The main idea of series expansion method is at: http://en.wikipedia.org/wiki/User:Peter483
The QED equation is:
are Dirac matrices;
a bispinor field of spin-1/2 particles (e.g. electron-positron field);
, called "psi-bar", is sometimes referred to as Dirac adjoint;
is the coupling constant, equal to the electric charge of the bispinor field;
is the covariant four-potential of the electromagnetic field generated by electron itself;
is the external field imposed by external source;
Using Lorentz gauge
, equation for
can be expressed as:
Then we seperate time partial derivative from other parts, we get:
For simplicity, we use
to replace operators in these two equations. And add
to the
equation:
......(1)
......(2)
here we have used
and
Add operator
to equation (1) and (2) and use (1)&(2) repeatedly, we will get the expression of higher order time partial derivative of
and
Next we will use an abbreviation for the expression of
and
according to the order of electric charge
:
Then it is our job to calculate
and
.
The expression of
and
is quite simple:
is a little complicated:
When
is even:
When
is odd:
Using
, we can get:
When
is even:
When
is odd:
Now we can see we must divide the situation into
is even and
is odd. For simplicity, we want to combine the two expressions into one equation.
We notice the function
and
.
When
is even:
and
When
is odd:
and
here
.
We should keep in mind that
.
has no meaning in the coordinates space. But since in the end we will transform the result into 3-dimension momentum space, we allow the use of
temporarily. It's the same situation with operator
and
.
Using the same method:
here
Then we will transform the result into 3-dimension momentum space:
Here we have used:
And we must keep in mind:
It means
is the 3-momentum representation of
instead of the conjugate of
In 3-dimension momentum space, operators in coordinate space become numbers we can easily move:
Using summation formula of geometric progression and binomial expansion, we get the expression:
in which:
Here we can
"the j-order total energy".
Then we use the Tylor series expansion:
Using
, we get:
For simplicity, we use an abbreviation:
The solution of
in 3-momentum space can be expressed as:
in which:
in which:
And for simplicity, we leave out the summation sign
We can get the solution of
in the same way:
Then we use an abbreviation:
The expression of
is quite simple:
consists two parts:
in which:
in which:
Here we have used:
is the 4-momentum representation of external field
And we also have used:
Higher order results can be achieved in the same way.
Now we analyse the term
, it comes from
. We can call this term "time-scalar sum up", because it contains scalars related to time.
When
,
. Obviously it becomes infinite when
.
Actually:
We can see when
,
.
It menas the possibility in 3-momentum space will gather at the point
.
Then we can use the relation
Now we can see that when
, the 1st order time-scalar sum up can be expressed as:
A more generalized expression is
The term
appears because of
for
, but usually they cancel each other, so we have:
.
In the same way as the
, we can derive a equation:
To achieve this, we make
all have an infinitesimal imaginary part and make sure
. Then we do an integral
. In every step, we integral at a line nearby real axis and a complex plane lower half circle (which forming a closed curve). Since
, the integral of complex plane lower half circle becomes zero and we can use the residue theory. Because we must finish the
steps of integral, the only way to get a non-zero integral result is:
Start from
, do integral at this order:
. After an integral
, we can see there's
residues we can use since
. And we must choose the residue at
and then do integral
.
Finally we can get the result:
Sometimes we can get
. For example:
The 2-order time-scalar sum up is
If
, we simply ignore the term
, so:
Another thing to say is that when we can't get
, make sure
with
becasue
is the only one which doesn't contain integration variables.
Calculation of QED in 3-dimension space:
http://blog.sina.com.cn/u/1070440741
peter483@sina.com
peter483@sina.com.cn