“…The decay rate of such an emitter located in the gap is modified due to two competitive processes: transfer of the energy from the emitter to the nanoparticle (observed exclusively for lossy nanoparticles) 32,43 and the coupling of the field originated by the emitter to the outgoing radiation. 44,45 The resulting modification of the emitter's decay rate, known as the Purcell effect, 33,34,46 has been extensively studied and applied to designing efficient nanoantennas for single photon emission, 31 enhancement of the fluorescence intensity, 32,47,48 and emission directivity. 45 Here, we consider our silicon dimer system as a near-IR antenna and compare its efficiency to that of a plasmonic dimer.…”