Nanoscopic Cellular Imaging: Confinement Broadens Understanding

Sep 7, 2016 - Nanoscopic Cellular Imaging: Confinement Broadens Understanding ... Coverage in Live-Cell Plasmon-Enhanced Single-Molecule Imaging...
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Nanoscopic Cellular Imaging: Confinement Broadens Understanding Stephen A. Lee, Aleks Ponjavic, Chanrith Siv, Steven F. Lee, and Julie S. Biteen ACS Nano, Just Accepted Manuscript • DOI: 10.1021/acsnano.6b02863 • Publication Date (Web): 07 Sep 2016 Downloaded from http://pubs.acs.org on September 12, 2016

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Nanoscopic Cellular Imaging: Confinement Broadens Understanding Stephen A. Lee1,§, Aleks Ponjavic2,§, Chanrith Siv1,§, Steven F. Lee2,*, Julie S. Biteen1,* 1 2 § *

Department of Chemistry, University of Michigan, Ann Arbor, MI 48109 Department of Chemistry, Cambridge University, Cambridge, United Kingdom Contributed equally to this work Address correspondence to: [email protected], [email protected]

Abstract In recent years, single-molecule fluorescence imaging has been reconciling a fundamental mismatch between optical microscopy and subcellular biophysics. However, the next step in nanoscale imaging in living cells can be accessed only by optical excitation confinement geometries. Here, we review three methods of confinement that can enable nanoscale imaging in living cells: excitation confinement by laser illumination with beam shaping; physical confinement by micron-scale geometries in bacterial cells; and nanoscale confinement by nanophotonics.

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KEYWORDS Super-resolution microscopy, single-molecule imaging, nanophotonics, light-sheet microscopy, bacterial biophysics, optical sectioning, plasmonic enhancement.

VOCABULARY Super-resolution imaging: Light microscopy with a spatial resolution smaller than the submicron diffraction limit of light Single-molecule fluorescence (SMF) microscopy: Sensitive fluorescence imaging attained by detecting and precisely localizing fluorescent emitters Optical sectioning: Decreasing out of focus excitation by illuminating a thin focal plane within a thick sample Photoactivatable labels: Dyes or fluorescent proteins that can be irreversibly switched from a dark (non-emissive) state to a fluorescent state. Localized surface plasmon resonance: Confined collective free electron oscillation which concentrates the local electromagnetic field and increases the local density of states Microbiome: Microbial cell community living within a certain environment

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There exists a fundamental mismatch between the limited spatial resolution of a light microscope and the nanoscale world of cellular biophysics. As a result, though the mysteries of subcellular biology have been investigated indirectly by biochemical approaches, the ability to directly observe intracellular processes remained elusive for many years. More recently, super-resolution innovations such as single-molecule fluorescence (SMF) microscopy and stimulated emission depletion (STED) microscopy, combined with a growing interest in developing the methods of physical chemistry for biology, have imparted an ability to detect, probe, and understand the processes occurring in cells.1 In particular, the development of SMF microscopy has enabled the direct visualization of dynamics,2-4 stoichiometry,5,6 and organization7,8 inside of cells. In this short review, we focus on confinement, a theme that has greatly increased the variety of biological specimens and the level of detail that can be probed by single-molecule superresolution microscopy. Other approaches, like STED microscopy, as well as other aspects of super-resolution imaging, such as the labeling, sample preparation, and microscopy innovations that have increased resolution, speed, and performance, have been reviewed extensively elsewhere.9-12 SMF super-localization microscopy permits single-molecule tracking,13-15 and super-resolution approaches like photoactivated localization microscopy (PALM)16 and stochastic optical reconstruction microscopy (STORM)17 overcome the diffraction limit in a densely labeled sample by detecting low concentrations of reporter molecules, trading off temporal resolution for increased spatial resolution. In all of these single-molecule methods, the location of each molecule is determined by analyzing the detected image. The localization precision—or spatial uncertainty on the position of the object11—in single-molecule imaging is fundamentally limitless; this precision and thus the achievable spatial resolution is only practically limited by the number of photons detected above background.18 Modern dyes have excellent fluorescence quantum yields, good absorption cross-sections, and can be pumped at power densities approaching saturation.19 Efficient detectors, high numerical aperture (NA) objective lenses, and sharp filters have improved SMF detection. However, outof-focus background limits the contrast of the fluorescence signal, particularly in biological specimens, which are prone to intrinsic background fluorescence.20 In the presence of background emission, the ability to localize single molecules precisely is degraded. Thus, although fluorescence microscopy is generalizable to a wide variety of samples, thick samples have evaded good super-resolution measurements due to this intrinsic fluorescent background and concerns about phototoxicity.21 These technological limitations have made the extension of SMF imaging to tissues and organisms difficult. Thus SMF imaging must be improved by reducing the fluorescence background, and here we contrast the advantages and disadvantages of three orthogonal styles of confinement (Figure 1 and Table 1): (1) excitation confinement through instrument innovation at the micron scale, (2) physical confinement in bacterial cells at the submicron scale, and (3) field confinement though plasmonic interactions at the nanoscale. The intent of this review is not to be exhaustive but rather to introduce each confinement style and give examples of major recent breakthroughs enabled by the technology.

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EXCITATION CONFINEMENT Limiting the light-exposed sample volume enables single-molecule fluorescence imaging (Figure 1a). In particular, we focus here on axial confinement (along the optical axis), which improves SMF imaging by reducing unwanted background light and increasing the image contrast. The techniques used for such optical confinement are summarized in Figure 1b-f and Table 1. Confocal Microscopy (200-500 nm). In confocal microscopy, a physical pinhole limits the collection volume radius to ~200 nm in the focal plane and ~500 nm along the optical axis.22 This probe volume is then scanned across the sample to build up an image. Scanning can be performed both in two23 and three24 dimensions. Still, while confocal confinement achieves diffraction-limited spatial resolution as well as background suppression, scanning decreases the practical temporal resolution relative to widefield illumination, worsens photobleaching,25,26 and increases phototoxicity.27 Despite these drawbacks, video-rate confocal SMF imaging has been achieved by removing the confocal pinhole to eliminate the need to scan, replacing the photodiode with a CCD array, and using optical sectioning to ensure sufficient contrast. Such video-rate confocal imaging has measured single-molecule membrane receptor diffusion on the cell surface28 and resolved transient single-molecule dynamics in the nuclear pore complex (Figure 2a-b).29 Stimulated emission depletion (STED) microscopy (laterally 10-100 nm). STED microscopy increases the resolution and contrast of confocal microscopy by using a depletion laser to reduce the effective confocal volume by providing a depletion zone about the beam profile (Figure 1b).30,31 With STED, lateral resolutions of ~2 nm have been achieved for nitrogen vacancies in diamond,32 and lateral resolutions as good as ~40-70 nm are typically achieved in biological samples.33-35 STED can be done with high label densities, and single-molecule STED imaging has been demonstrated on static fluorophores.30 Unfortunately, the phototoxicity of STED is even larger than that of confocal microscopy due to the ~GW/cm2 STED beam power densities. This issue can be somewhat alleviated with time gating36 or reversible saturable optical fluorescence transitions.37 Evanescent illumination: Total Internal Reflection Fluorescence (TIRF) Microscopy (100300nm). Non-propagating evanescent waves are created when light undergoes total internal reflection at a boundary. Because evanescent waves decay non-linearly within ~200 nm, TIRF illumination confines excitation to the sample surface, drastically reducing unwanted background fluorescence, and improving contrast (Figure 1e).38 Thus, though SMF detection has been possible for decades,39,40 TIRF microscopy was the major breakthrough that enabled SMF imaging in biological samples,38 and TIRF has become one of the most common and important techniques for SMF imaging in live cells.41 The major limitation of TIRF is that it practically constrains imaging to surfaces. This drawback is important because firm substrates, such as glass coverslips, can deleteriously affect soft, flexible biological membranes.42 Furthermore, even when such a non-physiological surface is coated with a soft, biologically inert polyelectrolyte

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coating,43 the substrate may interact with extracellular membrane proteins. For example, the human T-cell receptor is partially immobilized on polylysine-coated surfaces.44 In certain cases, the surface constraint of TIRF can be relaxed, 45 but these approaches, although impressive, are limited to specific cell shapes. Highly-inclined and laminated optical sheet (HILO) microscopy (5-10 µm). Illuminating the sample through the objective lens below the critical angle for TIRF produces a sheet of light inclined away from the coverslip surface.46,47 This method of excitation confinement is referred to as inclined or oblique illumination,11 or sometimes “pseudo-TIRF”46. Adding an aperture in the excitation beam path produces a laminated thin optical sheet to further reduce the sheet thickness to ~5-10 μm (Figure 2c).48 This HILO microscopy enables SMF imaging as deep as ~20 μm into cells and tissue. HILO has been used to study the dynamics and stoichiometry of ATP binding proteins on the apical surface of cells6 and to enable intracellular super-resolution imaging with nanopipette delivery.49 Furthermore, the cytoskeletal structure of the Caulobacter crescentus bacterium was resolved by combining HILO and a 3D super-resolution double-helix point spread function microscope (Figure 2d).8 Light-sheet microscopy (0.5-5 μm). Instead of through-objective widefield epi-illumination, excitation light can be introduced through a second objective lens perpendicular to the optical axis of the collection objective. Typically, a cylindrical lens is used to create a lateral ‘sheet’ in the sample plane, with an axial depth of ~0.5-5 μm, limited by the NA of the second objective lens (Figure 1c).50 In most cases, the decreased axial thickness in this single-plane illumination microscopy (SPIM) improves imaging contrast relative to HILO microscopy. The thickness of a light sheet can vary across the image, but zoom lenses51 or two-photon excitation52 produce more uniform illumination. Furthermore, inverted SPIM (iSPIM) enables diffraction-limited 3D imaging of large samples based on placing the excitation and acquisition objective lenses in a perpendicular configuration on separate piezo scanners.53 Though multiple planes are required for 3D reconstruction, 3D imaging can be done at high speeds by continuously switching excitation and acquisition between the objective lenses in dual-view iSPIM.54 SPIM has been used to study transient transcription factor binding in the cell nucleus,55 to image single RNA molecules inside cells,56 and to elucidate the mechanism of nuclear transport at a single-molecule level.57 SPIM can resolve the axial position of single molecules to the scale of the sheet thickness (Figure 2e-f). SPIM can also be combined with 3D localization methods such as the double-helix point spread function for 3D intracellular diffusion measurements.58 However, light-sheet microscopy imaging poses some engineering challenges, as it is difficult to introduce perpendicular light in close proximity to the acquisition objective lens, due to the fact that high NA objectives have short working distances. These issues of access can be overcome with microscopic mirrors in reflected light-sheet microscopy,55 and in single-objective SPIM.59 Beam shaping (300 nm). Most light-sheet microscopes use a standard TEM00 (Gaussian-like) transverse mode laser. Beam shaping can be combined with light-sheet microscopy to produce even thinner sheets. For instance, a Bessel beam can be formed using holography or an axicon

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lens, yielding a beam of constant radius over much larger distances.60 Bessel beams have the major advantage of being reconstructive, which limits aberrations caused by scattering and enables imaging deep into tissue. Furthermore, the combination of Bessel beams and structured illumination makes it possible to create very thin beams that surpass the diffraction limit (~300 nm).60 By quickly dithering this beam, a virtual 2D light sheet can be created; this Bessel beam plane illumination provides superior optical sectioning compared to the standard light sheet.61 Alternatively, curved Airy laser beams can be created using holography to form a special interference pattern.62 Light-sheet microscopy with Airy beams retains the long field of view offered by Bessel beam light sheets while improving image contrast.63 Alternatively, beam scanning can be entirely avoided by directly creating a ‘lattice’ light sheet.64 By combining lattice light-sheet microscopy with structured illumination, it is possible to perform high-speed super-resolution imaging of an entire cell.65 State of the art optical sectioning methods and lattice light-sheet microscopy have also recently been combined to study the dynamics of transcription factor proteins in stem cells at a single-molecule level demonstrating the extensive development and power of excitation confinement.66 PHYSICAL CONFINEMENT WITHIN A BACTERIAL CELL Microscopy in bacterial cells (1-5 µm). Excitation confinement enables SMF imaging in thick cells and tissues, but most bacteria are less than 2 µm thick.67 This small size confines fluorescent probes to a thickness that is comparable to the depth of field of a high NA microscope objective lens, thereby eliminating out-of-focus fluorescence (Figure 1f). Though the excitation confinement schemes described in the previous section can be used for imaging in bacteria,68,69 in most cases, physical confinement within these small cells enables high-contrast single-molecule detection and tracking inside bacterial cells without the need for 3D optics or excitation confinement.70-72 Because bacterial cell biology is accessible with the current state-of-the-art SMF microscopy, important biological processes can already be understood in bacterial cells. This increased understanding can be translated to eukaryotic systems as improved methods development—for instance the excitation confinement approaches described above—continues. On the other hand, the physical geometry of a bacterium produces important challenges for visualizing fluorescent molecules inside living bacteria: for instance due to a small total volume, barriers to dye entry, and possible artifacts induced by fluorescence labeling.73,74 Emerging solutions to the difficulties of subcellular imaging inside bacterial cells include a high-throughput method to introduce fluorescently labeled DNA and proteins into cells with electroporation75 and adapting image correlation approaches to highly confined volumes.76 Single-molecule tracking in bacteria. Fluorescent protein fusions are the most widely used labels for fluorescence imaging in living bacterial cells. Highly specific fusions can be genetically encoded, and photoactivatable fluorescent proteins77 can be switched from a dark

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state to a fluorescent state one at a time to enable single-particle tracking super-resolution imaging (sptPALM)78 of molecules in living bacterial cells to directly observe protein dynamics and understand protein function. Recently, the spatial distribution of translational and free ribosomal subunits measured by sptPALM in Escherichia coli (Figure 3a) gave rise to a model of fast translation initiation of nascent mRNA transcripts that was not previously revealed with electron or fluorescence microscopy.73 Single-molecule localization and tracking during amino acid starvation in E. coli uncovered that during stringent response, RelA synthesizes hyperphosphorylated GTP/GDP while bound to the 70S ribosome (Figure 3b).79 As well, two-color sptPALM in Bacillus subtilis led to the discovery that the highly conserved DNA mismatch repair protein MutS can only bind mismatches near the replisome and demonstrated that mismatch detection increases the MutS speed in vivo (Figure 3c).80 E. coli and B. subtilis are model bacteria for single-molecule imaging, but there is increasing research interest in studies of pathways in pathogenic and commensal bacteria. An emerging approach to single-molecule tracking in the heterogeneous cellular environment is a single-step analysis based on the cumulative probability distribution (CPD) of mean square displacements from all trajectories.81 With this approach, single-molecule investigations of cholera toxin regulation82 in Vibrio cholerae showed how proteins regulate cholera toxin expression while remaining localized to the cell inner membrane during DNA binding and transcription activation.83 The community is becoming increasingly aware of the importance of creating genetic fusions at the native promoter to ensure that native function and expression levels are maintained. Recently, CPD investigations of the virulence regulation protein TcpP labeled with the photoactivatable fluorescent protein PAmCherry at the native chromosomal locus in V. cholerae revealed a faster diffusing population that was not previously captured with ectopic expression (red curve in Figure 3d).84 Importantly, based on endogenously expressed TcpP-PAmCherry the underlying mechanism of membrane-bound transcription regulation in V. cholerae can now be investigated. Overall, bacteria are among the most successful and widespread organisms on Earth, and their rapid growth rates, simple growth media, and established genetics make these organisms ideal to understand life’s essential processes. Our understanding of basic bacterial cell physiology, as well as extensions to human health and disease, have benefited tremendously from super-resolution imaging in living bacterial cells,69-72 and it is expected that these advances will transfer to more complicated eukaryotic cells in the coming years.

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ELECTROMAGNETIC FIELD CONFINEMENT WITH PLASMONICS Nanophotonics (10-100 nm). Nanotechnology solutions which can complement superresolution imaging are appearing. The surface plasmon resonances that arise from collective oscillations of free electrons in metals are widely used spectroscopic sensors with sensitivity to refractive index change on a substrate.85 Further confining plasmons to subwavelength sized metal nanoparticles produces localized surface plasmon resonances which act as nanoantennas to enhance scattering process efficiency by concentrating the electromagnetic field, and to increase the absorption and emission of fluorescent dyes by increasing the local density of states.86,87 Nanoparticle plasmonics has found a home in cellular analysis with a host of different applications such as electro-chemical sensing, organelle imaging, biosensing, and photothermal imaging.88,89 Though only molecules that are close to a nanoscale feature are enhanced, recent advances have used holography to modulate hotspot positioning in real time, permitting real-time super-resolution surface-enhanced Raman scattering (SERS).90 Furthermore, plasmonic materials can confine light for selective and enhanced fluorescence excitation and emission to advance biological imaging.91 Excitingly, plasmonic nanoparticles can improve the brightness and photostability of probes in fluorescence imaging.92 These advantages, which are greatest for low quantum yield emitters, have been observed on the single-molecule level with over 1000-fold enhancements,93 and can also be extended to increase fluorescence brightness for higher quantum yield labels like fluorescent proteins.94 As plasmon-coupled fluorescence emerges for enhanced super-resolution imaging, much of the current research on plasmon-coupled fluorescence is focused on studying the physics governing the plasmon-dye system.95 Examinations of the spectral dependence, emission spectrum reshaping, distance dependence, and emission patterns have all improved our understanding of plasmon enhanced fluorescence.87,94-98 Live-cell fluorescence imaging achieves excitation confinement and emission enhancement based on plasmonic substrates directly underneath the cell (Figure 1d). For instance, confined light delivered via bowtie nanoapertures (BNAs) was used to image single fluorescent membrane lipids in CHO cells.99 These BNAs increased confinement and electric field density to produce an array of pinholes for multiplexed confocal imaging. The volumetric restriction obtained more accurate diffusion coefficients and thus a more precise model of membrane fluidity (Figure 4a). In a widefield plasmon-enhanced SMF approach, nanosphere lithography was used to fabricate large arrays of gold nanotriangle to plasmonically enhance the fluorescence of the V. cholerae virulence regulator TcpP-mCherry.91 The nanotriangles doubled the mCherry brightness in living cells (Figure 4b). These two-fold enhancements can be further improved by substrate optimization; enhancements in excess of 15 times are observed in vitro.95 Overall, plasmonics stands to fundamentally improve super-resolution by addressing SMF limitations through excitation confinement, enhanced electric field intensities, and increased local density of states.

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FUTURE OUTLOOK: TOWARD ANSWERING INCREASINGLY COMPLEX QUESTIONS Improving microscopy with optical solutions. Advanced technologies will continue to augment advanced microscopy by improving contrast and optimizing optical sectioning while still escaping the coverslip surface. The combination of light-sheet microscopy with two-photon excitation or STED microscopy has potential to greatly improve SMF contrast.100,101 Still, excitation confinement can only improve contrast up to a point; at this limit it becomes more beneficial to improve the efficiency of light collection. All microscopes suffer from noise and imaging artifacts due to optical imperfections; adaptive optics can correct these systematic aberrations:102 both holography103 and deformable mirrors104 have improved imaging through wave-front correction. Correcting aberrations becomes increasingly important in multicellular and deep-tissue imaging, where variations in refractive indices cause significant light scattering. Adaptive optics, which can correct for scattering even when using light-sheet microscopy,105 will therefore become indispensable. Alternative solutions to increased hardware complexity will simplify data acquisition. For instance, software-based information retrieval algorithms generate optimal optical sectioning with a “virtual light-sheet”.106 As microscopes become more complicated, more intricate sample geometries are required. Taking advantage of the freedom afforded by light-sheet microscopy to image single molecules in cells physically suspended away from a surface requires immobilization in space using methods such as gelation107 and optical trapping.108 It will be crucial to verify that cells remain unperturbed by establishing the influence that such immobilization methods have on the resting cell state.109 Ultimately, leaving the surface has made it possible to study both live and synthetic tissue at the single-molecule level; the combination of optical trapping110 or 3D-printed tissues111 with off-surface optical sectioning provides a unique platform for investigating interactions between cells. Application of these biophysical tools will lead to a wealth of discoveries about how signaling works on an intercellular scale. Direct observations of multiple components in bacterial cells. In parallel with technological development focused on imaging thicker and more complex biological samples, bacterial subcellular biology will remain an important target for SMF imaging experiments because these accessible, controllable systems provide natural confinement to the micron scale without complex optics. On the other hand, continuing to answer problems of increasing complexity about subcellular bacterial biophysics will require approaches that advance the state of the art beyond investigations of single proteins in isolated cells. While most single-molecule work has focused on proteins, for which labeling schemes are more well developed,9 improving the level of subcellular complexity accessible to SMF imaging requires the development of labeling and imaging methods that simultaneously and directly visualize the complex interactions between DNA, RNA, proteins, and lipids in live cells. The CRISPR/Cas9 system is now a near-ubiquitous tool for genome editing in biology.112 Excitingly,

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fluorescent protein fusions to the endonuclease-defective mutant dCas9 create an irreversibly bound probe capable of super-localizing a specific chromosomal locus.113 Ongoing research will continue to improve the sgRNA specificity114,115 and will provide multiple dCas9 probes for multi-color imaging.116,117 To visualize RNA, single-molecule fluorescence in situ hybridization (smFISH) targets mRNA transcripts with oligonucleotide fluorescent probes which is used to monitor transcriptional regulation.118 Super-resolution imaging based on smFISH permits precise quantification of gene expression even in bacteria,119 and can be extended for efficient multiplexing.120-122 Another important frontier in bacterial super-resolution imaging is the ability to combine chemical sensing with imaging,123 thereby merging high spatial resolution and accurate chemical specificity. pH- and force-sensing dyes can also be incorporated into single-molecule experiments,124 combining imaging with vibrational spectroscopy permits non-invasive chemical identification,125,126 and complementing non-destructive optical imaging with matrix-assisted laser desorption ionization (MALDI) mass spectrometry imaging maps molecular distributions with high specificity.127 Nanotechnology solutions to widen the scope of super-resolution imaging. Advances in nanotechnology, microfluidics,128,129 and plasmonics will continue to increase opportunities for SMF imaging of cells. Recent advances in fluorescence activated cell sorting (FACS) are improving bacterial cell sorting,130 which is vitally important for studying heterogeneous cell populations. Microfluidic devices allow single cell manipulation and analysis131 to enable multiple experiments on a single cell. In addition to sorting, microfluidics have made physiologically relevant conditions much more accessible. For instance, gradient hydrogels produced by a microfluidic mixing system enabled a study of hematopoietic stem cell differentiation as a function of niche cell concentration.132 As an alternative to chip-based microfluidics, individual cells identified by optical microscopy can be selected, manipulated, and sorted with a modified atomic force microscope with a microchanneled cantilever in fluidic force microscopy.133 Furthermore, though single-cell super-resolution experiments are common, bacterial cells do not exist in isolation; rather it is becoming increasingly obvious that most bacteria function as a part of a microbiome. We envision single-molecule imaging as a bridge for the gap between community-level observations and nanoscale biophysics. On one hand, tools like optical sectioning will find their place in studies of thick biofilms. On the other hand, 2D bacterial biofilm models134,135 will provide confinement in the axial direction while maintaining intercellular connectivity. Alternatively, sample confinement can make single cells behave as if they were in communities: for instance, volumetrically confined single Pseudomonas aeruginosa cells will undergo auto-induced quorum sensing, in an effective community of one.136 We envision a simple apparatus for studying protein function at the single-molecule level in single cells from a microbiome (Figure 5). This sample connects a microbial community co-

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culture137 to a nanofluidic sorting mechanism138 that prepares the sample for imaging. A more elaborate experiment might include tissue sectioning or imaging through mice139 or rabbits140 to understand how a microbiota interacts with a host.141 Overall, with the use of microfluidics, researchers can multiplex studies on individual cells in a variety of environments and with different stimuli, and extend single-cell measurements to the regime of cellular communities. Finally, looking forward, plasmonics will allow a variety of spectroscopies to be performed on the subcellular level to obtain dynamic chemical and structural information. Additionally, plasmonic nanoparticle arrays will improve the resolution of fluorescence microscopy to the order of the size of the emitter and reduce photobleaching for monitoring real-time protein dynamics.94 For instance, we envision combining plasmonics and nanofluidics to produce a platform for confined, physiological, enhanced imaging in bacteria (Figure 6). Overall, as technologies improve, all of the tools discussed here can be combined to reach higher levels of understanding about fundamental, subcellular biology. Through innovative combinations of confinement approaches, imaging modalities, and nanotechnologies, we will finally close the mismatch between the spatial resolution of light microscopy and the nanoscale world of cellular biophysics to enable a wealth of discoveries. ACKNOWLEDGEMENTS This work was generously supported by funding from the National Science Foundation (CAREER Award CHE-1252322) and the Engineering and Physical Sciences Research Council (EP/L027631/1). We would like to thank the Royal Society for the University Research Fellowship of SFL (UF120277).

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FIGURES AND TABLES

Figure 1. Confinement in cellular microscopy. (a) Typical relative reduction in background signal for a modern high numerical aperture objective as a function of axial confinement. (b-f) Modes of confinement and their relative scales.

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Table 1. Properties of excitation confinement in common biophysical imaging techniques

TIRF

Scale (nm) ~200

Typical Power Densities (kW/cm2) 0.01 – 10

Plasmonics

~10

0.1 – 10

Confocal

~300

102 – 105

STED*

40~70

102 – 104

Physical

Bacteria

1000 ~5000

0.1 – 10

Light-sheet

HILO

5000~ 10,000

0.1 – 10

Strategy

Technique

Evanescence

Scanning

Advantages -Simple implementation -High contrast -High speed -Best potential contrast

Disadvantages -Restricted to interfaces

-Requires metal nanoparticles

-No surface requirement -Medium contrast

-Slow due to point scanning -Prone to phototoxicity and photobleaching -Greatly improved -High phototoxicity contrast and photobleaching -Slow due to scanning -Small sample -Simple implementation

-Limited systems -Sample size limitation -Intracellular labeling with dyes is difficult

-Simple -Low contrast implementation -Small field of view -No surface due to aperture requirement -High speed SPIM 500~ 0.1 – 10 -Improved -Optical access issues 5000 contrast Beam ~300 0.1 – 1 -Even better -Expensive and complicated optics Shaping contrast -Large field of view *For comparison, this refers to continuous excitation STED; in the case of pulsed STED the instantaneous power is far higher than the quoted value.

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Figure 2. (a) Translocation of transport receptor importin β (red) through the nuclear pore complex (green) acquired with high-speed confocal microscopy. Time in seconds and scale bar is 1 µm.29 (b) Localization density map constructed from results in (a) with an overlay of the nuclear pore complex structure (yellow).29 (c) HILO microscopy excitation geometry.48 (d) 3D diffraction-limited (left) and 3D super-resolution images (right) of the bacterial cytoskeleton (red) and membrane (gray) of Caulobacter crescentus, acquired using HILO and a double helix point spread function. Inset: white-light image of the same cell.8 (e) Geometry used for SMF light-sheet microscopy.56 (f) Export of mRNA (top-white, bottom-red) across the nuclear envelope (bottom-green) observed by light-sheet microscopy.57

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Figure 3. Single-particle tracking of protein dynamics in bacteria reveals biological mechanisms. (a) Trajectories of individual free and mRNA-bound mEos2-labeled ribosomal subunits in E. coli show the degree of exclusion of bound subunits from the nucleoid.73 (b) Experimental trajectories for RelA-mEos2 in E. coli measure the dynamics of the stringent response.79 (c) The mismatch repair protein MutS-PAmCherry explores the B. subtilis cell, but accumulates near the replisome.80 (d) The virulence regulation protein TcpP-PAmCherry diffuses throughout the V. cholerae cellular membrane, and single-step analysis reveals three modes of motion (red, green, and blue curves).84 All scale bars: 1 µm.

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Figure 4. (a) Configuration for imaging mobile lipids in a CHO cell membrane via excitation by the confined field about a bowtie nanoaperture (left) and representative fluorescence time trace (right).99 (b) Configuration for imaging TcpP-PAmCherry in the periplasm of V. cholerae above a gold nanotriangle substrate (left) and associated histograms of fluorescence intensities with and without the plasmonic substrate (right).91

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Figure 5. Single-molecule imaging of microbial community members. (a) A microbiota is grown in a culture flask, (b) an aliquot of the co-culture is flowed through a nanofluidic device capable of separating and immobilizing bacteria by channel closing, and (c) labeled molecules within individual cells are imaged in situ using SMF microscopy.

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Figure 6. Single-cell analysis on a plasmonic substrate within a microfluidic channel will permit active control of the cellular environment. Two intracellular fluorescent proteins (red and green) couple to the plasmonic substrate for plasmon-enhanced two-color single-molecule imaging. (Inset) Electric field enhancement above each plasmonic nanotriangle.

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