Coherent nanoscale photon sources are of paramount importance to achieving all-optical communication. Several nanolasers smaller than the diffraction limit have been theoretically proposed and experimentally demonstrated using plasmonic cavities to confine optical fields. Such compact cavities exhibit large Purcell factors, thereby enhancing spontaneous emission, which feeds into the lasing mode. However, most plasmonic nanolasers reported so far have employed resonant nanostructures and therefore had the lasing restricted to the proximity of the resonance wavelength. Here, we report on an approach based on gold nanorod hyperbolic metamaterials for lasing. Hyperbolic metamaterials provide broadband Purcell enhancement due to large photonic density of optical states, while also supporting surface plasmon modes to deliver optical feedback for lasing due to nonlocal effects in nanorod media. We experimentally demonstrate the advantage of hyperbolic metamaterials in achieving lasing action by its comparison with that obtained in a metamaterial with elliptic dispersion. The conclusions from the experimental results are supported 2 with numerical simulations comparing the Purcell factors and surface plasmon modes for the metamaterials with different dispersions. We show that although the metamaterials of both types support lasing, emission with hyperbolic samples is about twice as strong with 35% lower threshold vs. the elliptic ones. Hence, hyperbolic metamaterials can serve as a convenient platform of choice for nanoscale coherent photon sources in a broad wavelength range.
TOC GraphicWe study lasing in two gold nanorod arrays coated with Rhodamine 101, one exhibiting hyperbolic dispersion at the lasing wavelength, the other with elliptic dispersion. Experiments show the hyperbolic metamaterial provides stronger emission with reduced threshold.
3Since its invention in 1960 1 , the laser has seen tremendous developments and has quickly revolutionized fundamental and applied fields such as metrology, medicine, data storage, fabrication and telecommunications among others 2 . With the ever growing need for data transfer speeds and compact devices, several efforts have been made in miniaturizing the laser for on-chip integration 3-7 . While photonic cavities have proven to exhibit high-Q factors enabling strong lasing, their miniaturization to the nanoscale is not viable since the diffraction limit requires the cavity length to be at least half the lasing wavelength [8][9][10] . In contrast, plasmonic cavities, which can be employed to achieve optical amplification and lasing action with charge oscillations, have successfully led to the design of coherent photon sources no longer limited by the diffraction limit 10 . Coupling of emitters with the strongly confined electromagnetic fields associated with plasmonic oscillations can significantly enhance spontaneous emission in certain modes, a process known as the Purcell effect 11 . This effect yields a redistribution of spontaneous emission over wavevector space ...