In mathematics, the polar decomposition of a square real or complex matrix is a factorization of the form , where is a unitary matrix and is a positive semi-definite Hermitian matrix ( is an orthogonal matrix and is a positive semi-definite symmetric matrix in the real case), both square and of the same size.[1]

Intuitively, if a real matrix is interpreted as a linear transformation of -dimensional space , the polar decomposition separates it into a rotation or reflection of , and a scaling of the space along a set of orthogonal axes.

The polar decomposition of a square matrix always exists. If is invertible, the decomposition is unique, and the factor will be positive-definite. In that case, can be written uniquely in the form , where is unitary and is the unique self-adjoint logarithm of the matrix .[2] This decomposition is useful in computing the fundamental group of (matrix) Lie groups.[3]

The polar decomposition can also be defined as where is a symmetric positive-definite matrix with the same eigenvalues as but different eigenvectors.

The polar decomposition of a matrix can be seen as the matrix analog of the polar form of a complex number as , where is its absolute value (a non-negative real number), and is a complex number with unit norm (an element of the circle group).

The definition may be extended to rectangular matrices by requiring to be a semi-unitary matrix and to be a positive-semidefinite Hermitian matrix. The decomposition always exists and is always unique. The matrix is unique if and only if has full rank. [4]

Intuitive interpretation

A real square matrix can be interpreted as the linear transformation of that takes a column vector to . Then, in the polar decomposition , the factor is an real orthonormal matrix. The polar decomposition then can be seen as expressing the linear transformation defined by into a scaling of the space along each eigenvector of by a scale factor (the action of ), followed by a rotation of (the action of ).

Alternatively, the decomposition expresses the transformation defined by as a rotation () followed by a scaling () along certain orthogonal directions. The scale factors are the same, but the directions are different.


The polar decomposition of the complex conjugate of is given by Note that

gives the corresponding polar decomposition of the determinant of A, since and . In particular, if has determinant 1 then both and have determinant 1.

The positive-semidefinite matrix P is always unique, even if A is singular, and is denoted as

where denotes the conjugate transpose of . The uniqueness of P ensures that this expression is well-defined. The uniqueness is guaranteed by the fact that is a positive-semidefinite Hermitian matrix and, therefore, has a unique positive-semidefinite Hermitian square root.[5] If A is invertible, then P is positive-definite, thus also invertible and the matrix U is uniquely determined by

Relation to the SVD

In terms of the singular value decomposition (SVD) of , , one has

where , , and are unitary matrices (called orthogonal matrices if the field is the reals ). This confirms that is positive-definite and is unitary. Thus, the existence of the SVD is equivalent to the existence of polar decomposition.

One can also decompose in the form

Here is the same as before and is given by
This is known as the left polar decomposition, whereas the previous decomposition is known as the right polar decomposition. Left polar decomposition is also known as reverse polar decomposition.

The polar decomposition of a square invertible real matrix is of the form

where is a positive-definite matrix and is an orthogonal matrix.

Relation to Normal matrices

The matrix with polar decomposition is normal if and only and commute: , or equivalently, they are simultaneously diagonalizable.

Construction and proofs of existence

The core idea behind the construction of the polar decomposition is similar to that used to compute the singular-value decomposition.

Derivation for normal matrices

If is normal, then it is unitarily equivalent to a diagonal matrix: for some unitary matrix and some diagonal matrix . This makes the derivation of its polar decomposition particularly straightforward, as we can then write

where is a diagonal matrix containing the phases of the elements of , that is, when , and when .

The polar decomposition is thus , with and diagonal in the eigenbasis of and having eigenvalues equal to the phases and absolute values of those of , respectively.

Derivation for invertible matrices

From the singular-value decomposition, it can be shown that a matrix is invertible if and only if (equivalently, ) is. Moreover, this is true if and only if the eigenvalues of are all not zero.[6]

In this case, the polar decomposition is directly obtained by writing

and observing that is unitary. To see this, we can exploit the spectral decomposition of to write .

In this expression, is unitary because is. To show that also is unitary, we can use the SVD to write , so that

where again is unitary by construction.

Yet another way to directly show the unitarity of is to note that, writing the SVD of in terms of rank-1 matrices as , where are the singular values of , we have

which directly implies the unitarity of because a matrix is unitary if and only if its singular values have unitary absolute value.

Note how, from the above construction, it follows that the unitary matrix in the polar decomposition of an invertible matrix is uniquely defined.

General derivation

The SVD of a squared matrix reads , with unitary matrices, and a diagonal, positive semi-definite matrix. By simply inserting an additional pair of s or s, we obtain the two forms of the polar decomposition of :

More generally, if is some rectangular matrix, its SVD can be written as where now and are isometries with dimensions and , respectively, where , and is again a diagonal positive semi-definite squared matrix with dimensions . We can now apply the same reasoning used in the above equation to write , but now is not in general unitary. Nonetheless, has the same support and range as , and it satisfies and . This makes into an isometry when its action is restricted onto the support of , that is, it means that is a partial isometry.

As an explicit example of this more general case, consider the SVD of the following matrix:

We then have
which is an isometry, but not unitary. On the other hand, if we consider the decomposition of
we find
which is a partial isometry (but not an isometry).

Bounded operators on Hilbert space

The polar decomposition of any bounded linear operator A between complex Hilbert spaces is a canonical factorization as the product of a partial isometry and a non-negative operator.

The polar decomposition for matrices generalizes as follows: if A is a bounded linear operator then there is a unique factorization of A as a product A = UP where U is a partial isometry, P is a non-negative self-adjoint operator and the initial space of U is the closure of the range of P.

The operator U must be weakened to a partial isometry, rather than unitary, because of the following issues. If A is the one-sided shift on l2(N), then |A| = {A*A}1/2 = I. So if A = U |A|, U must be A, which is not unitary.

The existence of a polar decomposition is a consequence of Douglas' lemma:

Lemma — If A, B are bounded operators on a Hilbert space H, and A*AB*B, then there exists a contraction C such that A = CB. Furthermore, C is unique if Ker(B*) ⊂ Ker(C).

The operator C can be defined by C(Bh) := Ah for all h in H, extended by continuity to the closure of Ran(B), and by zero on the orthogonal complement to all of H. The lemma then follows since A*AB*B implies Ker(B) ⊂ Ker(A).

In particular. If A*A = B*B, then C is a partial isometry, which is unique if Ker(B*) ⊂ Ker(C). In general, for any bounded operator A,

where (A*A)1/2 is the unique positive square root of A*A given by the usual functional calculus. So by the lemma, we have
for some partial isometry U, which is unique if Ker(A*) ⊂ Ker(U). Take P to be (A*A)1/2 and one obtains the polar decomposition A = UP. Notice that an analogous argument can be used to show A = P'U', where P' is positive and U' a partial isometry.

When H is finite-dimensional, U can be extended to a unitary operator; this is not true in general (see example above). Alternatively, the polar decomposition can be shown using the operator version of singular value decomposition.

By property of the continuous functional calculus, |A| is in the C*-algebra generated by A. A similar but weaker statement holds for the partial isometry: U is in the von Neumann algebra generated by A. If A is invertible, the polar part U will be in the C*-algebra as well.

Unbounded operators

If A is a closed, densely defined unbounded operator between complex Hilbert spaces then it still has a (unique) polar decomposition

where |A| is a (possibly unbounded) non-negative self adjoint operator with the same domain as A, and U is a partial isometry vanishing on the orthogonal complement of the range Ran(|A|).

The proof uses the same lemma as above, which goes through for unbounded operators in general. If Dom(A*A) = Dom(B*B) and A*Ah = B*Bh for all hDom(A*A), then there exists a partial isometry U such that A = UB. U is unique if Ran(B)Ker(U). The operator A being closed and densely defined ensures that the operator A*A is self-adjoint (with dense domain) and therefore allows one to define (A*A)1/2. Applying the lemma gives polar decomposition.

If an unbounded operator A is affiliated to a von Neumann algebra M, and A = UP is its polar decomposition, then U is in M and so is the spectral projection of P, 1B(P), for any Borel set B in [0, ∞).

Quaternion polar decomposition

The polar decomposition of quaternions H depends on the unit 2-dimensional sphere of square roots of minus one, known as the "pure quaternions". Given any r on this sphere, and an angle −π < a ≤ π, the versor is on the unit 3-sphere of H. For a = 0 and a = π, the versor is 1 or −1 regardless of which r is selected. The norm t of a quaternion q is the Euclidean distance from the origin to q. When a quaternion is not just a real number, then there is a unique polar decomposition . Here r, a, t are all uniquely determined such that r is a pure quaternion (i.e., r2 = -1), a satisfies 0 < a < π, and t > 0 .

Alternative planar decompositions

In the Cartesian plane, alternative planar ring decompositions arise as follows:

Numerical determination of the matrix polar decomposition

To compute an approximation of the polar decomposition A = UP, usually the unitary factor U is approximated.[8][9] The iteration is based on Heron's method for the square root of 1 and computes, starting from , the sequence

The combination of inversion and Hermite conjugation is chosen so that in the singular value decomposition, the unitary factors remain the same and the iteration reduces to Heron's method on the singular values.

This basic iteration may be refined to speed up the process:

See also


  1. ^ Hall 2015 Section 2.5
  2. ^ Hall 2015 Theorem 2.17
  3. ^ Hall 2015 Section 13.3
  4. ^ Higham, Nicholas J.; Schreiber, Robert S. (1990). "Fast polar decomposition of an arbitrary matrix". SIAM J. Sci. Stat. Comput. Philadelphia, PA, USA: Society for Industrial and Applied Mathematics. 11 (4): 648–655. CiteSeerX doi:10.1137/0911038. ISSN 0196-5204. S2CID 14268409.
  5. ^ Hall 2015 Lemma 2.18
  6. ^ Note how this implies, by the positivity of , that the eigenvalues are all real and strictly positive.
  7. ^ Sobczyk, G.(1995) "Hyperbolic Number Plane", College Mathematics Journal 26:268–80
  8. ^ Higham, Nicholas J. (1986). "Computing the polar decomposition with applications". SIAM J. Sci. Stat. Comput. Philadelphia, PA, USA: Society for Industrial and Applied Mathematics. 7 (4): 1160–1174. CiteSeerX doi:10.1137/0907079. ISSN 0196-5204.
  9. ^ Byers, Ralph; Hongguo Xu (2008). "A New Scaling for Newton's Iteration for the Polar Decomposition and its Backward Stability". SIAM J. Matrix Anal. Appl. Philadelphia, PA, USA: Society for Industrial and Applied Mathematics. 30 (2): 822–843. CiteSeerX doi:10.1137/070699895. ISSN 0895-4798.