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Volume 86, Issue 6, Pages (June 2004)

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1 Volume 86, Issue 6, Pages 4075-4093 (June 2004)
Ultrafine Membrane Compartments for Molecular Diffusion as Revealed by Single Molecule Techniques  Kotono Murase, Takahiro Fujiwara, Yasuhiro Umemura, Kenichi Suzuki, Ryota Iino, Hidetoshi Yamashita, Mihoko Saito, Hideji Murakoshi, Ken Ritchie, Akihiro Kusumi  Biophysical Journal  Volume 86, Issue 6, Pages (June 2004) DOI: /biophysj Copyright © 2004 The Biophysical Society Terms and Conditions

2 Figure 1 Typical images and trajectories of Cy3- and Gold-DOPE recorded at a 33-ms resolution (video rate) for 3.3s (100 frames). (a) SFVI of Cy3-DOPE. (b) SPT of Gold-DOPE (gold probes coated with anti-fluorescein antibody Fab fragments bound to fluorescein-DOPE, which was preincorporated in the cell membrane). The colors (purple, blue, green, orange, and red) represent the trajectories over time periods of 20 steps (every 660ms). The color sequence is consistent throughout this article. The actual video images are also shown. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

3 Figure 2 Distribution of diffusion coefficients in a 100-ms time-window (D100ms). D100ms is the same as D2–4 in Kusumi et al. (1993). Arrowheads indicate the median values. (A) D100ms estimated for Cy3- (top) and Gold-DOPE observed using our standard observation protocol (bottom), which involves the observation of all of the gold particles attached to the membrane longer than 3s, but the observation is limited for 20min after the addition of the gold probes. (B) (Top) D100ms for Gold-DOPE estimated for particles bound to the membrane surface for shorter periods (between 3 and 150s, the short-term reporters, solid bars) and for those bound for longer periods (5min or longer, the long-term reporters, open bars), indicating that those bound to the membrane for short periods exhibit diffusion coefficients comparable to Cy3-DOPE. See the text for details. Note that for the determination of the long-term reporters, we only observed for 5min, and did not examine how much longer than 5min they stayed on the membrane surface, whereas the observation following the standard protocol would include the short-term reporters as well as the gold probes that might have stayed much longer than 20min, and therefore, its D100ms distribution becomes broader than that for the short-term reporters and the long-term reporters combined. (Bottom) Fab fragments and the whole IgG of anti-fluorescein antibodies were labeled with Cy3, and their diffusion coefficients after binding to fluorescein-DOPE were measured. D100ms estimated for Cy3-Fab-DOPE (solid bars) and Cy3-IgG-DOPE (open bars). Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

4 Figure 3 Gold-DOPE observed at a 110-μs resolution exhibited hop diffusion. What appears to be simple Brownian diffusion at a 33-ms resolution (a, video rate) is actually fast hop diffusion, as visible in recordings at a 110-μs resolution (b, 300-fold faster than the video rate). (a) Each color represents 60 step periods (every 2s). (b) Each color indicates plausible confinement within a compartment, and black indicates intercompartmental hops. The residency time for each compartment is indicated. These compartments were detected by computer software we developed (Fujiwara et al., 2002) as well as by eye. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

5 Figure 4 Distributions of the compartment size (left) and the residency time (right) for Gold-DOPE indicate the presence of 41-nm compartments (median observed at a 25-μs resolution) and 15-ms residency time (median) in a compartment. Open bars and solid bars indicate the distributions observed at 110-μs and 25-μs resolutions, respectively. Arrowheads indicate the median values. The inset in the histogram for the compartment size shows more detailed distributions (25-μs resolution data). Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

6 Figure 5 Models for the mechanisms that could be responsible for the temporal corralling and hop diffusion of DOPE. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

7 Figure 6 The extracellular matrices and the extracellular domains of the membrane proteins are partially cleaved by treatment of cells with trypsin. (A) (a, b) After the amino groups of the cell surface proteins were first tagged with biotin, the cells were incubated with 10μg/ml trypsin (or trypsin-free medium) for 10min and then visualized with FITC-streptavidin (biotin labeling after trypsin treatment gave nearly the same results): a, no treatment; b, after trypsin treatment. The focus of the microscope is on the lamellipodia, where most SPT experiments were carried out. (c, d) The amount of remaining chondroitin sulfate glycosaminoglycan was quantitated by immunofluorescence staining before (c) and after (d) trypsin treatment. (B) Fluorescence intensity due to the remaining cell surface proteins and chondroitin sulfate after trypsin treatment (10min), plotted as a function of trypsin concentration. The fluorescence intensity (70×70 pixels ≈ 8×8μm) was normalized to that before trypsin treatment. The background was determined as the intensity in the area on the cover glass where no cell was attached, and was subtracted from the measured intensity in each area on the cell. A total of 40 cells were used for the measurements, with a total measured area of ∼3000μm2. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

8 Figure 7 Histograms showing the distributions of the compartment size (left) and the residency time (right) after various treatments (solid bars). Observations were carried out at a 110-μs resolution for a period of 278ms for each trajectory. The compartment size and the residency time were determined as described in the legend to Table 4. From top to bottom, trypsin treatment (10μg/ml, 10min, 68 particles), partial depletion of cholesterol by MβCD (4mM, 20min, 51 particles), partial depolymerization of f-actin by cytochalasin D (13μM, 5–15min, 68 particles), and stabilization of f-actin by jasplakinolide (0.5μM, 5–15min, 45 particles). In the bottom left corner, the distribution of the compartment size after cytochalasin D treatment is shown in a broader range. Arrowheads indicate median values. Open bars indicate the distributions before treatment (control, same as those in Fig. 4), and reflect the collective control results (before treatment) for all treatments. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

9 Figure 8 Apparent Dmicro (in a time-window of 100μs based on 25-μs resolution observations) plotted against compartment size, as determined for each trajectory in the control and bleb membranes. With a larger compartment size, the apparent Dmicro increased, suggesting that in smaller compartments, even a 25-μs resolution is insufficient to obtain true diffusion rates. This figure is generated using the same data set used to generate Fig. 4 (at a 25-μs resolution, solid bars) and the bleb data obtained at a 25-μs resolution. The average compartment size for NRK cells is indicated (dashed blue line). The dashed red line is a visual aid. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

10 Figure 9 Plots of log(MSD/time) against log(time) provide useful information on the changes of the diffusion characteristics that depend on the observation time intervals. MSD of the trajectories was estimated using data obtained at time resolutions of 25μs (5000 frames long), 110μs (5000 frames long), and 33ms (500 frames long), for the time-windows where the theoretically expected statistical errors in MSD are <40% (Qian et al., 1991). Then, the mean log(MSD/time) values (●) and their standard deviations (blue and yellow vertical bars, which may look like a band due to the high density of the data points here) were plotted as a function of log(time). Normal (simple Brownian) and anomalous diffusion can be distinguished in this display as lacking time-dependence (slope ∼ 0) and having negative slopes, respectively (Saxton, 1994; Feder et al., 1996). The best fit for the data obtained for the cell membrane using the three linear segments, depicted by blue lines, with α-values of 0.97 (50μs∼0.13ms), 0.53 (1∼10ms), and 0.94 (300ms∼2s) gives transitions at ∼0.1ms (or less) and between 10 and 100ms. (Fitted regions are shown in solid lines. To help the eye, they are extended, which are shown in broken lines. The fit between 1 and 10ms appears bad, but in fact there are many more points in the lower black sequence of ●; i.e., the fit was done correctly.) For comparison, the plots for the trajectories in bleb membranes (○=1000 frames; n=24) and the best regression result (orange line, α=∼1.0) are also shown. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

11 Figure 10 Two-dimensional, Brownian dynamics/Monte Carlo simulations indicate that ∼17% coverage of the boundary with 1-nm-ϕ transmembrane anchored proteins is sufficient to reproduce the experimentally determined hop rate of 2.3ms on average. The average residency time of Monte Carlo particles in a 40-nm compartment is plotted against percent of coverage of each side of the square compartment. The red broken line indicates the experimentally determined residency time (2.3ms). The results indicate that seven 1-nm proteins (∼17% coverage), six 2-nm proteins (∼30% coverage), or five 3-nm proteins (∼38% coverage), located along each side of the square compartment, were needed to reproduce the experimental residency time values of 2.3ms. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions

12 Figure 11 Summary of the hop diffusion parameters observed in various cell types. Biophysical Journal  , DOI: ( /biophysj ) Copyright © 2004 The Biophysical Society Terms and Conditions


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