The advent of novel lithographic techniques enabling the shaping of noble metals at the nanoscale is offering unprecedented opportunities for generating and manipulating light within subwavelength regions [1][2][3] . In recent years, the development of functional nanoscale elements such as plasmonic antennas, transducers between free radiation and localized energy [4,5] , has led to major advances in various research fields including single molecule detection [6][7][8] , directive nanosources of light [9][10][11] , vibrational spectroscopy [12][13][14] and nonlinear interactions at the nanoscale [15][16][17] . For the latter, while the enhanced local fields created by plasmonic structures can be exploited for upconverting light at the nanoscale and for ultrafast processing of optical signals [18][19] , their opacity prevents exploiting phase matching in order to reach high nonlinear emission, which severely limits their practical use. Therefore, the development of nanoscale devices exhibiting stronger nonlinear responses is highly required for proposing future efficient integrated nanophotonic components.One promising strategy for reaching higher nonlinear nanoscale responses is related to the integration of an active nonlinear medium in the near field of a plasmonic structure. Indeed, while most works in nonlinear nanophotonics have focused on intrinsic responses from pure