Subwavelength Demagnification Imaging and Lithography Using Hyperlens with a Plasmonic Reflector Layer

Unlike the case in magnification mode, it is found that hyperlens employed in demagnification and lithography manner encounters great degradation of imaging quality especially for high-resolution image features. This problem mainly arises from the transversal magnetic polarization feature of light which delivers reduced contrast of electronic components intensity profile at the imaging region. Hyperlens with plasmonic reflector layer is designed for subwavelength demagnification imaging and photolithography. Analytical equations and numerical simulations show amplification of reflected evanescent waves in photoresist sandwiched by hyperlens and plasmonic reflectors in cylindrical geometry. The image quality features including resolution, contrast, and intensity can be improved significantly. Also presented are the dependence and influence of geometry parameters on imaging quality. Numerical demonstrations are given with about 15 nm half-pitch resolution imaging at illuminating wavelength of 365 nm.     

Subwavelength-Sized Plasmonic Structures for Wide-Field Optical Microscopic Imaging with Super-Resolution

We propose a wide-field super-resolved optical microscopic imaging technique based on subwavelength slit arrays embedded in a thin silver film to generate surface plasmon (SP) standing wave interference patterns. These fringes carrying high spatial frequency information serve as excitation profiles to excite the nanoscale fluorescence objects. The super-resolved fluorescence density distribution is reconstructed from a weight sum of a series of fluorescence images with differently phase-shifted SP standing wave illumination. Simulation and experimental results show that the lateral resolution of the reconstructed fluorescence density image is enhanced by 0.28?λ _SP in two dimensions, which is twofold better than that of conventional high numerical aperture fluorescence microscopy. This technique benefits from a grating coupler to offer a simple way for the generation and phase shift of SP standing wave excitation profiles in two dimensions. The flat configuration, wide field, and noninvasive nature make this approach suitable for real-time analyzing the fine details of bio-samples in biochip applications.     

Far-Field Focusing of Spiral Plasmonic Lens

In this paper, we study the nanoscale-focusing effect in the far field for a spiral plasmonic lens with a concentric annular groove by using finite-difference time domain simulation. The simulation result demonstrates that a left-hand spiral plasmonic lens can concentrate an incident right-hand circular polarization light into a focal spot at the exit surface. And this spot can be focused into far field due to constructive interference of the scattered light by the annular groove. The focal length and the focal depth can be adjusted by changing the groove radius and number of grooves within a certain range. These properties make it possible to probe the signal of spiral plasmonic lens in far field by using conventional optical devices.     

Design of a Structured Bulk Plasmon Illumination Source for Enhancing Plasmonic Cavity Superlens Imaging

Plasmonics - A structured bulk plasmon illumination (BPI) source is designed for achieving a uniform high spatial frequency illumination field. By employing the hyperbolic metamaterial (HMM)...     

Near- and Far-Field Plasmonic Properties of Different Types of Eccentric Core-Shell Nanodimers

Finite element method (FEM) simulations have been carried out on free-standing and finite dielectric substrate-supported eccentric (i) silica core-gold nanoshell dimers and (ii) gold core-silica nanoshell dimers for understanding their near- and far-field plasmonic properties. In the case of eccentric silica core-gold nanoshell dimers, multiple peaks are observed in the near- and far-field spectra due to the plasmon hybridization. The number of peaks is found to be sensitive to the core offset parameters of the nanoshells forming nanodimer. The wavelength locations of the peaks due to the constructive coupling of the lower order modes found relatively more sensitive to the dielectric substrate. The number of peaks in the near- and far-field spectra found the same presence and absence of the dielectric substrate. The values of full width at half maximum (FWHM) of the peaks observed in the near-field spectra are found larger as compared to those observed in the far-field spectra. In contrast, in the case of eccentric gold core-silica nanoshell dimers, multiple peaks have not been observed. The FWHM of the observed peak is found sensitive to the core offset parameters of the nanoshells, and the number of peaks in the near field- and far-field spectra found not same in the presence and absence of the dielectric substrate. Moreover, the differences in near- and far-field spectra of plasmonically coupled (i) concentric nanoshells, (ii) eccentric nanoshells, and (iii) concentric and eccentric nanoshells also investigated numerically.

     

Design of Broadband Infrared Photodetectors Enhanced by Dual-Mode Plasmonic Resonant Cavities

Plasmonics - The signal-to-noise ratio of infrared photodetectors can be improved by using resonant cavities, whereas the enhancement effect usually occurs in a narrow wavelength range. Here, we...     

Super-Resolution Long-Depth Focusing by Radially Polarized Light Irradiation Through Plasmonic Lens in Optical Meso-field

In this paper, we propose a novel plasmonic lens design consisting of an annular slit and concentric grooves. The simulation results show that under radially polarized illumination, a super-resolution long depth of focus (DOF) spot can be achieved in optical meso-field due to the constructive interference of scattered light by the concentric grooves. We also analyze the influence of depth-tuned annular grooves on focusing performance, including focal length, DOF, and full-width half-maximum. Moreover, focusing efficiency can be enhanced (～350 %) by introducing a circular metallic grating which surrounds the annular slit. This plasmonic lens has potential applications in nano-imaging and nano-photolithography.     

Broadband Mid-Infrared Super-Resolution Imaging with Metallic Nanorod-Bridged Dimer Array

We propose a broadband mid-infrared super-resolution imaging system comprising a metallic nanorod-bridged dimer array. The imaging array enables super-resolution imaging of shaped dipole sources in the near field. A charge transfer plasmon (CTP) appears in a metallic nanorod-bridged dimer. By varying the radius of the junction, the plasmon resonance wavelength of CTP mode can be tuned into the mid-infrared region. Here, we investigate the broadband super-resolution imaging of the incoherent and coherent dipole sources at mid-infrared wavelengths. With the array pitch varying, we calculate the cross-sectional field intensity distributions at the source plane and the image plane by using the finite element method. The simulation results indicate that the broadband incoherent and coherent super-resolution imaging can be realized at mid-infrared wavelengths with the imaging array. The image quality is sensitively dependent on the source coherent, the array pitch, and the distance from the image plane to the array. In the same structural parameters, the image quality of coherent source of in-phase is lower than that of incoherent source. Increasing the array pitch improves the image quality but it also increases the size of the array. By reasonably choosing the array pitch of the array, the spatial resolution of ～λ/109 and ～λ/73 is obtained corresponding to the incoherent imaging case and coherent imaging case at the mid-infrared wavelength of 4390 nm. Moreover, the larger image-array distance results in the lower image quality.     

Resonant Broadband Field Enhancement in Cylindrical Plasmonic Structure Surrounded by Perovskite Environment

We demonstrate the optical response of metal nanoparticles and their interaction with organic-inorganic perovskite (methyl ammonia lead halide (CH₃NH₃PbI₃)) environment using discrete dipole approximation (DDA) simulation technique. Important optical properties like absorption, scattering, and electric field calculations for metal nanoparticle using different geometry have been analyzed. The metal nanoparticles embedded in the perovskite media strongly support surface plasmon resonances (SPRs). The plasmonic interaction of metal nanoparticles with perovskite matrix is a strong function of MNP’s shape, size, and surrounding environment that can manipulate the optical properties considerably. The cylindrical shape of MNPs embedded in perovskite environment supports the SPR which is highly tunable to subwavelength range of 400–800 nm. Wide range of particle sizes has been selected for Ag, Au, and Al spherical and cylindrical nanostructures surrounded by perovskite matrix for simulation. The chosen hybrid material and anisotropy of structure together make a complex function for resonance shape and width. Among all MNPs, 70-nm spherical silver nanoparticle (NP) and cylindrical Ag NP having diameter of 50 nm and length of 70 nm (aspect ratio 1.4) generate strong electric field intensity that facilitates increased photon absorption. The plasmonic perovskite interaction plays an important role to improve the absorption of photon inside the thin film perovskite environment that may be applicable to photovoltaics and photonics.

     

Scanning Super-Resolution Imaging in Enclosed Environment by Laser Tweezer Controlled Superlens

Super-resolution imaging using microspheres has attracted tremendous scientific attention recently because it has managed to overcome the diffraction limit and allowed direct optical imaging of structures below 100 nm without the aid of fluorescent microscopy. To allow imaging of specific areas on the surface of samples, the migration of the microspheres to specific locations on two-dimensional planes should be controlled to be as precise as possible. The common approach involves the attachment of microspheres on the tip of a probe. However, this technology requires additional space for the probe and could not work in an enclosed environment, e.g., in a microfluidic enclosure, thereby reducing the range of potential applications for microlens-based super-resolution imaging. Herein, we explore the use of laser trapping to manipulate microspheres to achieve super-resolution imaging in an enclosed microfluidic environment. We have demonstrated that polystyrene microsphere lenses could be manipulated to move along designated routes to image features that are smaller than the optical diffraction limit. For example, a silver nanowire with a diameter of 90 nm could be identified and imaged. In addition, a mosaic image could be constructed by fusing a sequence of images of a sample in an enclosed environment. Moreover, we have shown that it is possible to image Escherichia coli bacteria attached on the surface of an enclosed microfluidic device with this method. This technology is expected to provide additional super-resolution imaging opportunities in enclosed environments, including microfluidic, lab-on-a-chip, and organ-on-a-chip devices.     

Super-Resolution Imaging of Bacteria in a Microfluidics Device

Bacteria have evolved complex, highly-coordinated, multi-component cellular engines to achieve high degrees of efficiency, accuracy, adaptability, and redundancy. Super-resolution fluorescence microscopy methods are ideally suited to investigate the internal composition, architecture, and dynamics of molecular machines and large cellular complexes. These techniques require the long-term stability of samples, high signal-to-noise-ratios, low chromatic aberrations and surface flatness, conditions difficult to meet with traditional immobilization methods. We present a method in which cells are functionalized to a microfluidics device and fluorophores are injected and imaged sequentially. This method has several advantages, as it permits the long-term immobilization of cells and proper correction of drift, avoids chromatic aberrations caused by the use of different filter sets, and allows for the flat immobilization of cells on the surface. In addition, we show that different surface chemistries can be used to image bacteria at different time-scales, and we introduce an automated cell detection and image analysis procedure that can be used to obtain cell-to-cell, single-molecule localization and dynamic heterogeneity as well as average properties at the super-resolution level.     

Improving Imaging Contrast of Non-Contacted Plasmonic Lens by Off-Axis Illumination with High Numerical Aperture

Off-axis illumination plasmonic lens (OAIPL) is proposed and demonstrated to improve the imaging contrast in non-contacted application manner. The spatial Fourier components of light transmitted through the nano-patterns are greatly enhanced in the imaging process by shifting the wave vectors with high numerical aperture off-axis illumination. On the other hand, a reflector in the image area helps to tailor the ratio between electric field components in the tangential and normal directions. These two effects resultantly deliver significant improvement of imaging performance, including enhanced resolution, imaging contrast, and elongation of air gap thickness. In comparison to the case of normal illumination, the air gap thickness for 30 and 60 nm half-pitch resolution is extended to 25 and 100 nm by OAIPL with numerical aperture (NA)?=?1.55, respectively.     

Far-Field Raman Imaging of Short-Wavelength Particle Plasmons on Gold Nanorods

The surface plasmon fields of gold nanorods with a diameter of 100 nm and lengths of 1–5 m are imaged by using far-field Raman scattering of methylene blue adsorbed on the rods. When optically exciting the nanorods under total internal reflection with wave vector and electric field vector orientations along the rod axis, the plasmon field intensity along this axis is observed to be periodically modulated. This modulation is attributable to a beating of the exciting light wave and the nanorod plasmon mode. The plasmon wavelength deduced from the beat frequency is 379 nm, which is considerably smaller than the exciting laser wavelength of 647 nm. In general, Raman imaging is shown to be a powerful technique to probe local plasmon fields using far-field spectroscopy.     

Super-Resolution Imaging of Plasmodesmata Using Three-Dimensional Structured Illumination Microscopy

We used three-dimensional structured illumination microscopy (3D-SIM) to obtain subdiffraction (“super-resolution”) images of plasmodesmata (PD) expressing a green fluorescent protein-tagged viral movement protein (MP) in tobacco (Nicotiana tabacum). In leaf parenchyma cells, we were able to resolve individual components of PD (neck and central cavities) at twice the resolution of a confocal microscope. Within the phloem, MP-green fluorescent protein filaments extended outward from the specialized pore-PD that connect sieve elements (SEs) with their companion cells (CCs) along the tubular sieve element reticulum (SER). The SER was shown to interconnect individual pore-PD at the SE-CC interface. 3D-SIM resolved fine (less than 100 nm) endoplasmic reticulum threads running into individual pore-PD as well as strands that crossed sieve plate pores, structurally linking SEs within a file. Our data reveal that MP entering the SE from the CC may remain associated with the SER. Fluorescence recovery after photobleaching experiments revealed that this MP pool is relatively immobile compared with the membrane probe 3,3’-dihexyloxacarbocyanine iodide, suggesting that MP may become sequestered by the SER once it has entered the SE. The advent of 3D-SIM offers considerable potential in the subdiffraction imaging of plant cells, bridging an important gap between confocal and electron microscopy.Fluorescence-based imaging has revolutionized cell biology, allowing the localization of proteins to specific cells and organelles (Shaner et al., 2007; Frigault et al., 2009). However, conventional fluorescence microscopy is limited by the diffraction of light to approximately 200 nm in the lateral (x-y) plane and to about 500 nm in the axial (z) plane (Fernandez-Suarez and Ting, 2008; Huang et al., 2009). This is because light traveling through a lens cannot be focused to a point, only to an airy disc with a diameter of about half the wavelength of the visible emitted light (Huang et al., 2009). Confocal laser scanning microscopy has produced improvements in axial resolution due to the removal of out-of-focus flare, but it is also limited by diffraction (Huang et al., 2009). Thus, objects closer than about 200 nm cannot be resolved but appear merged into one. Many subcellular structures of interest to cell biologists lie below this resolution limit and have remained below the diffraction barrier. Such structures can be seen but not resolved.Recently, major innovations in biological imaging have broken the diffraction barrier. These include photoactivation localization microscopy (PALM) and stimulated emission and depletion (STED; for review, see Fernandez-Suarez and Ting, 2008; Huang et al., 2009). Most subdiffraction or “super-resolution” approaches have improved resolution in either the lateral (x-y) plane or the axial (z) plane, but usually not both (Schermelleh et al., 2008). Many of the structures of interest within plant cells lie some distance from the cell wall, posing problems for some super-resolution approaches (e.g. PALM) where the subject of interest must lie close to the coverslip (Huang et al., 2009). Recently, Schermelleh et al. (2008) described a subdiffraction multicolor imaging protocol using three-dimensional structured illumination microscopy (3D-SIM). In this method, objects beyond the diffraction limit are illuminated with multiple interfering beams of light transmitted through a series of diffraction gratings, producing a resolution of 100 nm in x-y and 200 nm in z (Schermelleh et al., 2008; Huang et al., 2009). These substantial increases in resolution are significant for plant cell imaging. The thickness of the plant cell wall is typically in the region of about 700 nm, allowing limited optical sectioning capacity with a confocal microscope (about 500 nm in z). A further advantage of 3D-SIM is that it permits the imaging of conventional fluorescent reporters and dyes that are compatible with confocal imaging, allowing a direct correlation of 3D-SIM and confocal images (Schermelleh et al., 2008).The phloem of higher plants is a major conduit for the long-distance transport of solutes (Oparka and Turgeon, 1999) and also functions as a “superhighway” for macromolecular trafficking (Lucas and Lee, 2004; Kehr and Buhtz, 2008; Lee and Cui, 2009). However, the phloem is difficult to image with conventional optical microscopy (Knoblauch and van Bel, 1998; Oparka and Turgeon, 1999; van Bel et al., 2002). Sieve elements (SEs), the conducting cells of the phloem, are enucleate yet contain a plethora of proteins and RNAs associated with long-distance signaling and defense (van Bel and Gaupels, 2004; Lee and Cui, 2009). Many of these macromolecules are synthesized in the companion cell (CC) and passed into the SE via the specialized pore-plasmodesmata (PD) that connect the two cell types (Oparka and Turgeon, 1999; van Bel et al., 2002). Pore-PD have been suggested to be a major “lifeline” from CC to SE (van Bel et al., 2002), but the exact nature of this pathway remains unresolved.Our current understanding of PD substructure is derived largely from electron microscope studies (Roberts, 2005). Such methods are time-consuming and do not permit facile protein localization within PD. Recent proteomics approaches have been successful in identifying new proteins associated with PD (Maule, 2008). Localization of these proteins with confocal microscopy results in the appearance of discrete punctae at the cell wall, consistent with the location of pit fields (Faulkner et al., 2008), but does not pinpoint specific protein locations within PD. In general, there is a growing gap between proteomics studies of plant organelles, including PD, and the ability to ascribe accurate addresses to these proteins (Millar et al., 2009; Moore and Murphy, 2009). The advent of 3D-SIM prompted us to explore the potential of subdiffraction imaging in plant cells, with a view to obtaining improved florescence resolution of PD. We used 3D-SIM to examine PD in a transgenic tobacco (Nicotiana tabacum) line expressing the viral movement protein (MP) of Tobacco mosaic virus (TMV) fused to GFP. Using a specific antibody to callose, a wall constituent located at the PD collar, we were able to resolve clearly the structure of single, simple PD in epidermal cells at 100-nm resolution, discriminating between the neck region of the pore and the central cavity to which it connects (Roberts and Oparka, 2003; Faulkner et al., 2008). 3D-SIM also revealed details of the central cavities of complex PD seen previously only with the electron microscope (Ding et al., 1992; Ehlers and Kollmann, 2001; Faulkner et al., 2008).Using 3D-SIM, we were able to image PD sequentially from the epidermis to the phloem within vascular bundles, producing unparalleled images of sieve plate pores and the specialized pore-PD that connect SEs with their CCs. In the SEs, MP was no longer restricted to the central cavities of PD but became distributed along the SE parietal layer, connecting all the pore-PD along the SE-CC interface. We were able to detect fine threads of MP-GFP that extended for up to 40 μm along the SE and also crossed individual sieve plate pores. Fluorescence recovery after photobleaching (FRAP) experiments revealed that this MP-GFP pool was relatively immobile within the SE parietal layer, suggesting that the SE may sequester TMV MP on or within the sieve element reticulum (SER).Our data reveal that 3D-SIM is especially suited to the subdiffraction imaging of plant cells and yields spatial information not previously possible with conventional fluorescence-based imaging. The unique optical sectioning capacity of 3D-SIM and the ability to produce multicolor imaging with conventional fluorophores offer enormous potential in plant cell biology.     

Super-Resolution Imaging of ESCRT-Proteins at HIV-1 Assembly Sites

The cellular endosomal sorting complex required for transport (ESCRT) machinery is involved in membrane budding processes, such as multivesicular biogenesis and cytokinesis. In HIV-infected cells, HIV-1 hijacks the ESCRT machinery to drive HIV release. Early in the HIV-1 assembly process, the ESCRT-I protein Tsg101 and the ESCRT-related protein ALIX are recruited to the assembly site. Further downstream, components such as the ESCRT-III proteins CHMP4 and CHMP2 form transient membrane associated lattices, which are involved in virus-host membrane fission. Although various geometries of ESCRT-III assemblies could be observed, the actual membrane constriction and fission mechanism is not fully understood. Fission might be driven from inside the HIV-1 budding neck by narrowing the membranes from the outside by larger lattices surrounding the neck, or from within the bud. Here, we use super-resolution fluorescence microscopy to elucidate the size and structure of the ESCRT components Tsg101, ALIX, CHMP4B and CHMP2A during HIV-1 budding below the diffraction limit. To avoid the deleterious effects of using fusion proteins attached to ESCRT components, we performed measurements on the endogenous protein or, in the case of CHMP4B, constructs modified with the small HA tag. Due to the transient nature of the ESCRT interactions, the fraction of HIV-1 assembly sites with colocalizing ESCRT complexes was low (1.5%-3.4%). All colocalizing ESCRT clusters exhibited closed, circular structures with an average size (full-width at half-maximum) between 45 and 60 nm or a diameter (determined using a Ripley’s L-function analysis) of roughly 60 to 100 nm. The size distributions for colocalizing clusters were narrower than for non-colocalizing clusters, and significantly smaller than the HIV-1 bud. Hence, our results support a membrane scission process driven by ESCRT protein assemblies inside a confined structure, such as the bud neck, rather than by large lattices around the neck or in the bud lumen. In the case of ALIX, a cloud of individual molecules surrounding the central clusters was often observed, which we attribute to ALIX molecules incorporated into the nascent HIV-1 Gag shell. Experiments performed using YFP-tagged Tsg101 led to an over 10-fold increase in ESCRT structures colocalizing with HIV-1 budding sites indicating an influence of the fusion protein tag on the function of the ESCRT protein.     

Investigating Sub-Spine Actin Dynamics in Rat Hippocampal Neurons with Super-Resolution Optical Imaging

Morphological changes in dendritic spines represent an important mechanism for synaptic plasticity which is postulated to underlie the vital cognitive phenomena of learning and memory. These morphological changes are driven by the dynamic actin cytoskeleton that is present in dendritic spines. The study of actin dynamics in these spines traditionally has been hindered by the small size of the spine. In this study, we utilize a photo-activation localization microscopy (PALM)–based single-molecule tracking technique to analyze F-actin movements with ∼30-nm resolution in cultured hippocampal neurons. We were able to observe the kinematic (physical motion of actin filaments, i.e., retrograde flow) and kinetic (F-actin turn-over) dynamics of F-actin at the single-filament level in dendritic spines. We found that F-actin in dendritic spines exhibits highly heterogeneous kinematic dynamics at the individual filament level, with simultaneous actin flows in both retrograde and anterograde directions. At the ensemble level, movements of filaments integrate into a net retrograde flow of ∼138 nm/min. These results suggest a weakly polarized F-actin network that consists of mostly short filaments in dendritic spines.     

Controllable Mode Hybridization and Interaction Within a Plasmonic Cavity Formed by Two Bimetallic Gratings

We theoretically study mode hybridization and interaction among surface plasmon polariton Bloch wave mode, Fabry–Perot cavity mode, and waveguide mode within a plasmonic cavity composed by two parallel planar bimetallic gratings. Four hybridized modes result from mode hybridization between surface plasmon polariton Bloch wave modes on the two gratings are observed. By changing the dielectric environment, mode hybridization behavior can be manipulated. Importantly, waveguide-plasmon polariton mode due to hybridization between grating supported surface plasmon polariton Bloch wave mode and cavity supported waveguide mode is observed. We demonstrate that surface plasmon polariton Bloch wave mode and Fabry–Perot cavity mode with the same mode symmetry can interact by presenting an anticrossing behavior, which can be controlled by laterally shifting one grating with respect to the other that causes a phase difference shift of the two involving modes. The proposed plasmonic cavity offers potentials for subwavelength lithography, tunable plasmonic filter, and controllable light-matter interaction.     

Ultra Sharp Fano Resonances Induced by Coupling between Plasmonic Stub and Circular Cavity Resonators

Plasmonics - A plasmonic waveguide system composed of metal-insulator-metal (MIM) stub coupled with circular cavity resonator was proposed to produce ultra sharp Fano resonances, which resulted...     

Corrected Super-Resolution Microscopy Enables Nanoscale Imaging of Autofluorescent Lung Macrophages

Observing the cell surface and underlying cytoskeleton at nanoscale resolution using super-resolution microscopy has enabled many insights into cell signaling and function. However, the nanoscale dynamics of tissue-specific immune cells have been relatively little studied. Tissue macrophages, for example, are highly autofluorescent, severely limiting the utility of light microscopy. Here, we report a correction technique to remove autofluorescent noise from stochastic optical reconstruction microscopy (STORM) data sets. Simulations and analysis of experimental data identified a moving median filter as an accurate and robust correction technique, which is widely applicable across challenging biological samples. Here, we used this method to visualize lung macrophages activated through Fc receptors by antibody-coated glass slides. Accurate, nanoscale quantification of macrophage morphology revealed that activation induced the formation of cellular protrusions tipped with MHC class I protein. These data are consistent with a role for lung macrophage protrusions in antigen presentation. Moreover, the tetraspanin protein CD81, known to mark extracellular vesicles, appeared in ring-shaped structures (mean diameter 93 ± 50 nm) at the surface of activated lung macrophages. Thus, a moving median filter correction technique allowed us to quantitatively analyze extracellular secretions and membrane structure in tissue-derived immune cells.