In linear algebra, the **Gram matrix** (or **Gramian matrix**, **Gramian**) of a set of vectors in an inner product space is the Hermitian matrix of inner products, whose entries are given by the inner product .^{[1]} If the vectors are the columns of matrix then the Gram matrix is in the general case that the vector coordinates are complex numbers, which simplifies to for the case that the vector coordinates are real numbers.

An important application is to compute linear independence: a set of vectors are linearly independent if and only if the Gram determinant (the determinant of the Gram matrix) is non-zero.

It is named after Jørgen Pedersen Gram.

For finite-dimensional real vectors in with the usual Euclidean dot product, the Gram matrix is , where is a matrix whose columns are the vectors and is its transpose whose rows are the vectors . For complex vectors in , , where is the conjugate transpose of .

Given square-integrable functions on the interval , the Gram matrix is:

where is the complex conjugate of .

For any bilinear form on a finite-dimensional vector space over any field we can define a Gram matrix attached to a set of vectors by . The matrix will be symmetric if the bilinear form is symmetric.

- In Riemannian geometry, given an embedded -dimensional Riemannian manifold and a parametrization for , the volume form on induced by the embedding may be computed using the Gramian of the coordinate tangent vectors: This generalizes the classical surface integral of a parametrized surface for :
- If the vectors are centered random variables, the Gramian is approximately proportional to the
**covariance matrix**, with the scaling determined by the number of elements in the vector. - In quantum chemistry, the Gram matrix of a set of basis vectors is the
**overlap matrix**. - In control theory (or more generally systems theory), the
**controllability Gramian**and**observability Gramian**determine properties of a linear system. - Gramian matrices arise in covariance structure model fitting (see e.g., Jamshidian and Bentler, 1993, Applied Psychological Measurement, Volume 18, pp. 79–94).
- In the finite element method, the Gram matrix arises from approximating a function from a finite dimensional space; the Gram matrix entries are then the inner products of the basis functions of the finite dimensional subspace.
- In machine learning, kernel functions are often represented as Gram matrices.
^{[2]}(Also see kernel PCA) - Since the Gram matrix over the reals is a symmetric matrix, it is diagonalizable and its eigenvalues are non-negative. The diagonalization of the Gram matrix is the singular value decomposition.

The Gram matrix is symmetric in the case the real product is real-valued; it is Hermitian in the general, complex case by definition of an inner product.

The Gram matrix is positive semidefinite, and every positive semidefinite matrix is the Gramian matrix for some set of vectors. The fact that the Gramian matrix is positive-semidefinite can be seen from the following simple derivation:

The first equality follows from the definition of matrix multiplication, the second and third from the bi-linearity of the inner-product, and the last from the positive definiteness of the inner product.
Note that this also shows that the Gramian matrix is positive definite if and only if the vectors are linearly independent (that is, for all ).^{[1]}

See also: Positive definite matrix § Decomposition |

Given any positive semidefinite matrix , one can decompose it as:

- ,

where is the conjugate transpose of (or in the real case).

Here is a matrix, where is the rank of . Various ways to obtain such a decomposition include computing the Cholesky decomposition or taking the non-negative square root of .

The columns of can be seen as *n* vectors in (or *k*-dimensional Euclidean space , in the real case). Then

where the dot product is the usual inner product on .

Thus a Hermitian matrix is positive semidefinite if and only if it is the Gram matrix of some vectors . Such vectors are called a **vector realization** of . The infinite-dimensional analog of this statement is Mercer's theorem.

If is the Gram matrix of vectors in then applying any rotation or reflection of (any orthogonal transformation, that is, any Euclidean isometry preserving 0) to the sequence of vectors results in the same Gram matrix. That is, for any orthogonal matrix , the Gram matrix of is also .

This is the only way in which two real vector realizations of can differ: the vectors are unique up to orthogonal transformations. In other words, the dot products and are equal if and only if some rigid transformation of transforms the vectors to and 0 to 0.

The same holds in the complex case, with unitary transformations in place of orthogonal ones.
That is, if the Gram matrix of vectors is equal to the Gram matrix of vectors in then there is a unitary matrix (meaning ) such that for .^{[3]}

- Because , it is necessarily the case that and commute. That is, a real or complex Gram matrix is also a normal matrix.
- The Gram matrix of any orthonormal basis is the identity matrix. Equivalently, the Gram matrix of the rows or the columns of a real rotation matrix is the identity matrix. Likewise, the Gram matrix of the rows or columns of a unitary matrix is the identity matrix.
- The rank of the Gram matrix of vectors in or equals the dimension of the space spanned by these vectors.
^{[1]}

The **Gram determinant** or **Gramian** is the determinant of the Gram matrix:

If are vectors in then it is the square of the *n*-dimensional volume of the parallelotope formed by the vectors. In particular, the vectors are linearly independent if and only if the parallelotope has nonzero *n*-dimensional volume, if and only if Gram determinant is nonzero, if and only if the Gram matrix is nonsingular. When *m* < *n* the determinant and volume are zero. When *m* = *n*, this reduces to the standard theorem that the absolute value of the determinant of *n* *n*-dimensional vectors is the *n*-dimensional volume. The Gram determinant is also useful for computing the volume of the simplex formed by the vectors; its volume is Volume(parallelotope) / *n*!.

The Gram determinant can also be expressed in terms of the exterior product of vectors by

When the vectors are defined from the positions of points relative to some reference point ,

then the Gram determinant can be written as the difference of two Gram determinants,

where each is the corresponding point supplemented with the coordinate value of 1 for an -st dimension.^{[citation needed]} Note that in the common case that *n* = *m*, the second term on the right-hand side will be zero.

Given a set of linearly independent vectors with Gram matrix , one can construct an orthonormal basis

The matrix is guaranteed to exist. Indeed, is Hermitian, and so can be decomposed as with a unitary matrix and a real diagonal matrix. Additionally, the are linearly independent if and only if is positive definite, which implies that the diagonal entries of are positive. is therefore uniquely defined by . One can check that these new vectors are orthonormal:

where we used .