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5.6. LINEAR OPERATORS                          207

                          Properties of a unitary operator U:
                                                U = U –1  or U U = UU = I,
                                                                ∗
                                                                        ∗
                                                 ∗
                                                 Ux  =  x   for all x in V.
                          A linear operator A in L(V, V)is saidtobe normal if
                                                                  ∗
                                                        A A = AA .
                                                          ∗
                          THEOREM. A bounded linear operator A is normal if and only if  Ax  =  A  x .
                          Remark. Any unitary or Hermitian operator is normal.


                       5.6.1-7. Transpose, symmetric, and orthogonal operators.

                       The transpose operator of a bounded linear operator A   L(V, V) in a real Hilbert space V
                       is the operator A T    L(V, V) such that for all x, y in V, the following relation holds:
                                                                   T
                                                     (Ax) ⋅ y = x ⋅ (A y).
                          THEOREM. Any bounded linear operator A in a real Hilbert space has a unique transpose
                       operator.
                          The properties of transpose operators in a real Hilbert space are similar to the properties
                                                                                 T
                                                                                             ∗
                       of adjoint operators considered in Paragraph 5.6.1-5 if one takes A instead of A .
                          A linear operator A   L(V, V) in a real Hilbert space V is said to be symmetric if
                                                 T
                                               A = A    or (Ax) ⋅ y = x ⋅ (Ay).
                          A linear operator A   L(V, V) in a real Hilbert space V is said to be skew-symmetric if
                                                T
                                              A =–A     or (Ax) ⋅ y =–x ⋅ (Ay).
                          The properties of symmetric linear operators in a real Hilbert space are similar to the
                                                                                             T
                       properties of Hermitian operators considered in Paragraph 5.6.1-5 if one takes A instead
                       of A .
                           ∗
                          A linear operator P   L(V, V) in a real Hilbert space V is said to be orthogonal if for
                       any x and y in V, the following relations hold:
                                                      (Px) ⋅ (Py)= x ⋅ y.
                       This relation is called the orthogonality condition.
                          Properties of orthogonal operator P:
                                                                       T
                                                 T
                                                               T
                                                P = P –1  or  P P = PP = I,
                                                 Px  =  x   for all x in V.
                       5.6.1-8. Positive operators. Roots of an operator.
                       A Hermitian (symmetric, in the case of a real space) operator A is said to be
                       a) nonnegative (resp., nonpositive), and one writes A ≥ 0 (resp., A ≤ 0)if (Ax) ⋅ x ≥ 0
                          (resp., (Ax) ⋅ x ≤ 0)for any x in V.
                       b) positive or positive definite (resp., negative or negative definite) and one writes A > 0
                          (A < 0)if (Ax) ⋅ x > 0 (resp., (Ax) ⋅ x < 0)for any x ≠ 0.
                          An mth root of an operator A is an operator B such that B m  = A.
                          THEOREM. If A is a nonnegative Hermitian (symmetric) operator, then for any positive
                       integer m there exists a unique nonnegative Hermitian (symmetric) operator A 1/m .
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