Step 1: Get the force vector right before doing anything else.
Saying the force is 2 N in the direction $\hat{i}+\hat{j}$ means its magnitude is 2 N and it points along the unit vector in that direction, not that the vector $\hat{i}+\hat{j}$ is simply doubled. The unit vector along $\hat{i}+\hat{j}$ is $\dfrac{\hat{i}+\hat{j}}{\sqrt2}$, so
\[
\vec{F} = 2\cdot\frac{\hat{i}+\hat{j}}{\sqrt2} = \sqrt2\hat{i} + \sqrt2\hat{j}
\]
Step 2: Set up the cross product with the correct vectors.
\[
\vec{r} = \hat{i}+\hat{j}+\hat{k}, \qquad \vec{F} = \sqrt2\hat{i}+\sqrt2\hat{j}+0\hat{k}
\]
Step 3: Expand the determinant.
\[
\vec{\tau} = \vec{r}\times\vec{F} =
\begin{vmatrix}
\hat{i} & \hat{j} & \hat{k} \\
1 & 1 & 1 \\
\sqrt2 & \sqrt2 & 0
\end{vmatrix}
= \hat{i}(1\cdot0 - 1\cdot\sqrt2) - \hat{j}(1\cdot0 - 1\cdot\sqrt2) + \hat{k}(1\cdot\sqrt2 - 1\cdot\sqrt2)
\]
Step 4: Simplify each component.
\[
\vec{\tau} = -\sqrt2\hat{i} + \sqrt2\hat{j} + 0\hat{k}
\]
Step 5: Conclusion.
\[
\boxed{-\sqrt2\hat{i}+\sqrt2\hat{j}}
\]