1. Computational Analysis of F-Actin Turnover in Cortical Actin Meshworks Using Fluorescent Speckle Microscopy 
A. Ponti, P. Vallotton, W.C. Salmon, C.M. Waterman-Storer, G. Danuser 
Biophysical Journal 
Volume 84, Issue 5, Pages (May 2003)
DOI: /S (03)
Copyright © 2003 The Biophysical Society Terms and Conditions

2. FIGURE 1
Dynamic simulations of a polymerizing and depolymerizing F-actin meshwork. (a) Physical model for the generation of an actin meshwork. The inset shows a comparison between simulated and real FSM image data. Scale bar, 1μm. (b) Mean speckle number density from five simulations of a meshwork that assembles for 120s and disassembles for 360s at equal rates (inset, mean fluorescence intensity development). Meshwork disassembly is associated with a decrease in the mean intensity. Once the steady-state speckle number density is reached (after 100s), the mean speckle density is independent of whether the meshwork is polymerizing or depolymerizing, but only dependent on the PSF volume. With NA=1.4 optics, the number density is 3.5–4 speckles per μm2.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

3. FIGURE 2
A computational scheme for kinetic analysis of FSM data (see text for details).
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

4. FIGURE 3
Separation of speckles, i.e., significant local maxima in the image from noise-related weak local maxima. (a) Images are low-pass filtered to remove high-frequency noise. Scale bar, 2.5μm. (Inset a 1) Zoom-up of a subregion after filtering. (Inset a 2) The same subregion displayed as an intensity function in ℝ2. (b) Definition of a speckle as an intensity peak above background. (c) Principles of statistical speckle selection (see text for additional explanations). (d) Example of a speckle lifetime history; time point of speckle birth (arrow) and time point after speckle death (arrowhead). (e–g) Statistical selection of speckles illustrated on an image. (e) Result of local maximum (red dots) extraction. (f) Local minima (blue dots) extraction and assignment of background intensities to local maxima by Delaunay triangulation of local minima (see text). (g) Local maxima failing the Student's t-test are not counted as speckles. The arrowheads in e and g indicate the position of one weak local maximum falling through the statistical selection.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

5. FIGURE 4
Gap closer. (a) The linking of six short-living speckles (full lines) separated in time by one frame and in space by less than the Airy disk diameter removes false birth and death events and reconstructs one long-living speckle (b). The linking of two speckles is only allowed if the gap frame contains a weak local maximum within distance of the Airy disk radius to both the false death position of the first speckle and the false birth position of the second speckle (arrows in panel a). Further details on the linking conditions are given in the text. Panel b displays the intensity differences ΔI=IL−IBG between peak and background, superimposed by the critical intensity difference ΔIC calculated with the noise model (dashed line).
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

6. FIGURE 5
Classification of births due to polymerization (a) and births due to depolymerization (b), respectively; deaths due to depolymerization (c); and deaths due to polymerization (d). See text for further explanation of the scheme.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

7. FIGURE 6
Speckle analysis on synthetic data. Synthetic FSM movies were created based on a model of meshwork assembly and disassembly and well-defined labeling ratios and optical parameters. (a) Net assembly rates (negative values denote disassembly) applied to generate synthetic 10×10μm2 FSM image stacks. (b) The normalized kinetic scores accurately match the input net assembly rates, except for smoothing due to averaging effects in the analysis.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

8. FIGURE 7
FSM analysis of F-actin turnover in the lamellipodium of a newt lung epithelial cell. (a) Overview of the cell area imaged by FSM. The kinetic analysis displayed in b refers to the region delimited by the white frame. (b) Eight panels showing kinetic maps over a period of 35s, starting at time point 220s. Two positions are selected to indicate the periodic cycling of the actin meshwork. The arrowhead points to a region cycling from depolymerization to polymerization back to depolymerization. The arrow points to a region where the cycle is 180° phase-shifted. Scale bar, 2.5μm. (c) The color map used for displaying 31 score classes in the kinetic maps. (d) The mean kinetic score per unit time and area (2.5×2.5μm2) over 600s for three selected regions (see colored boxes in a) reveals a space-independent cycling rate of ∼40s−1. (e) Overall power spectrum of the cycles in d. The spectrum has three predominant peaks, corresponding to cycling periods of 151s, 76s, and 43s. They are approximately in an octave ratio to one another. A second pair found in the data are the 26- and 28-s periods in octave to the 57-s cycle.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

9. FIGURE 8
Power spectra of synthetic data. (a) Analysis of a meshwork with constant net polymerization (inset). The spectrum is concentrated in the zero (DC) frequencies. (b) Analysis of a meshwork with alternating phases of net assembly and disassembly with a period of 9s. Here, the spectrum concentrates in a peak at the corresponding frequency.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

10. FIGURE 9
F-actin turnover after latrunculin-A perfusion. Cells were first imaged during 300s under control conditions and then perfused with 750nM of latrunculin A. (a) Frames showing the scores integrated over a period of 50s. Scale bar, 2.5μm. Comparison of the power spectra before (b) and after (c) latrunculin-A perfusion.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

11. FIGURE 10
Effects of intensity changes due to photobleaching tested on fixed newt lung epithelial cells with a speckled actin cytoskeleton. (a) An exposure time of 10s per image induced strong bleaching represented by green to dark-blue areas. (b) An exposure time of 5s and the addition of Oxyrase as an antifading agent reduced the bleaching dramatically. Scale bar, 2.5μm.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

12. FIGURE 11
(a) Characterization of bleach-induced scores (red) relative to scores measured in live cell experiments (blue). The score distributions are clearly distinct, so that score biases due to bleaching can be compensated (see text for a description of the bleaching correction). (b) Bleaching correction applied to an uncorrected panel of Fig. 7 and (c) to Fig. 10b. The maps show that the correction indeed eliminates the marginal bias induced by bleaching; however, it does not change the quality of kinetic maps from live cell experiments. The arrowheads in b indicate some depolymerization scores that are slightly diminished by the bleaching correction. Scale bars, 2.5μm.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

13. FIGURE 12
Characterization of kinetic scores induced by focal shifts. Fixed cells with a speckled actin cytoskeleton were imaged in a series, at 3-s exposure time and with Oxyrase added, where the focus was changed in steps of 100nm between frames. (a) Overview of the cell indicating the transition between the thick cell body and the much thinner (∼200nm) lamellipodium. Panels b–d show the kinetic maps calculated at the confidence levels α=85, 95, and 99%. Scale bar, 2.5μm.
Biophysical Journal  , DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions