x + tT(x). \,

Now T has no eigenvalues. So γ(t) is never the zero vector in H. Thus one can normalize γ to obtain a path in S:

\gamma_x'(t) = \frac{\gamma_x(t)}{\| \gamma_x(t)\|}.

The homotopy defined by

I_t (x) = \gamma'_x(t), \; t \in [0,1]

takes the identity to the shift.

Next we show that T is null-homotopic. For each

x  =(z_1, z_2, z_3, ...) \in S,

the path in S defined by (here one again needs the fact that T is an isometry)

\phi_x(t) = \sin \frac{\pi}{2} t \, (1, 0, \cdots)+  \cos \frac{\pi}{2} t \, Tx

goes from Tx to the element (1,0,0...). So the homotopy

I'_t (x) = \phi_x(t) \,

takes T to the constant map e. This, together with the homotopy I from the above, proves the claim.

[edit] Second constructive proof

Another manifestation of a separable infinite dimensional Hilbert space is, the function space L2[0,1] , complex-valued functions on the interval [0,1] square integrable with respect to the Lebesgue measure, modulo equality almost everywhere.

Given a function f in S and t ∈ [0,1], define


f_t(x) = \begin{cases}
    f(x/(1-t)) & \mbox{if }x < (1-t)  \\
    1 & \mbox{if } x \ge (1-t)
\end{cases}.

This is a "sped-up" version of f for the interval [0,(1 - t)], and the constant function 1 on [(1 - t),1]. Direct calculation shows that that ft lies in S for all t ∈ [0,1]. The map H on [0, 1] × S given by

H(t, f) (x) =  f_t(x)\,

is continuous and therefore a homotopy from the identity map on S to the constant map whose range is 1 ∈ L2[0,1].

[edit] References

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