9.4.
Eigenvalues and eigenvectors |
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We saw in the previous section that the analysis
of isometrics of
became possible under a special assumption. That assumption
motivates our next definition. |
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Let V be a vector space and T: V→V
be a linear transformation. A scalar
is
called an eigen-value for T if there exists a
non-zero vector v V
such that Tv = λv.
The non-zero vector v is called an
eigenvector for the eigenvalue
λ . |
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(i) Suppose V is one-dimensional vector space.
Then, the only possible linear transformations
T: V→V
are the following : for
fixed, T(v) = αv
for every v V
. Thus, α is an eigenvalue
of T and every v
≠
0
is an eigenvector for this eigenvalue.
(ii) Let T: →
be defined by T( x, y ) = ( 5x, 2y
) , "
( x, y)
∈ .
Then α = 5 and
α = 2 are eigenvalues of T, since T(1,0)
= 5(1,0) and T(0,1) = 2(0,1).
(iii) Let V be a finite dimensional inner-product
space over F
and S a non trivial proper
subspace of V.
Let
be the orthogonal complement of S. Let T: V→V
be the orthogonal projection of T onto S.
Since, both S and
are nontrivial subspace of V and
T(v) = v for every v∈S
and
T(v) = 0 for every v∈ ,
it follows that 0 and 1 are both
eigenvalues of T. We show that these are the only eigenvalues of
T.
Let 0 ≠
λ∈F
and v∈V
be such that v≠
0 and P(v) =λ(v).
Then P(P(v)) =
P(λv) = λ(P(v)).
--------- (*)
Since P is orthogonal projection ,

Thus, (*) gives
λP(v)
= P(v),
i.e. (1-λ)P(v)
= 0.
Since P(v) = λv
≠ 0, we get λ=1.
Thus, if λ
≠ 0 is an eigenvector, then λ
= 1.
(iv) Consider T : →
given by
T(x, y) = ( y, -x )∈ .
Then, for any
λ∈ℝ
and ( x, y )∈ ,
T( x, y ) =
λ( x, y
) iff -x =
x
,which is never possible.
Hence, T has no
eigenvalues.
(v) Let T :V→V
be invertible .Then
λ =0 is not an an
eigenvalue of T. for otherwise T(v) = 0 for some
v
≠ 0.
In general, given a linear transformation
T :V→V , it
is not obvious how to analyze: Whether
T has eigenvalues
or not ? And if it has, how to find them. The following theorem is
useful in this
regards. |
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| Above theorem motivates the following: |
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Let A be a nŚn matrix
over
F . A scalar
λ∈F
is called an eigenvalue for A if there exists a
nonzero
such
that Av =
λv .
And, any such nonzero vector is called as eigenvector for the
eigenvalue
λ.
Theorem 9.4.3 tells us that a scalar
λ∈F
is an eigenvalue for T iff it is an eigenvalue for the matrix
representation
of T with respect to every ordered basis of T. Further, eigenvalues
of a matrix A are
the solution of the equation det(A-λI).
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(i) Let T : →
be given by T( x, y ) = ( x + 3y, 4x
+ 2y ) ,
( x, y )∈
.
With respect to basis
B = { ( 1, 0 ), ( 0,
1 ) } of ,
 Thus,
λ∈ℝ
is an eigenvalue of T if and only if
det(
) = 0. since
0 =
det(
) =

= ( 1-λ
)( 2-λ
)-12

= (
λ + 2 (
λ - 5 ),
T has eigenvalues
λ = -2 and | |