action of the symmetry algebra from one particle to two and many particle states, one needs a notion of the coproduct. Hence, if $D$ is a representation of the symmetry algebra $\mathfrak{G}$ (which is here $\kappa$-Poincaré algebra, $\mathfrak{G} \equiv \mathfrak{iso}_{\kappa}(1,3) $ ), which acts on the space $V$ of physical states (asymptotic in and out states) as $ | \phi \rangle
\longrightarrow D(\Lambda) | \phi \rangle $, with $\Lambda \in
\mathfrak{G} $ and $| \phi \rangle \in V, $ then this action of the symmetry algebra can be extended to two particle states according to $$| \phi_1 \rangle \otimes | \phi_2 \rangle \longrightarrow (D \otimes
   D) \Delta (\Lambda) | \phi_1 \rangle \otimes | \phi_2 \rangle,$$ where $\Delta : \mathfrak{G} \longrightarrow  \mathfrak{G} \otimes
\mathfrak{G} $ is the coproduct. Since in noncommutative versions of QFT, in much the same way as in the standard QFT, one is concerned with the states of many identical particles, it is of importance to identify the exchange statistics that particles obey upon deformation. It is known that the (anti)symmetrization procedure in NCQFT, required to describe deformed bosons and fermions, is carried out with the help of the statistics flip operator $\tau$ (intertwiner), which needs to be 