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5.13 Orthogonal Projection                                                         433

                                    Connections with Gram–Schmidt and QR. Recall from (5.5.4) on p. 309
                                    that the vectors in the Gram–Schmidt sequence generated from a linearly inde-
                                                                 m
                                    pendent set {x 1 , x 2 ,..., x n }⊂   are u 1 = x 1 /  x 1   and
                                                                                   2
                                                      T
                                              I − U k U
                                                      k  x k
                                      u k = 
        T     
 ,  where  U k = u 1 | u 2 |···| u k−1  for k> 1.
                                           
  I − U k U
                                                     k  x k  2
                                    Since {u 1 , u 2 ,..., u k−1 } is an orthonormal basis for span {x 1 , x 2 ,..., x k−1 } ,
                                    it follows from (5.13.4) that U k U T  must be the orthogonal projector onto
                                                                   k
                                                                                                    T
                                                                     T
                                    span {x 1 , x 2 ,..., x k−1 } . Hence U k U = P k and (I−P k )x k =(I−U k U )x k ,
                                                                     k
                                                                                                    k

                                    so  
  I − U k U T  
  = ν k is the k th  projected height in (5.13.7). This means
                                                k  x k  2
                                    that when the Gram–Schmidt equations are written in the form of a QR fac-
                                    torization as explained on p. 311, the diagonal elements of the upper-triangular
                                    matrix R are the ν k ’s. Consequently, the product of the diagonal entries in R
                                    is the volume of the parallelepiped generated by the x k ’s. But the QR factor-

                                    ization of A = x 1 | x 2 |···| x n is unique (Exercise 5.5.8), so it doesn’t matter
                                    whether Gram–Schmidt or another method is used to determine the QR factors.
                                    Therefore, we arrive at the following conclusion.
                                    •  If A m×n = Q m×n R n×n is the (rectangular) QR factorization of a matrix
                                       with linearly independent columns, then the volume of the n-dimensional
                                       parallelepiped generated by the columns of A is V n = ν 1 ν 2 ··· ν n , where
                                       the ν k ’s are the diagonal elements of R. We will see on p. 468 what this
                                       means in terms of determinants.
                                        Of course, not all projectors are orthogonal projectors, so a natural question
                                    to ask is, “What characteristic features distinguish orthogonal projectors from
                                    more general oblique projectors?” Some answers are given below.


                                                         Orthogonal Projectors

                                                          n×n                     2
                                       Suppose that P ∈       is a projector—i.e., P = P. The following
                                       statements are equivalent to saying that P is an orthogonal projector.
                                       •   R (P) ⊥ N (P).                                      (5.13.8)
                                                                                  2
                                                                                           T
                                            T
                                       •   P = P    (i.e., orthogonal projector ⇐⇒ P = P = P ). (5.13.9)
                                       •    P  =1 for the matrix 2-norm (p. 281).             (5.13.10)
                                              2
                                    Proof.  Every projector projects vectors onto its range along (parallel to) its
                                    nullspace, so statement (5.13.8) is essentially a restatement of the definition of
                                    an orthogonal projector. To prove (5.13.9), note that if P is an orthogonal
                                    projector, then (5.13.3) insures that P is symmetric. Conversely, if a projector
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