We present a theoretical framework that accounts for the new D J and D sJ mesons measured in the open-charm sector. These resonances are properly described if considered as a mixture of conventional P −wave quark-antiquark states and four-quark components. The narrowest states are basically P −wave quark-antiquark mesons, while the dominantly four-quark states are shifted above the corresponding two-meson threshold, being broad resonances. We study the electromagnetic decay widths as basic tools to scrutiny their nature. The proposed explanation incorporates in a natural way the most recently discovered mesons in charmonium spectroscopy.