The product of two one- forms, written as
defines a linear map which
takes two vectors into the reals:
It is therefore a 0/2 tensor. denotes the
outer product. It is
the formal notation to show how the 0/2 tensor is formed from two
one- forms.
Note that this product is non- commutitative since gives a different result [ Assignment 3 ] i.e.
The most general 0/2 tensor is a linear sum of such outer products. So
where are the components of the map f and we have
used linearity.
If we take a basis for f
as [ 16 components ], then
But
so we have
Under a Lorentz transformation , the components of f become:
It follows that any 0/2 tensor can be uniquely decomposed into a symmetric and anti- symmetric part .
with the symmetric and anti- symmetric parts given by
and