In group theory, to account for electron spin, double group is introduced. The key difference between an ordinary point group and a double group is an extra element $\bar{E}$ with the meaning of a $2\pi$ rotation. Since only a $4\pi$ rotation restores a spin state, $\bar{E}^2 = E$, where $E$ is the identity.
Also, a $2\pi$ rotation always results in a $\pi$ phase in spinor. To put it another way, $\bar{E}=-1$. From this point of view, double group representation character of $\bar{E}$ should always be $-D$, where $D$ is the dimension of the representation.
However, character table of double groups does not follow this rule. For example, for two double groups $T_d$ and $O$, the character table is:
The character of $\bar{E}$ is positive in most representations. Does this mean that these representations are not physical? If so, it seems crystals with $T_d$ or $O$ symmetry have degeneracies everywhere, which is hardly acceptable to me.
Can anyone help me resolve this issue?