quantum yields (PLQY), and wide tunability, combined with low material costs. [10,11] In which case the identification of an appropriate metal NIR plasmonic nanostructure is the next challenge, with only some complex gold nanostructures, such as tetrapods, [12] nanorods, [13] nanocages, [14] nanostars, [15] and faceted gold nanoparticles [16] can be cited. However, their plasmonic resonance bands are still limited in their tunable range to no longer than 1.0 µm and in addition their commercial manufacturing is highly costly. More recently, semiconductor nanocrystals with plasmonic features have attracted much attention, [17][18][19][20] with one particular example, copper deficient copper chalcogenides, [21][22][23][24][25][26][27] offering tunable plasmonic bands covering a wide range of the NIR. Plasmonic resonance in such semiconductor plasmonic nanocrystals (PNCs) arises from the excess of free holes and can be easily and reversibly tuned throughout the entire NIR spectral range. Although it is expected that near-field enhancement of optical responses by such PNCs will be less effective as compared to the noble metals in the visible range due to the smaller number of free carriers, [18] there are a few encouraging reports for PNC enhanced Raman scattering [28] and upconversion visible emission. [29] Despite the huge potential of plasmonic enhancement of NIR optical responses, especially NIR absorption and photoluminescence (PL), this topic has not been studied as of yet, with copper chalcogenides PNCs considered mostly for thermal therapy. [18,20] To realize a miniature NIR emitter which exploits plasmonic enhancement of radiation, an appropriate matrix must be selected. Such a matrix must provide optical transparency and high loading of nanoscale emitters. Importantly, the emitters and PNCs should be separated from each other to prevent PL quenching by means of nonradiative energy transfer. [1,30] At the same time, the distance between the emitter and PNC should be short enough (≈5-20 nm) to provide an effective enhancement. [1] The nanoporous silicate matrix (NSM) can satisfy these demands. [31,32] Its porous structure provides the separation between embedded QDs and PNCs, while high porosity allows the high loading of the nanoparticles.Nowadays PbS QDs are considered as a promising material for NIR photovoltaic and light-emitting devices. [33][34][35][36][37] However, the efficiency of the PbS QD light emitters is still far behind that for visible QDLEDs. [38,39] Here we report high (up to ≈20 times Strong enhancement of near-infrared (NIR) emission of lead sulfide quantum dots (QDs) induced by Cu 2−x Se semiconductor plasmonic nanocrystals (PNCs), both embedded into nanoporous silicate matrix is reported. The emission enhancement comes from resonant interaction of QD optical transition dipole with the near field of plasmons of semiconductor PNCs. Possible mechanisms of QD photoluminescence broadening and shift, including Rabi splitting and trap-state-related photoluminescence enhancement, are considered. ...