When \(\psi_A\) and \( \psi_A \) are the wave functions of atomic orbitals, then \( \sigma^{*} \) is represented by:
\( \psi_{A} + \psi_{B} \)
\( \psi_{A} - 2 \psi_{B} \)
\( \psi_{A} + 2 \psi_{B} \)
\( \psi_{A} - \psi_{B} \)