The Wigner-Eckart Theorem states that in state $| j = 1 , m \rangle$ : $$ \langle 1 ,m_1| Y^{m_{2}}_1 |1,m_{2}\rangle = \int d\Omega Y^{{*}^{m_1}}_1 Y^{m_2}_{1} Y^{m_3}_{1} = C^{1 1 1}_{m_{1} m_{2} m_{3}} \langle j|| Y^{m_{2}}_1||j\rangle $$
In the general case, to find $\langle j|| Y^{m_{2}}_1||j\rangle$ we set $m_1 = m_2 = m_3 = 0$ and get:
$$\int d\Omega Y^{{*}^{0}}_1 Y^{0}_{1} Y^{0}_{1} = C^{1 1 1}_{0 0 0} \langle j|| Y^{m_{2}}_1||j\rangle $$
The result given by the integration is zero, so this means that $\langle j|| Y^{m_{2}}_1||j\rangle$ or $ C^{1 1 1}_{0 0 0} = 0 $ (the Clebcsh-Gordon coeffiecient is zero), according to Wolfram $C^{1 1 1}_{0 0 0} = 0$.
So in this the Wigner-Eckart isn't applicable because we can't find the matrix element $\langle j|| Y^{m_{2}}_1||j\rangle$ or we have to set the $m$ to something else?