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206                                 ALGEBRA

                          The rank of a linear operator A is the dimension of its range: rank (A)= dim (im A).
                          Properties of the rank of a linear operator:

                                              rank (AB) ≤ min{rank (A), rank (B)},
                                              rank (A)+ rank (B)– n ≤ rank (AB),

                       where A and B are linear operators in L(V, V)and n =dim V.
                          Remark. If rank (A)= n then rank (AB)=rank (BA)=rank (B).

                          THEOREM. Let A : V→ V be a linear operator. Then the following statements are
                       equivalent:
                                                       –1
                       1. A is invertible (i.e., there exists A ).
                       2. ker A = 0.
                       3. im A = V.
                       4. rank (A)= dim V.


                       5.6.1-5. Notion of a adjoint operator. Hermitian operators.

                       Let A   L(V, V) be a bounded linear operator in a Hilbert space V. The operator A in
                                                                                                  ∗
                       L(V, V) is called its adjoint operator if
                                                      (Ax) ⋅ y = x ⋅ (A y)
                                                                    ∗
                       for all x and y in V.
                          THEOREM. Any bounded linear operator A in a Hilbert space has a unique adjoint
                       operator.
                          Properties of adjoint operators:
                                                                ¯
                                                                         ∗ ∗
                                                ∗
                                           ∗
                                                     ∗
                                                                   ∗
                                                             ∗
                                    (A + B) = A + B ,   (λA) = λA ,(A ) = A,
                                              ∗
                                                ∗
                                                          ∗
                                    (AB) = B A ,        O = O,         I = I,
                                         ∗
                                                                       ∗
                                                                                   2
                                               ∗ –1
                                    (A ) =(A ) ,         A   =  A ,     A A  =  A  ,
                                                                         ∗
                                                           ∗
                                       –1 ∗
                                    (Ax) ⋅ (By) ≡ x ⋅ (A By) ≡ (B Ax) ⋅ y  for all x and y in V,
                                                              ∗
                                                     ∗
                                                                               ¯
                       where A and B are bounded linear operators in a Hilbert space V, λ is the complex conjugate
                       of a number λ.
                          A linear operator A   L(V, V) in a Hilbert space V is said to be Hermitian (self-adjoint) if
                                                A = A   or  (Ax) ⋅ y = x ⋅ (Ay).
                                                 ∗
                          A linear operator A   (V, V) in a Hilbert space V is said to be skew-Hermitian if
                                              A =–A     or  (Ax) ⋅ y =–x ⋅ (Ay).
                                                ∗
                       5.6.1-6. Unitary and normal operators.
                       A linear operator U   L(V, V) in a Hilbert space V is called a unitary operator if for all x
                       and y in V, the following relation holds:
                                                      (Ux) ⋅ (Uy)= x ⋅ y.
                       This relation is called the unitarity condition.
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