The D+G peak, unlike the 2D peak, needs to be activated by a defect scattering site in order to provide momentum conservation in the Raman scattering process. Whenever a high wavevector phonon is emitted during the Raman process, there will be quasi-momentum missmatch among the hole in the valence band and the excited electron in the conduction band. This prevents radiative recombination unless a scattering site provides elastic scattering to bridge the missmatch. The pure D-band is the most simple example for this - however, as the phonon responsible for the G-band has very little wavevector (its a so-called zone-center or Gamma-point phonon) and hence is recorded without the presence of a defect, the D+G-band will also need a defect for activation. The appearance of the 2D-band at the double frequency of the D-band is a little different in this respect, as it will not require a defect for action - it just uses the same phonon twice to move the electron as well as the hole through the Brillouin-zone and hence there will be no more missmatch (you could also say the electron gets shuttled forward and backward using the same phonon twice).