Understanding cell biology greatly benefits from the development of advanced diagnostic probes. Here we introduce a 22-nm spaser (plasmonic nanolaser) with the ability to serve as a super-bright, water-soluble, biocompatible probe capable of generating stimulated emission directly inside living cells and animal tissues. We have demonstrated a lasing regime associated with the formation of a dynamic vapour nanobubble around the spaser that leads to giant spasing with emission intensity and spectral width >100 times brighter and 30-fold narrower, respectively, than for quantum dots. The absorption losses in the spaser enhance its multifunctionality, allowing for nanobubble-amplified photothermal and photoacoustic imaging and therapy. Furthermore, the silica spaser surface has been covalently functionalized with folic acid for molecular targeting of cancer cells. All these properties make a nanobubble spaser a promising multimodal, super-contrast, ultrafast cellular probe with a single-pulse nanosecond excitation for a variety of in vitro and in vivo biomedical applications.
Plasmonic nanolasers
(spasers) are of intense interest, attributable
to their ability to generate a high-intensity coherent radiation.
We infiltrated a three-dimensional silica-based photonic crystal (PhC)
film with spasers, composed of spherical gold cores, surrounded by
silica shells with dye molecules. In spasers, the gold nanospheres
supported the surface plasmons and the dye molecules transferred incoming
optical energy to the surface plasmons. Our experiments show that
such a structure, consisting of a PhC, which acts as an external distributed
feedback resonator, and spasers, can serve as a coherent source of
electromagnetic radiation. Spasers were locked in phase by the common
radiation causing a phenomenon called the lasing spaser: the emission
of spatially and temporarily coherent light normal to the surface
of the PhC film. The far-field radiation patterns appeared in the
shape of the Star-of-David, which is due to the dispersion along the
Brillouin zone boundary. The infiltration of the spasers into the
PhC led to drastic narrowing of the emission peak and an 80-fold decrease
in the spaser generation threshold with respect to the same spasers
in a suspension at room temperature.
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