The vector $\mathrm{H}$ in the far field of an antenna satisfies
- $\nabla \cdot \overrightarrow{\mathrm{H}}=0$ and $\nabla \times \overrightarrow{\mathrm{H}}=0$
- $\nabla \cdot \overrightarrow{\mathrm{H}} \neq 0$ and $\nabla \times \overrightarrow{\mathrm{H}} \neq 0$
- $\nabla \cdot \vec{\text{H}}=0$ and $\nabla \times \vec{\text{H}} \neq 0$
- $\nabla \cdot \overrightarrow{\mathrm{H}} \neq 0$ and $\nabla \times \overrightarrow{\mathrm{H}}=0$