Peter J. Verveer

Growth factor-induced MAPK network topology shapes Erk response determining PC-12 cell fate

The mitogen-activated protein kinase (MAPK) network is a conserved signalling module that regulates cell fate by transducing a myriad of growth-factor signals. The ability of this network to coordinate and process a variety of inputs from different growth-factor receptors into specific biological responses is, however, still not understood. We investigated how the MAPK network brings about signal specificity in PC-12 cells, a model for neuronal differentiation. Reverse engineering by modular-response analysis uncovered topological differences in the MAPK core network dependent on whether cells were activated with epidermal or neuronal growth factor (EGF or NGF). On EGF stimulation, the network exhibited negative feedback only, whereas a positive feedback was apparent on NGF stimulation. The latter allows for bi-stable Erk activation dynamics, which were indeed observed. By rewiring these regulatory feedbacks, we were able to reverse the specific cell responses to EGF and NGF. These results show that growth factor context determines the topology of the MAPK signalling network and that the resulting dynamics govern cell fate.

Ezrin is a downstream effector of trafficking PKC-integrin complexes involved in the control of cell motility

Protein kinase C (PKC) α has been implicated in β1 integrin‐mediated cell migration. Stable expression of PKCα is shown here to enhance wound closure. This PKC‐driven migratory response directly correlates with increased C‐terminal threonine phosphorylation of ezrin/moesin/radixin (ERM) at the wound edge. Both the wound migratory response and ERM phosphorylation are dependent upon the catalytic function of PKC and are susceptible to inhibition by phosphatidylinositol 3‐kinase blockade. Upon phorbol 12,13‐dibutyrate stimulation, green fluorescent protein–PKCα and β1 integrins co‐sediment with ERM proteins in low‐density sucrose gradient fractions that are enriched in transferrin receptors. Using fluorescence lifetime imaging microscopy, PKCα is shown to form a molecular complex with ezrin, and the PKC‐co‐precipitated endogenous ERM is hyperphosphorylated at the C‐terminal threonine residue, i.e. activated. Electron microscopy showed an enrichment of both proteins in plasma membrane protrusions. Finally, overexpression of the C‐terminal threonine phosphorylation site mutant of ezrin has a dominant inhibitory effect on PKCα‐induced cell migration. We provide the first evidence that PKCα or a PKCα‐associated serine/threonine kinase can phosphorylate the ERM C‐terminal threonine residue within a kinase–ezrin molecular complex in vivo.

Imaging the intracellular trafficking and state of the AB5 quaternary structure of cholera toxin

The subcellular localization and corresponding quaternary state of fluorescent labelled cholera toxin were determined at different time points after exposure to living cells by a novel form of fluorescence confocal microscopy. The compartmentalization and locus of separation of the pentameric B subunits (CTB) from the A subunit (CTA) of the toxin were evaluated on a pixel‐by‐pixel (voxel‐by‐voxel) basis by measuring the fluorescence resonance energy transfer (FRET) between CTB labelled with the sulfoindocyanine dye Cy3 and an antibody against CTA labelled with Cy5. The FRET efficiency was determined by a new technique based on the release of quenching of the Cy3 donor after photodestruction of the Cy5 acceptor in a region of interest within the cell. The results demonstrate vesicular transport of the holotoxin from the plasma membrane to the Golgi compartment with subsequent separation of the CTA and CTB subunits. The CTA subunit is redirected to the plasma membrane by retrograde transport via the endoplasmic reticulum whereas the CTB subunit persists in the Golgi compartment.

High-resolution three-dimensional imaging of large specimens with light sheet–based microscopy

We report that single (or selective) plane illumination microscopy (SPIM), combined with a new deconvolution algorithm, provides a three-dimensional spatial resolution exceeding that of confocal fluorescence microscopy in large samples. We demonstrate this by imaging large living multicellular specimens obtained in a three-dimensional cell culture. The ability to rapidly image large samples at high resolution with minimal photodamage provides new opportunities especially for the study of subcellular processes in large living specimens.

EGFR activation coupled to inhibition of tyrosine phosphatases causes lateral signal propagation

The epidermal growth factor receptor (EGFR) belongs to the receptor tyrosine kinase (RTK) superfamily and is involved in regulating cell proliferation, differentiation and motility. Growth factor binding induces receptor oligomerization at the plasma membrane, which leads to activation of the intrinsic RTK activity and trans-phosphorylation of tyrosine residues in the intracellular part of the receptor. These residues are docking sites for proteins containing Src homology domain 2 and phosphotyrosine-binding domains that relay the signal inside the cell. In response to EGF attached to beads, lateral propagation of EGFR phosphorylation occurs at the plasma membrane, representing an early amplification step in EGFR signalling. Here we have investigated an underlying reaction network that couples RTK activity to protein tyrosine phosphatase (PTP) inhibition by reactive oxygen species. Mathematical analysis of the chemical kinetic equations of the minimal reaction network detects general properties of this system that can be observed experimentally by imaging EGFR phosphorylation in cells. The existence of a bistable state in this reaction network explains a threshold response and how a high proportion of phosphorylated receptors can be maintained in plasma membrane regions that are not exposed to ligand.

Global Analysis of Fluorescence Lifetime Imaging Microscopy Data

Global analysis techniques are described for frequency domain fluorescence lifetime imaging microscopy (FLIM) data. These algorithms exploit the prior knowledge that only a limited number of fluorescent molecule species whose lifetimes do not vary spatially are present in the sample. Two approaches to implementing the lifetime invariance constraint are described. In the lifetime invariant fit method, each image in the lifetime image sequence is spatially averaged to obtain an improved signal-to-noise ratio. The lifetime estimations from these averaged data are used to recover the fractional contribution to the steady-state fluorescence on a pixel-by-pixel basis for each species. The second, superior, approach uses a global analysis technique that simultaneously fits the fractional contributions in all pixels and the spatially invariant lifetimes. In frequency domain FLIM the maximum number of lifetimes that can be fit with the global analysis method is twice the number of lifetimes that can be fit with conventional approaches. As a result, it is possible to discern two lifetimes with a single-frequency FLIM setup. The algorithms were tested on simulated data and then applied to separate the cellular distributions of coexpressed green fluorescent proteins in living cells.

A QUANTITATIVE COMPARISON OF IMAGE RESTORATION METHODS FOR CONFOCAL MICROSCOPY

In this paper, we compare the performance of three iterative methods for image restoration: the Richardson–Lucy algorithm, the iterative constrained Tikhonov–Miller algorithm (ICTM) and the Carrington algorithm. Both the ICTM and the Carrington algorithm are based on an additive Gaussian noise model, but differ in the way they incorporate the non‐negativity constraint. Under low light‐level conditions, this additive (Gaussian) noise model is a poor description of the actual photon‐limited image recording, compared with that of a Poisson process. The Richardson–Lucy algorithm is a maximum likelihood estimator for the intensity of a Poisson process. We have studied various methods for determining the regularization parameter of the ICTM and the Carrington algorithm and propose a (Gaussian) prefiltering to reduce the noise sensitivity of the Richardson–Lucy algorithm. The results of these algorithms are compared on spheres convolved with a point spread function and distorted by Poisson noise. Our simulations show that the Richardson–Lucy algorithm, with Gaussian prefiltering, produces the best result in most of the tests. Finally, we show an example of how restoration methods can improve quantitative analysis: the total amount of fluorescence inside a closed object is measured in the vicinity of another object before and after restoration.

Multi-view image fusion improves resolution in three-dimensional microscopy

A non-blind, shift-invariant image processing technique that fuses multi-view three-dimensional image data sets into a single, high quality three-dimensional image is presented. It is effective for 1) improving the resolution and isotropy in images of transparent specimens, and 2) improving the uniformity of the image quality of partially opaque samples. This is demonstrated with fluorescent samples such as Drosophila melanogaster and Medaka embryos and pollen grains imaged by Selective Plane Illumination Microscopy (SPIM). The application of the algorithm to SPIM data yields high-resolution images of organ structure and gene expression, in some cases at a sub-cellular level, throughout specimens ranging from several microns up to a millimeter in size.

A comparison of image restoration approaches applied to three-dimensional confocal and wide-field fluorescence microscopy.

We have compared different image restoration approaches for fluorescence microscopy. The most widely used algorithms were classified with a Bayesian theory according to the assumed noise model and the type of regularization imposed. We considered both Gaussian and Poisson models for the noise in combination with Tikhonov regularization, entropy regularization, Goods roughness and without regularization (maximum likelihood estimation). Simulations of fluorescence confocal imaging were used to examine the different noise models and regularization approaches using the mean squared error criterion. The assumption of a Gaussian noise model yielded only slightly higher errors than the Poisson model. Goods roughness was the best choice for the regularization. Furthermore, we compared simulated confocal and wide‐field data. In general, restored confocal data are superior to restored wide‐field data, but given sufficient higher signal level for the wide‐field data the restoration result may rival confocal data in quality. Finally, a visual comparison of experimental confocal and wide‐field data is presented.

An optical sectioning programmable array microscope implemented with a digital micromirror device.

The defining feature of a programmable array microscope (PAM) is the presence of a spatial light modulator in the image plane. A spatial light modulator used singly or as a matched pair for both illumination and detection can be used to generate an optical section. Under most conditions, the basic optical properties of an optically sectioning PAM are similar to those of rotating Nipkow discs. The method of pattern generation, however, is fundamentally different and allows arbitrary illumination patterns to be generated under programmable control, and sectioning strategies to be changed rapidly in response to specific experimental conditions. We report the features of a PAM incorporating a digital micromirror device, including the axial sectioning response to fluorescent thin films and the imaging of biological specimens. Three axial sectioning strategies were compared: line scans, dot lattice scans and pseudo‐random sequence scans. The three strategies varied widely in light throughput, sectioning strength and robustness when used on real biological samples. The axial response to thin fluorescent films demonstrated a consistent decrease in the full width at half maximum (FWHM), accompanied by an increase in offset, as the unit cells defining the patterns grew smaller. Experimental axial response curves represent the sum of the response from a given point of illumination and cross‐talk from neighbouring points. Cross‐talk is minimized in the plane of best focus and when measured together with the single point response produces a decrease in FWHM. In patterns having constant throughput, there appears to be tradeoff between the FWHM and the size of the offset. The PAM was compared to a confocal laser scanning microscope using biological samples. The PAM demonstrated higher signal levels and dynamic range despite a shorter acquisition time. It also revealed more structures in x‐z sections and less intensity drop‐off with scanning depth.