Proofs
Here we provide two proofs. The first[2] operates in the general case, using linear maps. The second proof[6] looks at the homogeneous system
where
is a
with rank
and shows explicitly that there exists a set of
linearly independent solutions that span the null space of
.
While the theorem requires that the domain of the linear map be finite-dimensional, there is no such assumption on the codomain. This means that there are linear maps not given by matrices for which the theorem applies. Despite this, the first proof is not actually more general than the second: since the image of the linear map is finite-dimensional, we can represent the map from its domain to its image by a matrix, prove the theorem for that matrix, then compose with the inclusion of the image into the full codomain.
First proof
Let
be vector spaces over some field
and
defined as in the statement of the theorem with
.
As
is a subspace, there exists a basis for it. Suppose
and let
be such a basis.
We may now, by the Steinitz exchange lemma, extend
with
linearly independent vectors
to form a full basis of
.
Let
such that
is a basis for
.
From this, we know that


We now claim that
is a basis for
.
The above equality already states that
is a generating set for
; it remains to be shown that it is also linearly independent to conclude that it is a basis.
Suppose
is not linearly independent, and let
for some
.
Thus, owing to the linearity of
, it follows that
This is a contradiction to
being a basis, unless all
are equal to zero. This shows that
is linearly independent, and more specifically that it is a basis for
.
To summarize, we have
, a basis for
, and
, a basis for
.
Finally we may state that


This concludes our proof.
Second proof
Let
be an
matrix with
linearly independent columns (i.e.
). We will show that:
- There exists a set of
linearly independent solutions to the homogeneous system
. - That every other solution is a linear combination of these
solutions.
To do this, we will produce an
matrix
whose columns form a basis of the null space of
.
Without loss of generality, assume that the first
columns of
are linearly independent. So, we can write
where
is an
matrix with
linearly independent column vectors, and
is an
matrix such that each of its
columns is linear combinations of the columns of
.
This means that
for some
matrix
(see rank factorization) and, hence,

Let
where
is the
identity matrix. So,
is an
matrix such that

Therefore, each of the
columns of
are particular solutions of
.
Furthermore, the
columns of
are linearly independent because
will imply
for
:
Therefore, the column vectors of
constitute a set of
linearly independent solutions for
.
We next prove that any solution of
must be a linear combination of the columns of
.
For this, let

be any vector such that
. Since the columns of
are linearly independent,
implies
.
Therefore,

This proves that any vector
that is a solution of
must be a linear combination of the
special solutions given by the columns of
. And we have already seen that the columns of
are linearly independent. Hence, the columns of
constitute a basis for the null space of
. Therefore, the nullity of
is
. Since
equals rank of
, it follows that
. This concludes our proof.
This theorem is a statement of the first isomorphism theorem of algebra for the case of vector spaces; it generalizes to the splitting lemma.
In more modern language, the theorem can also be phrased as saying that each short exact sequence of vector spaces splits. Explicitly, given that
is a short exact sequence of vector spaces, then
, hence
Here
plays the role of
and
is
, i.e.

In the finite-dimensional case, this formulation is susceptible to a generalization: if
is an exact sequence of finite-dimensional vector spaces, then[9]
The rank–nullity theorem for finite-dimensional vector spaces may also be formulated in terms of the index of a linear map. The index of a linear map
, where
and
are finite-dimensional, is defined by

Intuitively,
is the number of independent solutions
of the equation
, and
is the number of independent restrictions that have to be put on
to make
solvable. The rank–nullity theorem for finite-dimensional vector spaces is equivalent to the statement

We see that we can easily read off the index of the linear map
from the involved spaces, without any need to analyze
in detail. This effect also occurs in a much deeper result: the Atiyah–Singer index theorem states that the index of certain differential operators can be read off the geometry of the involved spaces.