Recall that
given a 
-dimensional vector subspace of a vector space 
 of dimension
 one can always find an 
-dimensional vector subspace 
 of 
(see Exercise 3.3.20.9) satisfying
The subspace 
 is called the complementary subspace of 
 in 
We now define an important class of linear transformations
on an inner product space, called orthogonal projections.
Remark  5.3.2   
The map 
 is well defined due to the following reasons:
- 
 implies that for every 
 we can find
 and 
 such that 
 
- 
 implies that the expression
            
 is unique for every 
 
 
The next proposition states that the map defined above is a linear
transformation from 
 to 
 We omit the proof, as it follows directly
from the above remarks.
Remark  5.3.5   
- The projection map 
 depends on the complementary subspace 
 
- Observe that for a fixed subspace 
 there are infinitely many choices
for the complementary subspace 
 
- It will be shown later that if
 is an inner product space with inner product, 
then the subspace 
 is unique if we put an additional condition that
 
 
We now prove some basic properties about projection maps.
THEOREM  5.3.6   
Let 
 and 
 be complementary subspaces of a vector space 
 Let
 be a projection operator of 
 onto 
along 
 Then
- the null space of 
 
 
- the range space of 
 
 
- 
 The condition 
 is equivalent to
 
 
The next result uses the Gram-Schmidt orthogonalisation process to get
the complementary subspace in  such a way that the vectors in different subspaces
are orthogonal.
DEFINITION  5.3.8 (Orthogonal Subspace of  a Set)    
Let 
 be an inner product space. Let 
 be a non-empty subset of 
.
We define 
 
EXAMPLE  5.3.9   
Let 
. 
. Then 
.
 
- 
, Then 
.
 
- Let 
 be any subset of 
 containing a non-zero real number.  Then 
.
 
 
THEOREM  5.3.10   
Let 
 be a subset of a finite dimensional inner product space 
with inner product 
 Then
 is a subspace of 
 
- Let 
 be equal to a subspace 
. Then the subspaces 
 and 
 are complementary. Moreover, if
 and 
 then 
 and
 
 
Proof.
We leave the prove of the first part for the reader. The prove of the
second part is as follows: 
Let 

 and 

 Let 

be a basis of 

 By Gram-Schmidt orthogonalisation process, we get an
orthonormal basis, say, 

 of 

 Then,
for any 
So, 

 Also, for any 

by definition of 

So, 

 That is,

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DEFINITION  5.3.12 (Self-Adjoint Transformation/Operator)    
Let 
 be an inner product space with inner product 
A linear transformation 
 is called
a self-adjoint operator if 
 for every 
 
Remark  5.3.14   
- By Proposition 5.3.3, the map 
 defined above
is a linear transformation.
 
- 
 
-  Let 
 with 
 and 
for some 
 and 
 Then we know that
 whenever 
 Therefore,
for every 
Thus, the orthogonal projection operator is a self-adjoint operator.
 
- Let 
 and 
 Then 
 for all 
Therefore, using Remarks 5.3.14.2
and 5.3.14.3, we get
 for every 
 
- In particular,
 as 
. Thus,
, for every 
.
Hence, for any 
 and 
 we have
Therefore,  
and the equality holds
if and only if 
 Since 
 we see that
That is, 
 is the vector nearest to 
 This can also be stated
as:    the vector 
 solves the following minimisation problem:
 
 
Subsections
A K Lal
2007-09-12