The behavior of the unit vectors under inversion (reflection through the origin) can be determined as follows:
- In spherical coordinates, the position vector is given by:
\[
\mathbf{r} = r \hat{r}
\]
- Under inversion \( \mathbf{r} \to -\mathbf{r} \), the radial unit vector transforms as:
\[
\hat{r} \to -\hat{r}
\]
- The polar unit vector \( \hat{\theta} \) is defined as:
\[
\hat{\theta} = \frac{\partial \hat{r}}{\partial \theta}
\]
- Since \( \hat{r} \) changes sign under inversion, its derivative with respect to \( \theta \) remains unchanged.
- Therefore, \( \hat{\theta} \) has even parity.
- The azimuthal unit vector \( \hat{\phi} \) is defined as:
\[
\hat{\phi} = \frac{1}{\sin\theta} \frac{\partial \hat{r}}{\partial \phi}
\]
- Since \( \hat{r} \) changes sign under inversion, its derivative with respect to \( \phi \) also changes sign.
- Hence, \( \hat{\phi} \) has odd parity.