In Clifford groups, a nonassociative product is defined which leads to the
definition of nonassociative groups. These nonassociative groups have matri
x representations on the condition that the "row by column" product of two
matrices is replaced by the "column by column" product. A nonassociative gr
oup of transformations connected with the Lorentz group is determined, toge
ther with its irreducible, double-valued matrix representation, whose matri
ces undergo the "column by column" product.