The classical distribution theory founded by Laurent Schwartz [26] has an intrinsic multiplication problem. He indicates this in his paper [27]. This problem is clearly demonstrated by selecting two particular distributions and attempting to define a multiplication that enjoys commutative, associative, and unit identity properties. This process leads to the contradiction, 1 = eP I [lo]. A new generalized function theory developed by J. Colombeau [4-91 provides a solution to the multiplication problem and also develops a general integration theory. T. Todorov reexamines the new generalized function theory in the spirit of non-denumerable sequences termed ultrapowers [29]. The L. Schwartz distribution theory was reexamined in the spirit of fundamental sequences [ 16,333. However, there are new considerations in the theory of new generalized function theory requiring an algebraic notion of a particular ideal contained in a specified test function space. A brief review of these constructions can be found in Section 7 and a comprehensive review can be found in Ref. [25]. A principle application for our development will be modeling a physical system consisting of an “infinite” number of particles. A system of n-particles termed bosoms or fermions has previously been modeled by n-dimensional symmetric or antisymmetric functions. When this system is enlarged to an infinite number of particles, the model for the state space vector has the form,