where the matrices D(P) for each point group operation P in section 2.1 are given in full in Table 2.Note that the functions xnew , ynew , znew defined by (eq. 1) and Table 2 happen to be extremely simple. Each of them has one of the six forms (+x, -x, +y, -y, +z, -z), regardless of which point group operation is considered. These very simple transformation properties make it relatively easy for the reader to verify many of the algebraic statements in this article.
It may seem strange to have chosen a convention in which a particle is rotated through an angle -2π/n rather than +2π/n. It will turn out later that vibrational displacement vectors are subjected to this negative rotation, while the molecule-fixed axis system is subjected to the corresponding positive rotation [12,13].
Conventions for the application of a point group operation P to a function f of the variables x,y,z are fixed by the following definition
Note that the transformed function g is still a function of the original variables x,y,z; it was obtained from the untransformed function f (x,y,z) by substituting everywhere xPnew(x,y,z) for x, etc. The effect of two point group operations in succession is defined by (eq. 3)
where g is obtained from f as in (eq. 2) and h is obtained from g(x,y,z) by substituting everywhere xQnew(x,y,z) for x, etc.
It can be seen that the results of the operation Q P correspond to replacing x in the function f(x,y,z), by xQPnew(x,y,z), etc., where
Because the order of the matrices D(P)D(Q) is opposite to the order of the operators Q P, the transposes of the matrices D(P) form a representation  of the group Td, not the matrices themselves. Avoiding this slight complication would have required adopting a form of (eq. 1) written in terms of (x,y,z) row vectors post multiplied by the D(P)'s.