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We have seen that eigenvalues are the roots of the characteristic polynomial, and therefore may be complex numbers,
even when a matrix has entries that are real. This section is devoted to a remarkable theorem proved by S.A.
Gershgorin in 1931. Gershgorin’s theorem says that the \(n\) eigenvalues of an \(n \times n\) matrix can be found in a region in
the complex plane consisting of \(n\) disks. We explore the theorem for the case \(n=3\) before proving the result. If you
have never plotted complex numbers before, you may wish to try Exploration exp:geometry_complex_numbers in Complex Numbers before
proceeding.
In the GeoGebra exploration below, you can adjust any of the entries of the \(3 \times 3\) matrix \(A\). The three eigenvalues are plotted as
dots in the complex plane. The Gershgorin region is the union of three closed disks whose boundaries are plotted in red.
Notice that the eigenvalues are always in the Gershgorin region.
As you experiment with the interactive, see if you can answer the following questions.
1.
Is it always true that each disk contains an eigenvalue? YesNo
2.
What is the center of each disk?
3.
What is the radius of each disk?
4.
Are there some matrices for which one of the disks does not intersect the others? Where none of the disks
intersect?
5.
Try using a matrix with complex number entries. How is the visual pattern of eigenvalues for such a matrix different from
a matrix whose entries are real numbers?
In the exploration above you were able to see the eigenvalues of a \(3 \times 3\) matrix. The eigenvalues are contained in the Gershgorin
region, which consists of three disks.
In general, for an \(n \times n\) matrix \(A=[a_{ij}]\), the Gershgorin region consists of \(n\) disks in the complex plane:
The centers of the disks are given by the \(n\) diagonal entries of \(A\).
We get the radius of the disk with center \(a_{ii}\) by adding the absolute values of each of the other elements in row \(i\).
We state this all formally in the following theorem.
Gershgorin Let \(A=[a_{ij}]\) be an \(n\times n\) complex matrix. Then for \(1<i<n\), we define the absolute deleted row sum to be
\[ r_i(A):= \sum _{i \ne j} |a_{ij}|. \]
Now we can define the \(i\)th Gershgorin disk of \(A\) to be
Then the eigenvalues of \(A\) are contained in the Gershgorin region \(\Gamma (A)\).
The fact that (eqn:Gersh_disk) represents a disk in the complex plane is a direct result of the complex distance formula (see Complex
Numbers for more information). Before proving Gershgorin’s theorem, we provide an example and a video to aid in
understanding exactly what the theorem says.
Plot the eigenvalues and the Gershgorin region of each of the following matrices.
\(\Gamma (A)\) consists of two disks. The first is centered at 1 with a radius of 1. The second is centered at 0 with a radius of
2, so we see that the first disk is contained in the second. The eigenvalues, 2 and \(-1\), are both contained in \(\Gamma (A)\) (with
2 being on the boundary).
2.
\(B\) is a matrix with complex entries, which makes for a more interesting Gershgorin region. See Complex Matrices
for more on matrices like this one.
Since \(B\) is upper triangular, its eigenvalues are its diagonal entries. These are the centers of the Gershgorin
disks, which proves that the eigenvalues of \(B\) are contained in \(\Gamma (B)\). \(\Gamma (B)\) consists of four disks. The first is centered at \(1+i\)
with a radius of \(2\), since the absolute value of \(i\) is 1. The second is centered at 4 with a radius of \(\sqrt {2}\). The third disk
is centered at 2 with a radius of 1. The fourth disk is centered at \(-1\) with a radius of zero, so in fact, consists only
of the eigenvalue \(-1\).
Proof of Gershgorin’s Theorem Let \(\lambda \) be an eigenvalue of \(A\) with corresponding eigenvector \(\vec {x}=\begin{bmatrix} x_1 \\ x_2 \\ \vdots \\ x_n \end{bmatrix}\) so that \(A\vec {x}=\lambda \vec {x}\). Let \(x_k\) be an entry of \(\vec {x}\)
such that \(|x_k|\) is greater than or equal to the absolute value of every other entry in \(\vec {x}\). Then considering row \(k\) of the
equation
Here equations eqn:pr1 and eqn:pr4 follow from property C2 of Complex Numbers, inequality eqn:pr3 follows from the Triangle Inequality (C12 of
Complex Numbers), and we arrive at inequality eqn:pr5 by replacing each \(\vec {x}_j\) in inequality eqn:pr4 by \(\vec {x}_k\).
These inequalties show that \(|\lambda - a_{kk}| \le \sum _{j\ne k} |a_{kj}|\), so \(\lambda \in \Gamma _k(A)\), and hence \(\lambda \in \Gamma (A)\), as desired.
Sketch the Gershgorin region for each matrix and, if possible, use it as an aid for determining whether or not the matrix is
singular.
We can check our sketches of the Gershgorin regions using the GeoGebra interactive in Exploration init:GershDisks3x3.
1.
If we sketch the Gershgorin region of matrix \(A\), we see that the zero vector is not contained in it. It follows that
zero cannot be an eigenvalue of matrix \(A\), and we conclude that \(A\) is nonsingular.
2.
The Gershgorin region of matrix \(B\) contains the zero vector, so there we cannot determine from the Gershgorin
region whether or not \(B\) is singular. Instead, if we perform Gaussian elimination on matrix \(B\), we will see it is not
of full rank, and so \(B\) is singular.
3.
The Gershgorin region of matrix \(C\) contains the zero vector, so again we cannot determine from the Gershgorin
region whether or not \(C\) is singular. Observe that \(C\) is an upper triangular matrix with non-zero entries along the
diagonal. Therefore \(\det {C}\neq 0\). We conclude that \(C\) is non-singular.
Practice Problems
Problems -
Sketch the Gerhgorin region for each matrix. What, if anything, does the region tell us about the matrix being singular or
nonsingular? If the test is inconclusive, test for singularity in some other way.