Abstract:The tailored spatial
polarization of coherent light beams is important
for applications ranging from microscopy to biophysics to quantum
optics. Miniaturized light sources are needed for integrated, on-chip
photonic devices with desired vector beams; however, this issue is
unresolved because most lasers rely on bulky optical elements to achieve
such polarization control. Here, we report on quantum dot-plasmon
lasers with engineered polarization patterns controllable by near-field
coupling of colloidal quantum … Show more
“…A QD–plasmon laser with controlled polarization patterns was demonstrated with a Ag NP lattice covered with a layer of CdSe/CdS core–shell QDs (Figure 12d ). [ 120 ] Here, a waveguiding stack formed by the silica substrate, the QD layer and air was considered, and accordingly, waveguide‐surface lattice resonance (W TM ‐SLR or W TE ‐SLR) is formed through hybridization of the surface plasmons with the transverse electric (TE) or TM waveguide modes. When the PL emission of the QDs matches well with the W‐SLR modes, lasing occurs (Figure 12e ), and it can be selected to be radially polarized or azimuthally polarized by varying the thickness of the QD layer and the polarization of the excited light.…”
“…d) Schematic of QD-plasmon laser consisting of Ag NP lattice coating QD layer on top with varied thicknesses and the corresponding far-field emission beams in radical or azimuthal polarization. e) Lasing (red) observed where the QD PL spectrum (blue) overlapped with the hybrid waveguide-surface lattice resonance (W-SLR) of the composite structure (black).d,e) Adapted with permission [120]. Copyright 2020, American Chemical Society.…”
Colloidal quantum dot (QD), a solution-processable nanoscale optoelectronic building block with well-controlled light absorption and emission properties, has emerged as a promising material system capable of interacting with various photonic structures. Integrated QD/photonic structures have been successfully realized in many optical and optoelectronic devices, enabling enhanced performance and/or new functionalities. In this review, the recent advances in this research area are summarized. In particular, the use of four typical photonic structures, namely, diffraction gratings, resonance cavities, plasmonic structures, and photonic crystals, in modulating the light absorption (e.g., for solar cells and photodetectors) or light emission (e.g., for color converters, lasers, and light emitting diodes) properties of QD-based devices is discussed. A brief overview of QD-based passive devices for on-chip photonic circuit integration is also presented to provide a holistic view on future opportunities for QD/photonic structure-integrated optoelectronic systems.
“…A QD–plasmon laser with controlled polarization patterns was demonstrated with a Ag NP lattice covered with a layer of CdSe/CdS core–shell QDs (Figure 12d ). [ 120 ] Here, a waveguiding stack formed by the silica substrate, the QD layer and air was considered, and accordingly, waveguide‐surface lattice resonance (W TM ‐SLR or W TE ‐SLR) is formed through hybridization of the surface plasmons with the transverse electric (TE) or TM waveguide modes. When the PL emission of the QDs matches well with the W‐SLR modes, lasing occurs (Figure 12e ), and it can be selected to be radially polarized or azimuthally polarized by varying the thickness of the QD layer and the polarization of the excited light.…”
“…d) Schematic of QD-plasmon laser consisting of Ag NP lattice coating QD layer on top with varied thicknesses and the corresponding far-field emission beams in radical or azimuthal polarization. e) Lasing (red) observed where the QD PL spectrum (blue) overlapped with the hybrid waveguide-surface lattice resonance (W-SLR) of the composite structure (black).d,e) Adapted with permission [120]. Copyright 2020, American Chemical Society.…”
Colloidal quantum dot (QD), a solution-processable nanoscale optoelectronic building block with well-controlled light absorption and emission properties, has emerged as a promising material system capable of interacting with various photonic structures. Integrated QD/photonic structures have been successfully realized in many optical and optoelectronic devices, enabling enhanced performance and/or new functionalities. In this review, the recent advances in this research area are summarized. In particular, the use of four typical photonic structures, namely, diffraction gratings, resonance cavities, plasmonic structures, and photonic crystals, in modulating the light absorption (e.g., for solar cells and photodetectors) or light emission (e.g., for color converters, lasers, and light emitting diodes) properties of QD-based devices is discussed. A brief overview of QD-based passive devices for on-chip photonic circuit integration is also presented to provide a holistic view on future opportunities for QD/photonic structure-integrated optoelectronic systems.
“…[ 5 ] Then further demonstrations were reported including semiconductor‐based plasmonic nanocavities, [ 6–11 ] metal‐cladding nanoresonators, [ 12–14 ] and lattice plasmon resonances. [ 15–18 ] Among these plasmonic nanolasers, the semiconductor nanowire (NW)‐based plasmonic lasers, [ 8–11,19,20 ] which support a plasmonic‐waveguide mode propagating along the NW axis, have attracted a high level of interest due to their potential benefits in on‐chip integration and optical signal propagation. [ 21,22 ]…”
Plasmonic nanolasers provide a valuable opportunity for expanding sub‐wavelength applications. Due to the potential of on‐chip integration, semiconductor nanowire (NW)‐based plasmonic nanolasers that support the waveguide mode attract a high level of interest. To date, perovskite quantum dots (QDs) based plasmonic lasers, especially nanolasers that support plasmonic‐waveguide mode, are still a challenge and remain unexplored. Here, metallic NW coupled CsPbBr3 QDs plasmonic‐waveguide lasers are reported. By embedding Ag NWs in QDs film, an evolution from amplified spontaneous emission with a full width at half maximum (FWHM) of 6.6 nm to localized surface plasmon resonance (LSPR) supported random lasing is observed. When the pump light is focused on a single Ag NW, a QD‐NW coupled plasmonic‐waveguide laser with a much narrower emission peak (FWHM = 0.4 nm) is realized on a single Ag NW with the uniform polyvinylpyrrolidone layer. The QDs serve as the gain medium while the Ag NW serves as a resonant cavity and propagating plasmonic lasing modes. Furthermore, by pumping two Ag NWs with different directions, a dual‐wavelength lasing switch is realized. The demonstration of metallic NW coupled QDs plasmonic nanolaser would provide an alternative approach for ultrasmall light sources as well as fundamental studies of light matter interactions.
“…Vector beams are optical modes with a spatially inhomogeneous field structure. Cylindrical vector beams, for example, are characterized by polarization singularities that can be produced with birefringent crystals, polarizing prisms, or nanostructured media [1,2]. These elements are either directly integrated within a laser cavity or used as external passive elements in free space.…”
Harnessing the spontaneous emission of incoherent quantum emitters is one of the hallmarks of nano-optics. Yet, an enduring challenge remains-making them emit vector beams, which are complex forms of light associated with fruitful developments in fluorescence imaging, optical trapping and high-speed telecommunications. Vector beams are characterized by spatially varying polarization states whose construction requires coherence properties that are typically possessed by lasers-but not by photons produced by spontaneous emission. Here, we show a route to weave the spontaneous emission of an ensemble of colloidal quantum dots into vector beams. To this end, we use holographic nanostructures that impart the necessary spatial coherence, polarization and topological properties to the light originating from the emitters. We focus our demonstration on vector vortex beams, which are chiral vector beams carrying non-zero orbital angular momentum, and argue that our approach can be extended to other forms of vectorial light.
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