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Multicomplex number

In mathematics, the multicomplex number systems \mathbb {C} _{n} are defined inductively as follows: Let C0 be the real number system. For every n > 0 let in be a square root of −1, that is, an imaginary unit. Then \mathbb {C} _{n+1}=\lbrace z=x+yi_{n+1}:x,y\in \mathbb {C} _{n}\rbrace. In the multicomplex number systems one also requires that i_{n}i_{m}=i_{m}i_{n} (commutativity). Then \mathbb {C} _{1} is the complex number system, \mathbb {C} _{2} is the bicomplex number system, \mathbb {C} _{3} is the tricomplex number system of Corrado Segre, and \mathbb {C} _{n} is the multicomplex number system of order n.

Each \mathbb {C} _{n} forms a Banach algebra. G. Bayley Price has written about the function theory of multicomplex systems, providing details for the bicomplex system \mathbb {C} _{2}.

The multicomplex number systems are not to be confused with Clifford numbers (elements of a Clifford algebra), since Clifford's square roots of −1 anti-commute (i_{n}i_{m}+i_{m}i_{n}=0 when mn for Clifford).

Because the multicomplex numbers have several square roots of, 1 that commute, they also have zero divisors: (i_{n}-i_{m})(i_{n}+i_{m})=i_{n}^{2}-i_{m}^{2}=0 despite i_{n}-i_{m}\neq 0 and i_{n}+i_{m}\neq 0, and (i_{n}i_{m}-1)(i_{n}i_{m}+1)=i_{n}^{2}i_{m}^{2}-1=0 despite i_{n}i_{m}\neq 1 and i_{n}i_{m}\neq -1. Any product i_{n}i_{m} of two distinct multicomplex units behaves as the j of the split-complex numbers, and therefore the multicomplex numbers contain a number of copies of the split-complex number plane.

With respect to subalgebra \mathbb {C} _{k}, k = 0, 1, ..., n − 1, the multicomplex system \mathbb {C} _{n} is of dimension 2nk over \mathbb {C} _{k}.

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