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Matrix Similarity

Matrix similarity relates square matrices that represent the same linear operator in different bases, preserving its algebraic structure and spectral properties.

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Matrix similarity is a relation in linear algebra between two square matrices that represent the same linear operator in possibly different coordinate systems. Matrices A,B∈Fn×nA,B\in F^{n\times n}, over a field FF, are similar if an invertible matrix P∈Fn×nP\in F^{n\times n} exists such that

B=P−1AP.B=P^{-1}AP.

The operation is called a similarity transformation. It changes the matrix representation, rather than the underlying operator. (pressbooks.cuny.edu)

Definition and change of basis

Let T:V→VT:V\to V act on a finite-dimensional vector space, and let E\mathcal E and F\mathcal F be ordered bases. Suppose AA represents TT in E\mathcal E, and the columns of PP are the coordinates of the F\mathcal F-basis vectors in E\mathcal E. Then

[v]E=P[v]F.[v]_{\mathcal E}=P[v]_{\mathcal F}.

Applying TT and converting its output back gives

[T(v)]F=P−1AP[v]F.[T(v)]_{\mathcal F}=P^{-1}AP[v]_{\mathcal F}.

Thus B=P−1APB=P^{-1}AP represents TT in F\mathcal F. Conversely, any invertible PP defines such a basis change. (pressbooks.cuny.edu)

Similarity is an equivalence relation: it is reflexive, symmetric, and transitive. Reflexivity uses the identity matrix; symmetry uses the inverse of the transforming matrix. If B=P−1APB=P^{-1}AP and C=Q−1BQC=Q^{-1}BQ, then

C=(PQ)−1A(PQ).C=(PQ)^{-1}A(PQ).

Consequently, square matrices of a fixed size over a fixed field divide into similarity classes. (pressbooks.cuny.edu)

Preserved properties

Similar matrices have the same characteristic polynomial, because

tI−B=P−1(tI−A)PtI-B=P^{-1}(tI-A)P

and therefore

det⁡(tI−B)=det⁡(tI−A).\det(tI-B)=\det(tI-A).

They consequently have the same eigenvalues, including algebraic multiplicities, as well as the same determinant and trace. Their rank is also identical, since multiplication by invertible matrices preserves rank. (ocw.mit.edu)

More generally, for every polynomial pp,

p(B)=P−1p(A)P.p(B)=P^{-1}p(A)P.

It follows that p(A)=0p(A)=0 exactly when p(B)=0p(B)=0, so similar matrices have the same minimal polynomial: the monic polynomial of least degree annihilating the matrix. (math.uci.edu)

Eigenvectors themselves need not have identical coordinates. From Av=λvAv=\lambda v, one obtains

B(P−1v)=λ(P−1v).B(P^{-1}v)=\lambda(P^{-1}v).

The corresponding eigenspaces therefore have equal dimensions. The same calculation applies to (A−λI)k(A-\lambda I)^k, preserving the dimensions of its null spaces and hence the generalized-eigenvector structure associated with each eigenvalue. (ocw.mit.edu)

Examples and limits of spectral tests

For a simple example, take

A=(1002),P=(1101).A=\begin{pmatrix}1&0\\0&2\end{pmatrix}, \qquad P=\begin{pmatrix}1&1\\0&1\end{pmatrix}.

Direct multiplication gives

P−1AP=(1−102).P^{-1}AP=\begin{pmatrix}1&-1\\0&2\end{pmatrix}.

The matrices look different, but the calculation exhibits their similarity explicitly. This illustrates why off-diagonal entries are not similarity invariants. (sites.wcsu.edu)

Conversely, identical eigenvalues do not establish similarity. Consider

I2=(1001),J=(1101).I_2=\begin{pmatrix}1&0\\0&1\end{pmatrix}, \qquad J=\begin{pmatrix}1&1\\0&1\end{pmatrix}.

Both have characteristic polynomial (t−1)2(t-1)^2, determinant 11, trace 22, and rank 22. Nevertheless, they are not similar: P−1I2P=I2P^{-1}I_2P=I_2 for every invertible PP. Their minimal polynomials also differ, being t−1t-1 and (t−1)2(t-1)^2, respectively. Thus these commonly used invariants are necessary tests, not a complete classification. (ocw.mit.edu)

Diagonalization and canonical forms

Diagonalization is a special case of similarity. A matrix is diagonalizable over FF precisely when it has a basis of eigenvectors with coordinates in FF. If those vectors form the columns of PP, then P−1APP^{-1}AP is diagonal. Two diagonalizable matrices over the same field are similar exactly when their eigenvalues agree with multiplicities. (ocw.mit.edu)

When the characteristic polynomial splits into linear factors—for example, over the complex numbers—every square matrix is similar to a Jordan normal form. Its blocks record eigenvalues and generalized-eigenvector chains. Two such matrices are similar exactly when their Jordan blocks agree, apart from block order. Diagonalizability corresponds to all blocks having size one. (pmelvin.blogs.brynmawr.edu)

Over an arbitrary field, rational canonical form provides a complete classification without requiring the eigenvalues to belong to that field. Its invariant-factor polynomials determine a unique canonical representative, and two matrices are similar exactly when these representatives coincide. (pmelvin.blogs.brynmawr.edu)

Testing similarity and numerical computation

The defining equation can be rewritten as

AP=PB.AP=PB.

For fixed AA and BB, this is a homogeneous system of linear equations in the entries of PP. Similarity holds precisely when its solution space contains an invertible matrix. A nonzero solution alone is insufficient, since it may be singular. Canonical forms offer an alternative exact test. (sites.wcsu.edu)

In numerical linear algebra, Schur decomposition uses restricted similarity transformations. A complex matrix has a representation A=QTQ∗A=QTQ^*, with QQ a unitary matrix and TT upper triangular; Q∗Q^* denotes the conjugate transpose. For real matrices, QQ can be an orthogonal matrix, while TT is block upper triangular with diagonal blocks of size one or two. These forms support practical eigenvalue computation while retaining the original eigenvalues. (netlib.org)