Imaging Of Thick Specimens Research Articles

Alternative Forward Models for Imaging Thick Specimens in Transmission Electron Microscopy.

I have investigated two different forward models for image formation in transmission electron microscopy of thick specimens, the 3DCtf model, which introduces a defocus gradient in the linear approximation, and the multislice model. An important result is that the 3DCtf model does not seem to be compatible with the multislice image formation model. A second very useful finding is that the exit wave in the multislice model has an imaginary part, which, in first-order approximation, is a pure projection of the specimen and is not affected by the defocus gradient. The defocus gradient only comes into play in real valued and higher-order imaginary terms. If the multislice model is closer to reality than the 3DCtf-model, then the best way to retrieve the specimen projection for thicker specimens should be a procedure for retrieving the exit wave's imaginary term, for example using images recorded at different defocus values.

Unraveling the Chemistry of meso-Cl Tricarbocyanine Dyes in Conjugation Reactions for the Creation of Peptide Bonds.

Tricarbocyanine dyes have become popular tools in life sciences and medicine. Their near-infrared (NIR) fluorescence makes them ideal agents for imaging of thick specimens or in vivo imaging, e.g., in fluorescence-guided surgery. Among other types of cyanine dyes, meso-Cl tricarbocyanine dyes have received a surge of interest, as it emerged that their high reactivity makes them inherently tumor-targeting. As such, significant research efforts have focused on conjugating these to functional moieties. However, the syntheses generally suffer from low yields. Hereby, we report on the reaction of meso-Cl dyes with a small selection of coupling reagents to give the corresponding keto-polymethines, potentially explaining low yields and the prevalence of monofunctionalized cyanine conjugates in the current state of the art of functional near-infrared dyes. We present the synthesis and isolation of the first keto-polymethine-based conjugate and present preliminary investigation in the prostate cancer cell lines PC3 and DU145 by confocal microscopy and discuss changes to optical properties in biological media.

Quadriwave gradient light inteference microscopy for lable-free thick sample imaging

Due to the multiple scattering effect, quantitative phase imaging of thick specimens is challenging in biomedicine research. Phase gradient methods with partially coherent illumination in the reflection geometry have significant potential. However, to reconstruct two-dimensional (2D) phase information robustly, these methods cannot avoid changing the shear direction orthogonally. Here we propose a rotation-free method named quadriwave gradient light interference microscopy (qGLIM). qGLIM excludes conventional shear components and uses an amplitude-type spatial light modulator (SLM) to perform lateral shearing and phase shifting. By displaying checkerboard gratings on the SLM, we can reconstruct phase gradient information in orthogonal shear directions simultaneously. We extract the phase quantitatively by applying the phase-shifting technique and deconvolution algorithm. We demonstrate this approach by standard samples, thin samples, and thick multiple scattering samples.

2.5D microscopy with polarization independent SLM for enhanced detection efficiency and aberration correction.

Fast, volumetric imaging by fluorescence microscopy is essential in studying biological phenomena and cellular functions. Recently, single-shot 2.5D microscopy showed promising results for high-throughput quantitative subcellular analysis via extended depth of field imaging without sequential z-scanning; however, the detection efficiency was limited and it lacked depth-induced aberration correction. Here we report that a spatial light modulator (SLM) in a polarization insensitive configuration can significantly improve the detection efficiency of 2.5D microscopy, while also compensating for aberrations at large imaging depths caused by the refractive index mismatch between the sample and the immersion medium. We highlight the improved efficiency via quantitative single-molecule RNA imaging of mammalian cells with a 2-fold improvement in the fluorescence intensity compared to a conventional SLM-based microscopy. We demonstrate the aberration correction capabilities and extended depth of field by imaging thick specimens with fewer z-scanning steps.

In situ structure of virus capsids within cell nuclei by correlative light and cryo-electron tomography

Cryo electron microscopy (cryo-EM), a key method for structure determination involves imaging purified material embedded in vitreous ice. Images are then computationally processed to obtain three-dimensional structures approaching atomic resolution. There is increasing interest in extending structural studies by cryo-EM into the cell, where biological structures and processes may be imaged in context. The limited penetrating power of electrons prevents imaging of thick specimens (> 500 nm) however. Cryo-sectioning methods employed to overcome this are technically challenging, subject to artefacts or involve specialised and costly equipment. Here we describe the first structure of herpesvirus capsids determined by sub-tomogram averaging from nuclei of eukaryotic cells, achieved by cryo-electron tomography (cryo-ET) of re-vitrified cell sections prepared using the Tokuyasu method. Our reconstructions confirm that the capsid associated tegument complex is present on capsids prior to nuclear egress. We demonstrate that this method is suited to both 3D structure determination and correlative light/electron microscopy, thus expanding the scope of cryogenic cellular imaging.

TEM bright field imaging of thick specimens: nodes in Thon ring patterns

The thickness of an object will, at some point, exceed the depth of field of a transmission electron microscope; the value at which this occurs, depends on the resolution and the wavelength considered. An image is then no longer a true projection of the 3D structure. This effect will be expressed in the power spectrum. Here, we first demonstrate this phenomenon experimentally, using carbon foils of different thicknesses and working at 40, 60, 80 and 300 kV. Since we determined the thicknesses of the foils by tomography, we are also able to confirm experimentally that in the case of a thick object, the Thon ring pattern can be described as the sum of the power spectra originating from thin, independently scattering slices. Thus, a sinc function envelope is observed that attenuates the Thon rings' amplitudes, yielding "nodes" in the pattern at which the amplitudes are zero. These nodes move to lower spatial frequencies with decreasing acceleration voltages and increasing thicknesses. Conversely, the object thickness can be directly derived from node positions at a particular acceleration voltage. We validate our approach by applying it to frozen-hydrated bacteria with experimentally determined thicknesses. Our model will contribute to more reliably determining the defocus to be used with contrast transfer function correction for thicker objects and at lower acceleration voltages.

Aberration correction for improving the image quality in STED microscopy using the genetic algorithm

With a purely optical modulation of fluorescent behaviors, stimulated emission depletion (STED) microscopy allows for far-field imaging with a diffraction-unlimited resolution in theory. The performance of STED microscopy is affected by many factors, of which aberrations induced by the optical system and biological samples can distort the wave front of the depletion beam at the focal plane to greatly deteriorate the spatial resolution and the image contrast. Therefore, aberration correction is imperative for STED imaging, especially for imaging thick specimens. Here, we present a wave front compensation approach based on the genetic algorithm (GA) to restore the distorted laser wave front for improving the quality of STED images. After performing aberration correction on two types of zebrafish samples, the signal intensity and the imaging resolution of STED images were both improved, where the thicknesses were 24 μm and 100 μm in the zebrafish retina sample and the zebrafish embryo sample, respectively. The results showed that the GA-based wave front compensation approach has the capability of correction for both system-induced and sample-induced aberrations. The elimination of aberrations can prompt STED imaging in deep tissues; therefore, STED microscopy can be expected to play an increasingly important role in super-resolution imaging related to the scientific research in biological fields.

Going deeper: three-dimensional study of γδ T cells in mouse reproductive tract using tissue clearing methods.

Several tissue clearing methods have been developed for three-dimensional imaging of thick specimens. Here, we applied CUBIC and ScaleS approaches to whole-mounted vaginal wall to reveal spatial distribution of γδ T lymphocytes, the key cells engaged in the epithelial homeostasis control and immune surveillance. Both methods rendered the tissue transparent and enabled detection of the green fluorescent protein (GFP)-expressing γδ T cells in vaginal samples of Tcrd-H2BeGFP transgenic mice. Upon additional immunolabeling, however, only CUBIC preserved the GFP signal and allowed for cell localization assessment during the estrous cycle. Using a combination of single- and two-photon microscopy, we found that during the diestrus phase the number of γδ T cells in the vaginal wall increased compared to estrus, while the proportion of cells residing in epithelium and stroma remained constant, irrespective of the cycle phase, and was close to 3:1, respectively. Moreover, the distance from epithelial γδ T cells to laminin-positive basal membrane and collagen-rich stroma also increased in diestrus in spite of thinning of epithelium upon shedding cornified cells. Our data indicate that γδ T cells sense sex hormone fluxes which influence their number and position them closer to the vaginal lumen in the diestrus phase.

Multi-slice ptychographic tomography

Ptychography is a form of Coherent Diffractive Imaging, where diffraction patterns are processed by iterative algorithms to recover an image of a specimen. Although mostly applied in two dimensions, ptychography can be extended to produce three dimensional images in two ways: via multi-slice ptychography or ptychographic tomography. Ptychographic tomography relies on 2D ptychography to supply projections to conventional tomographic algorithms, whilst multi-slice ptychography uses the redundancy in ptychographic data to split the reconstruction into a series of axial slices. Whilst multi-slice ptychography can handle multiple-scattering thick specimens and has a much smaller data requirement than ptychographic tomography, its depth resolution is relatively poor. Here we propose an imaging modality that combines the benefits of the two approaches, enabling isotropic 3D resolution imaging of thick specimens with a small number of angular measurements. Optical experiments validate our proposed method.

Structural variability and complexity of the giant Pithovirus sibericum particle revealed by high-voltage electron cryo-tomography and energy-filtered electron cryo-microscopy

The Pithoviridae giant virus family exhibits the largest viral particle known so far, a prolate spheroid up to 2.5 μm in length and 0.9 μm in diameter. These particles show significant variations in size. Little is known about the structure of the intact virion due to technical limitations with conventional electron cryo-microscopy (cryo-EM) when imaging thick specimens. Here we present the intact structure of the giant Pithovirus sibericum particle at near native conditions using high-voltage electron cryo-tomography (cryo-ET) and energy-filtered cryo-EM. We detected a previously undescribed low-density outer layer covering the tegument and a periodical structuring of the fibres in the striated apical cork. Energy-filtered Zernike phase-contrast cryo-EM images show distinct substructures inside the particles, implicating an internal compartmentalisation. The density of the interior volume of Pithovirus particles is three quarters lower than that of the Mimivirus. However, it is remarkably high given that the 600 kbp Pithovirus genome is only half the size of the Mimivirus genome and is packaged in a volume up to 100 times larger. These observations suggest that the interior is densely packed with macromolecules in addition to the genomic nucleic acid.

Gradient light interference microscopy for 3D imaging of unlabeled specimens

Multiple scattering limits the contrast in optical imaging of thick specimens. Here, we present gradient light interference microscopy (GLIM) to extract three-dimensional information from both thin and thick unlabeled specimens. GLIM exploits a special case of low-coherence interferometry to extract phase information from the specimen, which in turn can be used to measure cell mass, volume, surface area, and their evolutions in time. Because it combines multiple intensity images that correspond to controlled phase shifts between two interfering waves, gradient light interference microscopy is capable of suppressing the incoherent background due to multiple scattering. GLIM can potentially become a valuable tool for in vitro fertilization, where contrast agents and fluorophores may impact the viability of the embryo. Since GLIM is implemented as an add-on module to an existing inverted microscope, we anticipate that it will be adopted rapidly by the biological community.

Autofocusing Airy beam STED microscopy with long focal distance

Stimulated emission depletion (STED) is a very important technique in super-resolution microscopy. Until now, while autofocusing Airy beam (AAB) has been an attractive theme for both theoretical and applied researches, there are almost no report on AABs being used in STED microscopy. In this paper, we propose a novel STED microscopy based on AABs. A radially symmetric 3/2 phase plate is involved to simultaneously generate autofocusing excitation- and depletion-Airy beams. Remarkably, the AAB can auto-focus to a wavelength-scale spot with a long focal depth (several millimeters): on the contrary, the working distance of a conventional high numerical aperture (NA) objective is usually very short (about 200 μm). Our calculations indicate that the AAB based STED microscopy can achieve a super-resolution spot with FWHM of 58 nm while the focal length is 4.638 mm. Moreover, with properties of non-diffracting and self-healing, the Airy beam could enable a reduction of the scattering distortion induced by the specimens and has a great potential in imaging thick specimens.

Image scanning microscopy: an overview.

For almost a century, the resolution of optical microscopy was thought to be limited by Abbé's law describing the diffraction limit of light. At the turn of the millennium, aided by new technologies and fluorophores, the field of optical microscopy finally surpassed the diffraction barrier: a milestone achievement that has been recognized by the 2014 Nobel Prize in Chemistry. Many super-resolution methods rely on the unique photophysical properties of the fluorophores to improve resolution, posing significant limitations on biological imaging, such as multicoloured staining, live-cell imaging and imaging thick specimens. Structured Illumination Microscopy (SIM) is one branch of super-resolution microscopy that requires no such special properties of the applied fluorophores, making it more versatile than other techniques. Since its introduction in biological imaging, SIM has proven to be a popular tool in the biologist's arsenal for following biological interaction and probing structures of nanometre scale. SIM continues to see much advancement in design and implementation, including the development of Image Scanning Microscopy (ISM), which uses patterned excitation via either predefined arrays or raster-scanned single point-spread functions (PSF). This review aims to give a brief overview of the SIM and ISM processes and subsequent developments in the image reconstruction process. Drawing from this, and incorporating more recent achievements in light shaping (i.e. pattern scanning and super-resolution beam shaping), this study also intends to suggest potential future directions for this ever-expanding field.

Cellular resolution multiplexed FLIM tomography with dual-color Bessel beam.

Fourier multiplexed FLIM (FmFLIM) tomography enables multiplexed 3D lifetime imaging of whole embryos. In our previous FmFLIM system, the spatial resolution was limited to 25 μm because of the trade-off between the spatial resolution and the imaging depth. In order to achieve cellular resolution imaging of thick specimens, we built a tomography system with dual-color Bessel beam. In combination with FmFLIM, the Bessel FmFLIM tomography system can perform parallel 3D lifetime imaging on multiple excitation-emission channels at a cellular resolution of 2.8 μm. The image capability of the Bessel FmFLIM tomography system was demonstrated by 3D lifetime imaging of dual-labeled transgenic zebrafish embryos.

Optical phase conjugation assisted scattering lens: variable focusing and 3D patterning.

Variable light focusing is the ability to flexibly select the focal distance of a lens. This feature presents technical challenges, but is significant for optical interrogation of three-dimensional objects. Numerous lens designs have been proposed to provide flexible light focusing, including zoom, fluid, and liquid-crystal lenses. Although these lenses are useful for macroscale applications, they have limited utility in micron-scale applications due to restricted modulation range and exacting requirements for fabrication and control. Here, we present a holographic focusing method that enables variable light focusing without any physical modification to the lens element. In this method, a scattering layer couples low-angle (transverse wave vector) components into a full angular spectrum, and a digital optical phase conjugation (DOPC) system characterizes and plays back the wavefront that focuses through the scattering layer. We demonstrate micron-scale light focusing and patterning over a wide range of focal distances of 22–51 mm. The interferometric nature of the focusing scheme also enables an aberration-free scattering lens. The proposed method provides a unique variable focusing capability for imaging thick specimens or selective photoactivation of neuronal networks.

SW 2PE-STED Nanoscopy

With this work we present a new approach to two-photon excitation - stimulated emission depletion microscopy (2PE-STED), exploiting the very same wavelength for excitation and depletion [1]. It is well known that two-photon excitation (2PE) fluorescence microscopy is a technique particularly suitable for three-dimensional (3D), deep tissue and in vivo imaging applications. Since 2009, 2PE microscopy has been proposed coupled with stimulated emission depletion (STED) technique, bringing the super-resolution ability to the multi-photon excitation technique [2, 3].Unfortunately, the use of two distinct wavelengths for excitation and depletion requires mostly a special optical filter design to make the setup invariable in terms of the choice of the marker dye and potential light beam distortions have to be treated separately. Working with only just one wavelength for excitation and STED one would directly simplify the imaging formation scheme. We propose an imaging method to perform 2PE-STED imaging using a single wavelength (SW) and, consequently, the very same laser source for 2P excitation and depletion. We show that this method allows super-resolved imaging using a standard fluorophore like ATTO647n achieving a resolution below 80nm. Therefore it allows an easy coupling to a conventional commercial confocal microscope. The SW 2PE-STED nanoscopy is a promising technique to better actively control distortions when imaging thick highly scattering specimens, it will allow foreseeing advances in the imaging of thick specimens at nanoscale resolution.[1] P. Bianchini, B. Harke, S. Galiani, G. Vicidomini, and A. Diaspro, “Single-wavelength two-photon excitation-stimulated emission depletion (SW 2PE-STED) superresolution imaging”, PNAS 109, 6390-6393 (2012).[2] G. Moneron and S. W. Hell, “Two-photon excitation STED microscopy,” Opt Express 17, 14567-14573 (2009).[3] J. B. Ding, K. T. Takasaki, and B. L. Sabatini, “Supraresolution imaging in brain slices using stimulated-emission depletion two-photon laser scanning microscopy,” Neuron 63, 429-437 (2009).

Adaptive optics enables 3D STED microscopy in aberrating specimens

Stimulated emission depletion (STED) microscopy allows fluorescence far-field imaging with diffraction-unlimited resolution. Unfortunately, extending this technique to three-dimensional (3D) imaging of thick specimens has been inhibited by sample-induced aberrations. Here we present the first implementation of adaptive optics in STED microscopy to allow 3D super-resolution imaging in strongly aberrated imaging conditions, such as those introduced by thick biological tissue.

The Probe Profile and Lateral Resolution of Scanning Transmission Electron Microscopy of Thick Specimens

Lateral profiles of the electron probe of scanning transmission electron microscopy (STEM) were simulated at different vertical positions in a micrometers-thick carbon sample. The simulations were carried out using the Monte Carlo method in CASINO software. A model was developed to fit the probe profiles. The model consisted of the sum of a Gaussian function describing the central peak of the profile and two exponential decay functions describing the tail of the profile. Calculations were performed to investigate the fraction of unscattered electrons as a function of the vertical position of the probe in the sample. Line scans were also simulated over gold nanoparticles at the bottom of a carbon film to calculate the achievable resolution as a function of the sample thickness and the number of electrons. The resolution was shown to be noise limited for film thicknesses less than 1 μm. Probe broadening limited the resolution for thicker films. The validity of the simulation method was verified by comparing simulated data with experimental data. The simulation method can be used as quantitative method to predict STEM performance or to interpret STEM images of thick specimens.

Methods for Imaging Thick Specimens: Confocal Microscopy, Deconvolution, and Structured Illumination

When a thick specimen is viewed through a conventional microscope, one sees the sum of a sharp image of an in-focus region plus blurred images of all of the out-of-focus regions. High background, scattering, and aberrations are all problems when viewing thick specimens. Several methods are available to deal with these problems in living samples. These methods can be grouped into three classes: primarily optical (e.g., confocal microscopy, multiphoton microscopy), primarily computational (e.g., deconvolution techniques), and mixed (e.g., structured illumination) approaches. This article describes these techniques, which make it possible to see details within thick specimens (e.g., the interiors of cells within living tissue) by optical sectioning, without the artifacts associated with physically sectioning the specimen.

Extended depth-of-field microscopic imaging with a variable focus microscope objective

Increasing the depth-of-field (DOF) while maintaining high resolution imaging has been a classical challenge for conventional microscopes. Extended DOF (EDOF) is especially essential for imaging thick specimens. We present a microscope capable of capturing EDOF images in a single shot. A volumetric optical sampling method is applied by rapidly scanning the focus of a vari-focal microscope objective throughout the extended depths of a thick specimen within the duration of a single detector exposure. An EDOF image is reconstructed by deconvolving the captured image with the response function of the system. Design of a vari-focal objective and algorithms for restoring EDOF images are presented. Proof-of-concept experimental results demonstrate significantly extended DOF compared to the conventional microscope counterparts.