We demonstrate temporal coherent control in two-photon transitions. A pair of broadband ( $\mathrm{\Delta }\lambda \sim 20\mathrm{nm}$ ), ultrashort ( $\mathrm{\Delta }t\sim 100\mathrm{fs}$ ), collinear pulses with a variable time delay excites the rubidium atoms into the $5\mathrm{D}$ state from the $5\mathrm{S}$ ground state where the two-photon transitions are enhanced by the intermediate level $5\mathrm{P}$ . The excited atoms radiate $5\mathrm{\mu m}$ ( $5\mathrm{D}–6\mathrm{P}$ ) and $420\mathrm{nm}$ ( $6\mathrm{P}–5\mathrm{S}$ ) light. As a result of tuning the wavelength of the input laser, a superfluorescence at $420\mathrm{nm}$ exhibits different temporal behaviors. A switching from a beating at the frequency given by the difference between the sequential atomic transitions that involve the $5{\mathrm{P}}_{3/2}$ intermediate level, to a quantum beating due to two different two-photon excitation paths, $5\mathrm{S}\to 5{\mathrm{P}}_{1/2}\to 5\mathrm{D}$ and $5\mathrm{S}\to 5{\mathrm{P}}_{3/2}\to 5\mathrm{D}$ is observed. Based on the simple atom-field interaction theory, an analytic solution, which qualitatively elucidates experimental results, is obtained.