At a given time t, the rotation matrix R has the value:
$$R= \begin{pmatrix} 0.675 & −0.1724 &0.7174\\0.2474 & 0.9689& 0 &\\−0.6951& 0.1775&0.6967. \end{pmatrix}$$
The angular velocity in a body fixed frame $\hat ω^b$ at that same time t is:
$$\hat ω^b=\begin{pmatrix}0& −1 &0.9689&\\1 & 0 &−0.2474\\−0.9689&0.2474&0. \end{pmatrix}$$ What is $\hatω^s$, the angular velocity in an inertial frame?
I know that \begin{align*}\omega^s:\dot q &= \dot RR^Tq\\&=R\hat\omega^b\end{align*}
Therfore I did on Matlab:
>> R = [0.675 -0.1724 0.7174; 0.2474 0.9689 0; -0.6951 0.1775 0.6967];
>> wb= [0 -1 0.9689; 1 0 -0.2474; -0.9689 0.2747 0];
>> R*wb
ans =
-0.8675 -0.4779 0.6967
0.9689 -0.2474 0
-0.4975 0.8865 -0.7174
Which is none of the provided answer:

No, that's not the angular velocity, that's the matrix version of $\omega\times$, and while we're at it the angular velocity of what in the body frame of what? Can you please explain the setup of the problem? How many bodies are there? What is rotating and what isn't? How is the inertial frame defined?
From what you wrote I would just read off the components of $\omega^b$ (a vector, not a matrix) and multiply them be $R$, trying to see if it agrees with any one of those answers, but without any further details it's tough to give you good advice here.