  Let $\mathbb F$ denote a field, and let $V$ denote a vector space over
$\mathbb F$ with finite positive dimension. We consider an ordered pair of
$\mathbb F$-linear maps $A: V \to V$ and $A^*:V\to V$ such that (i) each of
$A,A^*$ is diagonalizable; (ii) there exists an ordering $\lbrace
V_i\rbrace_{i=0}^d$ of the eigenspaces of $A$ such that $A^* V_i \subseteq
V_{i-1} + V_i+ V_{i+1}$ for $0 \leq i \leq d$, where $V_{-1} = 0$ and $V_{d+1}=
0$; (iii) there exists an ordering $\lbrace V^*_i\rbrace_{i=0}^{\delta}$ of the
eigenspaces of $A^*$ such that $A V^*_i \subseteq V^*_{i-1} + V^*_i+ V^*_{i+1}
$ for $0 \leq i \leq \delta $, where $V^*_{-1} = 0$ and $V^*_{\delta+1}= 0$;
(iv) there does not exist a subspace $U$ of $V$ such that $AU\subseteq U$,
$A^*U \subseteq U$, $U\not=0$, $U\not=V$. We call such a pair a tridiagonal
pair on $V$. We assume that $A, A^*$ belongs to a family of tridiagonal pairs
said to have $q$-Racah type. There is an infinite-dimensional algebra
$\boxtimes_q$ called the $q$-tetrahedron algebra; it is generated by four
copies of $U_q(\mathfrak{sl}_2)$ that are related in a certain way. Using $A,
A^*$ we construct two $\boxtimes_q$-module structures on $V$. In this
construction the two main ingredients are the double lowering map $\psi:V\to V$
due to Sarah Bockting-Conrad, and a certain invertible map $W:V\to V$ motivated
by the spin model concept due to V. F. R. Jones.
