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An additional argument that vesicular traffic does not play a major role in the observed movement of the GFP chimeras during FLIP is that vesicles traveling through the cytoplasm should have an equal probability of fusing with acceptor membranes in stacks that are equidistant from a donor membrane. We found, however, that some stacks show very little loss of fluorescence during FLIP compared with others, even though they are equidistant from the zone of photobleaching. Moreover, there appears to be little or no interstack communication after microtubule depolymerization, when Golgi stacks reversibly scatter throughout the cytoplasm. These results are difficult to explain by vesicle traffic but are easily explained by differences in lateral continuities between Golgi stacks.
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FLIP experiments at 37°C with cells expressing Man II-GFP and KDELR-GFP also showed loss of fluorescence throughout the Golgi complex, suggesting that these molecules diffuse rapidly between Golgi stacks. In cells expressing GFP chimeras in the Golgi, FLIP of a region of the cytoplasm that did not contain Golgi, but presumably did contain ER, did not result in significant loss of Golgi fluorescence over this time frame, suggesting that Golgi membranes are not in direct continuity with the ER.
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The data, however, do not rule out the possibility that native Man II and GalTase ever oligomerize. They only indicate that such complex formation is not required for efficient Golgi targeting and retention of these proteins.
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As one example, for models that assume the existence of functionally discrete Golgi cisternae or subcompartments [J. E. Rothman and L. Orci, Nature 355, 409 (1992)], our findings would imply that mechanisms exist for ensuring that membrane continuities between adjacent stacks only form between homologous membranes (that is, cis to cis and trans to trans). Otherwise, Golgi cisternae within a Golgi stack could not remain completely separate and distinct from each other.
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The microscope system described in (15) was used in the quantitative FPR experiments. The FPR beam was imaged into the sample as a stripe 2 μm wide. Because the stripe extended across the entire width of the Golgi or ER and bleached through the whole depth, diffusion was into and out of a line bounded on its sides, and not on its end. Hence, recovery of fluorescence was due to one-dimensional diffusion. The imposition of one-dimensional geometry on a complicated membrane as well as the mathematics for this case are covered in C-L. Wey, M. A. Edidin, R. A. Cone, Biophys. J. 33, 225 (1981). Briefly, a tortuous diffusion path reduces the apparent D, so our measurements in that case would be an underestimation.
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4 precipitation. Fluorescent cells were imaged at 37°C in buffered medium with a Zeiss LSM 410 confocal microscope system having a 100× Zeiss planapo objective (NA 1.4). The GFP molecule was excited with the 488 line of a krypton-argon laser and imaged with a 515-540 bandpass filter. Images were transferred to a Macintosh computer for editing and were printed with a Fujix Pictrography 3000 Digital Printer.
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We thank R. Klausner, E. Siggia, J. Bonifacino, J. Zimmerberg, J. Donaldson, J. Presley, J. Ellenberg, and K. Zaal for valuable comments and suggestions, and M. Chalfie, K. Moremen, M. Fukuda, R. Poljak, and V. Hsu for generous gifts of reagents. M.E. is supported by grant R37 AI 14584. Quicktime movies are available at http://www.uchc.edu/htterasaki/ flip.html.
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