  Let $\mathbb S$ be a Clifford module for the complexified Clifford algebra
$\mathbb{C}\ell(\mathbb R^n)$, $\mathbb S'$ its dual, $\rho$ and $\rho'$ be the
corresponding representations of the spin group ${\rm Spin}(n)$. The group $G=
{\rm Spin}(1,n+1)$ is a (twofold) covering of the conformal group of $\mathbb
R^n$. For $\lambda, \mu\in \mathbb C$, let $\pi_{\rho, \lambda}$ (resp.
$\pi_{\rho',\mu}$) be the spinorial representation of $G$ realized on a
(subspace of) $C^\infty(\mathbb R^n,\mathbb S)$ (resp. $C^\infty(\mathbb
R^n,\mathbb S')$). For $0\leq k\leq n$ and $m\in \mathbb N$, we construct a
symmetry breaking differential operator $B_{k;\lambda,\mu}^{(m)}$ from
$C^\infty(\mathbb R^n \times \mathbb R^n,\mathbb{S}\,\otimes\, \mathbb{S}')$
into $C^\infty(\mathbb R^n, \Lambda^*_k(\mathbb R^n) \otimes \mathbb{C})$ which
intertwines the representations $\pi_{\rho, \lambda}\otimes \pi_{\rho',\mu} $
and $\pi_{\tau^*_k,\lambda+\mu+2m}$, where $\tau^*_k$ is the representation of
${\rm Spin}(n)$ on the space $\Lambda^*_k(\mathbb R^n) \otimes \mathbb{C}$ of
complex-valued alternating $k$-forms on $\mathbb{R}^n$.
