In mathematics, a matrix of ones or all-ones matrix is a matrix with every entry equal to one. For example:

J 2 = [ 1 1 1 1 ] , J 3 = [ 1 1 1 1 1 1 1 1 1 ] , J 2 , 5 = [ 1 1 1 1 1 1 1 1 1 1 ] , J 1 , 2 = [ 1 1 ] . {\displaystyle J_{2}={\begin{bmatrix}1&1\\1&1\end{bmatrix}},\quad J_{3}={\begin{bmatrix}1&1&1\\1&1&1\\1&1&1\end{bmatrix}},\quad J_{2,5}={\begin{bmatrix}1&1&1&1&1\\1&1&1&1&1\end{bmatrix}},\quad J_{1,2}={\begin{bmatrix}1&1\end{bmatrix}}.\quad }

Some sources call the all-ones matrix the unit matrix, but that term may also refer to the identity matrix, a different type of matrix.

A vector of ones or all-ones vector is matrix of ones having row or column form; it should not be confused with unit vectors.

Properties

For an n × n matrix of ones J, the following properties hold:

When J is considered as a matrix over the real numbers, the following additional properties hold:

Applications

The all-ones matrix arises in the mathematical field of combinatorics, particularly involving the application of algebraic methods to graph theory. For example, if A is the adjacency matrix of an n-vertex undirected graph G, and J is the all-ones matrix of the same dimension, then G is a regular graph if and only if AJ = JA. As a second example, the matrix appears in some linear-algebraic proofs of Cayley's formula, which gives the number of spanning trees of a complete graph, using the matrix tree theorem.

The logical square roots of a matrix of ones, logical matrices whose square is a matrix of ones, can be used to characterize the central groupoids. Central groupoids are algebraic structures that obey the identity ( a ⋅ b ) ⋅ ( b ⋅ c ) = b {\displaystyle (a\cdot b)\cdot (b\cdot c)=b}. Finite central groupoids have a square number of elements, and the corresponding logical matrices exist only for those dimensions.

See also