In mathematics, the Kronecker product, denoted by ⊗, is an operation on two matrices of arbitrary size resulting in a block matrix. It gives the matrix of the tensor product with respect to a standard choice of basis. The Kronecker product should not be confused with the usual matrix multiplication, which is an entirely different operation. It is named after German mathematician Leopold Kronecker.
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If A is an m-by-n matrix and B is a p-by-q matrix, then the Kronecker product A ⊗ B is the mp-by-nq block matrix
More explicitly, we have
If A and B represent linear transformations V1 → W1 and V2 → W2, respectively, then A ⊗ B represents the tensor product of the two maps, V1 ⊗ V2 → W1 ⊗ W2.
The Kronecker product is a special case of the tensor product, so it is bilinear and associative:
where A, B and C are matrices and k is a scalar.
The Kronecker product is not commutative: in general, A B and B A are different matrices. However, A B and B A are permutation equivalent, meaning that there exist permutation matrices P and Q such that
If A and B are square matrices, then A B and B A are even permutation similar, meaning that we can take P = QT.
If A, B, C and D are matrices of such size that one can form the matrix products AC and BD, then
This is called the mixed-product property, because it mixes the ordinary matrix product and the Kronecker product. It follows that A B is invertible if and only if A and B are invertible, in which case the inverse is given by
The operation of transposition is distributive over the Kronecker product:
If A is n-by-n, B is m-by-m and denotes the k-by-k identity matrix then we can define what is sometimes called the Kronecker sum, , by
(Note that this is different from the direct sum of two matrices.) This operation is related to the tensor product on Lie algebras.
We have the following formula for the matrix exponential which is useful in the numerical evaluation of certain continuous-time Markov processes ,
Kronecker sums appear naturally in physics when considering ensembles of non-interacting systems. Let be the Hamiltonian of the i-th such system. Then the total Hamiltonian of the ensemble is .
Suppose that A and B are square matrices of size n and m respectively. Let λ1, ..., λn be the eigenvalues of A and μ1, ..., μm be those of B (listed according to multiplicity). Then the eigenvalues of A B are
It follows that the trace and determinant of a Kronecker product are given by
If A and B are rectangular matrices, then one can consider their singular values. Suppose that A has rA nonzero singular values, namely
Similarly, denote the nonzero singular values of B by
Then the Kronecker product A B has rArB nonzero singular values, namely
Since the rank of a matrix equals the number of nonzero singular values, we find that
The Kronecker product of matrices corresponds to the abstract tensor product of linear maps. Specifically, if the vector spaces V, W, X, and Y have bases {v1, ... , vm}, {w1, ... , wn}, {x1, ... , xd}, and {y1, ... , ye}, respectively, and if the matrices A and B represent the linear transformations S : V → X and T : W → Y, respectively in the appropriate bases, then the matrix A ⊗ B represents the tensor product of the two maps, S ⊗ T : V ⊗ W → X ⊗ Y with respect to the basis {v1 ⊗ w1, v1 ⊗ w2, ... , v2 ⊗ w1, ... , vm ⊗ wn} of V ⊗ W and the similarly defined basis of X ⊗ Y with the property that A ⊗ B(vi ⊗ wj) = (Avi)⊗(Bwj), where i and j are integers in the proper range.[1]
When V and W are Lie algebras, and S : V → V and T : W → W are Lie algebra homomorphisms, the Kronecker sum of A and B represents the induced Lie algebra homomorphisms V ⊗ W → V ⊗ W.
The Kronecker product of the adjacency matrices of two graphs is the adjacency matrix of the tensor product graph. The Kronecker sum of the adjacency matrices of two graphs is the adjacency matrix of the Cartesian product graph. See,[2] answer to Exercise 96.
The Kronecker product can be used to get a convenient representation for some matrix equations. Consider for instance the equation AXB = C, where A, B and C are given matrices and the matrix X is the unknown. We can rewrite this equation as
Here, vec(X) denotes the vectorization of the matrix X formed by stacking the columns of X into a single column vector. It now follows from the properties of the Kronecker product that the equation AXB = C has a unique solution if and only if A and B are nonsingular (Horn & Johnson 1991, Lemma 4.3.1).
If X is row-ordered into the column vector x then can be also be written as (Jain 1989, 2.8 Block Matrices and Kronecker Products)
The Kronecker product is named after Leopold Kronecker, even though there is little evidence that he was the first to define and use it. Indeed, in the past the Kronecker product was sometimes called the Zehfuss matrix, after Johann Georg Zehfuss.
Two related matrix operations are the Tracy-Singh and Khatri-Rao products which operate on partitioned matrices. Let the m-by-n matrix A be partitioned into the -by- blocks and -by- matrix into the -by- blocks Bkl with of course , , and
The Tracy-Singh product[3][4] is defined as
which means that the th subblock of the mp-by-nq product is the -by- matrix , of which the th subblock equals the -by- matrix . Essentially the Tracy-Singh product is the pairwise Kronecker product for each pair of partitions in the two matrices.
For example, if A and B both are 2-by-2 partitioned matrices e.g.:
we get:
The Khatri-Rao product[5][6] is defined as
in which the th block is the -by- sized Kronecker product of the corresponding blocks of and , assuming the number of row and column partitions of both matrices is equal. The size of the product is then -by-. Proceeding with the same matrices as the previous example we obtain:
This is a submatrix of the Tracy-Singh product of the two matrices (each partition in this example is a partition in a corner of the Tracy-Singh product).
A column-wise Kronecker product of two matrices may also be called the Khatri-Rao product. This product assumes the partitions of the matrices are their columns. In this case , , and . The resulting product is a -by- matrix of which each column is the Kronecker product of the corresponding columns of and . Using the matrices from the previous examples with the columns partitioned:
so that: