The ground state of \({ }_{82}^{207} \mathrm{~Pb}\) nucleus has spin-parity \(J^\pi=\left(\frac{1}{2}\right)^-\), while the first excited state has \(J^\pi=\left(\frac{5}{2}\right)^{-}\). For the transition from the first excited state to the ground state, possible multipolarities of emitted electromagnetic radiation are