Page 1
Review
⌅⌅ minimal solution of Ax = b :
solution with the smallest norm:least energy, least power, etc.
⌅⌅ Theorem 6.13: A 2 Mm⇥n(F ); b 2 Fm; and s is a minimal solu- tion of Ax = b.
Then
⌅ s 2 R(LA⇤).
⌅ s is the only solution in R(LA⇤).
That is, AA⇤u = b ) s = A⇤u.
⌅ s is unique.
⌅⌅ Compare x = s + y, s 2 R(LA⇤), y 2 N(LA) vs Theorem 3.9:
K = {s} + KH.
Page 2
Normal and self-adjoint operator
⌅⌅ We now investigate diagonalizability of a linear operator on an inner product space.
⌅⌅ Lemma 6.14 V is an inner product space; dim(V ) < 1; T : V ! V is a linear operator. Then
T has an eigenvector ) T⇤ has an eigenvector.
⌅⌅ Theorem 6.14 (Schur): din(V ) < 1; T : V ! V is a linear opera- tor; and fT(t) splits. Then 9 an orthonormal basis such that [T ] is upper triangular.
⌅ Schur’s theorem does not say that [T ] is invertible.
⌅ Neither does it say that [T ] is diagonalizable.
⌅ in the theorem is not unique; nor [T ] .
Page 3
⌅ T is diagonalizable ) [T ] is diagonal for some . ) [T ⇤] = [T ]⇤ is diagonal.
) [T T ⇤] = [T ] [T ]⇤ = [T ]⇤[T ] = [T⇤T ] [diagonal]
) T T ⇤ = T ⇤T [rep is unique]
Does this commutativity imply diagonalizability?
⌅ normal operator T on an inner product space: T T⇤ = T⇤T
⌅ normal matrix A : AA⇤ = A⇤A
⌅ T (A) is normal , [T ] is normal.
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Page 4
⌅⌅ Theorem 6.15 : V is an inner product space; T : V ! V is normal.
Then
1. 8x 2 V, ||T (x)|| = ||T⇤(x)||.
2. 8c 2 F, T cI is normal.
3. T (x) = x , T⇤(x) = x. That is, T and T⇤ have the same eigenvector x with the respective eigenvalues and .
4. T (x1) = 1x1; T (x2) = 2x2; 1 6= 2 ) hx1, x2i = 0.
⌅⌅ Theorem 6.16 : V is an inner product space over the ”complex”
field; dim(V ) < 1; T : V ! V is linear. Then T is normal if and only if there exists an orthonormal basis for V consisting of eigenvectors of T .
⌅⌅ [End of Review]
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⌅⌅ self-adjoint (Hermitian) operator T on an inner product space:
T = T ⇤.
⌅ self-adjoint (Hermitian) matrix A: A = A⇤
⌅ these definitions apply to both the real and complex field.
⌅ For complex matrices, self-adjoint means conjugate symmetric.
⌅ For real matrices, self-adjoint means symmetric.
⌅ For orthonormal , T = T⇤ , [T ] = [T ]⇤
⌅ self-adjoint ) normal; normal 6) self-adjoint
Page 6
⌅⌅ Lemma 6.17: V is an inner product space; dim(V ) < 1; T : 1. Every eigenvalue of T is real.
2. fT(t) splits over the real field.
proof: ”1”: Let T (x) = x, x 6= 0.
) hx, xi = hT (x), xi = hx, T⇤(x)i = hx, T (x)i= hx, xi = hx, xi
2 follows from 1.
⌅⌅ Theorem 6.17: V is an inner product space over the ”real” field;
dim(V ) < 1; T : V ! V is linear. Then T is self-adjoint if and only if there exists an orthonormal basis for V consisting of eigenvectors of T .
is
set
卵呵Page 7
proof:
”only if”: Assume T = T⇤.
) fT(t) splits (over the real field). [Lemma 6.17]
) 9 , orthonormal, such that [T ] is upper triangular. [Schur’s Thm]
) [T ]⇤ = [T⇤] = [T ] [self-adjoint]
) [T ] is (real) diagonal.
) consists of eigenvectors of T .
”if” : Assume an orthonormal basis of eigenvectors of T . ) [T ] is (real) diagonal.
) [T ⇤] = [T ]⇤ = [T ]
) T⇤ = T [rep is unique]
Page 8
Unitary and orthogonal operator
⌅⌅ V is an inner product space; dim(V ) < 1; T : V ! V is linear.
⌅ unitary operator: 8x 2 V (C), ||T (x)|| = ||x||
⌅ orthogonal operator: 8x 2 V (R), ||T (x)|| = ||x||
⌅⌅ Lemma 6.18: V is an inner product space; dim(V ) < 1; U : V ! V is self-adjoint. Then 8x 2 V, hx, U(x)i = 0 ) U = T0.
proof.
Assume U is self-adjoint and 8x 2 V, hx, U(x)i = 0.
) 9 = {v1, · · · , vn} orthonormal and consisting of eigenvectors of U. [Thm 6.16, 6.17]
) ihvi, vii = hvi, ivii = hvi, U (vi)i = 0, i = 1, · · · , n ) i = 0, i = 1, · · · , n
) 8x 2 V,
U (x) = U (Pn
i=1 aivi) = Pn
i=1 aiU (vi) = Pn
i=1 ai uvi = 0
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Page 9
⌅⌅ Theorem 6.18: V is an inner product space; dim(V ) < 1; T : V ! V is linear. Then these are all equivalent.
1. T T⇤ = T ⇤T = I
2. 8x, y 2 V, hT (x), T (y)i = hx, yi
3. is an orthonormal basis ) T ( ) is an orthonormal basis.
4. There exists an orthonormal basis such that T ( ) is an or- thonormal basis.
5. 8x 2 V, ||T (x)|| = ||x||
⌅ 5 means length-preserving; 2 means sort of angle-preserving.
⌅ rotation and reflection in R2 are orthogonal.
⌅ unitary or orthogonal ) normal; not conversely.
proof: ”1)2”: Assume T T⇤ = T⇤T = I ) hT (x), T (y)i = hx, T ⇤T (y)i = hx, yi
unitary.arthogor.ae
.Page 10
”2)3” : Assume ”2” and an orthonormal basis {v1, · · · , vn}.
) hT (vi), T (vj)i = hvi, vji = ij
) {T (vi), · · · , T (vn)} is an orthonormal basis.
”3)4” : Obvious.
”4)5” : Assume = {v1, · · · , vn} and T ( ) are orthonormal.
) ||T (x)||2 = ||T (Pn
i=1 aivi)||2 = || Pn
i=1 aiT (vi)||2
= hPn
i=1 aiT (vi), Pn
j=1 ajT (vj)i
= Pn
i=1
Pn
j=1 aiajhT (vi), T (vj)i = Pn
i=1 |ai|2 = ||x||2
”5)1”: Assume 8x 2 V, ||T (x)|| = ||x||.
) hx, xi = hT (x), T (x)i = hx, T⇤T (x)i ) 8x 2 V, hx, (I T ⇤T )(x)i = 0
) (I T ⇤T ) = T0, [(I T⇤T ) is self-adjoint; Lemma6.18]
) T⇤T = I ) T T⇤ = I [Thm 2.17c]
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Page 11
⌅⌅ T is unitary or orthogonal; v is an eigenvector.
) ||v|| = ||T (v)|| = || v|| = | |||v||
) | | = 1
⌅⌅ example: linear operators on R2
⌅ T✓: rotation by ✓; T✓⇤ = T ✓ ) T✓T✓⇤ = T✓T ✓ = I
⌅ T: reflection about a line or the origin; T⇤ = T! T T ⇤ = T T = I
⌅⌅ unitary matrix: AA⇤ = A⇤A = I
⌅ orthogonal matrix over the real field : AAt = AtA = I
⌅ real unitary matrix = orthogonal matrix
⌅ columns from an orthonormal basis for F n.
⌅ rows form an orthonormal basis for Fn.
⌅ T is unitary , [T ] is unitary for an orthonormal .
⌅ T is orthogonal , [T ] is orthogonal for an orthonormal .
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Page 12
⌅⌅ A matrix A is unitarily equivalent to B : 9 a unitary matrix Q such that A = Q⇤BQ.
⌅ A real matrix A is textbforthogonally equivalent to real B : 9 an orthogonal matrix Q such that A = QtBQ.
⌅ A and B are unitarily equivalent ) they are similar, but not con- versely.
⌅⌅ Theorem 6.19: A complex n ⇥ n matrix A is normal.
, A is unitarily equivalent to a diagonal matrix.
⌅ This is the matrix version of Theorem 6.16.
proof: ”)”: Assume A is normal and is the std basis for Fn. ) LA is normal and [LA] = A.
) 9 an orthonormal basis of eigenvectors of LA. [Thm 6.16]
) [LA] = D, diagonal.
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Page 13
) A = [LA] = [I] [LA] [I] = Q 1DQ.
We show that Q = [I] is unitary if and are orthonormal.
Let = (u1, · · · , un) and = (v1, · · · , vn), both orthonormal.
) vj = Pn
i=1hvj, uiiui ) Qij = hvj, uii ) Q⇤ij = Qji = hvi, uji = huj, vii = ([I] )ij
) QQ⇤ = [I] [I] = I, and similarly, Q⇤Q = I.
”(”: Assume Q, unitary, and D, diagonal, are such that A = Q⇤DQ.
) AA⇤ = Q⇤DQ(Q⇤DQ)⇤ = Q⇤DQQ⇤D⇤Q
= Q⇤DD⇤Q = Q⇤D⇤DQ = Q⇤D⇤QQ⇤DQ = (Q⇤DQ)⇤Q⇤DQ =
= A⇤A [diagonals commute]
Page 14
⌅⌅ Theorem 6.20: A real n ⇥ n matrix A is symmetric.
, A is orthogonally equivalent to a real diagonal matrix.
⌅ This is the matrix version of Theorem 6.17.
⌅⌅ Theorem 6.21 (Schur) : A 2 Mn⇥n(F ); fA(t) splits over F . Then
1. If F = C, then A is unitarily equivalent to a complex upper triangular matrix.
2. If F = R, then A is orthogonally equivalent to a real upper triangular matrix.
⌅ This is the matrix version of Schur’s Theorem 6.14.
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Page 15
Orthogonal projection and spectral theorem
⌅⌅ LetV = W1 L
W2 for subspaces W1 and W2.
Then, 8x 2 V, x = x1 + x2 for some s1 2 W1, x2 2 W2.
⌅ projection T on W1 along W2 : T (x1 + x2) = x1
⌅ R(T ) = W1 = {x 2 V : T (x) = x}
⌅ N (T ) = W2 = {x 2 V : T (x) = 0}
⌅ For a projection T on W1,we can choose various W2.
⌅ If T is an ”orthogonal” projection on W1, then W2 is unique.
⌅⌅ T is a projection , T = T2 [alt def]
proof: ” ) ” : 8x 2 V, T2(x) = T (x1) = T (x1 + 0) = x1
” ( ”: Assume that T = T 2.
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Page 16
First we show that R(T ) \ N(T ) = {0}.
Assume x 2 R(T ) \ N(T ).
x 2 R(T ) ) 9u such that T (u) = x ) T2(u) = T (u) = x x 2 N(T ) ) T (x) = 0 ) T2(x) = T (x) = 0
) x = 0, (* T2(u) = T (x) = x = 0) Now we show that V = R(T ) + N(T ).
8x 2 V , let x1 = T (x) and x2 = x x1. ) x1 2 R(T )
T (x2) = T (x) T (x1) = T (x) T2(x) = 0 ) x2 2 N(T ) V = R(T ) L
N (T )
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Page 17
⌅⌅ orthogonal projection T :
R(T )? = N (T ) and N(T )? = R(T )
⌅ If dim(V ) < 1, (R(T )? = N (T ) , N(T )? = R(T )).
⌅ Given a subspace W, T (y) = u, [Thm 6.6]
where y = u + z, u 2 W, z 2 W?,
defines an orthogonal projection on W .
⌅ A truncated Fourier series, for k < n, u = Pk
i=1hy, vii is an orthogonal projection on span({v1, · · · , vk}).
⌅ There is only one orthogonal projection on W .
⌅ The orthogonal projection on W provides the best approximation.
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Page 18
⌅⌅ Theorem 6.24: V is an inner product space:T : V ! V is linear.
Then T is an orthogonal projection , T2 = T = T⇤. Proof:
” ) ”: Assume T is an orthogonal projection.
) T2 = T [projection]
) V = R(T ) L
N (T ); R(T )? = N (T )
) 8x, y 2 V, x x1 + x2 and y = y1 + y2, for some x1, y1 2 R(T ) and x2, y2 2 N(T ).
) hx, T (y)i = hx1 + x2, y1i = hx1, y1i + hx2, y1i = hx1, y1i = hx1, y1i + hx1, y2i = hx1, y1 + y2i = hT (x), yi = hx, T⇤(y)i
” ( ”: Assume T2 = T = T ⇤ ) T is a projection.
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Let x 2 R(T ) and y 2 N(T ). ) T (x) = x, T (y) = 0.
) hx, yi = hT (x), yi = hx, T⇤(y)i = hx, T (y)i = hx, 0i = 0 ) x 2 N(T )? and y 2 R(T )?
) R(T ) ✓ N(T )? and N(T ) ✓ R(T )? (1) Let x 2 N(T )?
) x = x1 + x2, x1 2 R(T ), x2 2 N(T ) [projection]
) 0 = hx, x2i = hx1, x2i + hx2, x2i = ||x2||2 [x1 2 N(T )? (1)]
) x2 = 0 ) x = x1 2 R(T ) ) N(T )? ✓ R(T ) ) N(T )? = R(T ) [(1), cf textbook]
Let y 2 R(T )?.
) y = y1 + y2, y1 2 R(T ), y2 2 N(T ) [projection]
) 0 = hy, y1i = hy1, y1i + hy2, y1i = ||y1||2[y2 2 R(T )? (1)]
) y1 = 0 ) y = y2 2 N(T ) ) R(T )? ✓ N(T ) ) R(T )? = N (T ) [(1), cf textbook]
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Page 1
Review
⌅⌅ self-adjoint (Hermitian) operator T : T = T ⇤.
⌅ self-adjoint (Hermitian) matrix A: A = A⇤
⌅ A: Conjugate symmetric.
⌅⌅ Theorem 6.17: For finite V over the ”real” field, T is self-adjoint iff 9 an orthonormal basis for V consisting of eigenvectors of T . proof:
”only if”: Assume T = T⇤.
) fT(t) splits (over the real field). [Lemma 6.17]
) 9 , orthonormal, s. t. [T ] is upper triangular. [Schur’s Thm]
) [T ]⇤ = [T⇤] = [T ] [self-adjoint]
) [T ] is (real) diagonal.
) consists of eigenvectors of T .
(real eisen Values)
Page 2
Unitary and orthogonal operator
⌅⌅ V is an inner product space; dim(V ) < 1; T : V ! V is linear.
⌅ unitary operator: 8x 2 V (C), ||T (x)|| = ||x||
⌅ orthogonal operator: 8x 2 V (R), ||T (x)|| = ||x||
⌅⌅ Lemma 6.18: V is an inner product space; dim(V ) < 1; U : V ! V is self-adjoint. Then 8x 2 V, hx, U(x)i = 0 ) U = T0.
proof.
Assume U is self-adjoint and 8x 2 V, hx, U(x)i = 0.
) 9 = {v1, · · · , vn} orthonormal and consisting of eigenvectors of U. [Thm 6.16, 6.17]
) ihvi, vii = hvi, ivii = hvi, U (vi)i = 0, i = 1, · · · , n ) i = 0, i = 1, · · · , n
) 8x 2 V,
U (x) = U (Pn
i=1 aivi) = Pn
i=1 aiU (vi) = Pn
i=1 ai ivi = 0
T.' Normal .TT#=TT
⇒ 丁以二 干叉T I
Page 3
⌅⌅ Theorem 6.18: The followings are all equivalent.
1. T T⇤ = T ⇤T = I
2. 8x, y 2 V, hT (x), T (y)i = hx, yi
3. 9 an orthonormal basis s. t. T ( ) is an orthonormal basis.
4. 8x 2 V, ||T (x)|| = ||x||
proof: ”1”: T T ⇤ = T ⇤T = I
) ”2”: hT (x), T (y)i = hx, T⇤T (y)i = hx, yi
)”3” for = {v1, · · · , vn}, hT (vi), T (vj)i = hvi, vji = ij
) {T (vi), · · · , T (vn)} is an orthonormal basis.
)”4” : ||T (x)||2 = ||T (Pn
i=1 aivi)||2 = hPn
i=1 aiT (vi), Pn
j=1 ajT (vj)i
= Pn
i=1 Pn
j=1 aiajhT (vi), T (vj)i = Pn
i=1 |ai|2 = ||x||2 )”1”: Assume 8x 2 V, ||T (x)|| = ||x||.
) hx, xi = hT (x), T (x)i = hx, T⇤T (x)i ) T⇤T = I ) T T⇤ = I [Thm 2.17c]
Page 4
⌅⌅ unitary matrix: AA⇤ = A⇤A = I
⌅ orthogonal matrix over the real field : AAt = AtA = I
⌅ T is unitary , [T ] is unitary for an orthonormal .
⌅ T is orthogonal , [T ] is orthogonal for an orthonormal .
⌅⌅ A matrix A is unitarily (or orthogonally) equivalent to B : 9 a unitary matrix Q such that A = Q⇤BQ(or QtBQ).
⌅⌅ Theorem 6.19: A is a complex and normal matrix.
, A is unitarily equivalent to a diagonal matrix.
proof: ”)”: LA is normal, where [LA] = A.
) 9 an orthonormal basis of eigenvectors of LA. [Thm 6.16]
) [LA] = D ) A = [LA] = [I] [LA] [I] = Q 1DQ
) A = Q⇤DQ since Q = [I] is unitary for orthonormal and . (* Qij = hvj, uii, Q⇤ij = Qji = hvi, uji = huj, vii = ([I] )ij)
Page 5
⌅⌅ Theorem 6.20: A real n ⇥ n matrix A is symmetric(self-adjoint).
, A = QtDQ, where D is a real diagonal matrix.
⌅⌅ Theorem 6.21 (Schur) : A 2 Mn⇥n(F ); fA(t) splits over F . Then 1. If F = C, then A = Q⇤U Q, where U is a complex upper
triangular matrix.
2. If F = R, then A = QtU Q, where U is a real upper triangular matrix.
Orthogonal projection and spectral theorem
⌅ projection T on W1 along W2 : T (x1 + x2) = x1
⌅ R(T ) = W1 = {x 2 V : T (x) = x}
⌅ N (T ) = W2 = {x 2 V : T (x) = 0}
) V = R(T ) L
N (T ).
Page 6
⌅ For a projection T on W1,we can choose various W2.
⌅ If T is an ”orthogonal” projection on W1, then W2 is unique.
⌅⌅ T is a projection , T = T2 [alt def]
⌅⌅ orthogonal projection T :
R(T )? = N (T ) and N(T )? = R(T )
⌅ If dim(V ) < 1, (R(T )? = N (T ) , N(T )? = R(T )).
⌅ Given a subspace W, T (y) = u, where y = u + z, u 2 W, z 2 W?, is an orthogonal projection on W .
⌅ A truncated Fourier series, for k < n, u = Pk
i=1hy, vii is an orthogonal projection on span({v1, · · · , vk}).
⌅ The orthogonal projection on W provides the best approximation.
⌅ [End of Review]
Page 7
⌅⌅ Theorem 6.24: V is an inner product space:T : V ! V is linear.
Then T is an orthogonal projection , T2 = T = T⇤. Proof:
” ) ”: Assume T is an orthogonal projection.
) T2 = T [projection]
) V = R(T ) L
N (T ); R(T )? = N (T )
) 8x, y 2 V, x = x1+ x2 and y = y1+ y2, for some x1, y1 2 R(T ) and x2, y2 2 N(T ).
) hx, T (y)i = hx1 + x2, y1i = hx1, y1i + hx2, y1i = hx1, y1i = hx1, y1i + hx1, y2i = hx1, y1 + y2i = hT (x), yi = hx, T⇤(y)i
” ( ”: Assume T2 = T = T ⇤ ) T is a projection.
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Page 8
Let x 2 R(T ) and y 2 N(T ). ) T (x) = x, T (y) = 0.
) hx, yi = hT (x), yi = hx, T⇤(y)i = hx, T (y)i = hx, 0i = 0 ) x 2 N(T )? and y 2 R(T )?
) R(T ) ✓ N(T )? and N(T ) ✓ R(T )? (1) Let x 2 N(T )?
) x = x1 + x2, x1 2 R(T ), x2 2 N(T ) [projection]
) 0 = hx, x2i = hx1, x2i + hx2, x2i = ||x2||2, [*x1 2 N(T )? (1)]
) x2 = 0 ) x = x1 2 R(T ) ) N(T )? ✓ R(T ) ) N(T )? = R(T ) [(1)]
Let y 2 R(T )?.
) y = y1 + y2, y1 2 R(T ), y2 2 N(T ) [projection]
) 0 = hy, y1i = hy1, y1i + hy2, y1i = ||y1||2, [* y2 2 R(T )? (1)]
) y1 = 0 ) y = y2 2 N(T ) ) R(T )? ✓ N(T ) ) R(T )? = N (T ) [(1)]
方器
Page 9
⌅⌅ Theorem 6.25 (The spectral theorem): V is an inner product space over F ; dim(V ) < 1; T : V ! V is a linear operator with
distinct eigenvalues: spectrum 1 · · · k
corresponding eigenspaces W1 · · · Wk orthogonal projection on Wi T1 · · · Tk
and T is normal if F = C and self-adjoint if F = R. Then the following statements are true.
1. V = W1 · · · Wk. 2. Wi? = kj=1,j6=iWj. 3. TiTj = T0, i 6= j.
4. T1 + · · · + Tk = I.
5. T = 1T1 + · · · + kTk: spectral decomposition a
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Page 10
proof of 5: x 2 V
) x = x1 + · · · + xk, xi 2 Wi [1]
T (x) = T (x1) + · + T (xk)
= 1x1 + · · · + kxk
= 1T1(x) + · · · + kTk(x)
= ( 1T1 + · · · + kTk)(x)
Page 11
⌅⌅ example: consider T = LA, where A =
0 BB
@
2 0 0 0 0 3 0 0 0 0 3 0 0 0 0 5
1 CC A.
1 = 2, W1 = {(a1, 0, 0, 0)t : a1 2 R}, T1 = LA1,
2 = 3, W2 = {(0, a2, a3, 0)t : a2, a3 2 R}, T2 = LA2,
3 = 5, W3 = {(0, 0, 0, a4)t : a4 2 R}, T3 = LA3, where A1 =
0 BB
@
1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
1 CC
A , A2 = 0 BB
@
0 0 0 0 0 1 0 0 0 0 1 0 0 0 0 0
1 CC
A, and A3 = 0 BB
@
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1
1 CC A.
T = 1T1 + 2T2 + 3T3 : LA = 2LA1 + 3LA2 + 5LA3
Page 12
⌅⌅ example: consider T = LA, where A =
✓ 1 2 2 1
◆ .
1 = 3, W1 = {(a1, a2)t 2 R2 : a1 = a2}, T1 = LA1,
2 = 1, W2 = {(a1, a2)t 2 R2 : a1 + a2 = 0}, T2 = LA2, where A1 = 12
✓ 1 1 1 1
◆
and A2 = 12
✓ 1 1
1 1
◆ . T = 1T1 + 2T2 : LA = 3LA1 LA2
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Page 13
⌅⌅ Corollary 6.25.2: V is an inner product space over C; dim(V ) <
1; T : V ! V is unitary , T is normal and | | = 1 for every eigenvalue of T .
Proof.
”)” If T is unitary, then T is normal and every eigenvalue of T has absolute value 1 (* ||T(x)|| = ||x||).
”(” Let T = 1T1 + 2T2 + · · · + kTk be the spectral decompo- sition of T . If | | = 1 for every eigenvalue of T , then by 3. of the spectral theorem,
T T⇤ = ( 1T1 + 2T2 + · · · + kTk)( 1T1⇤ + 2T2⇤ + · · · + kTk⇤)
= | 1|2T1T1⇤ + | 2|2T2T2⇤ + · · · + | k|2TkTk⇤
= (T1 + T2 + · · · + Tk)(T1 + T2 + · · · + Tk)⇤
= I
Hence T is unitary.
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⌅⌅ Corollary 6.25.3: V is an inner product space over C; dim(V ) <
1; T : V ! V is normal. Then T is self-adjoint , every eigen- value of T is real.
Proof.
”)” T ⇤ = T ) 1T1 + 2T2 + · · · + kTk = 1T1 + 2T2 + · · · +
kTk ) i is real.
”(” Let T = 1T1 + 2T2 + · · · + kTk be the spectral decom- position of T . Suppose that every eigenvalue of T is real. Then Ti⇤(vi) = ivi = Ti(vi), so T⇤ = 1T1 + 2T2 + · · · + kTk =
1T1 + 2T2 + · · · + kTk) = T.
e . 一一
t t *
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⌅⌅ Reflection is an example that is both self adjoint and unitary.
T =
cos2✓ sin2✓
sin2✓ cos2✓
T = T
( f
#T = I = ㅜㅜ丁杆