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Linear Algebra




                    Notes          Corollary: Let V be a finite-dimensional vector space over the field F. Each basis for V* is the
                                   dual of some basis for V.

                                   Proof: Let  *= f  1 ,..., f n be a basis for V*. By Theorem 2 of unit 10 there is a basis  L 1 ,...,L for
                                                                                                           n
                                   V** such that

                                                 L f     .                                                 ...(5)
                                                  i  i  ij
                                   Using the corollary above, for each i there is a vector , in V such that
                                                 L (f) = f()
                                                  i     i
                                   for every f in V*, i.e., such that L  L  . It follows immediately that   ,...,  is a basis for V and
                                                            i   i                         1   n
                                   that  * is the dual of this basis.

                                   In view of Theorem 1, we usually identify  with  L and say that V ‘is’ the dual space of V* or
                                   that the spaces V, V* are naturally in duality with one another. Each is the dual space of the other.
                                   In the last corollary we have an illustration of how that can be useful. Here is a further illustration.
                                   If E is a subset of V*, then the annihilator  E  is (technically) a subset of  V**. If we choose to
                                                                       0
                                                                     0
                                   identify V and V** as in Theorem (1), then E  is a subspace of V, namely, the set of all   in V such
                                   that  f  = 0 for all f in E. In a corollary of Theorem 3 of unit 10 we noted that each subspace W
                                   is determined by its annihilator W°. How is it determined? The answer is that W is the subspace
                                   annihilated by all f in W°, that is, the intersection of the null spaces of all f’s in W°. In our present
                                   notation for annihilators, the answer may be phrased very simply:  W = (W°)°.

                                   Theorem 2: If S is any subset of a finite-dimensional vector space V, then (S°)° is the subspace
                                   spanned by S.

                                   Proof: Let W be the subspace spanned by S. Clearly W° = S°. Therefore, what we are to prove is
                                   that W = W°°. We have given one proof. Here is another. By Theorem 3 of unit 10.

                                          dimW   dimW    dimV
                                                                                                           ...(6)
                                          dimW    dimW     dimV  *

                                   and since dimV  dimV  * we have
                                          dimW   dimW   .

                                   Since W is a subspace of W°°, we see that W = W°°.
                                   The results of this section hold for arbitrary vector spaces; however the proofs require the use of
                                   the so-called Axiom of Choice. Here we shall not tackle annihilators for general vector spaces.
                                   But, there are two  results about  linear functionals  on arbitrary  vector spaces  which are  so
                                   fundamental that we should include them.
                                   Let V be a vector space. We want to define hyperspaces in V. Unless V is finite-dimensional, we
                                   cannot do that with the dimension of the hyperspace. But, we can express the idea that a space N
                                   falls just one dimension short of filling out V, in the following way:
                                   1.  N is a proper subspace of V;
                                   2.  If W is a subspace of V which contains N, then either W = N or W = V.
                                   Conditions (1) and (2) together say that  N is a proper subspace and there is no larger proper
                                   subspace, in short, N is a maximal proper subspace.




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