We obtain various characterizations of the fundamental operators of -contraction and -contraction. We also demonstrate some important relations between the fundamental operators of a -contraction and a -contraction. We describe functional models for and . We give a complete set of unitary invariants for a pure -contraction and a pure -contraction. We demonstrate the functional models for a certain class of completely non-unitary -contraction and completely non-unitary -contraction which satisfy the following conditions: \begin{equation}\label{Condition 1} \begin{aligned} &T^_iT_7 = T_7T^_i ,, ,, 1 \leqslant i \leqslant 6 \end{aligned} \end{equation} and \begin{equation}\label{Condition 2} \begin{aligned} &S^_iS_3 = S_3S^_i, \tilde{S}^_jS_3 = S_3\tilde{S}^_j ,, ,, 1 \leqslant i, j \leqslant 2, \end{aligned} \end{equation} respectively. We also describe a functional model for a completely non-unitary tetrablock contraction that satisfies \begin{equation}\label{Condition 3} \begin{aligned} A^_iP = PA^_i ,, . \end{aligned} \end{equation} By exhibiting counter examples, we show that such abstract model of tetrablock contraction, -contraction and -contraction may not exist if we drop the hypothesis of the above equations, respectively…

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