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Unit 31: Finite Dimensional Spectral Theory




          Now Ty =  y      T (y , y , …) =  (y , y , …)                                         Notes
                              1  2        1  2
                           (0, y , y , …) = ( y ,  y  …)
                              1  2       1   2
                            y  = 0,  y  = y , ……
                             1     2   1
          Now y is a non-zero vector   y   0
                                    1
                  y  = 0   = 0.
                   1
          Then  y  = y    y  = 0 and this contradicts the fact that y is a non-zero vector. Therefore T cannot
                 2  1   1
          have an eigenvalue.
          31.1.5 Spectrum of an Operator

          The set of all eigenvalues of an operator is called the spectrum of T and is denoted by  (T).

          Theorem 1: If T is an arbitrary operator on a finite dimensional Hilbert space H, then the spectrum
          of T namely   (T) is a finite subset of the complex plane and the number of points in  (T) does
          not exceed the dimension n of H.
          Proof: First we shall show that an operator T on a finite dimensional Hilbert space h is singular
          if and only if there exists a non-zero vector x   H such that Tx = 0.
          Let  a non-zero vector x  H s.t. Tx = 0. We can write Tx = 0 as Tx = T0. Since x  0, the two distinct
          elements x, 0   H have the same image under T. Therefore T is not one-to-one. Hence T  does
                                                                                 –1
          not exist. Hence it is singular.
          Conversely, let T is singular. Let  no non-zero vector such that Tx = 0. This means Tx = 0   x =
          0. Then T must be one-to-one. Since H is finite dimensional and T is one-to-one, T is onto, so that
          T is a non-singular, contradicting the hypothesis that T is singular. Hence there must be non-
          zero vector x s.t. Tx = 0.
          Now if T is an operator on a finite dimensional Hilbert space H of dimension n. Then A scalar
               (T), if there exists a non-zero vector x such that (T –  I)x = 0.

          Now (T –  I)x = 0   (T –  I) is a singular.
          (T –  I) is singular   det (T –  I) = 0. Thus   (T)   satisfies the equation det (T –  I) = 0.
          Let B be an ordered basis for H. Thus det (T –  I)
                         = det ([T –  I] )
                                   B
          But det ([T –  I] ) = det ([T]  –  [I] )
                       B        B    B
          Thus det (T –  I) = det ([T]  –  [ ]).
                               B    ij
          So det (T –  I) = 0   det ([T]  –  [ ]) = 0  … (1)
                                 B    ij
          If [T]  = [ ] is a matrix of T then (1) gives
              B    ij
                              
                    11    12      1n
                              
                    22    22      2n          … (2)
                             
                             
                    n1            nn
          The expression of determinant of (2) gives a polynomial equation of degree n in   with complex
          coefficients in the variable  . This equation must have at least one root in the field of complex
          number (by fundamental theorem of algebra). Hence every operator T on H has eigenvalue so






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