Quantum Mechanics for Engineers 

© Leon van Dommelen 

Subsections
2.7 Additional Points
This subsection describes a few further issues of importance for this
book.
2.7.1 Dirac notation
Physicists like to write inner products such as
in Dirac notation
:
since this conforms more closely to how you would think of it
in linear algebra:
The various advanced ideas of linear algebra can be extended to
operators in this way, but they will not be needed in this book.
One thing will be needed in some more advanced addenda, however. That
is the case that operator is not Hermitian. In that case,
if you want to take to the other side of the inner product, you
need to change it into a different operator. That operator is called
the “Hermitian conjugate” of . In physics, it is almost
always indicated as . So, simply by definition,
Then there are some more things that this book will not use. However,
you will almost surely encounter these when you read other books on
quantum mechanics.
First, the dagger is used much like a generalization of
complex conjugate,
etcetera. Applying a dagger a second time gives the original back.
Also, if you work out the dagger on a product, you need to reverse the
order of the factors. For example
In words, putting into the left side of an inner
product gives .
The second point will be illustrated for the case of vectors in
three dimensions. Such a vector can be written as
Here , , and are the three unit
vectors in the axial directions. The components ,
and can be found using dot products:
Symbolically, you can write this as
In fact, the operator in parentheses can be defined by saying
that for any vector , it gives the exact same vector
back. Such an operator is called an “identity operator.”
The relation
is called the “completeness relation.” To see why, suppose you leave off the
third part of the operator. Then
The component is gone! Now the vector gets
projected onto the plane. The operator has become a
“projection operator” instead of an identity operator by not
suming over the complete set of unit vectors.
You will almost always find these things in terms of bras and kets.
To see how that looks, define
Then
so the completeness relation looks like
If you do not sum over the complete set of kets, you get a projection
operator instead of an identity one.
2.7.2 Additional independent variables
In many cases, the functions involved in an inner product may depend
on more than a single variable . For example, they might
depend on the position in threedimensional space.
The rule to deal with that is to ensure that the inner product
integrations are over all independent variables. For example,
in three spatial dimensions:
Note that the time is a somewhat different variable from the rest,
and time is not included in the inner product integrations.