Sylvester's Law of Inertia

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## Statement

## Statement in terms of eigenvalues

## Law of inertia for quadratic forms

## Generalizations

## See also

## References

## External links

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Sylvester's Law of Inertia

**Sylvester's law of inertia** is a theorem in matrix algebra about certain properties of the coefficient matrix of a real quadratic form that remain invariant under a change of basis. Namely, if *A* is the symmetric matrix that defines the quadratic form, and *S* is any invertible matrix such that *D* = *SAS*^{T} is diagonal, then the number of negative elements in the diagonal of *D* is always the same, for all such *S*; and the same goes for the number of positive elements.

This property is named after James Joseph Sylvester who published its proof in 1852.^{[1]}^{[2]}

Let *A* be a symmetric square matrix of order *n* with real entries. Any non-singular matrix *S* of the same size is said to transform *A* into another symmetric matrix , also of order *n*, where *S*^{T} is the transpose of *S*. It is also said that matrices *A* and *B* are congruent. If *A* is the coefficient matrix of some quadratic form of **R**^{n}, then *B* is the matrix for the same form after the change of basis defined by *S*.

A symmetric matrix *A* can always be transformed in this way into a diagonal matrix *D* which has only entries 0, +1 and -1 along the diagonal. Sylvester's law of inertia states that the number of diagonal entries of each kind is an invariant of *A*, i.e. it does not depend on the matrix *S* used.

The number of +1s, denoted *n*_{+}, is called the **positive index of inertia** of *A*, and the number of -1s, denoted *n*_{-}, is called the **negative index of inertia**. The number of 0s, denoted *n*_{0}, is the dimension of the null space of *A*, known as the nullity of *A*. These numbers satisfy an obvious relation

The difference, , is usually called the **signature** of *A*. (However, some authors use that term for the triple consisting of the nullity and the positive and negative indices of inertia of *A*; for a non-degenerate form of a given dimension these are equivalent data, but in general the triple yields more data.)

If the matrix *A* has the property that every principal upper left minor *?*_{k} is non-zero then the negative index of inertia is equal to the number of sign changes in the sequence

The law can also be stated as follows: two symmetric square matrices of the same size have the same number of positive, negative and zero eigenvalues if and only if they are congruent^{[3]} (, for some non-singular ).

The positive and negative indices of a symmetric matrix *A* are also the number of positive and negative eigenvalues of *A*. Any symmetric real matrix *A* has an eigendecomposition of the form *QEQ*^{T} where *E* is a diagonal matrix containing the eigenvalues of *A*, and *Q* is an orthonormal square matrix containing the eigenvectors. The matrix *E* can be written *E* = *WDW*^{T} where *D* is diagonal with entries 0, +1, or −1, and *W* is diagonal with *W*_{ii} = ?|*E*_{ii}|. The matrix *S* = *QW* transforms *D* to *A*.

In the context of quadratic forms, a real quadratic form *Q* in *n* variables (or on an *n*-dimensional real vector space) can by a suitable change of basis (by non-singular linear transformation from x to y) be brought to the diagonal form

with each *a*_{i} ? {0, 1, −1}. Sylvester's law of inertia states that the number of coefficients of a given sign is an invariant of *Q*, i.e., does not depend on a particular choice of diagonalizing basis. Expressed geometrically, the law of inertia says that all maximal subspaces on which the restriction of the quadratic form is positive definite (respectively, negative definite) have the same dimension. These dimensions are the positive and negative indices of inertia.

Sylvester's law of inertia is also valid if *A* and *B* have complex entries. In this case, it is said that *A* and *B* are *-congruent if and only if there exists a non-singular complex matrix *S* such that .

In the complex scenario, a way to state Sylvester's law of inertia is that if *A* and *B* are Hermitian matrices, then *A* and *B* are *-congruent if and only if they have the same inertia. A theorem due to Ikramov generalizes the law of inertia to any normal matrices *A* and *B*:^{[4]}

If *A* and *B* are normal matrices, then *A* and *B* are congruent if and only if they have the same number of eigenvalues on each open ray from the origin in the complex plane.

**^**Sylvester, James Joseph (1852). "A demonstration of the theorem that every homogeneous quadratic polynomial is reducible by real orthogonal substitutions to the form of a sum of positive and negative squares" (PDF).*Philosophical Magazine*. 4th Series.**4**(23): 138-142. doi:10.1080/14786445208647087. Retrieved .**^**Norman, C.W. (1986).*Undergraduate algebra*. Oxford University Press. pp. 360-361. ISBN 978-0-19-853248-4.**^**Carrell, James B. (2017).*Groups, Matrices, and Vector Spaces: A Group Theoretic Approach to Linear Algebra*. Springer. p. 313. ISBN 978-0-387-79428-0.**^**Ikramov, Kh. D. (2001). "On the inertia law for normal matrices".*Doklady Mathematics*.**64**: 141-142.

- Garling, D. J. H. (2011).
*Clifford algebras. An introduction*. London Mathematical Society Student Texts.**78**. Cambridge: Cambridge University Press. ISBN 978-1-107-09638-7. Zbl 1235.15025.

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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