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Journal of Bacteriology, January 2006, p. 805-808, Vol. 188, No. 2
0021-9193/06/$08.00+0 doi:10.1128/JB.188.2.805-808.2006
Copyright © 2006, American Society for Microbiology. All Rights Reserved.
Department of Regulation Biology, Saitama University, Saitama, 338-8570, Japan,1 Okazaki Institute for Integrative Bioscience, National Institutes of Natural Sciences, Myodaiji-cho, Okazaki 444-8787, Japan,2 Department of Biochemistry and Molecular Biology, Saitama University, Saitama, 338-8570, Japan3
Received 23 June 2005/ Accepted 27 October 2005
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The enzyme ribulose-1,5-bisphosphate carboxylase/oxygenase (RuBisCO) within these bodies appears to be packed into paracrystalline arrays, at least under some conditions (9, 15), but it is not clear whether such a well-defined molecular assembly of enzyme molecules is of physiological significance or merely a preparation artifact (1). The ordered arrangement may be disturbed during cell rupture and purification; on the other hand, it may sometimes be created as a drying artifact during preparation of the negative staining (2).
The ultimate goal of biological electron microscopy is to visualize ultrastructures in cells as they are in the living state. Rapidly frozen ice-embedded cells provide the most realistic images since they are free from artifacts introduced by lengthy sample preparation processes. However, detailed structures could not be visualized in them by conventional transmission electron microscopy (TEM) because of low contrast. The low contrast of nonstained biological samples can be overcome through the use of phase-contrast methods: that is, techniques using phase plates, which are frequently applied in visible light microscopy. Due to the fundamental issue of the electric charge imparted to phase plates by electron collisions (13), however, these methods have not yet been applied to TEM. Recently, the charging issue has been successfully resolved (7, 8) and novel forms of electron microscopy have been introduced: Zernike phase contrast (4) and Hilbert differential contrast (HDC) (6, 12). Among these methods, HDC, of which the experimental schematics are shown in Fig. 1A, is particularly useful because of its high contrast. Like differential interference contrast used in light microscopy, HDC can display topographical features of images through the effect of a phase plate inserted in the back focal plane of the objective lens (Fig. 1A). The
-phase plate covering the half-plane of the aperture (Fig. 1B) converts the phase retardation by transparent objects to amplitude contrast. Image formation theory recognizes this conversion as the conversion of the image modulation function, the so-called contrast transfer function (CTF), from the sine functional modulation unique to conventional TEM (Fig. 1C) to the cosine functional modulation (Fig. 1C) (6, 13). Due to the intense low-frequency components recoverable with the cosine CTF, HDC can provide high contrast. In contrast to Zernike phase contrast (4, 5), which also carries the cosine CTF, the HDC CTF is an odd function characterized by a big jump at the frequency origin (6). This odd nature is transferred to the point spread function (PSF) of HDC, which has an antisymmetric profile. The antisymmetric double peak, which stands in contradistinction to the symmetry of the conventional PSF, is responsible for the differential contrast (6). The HDC-TEM has allowed us to visualize detailed ultrastructures of ice-embedded whole cells of the cyanobacterium Synechococcus sp. strain PCC 7942 (11). Thus, the HDC-TEM provides novel opportunities to examine subcellular structures in the living state. In the present study, the obtained HDC-TEM images of carboxysomes were carefully analyzed and compared with conventional TEM images of ultrathin sections.
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FIG. 1. (A) Schematics of HDC-TEM. (B) A half-plane phase plate is shown. It is set exactly at the back focal plane, where usually an aperture is situated. (C) Schematics of the CTF of HDC.
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For preparation of ice-embedded cyanobacteria, the cells were collected in 0.2 M sucrose solution by centrifugation and dropped on a copper grid coated with carbon film. In log-phase growth of some gram-negative bacteria, turgor is known to be in the range of 0.5 M (3). Thus, 0.2 M sucrose may not have significant effect on altering the interior of the cyanobacterial cells. Holthuijzen et al. (10) stored carboxysomes in 20% (wt/wt) sucrose. After removing excess liquid carefully with the tip of a filter paper, the sample was frozen rapidly in liquid ethane using a Leica rapid freezing device (Leica EM CPC system). During the process of removing water, a number of cells were ruptured accidentally, although most of the cells remained intact and were covered by a thin layer of ice. The grid with ice-embedded cells was transferred to the specimen chamber of the TEM by a cryo-transfer system. The specimen chamber was cooled with liquid helium to reduce specimen damage caused by the electron dose. For observation, a JEOL JEM-3100FFC electron microscope with the HDC phase plate inserted into the back focal plane of the objective lens was operated at 300 kV.
For conventional chemical fixation, the cells were fixed in 2% glutaraldehyde in 0.05 M potassium phosphate buffer (pH 7.0) for 2 h at room temperature and in a refrigerator overnight. After rinsing in the buffer, the cells were postfixed with 2% OsO4 in the buffer for 2 h at room temperature. They were then dehydrated in an acetone series and embedded in Spurr's resin. Ultrathin sections (silver-gold) were cut with a diamond knife on a Sorvall MT2-B ultramicrotome. After staining with uranyl acetate and lead citrate, the sections were observed with a Hitachi H-7500 TEM at an accelerating voltage of 100 kV.
Ice-embedded whole cells of the cyanobacterium Synechococcus sp. strain PCC 7942 were observed by HDC-TEM and conventional TEM for comparison. In contrast to the obscure image obtained by conventional TEM of the same ice-embedded cyanobacterial cell (Fig. 2A), detailed ultrastructure inside the cell was visualized with high contrast by HDC-TEM (Fig. 2B). The cells were surrounded by smooth cell walls and packed with various particles, filaments, and membranous structures (Fig. 2B). Among these, carboxysomes were easily recognized because of their characteristic polyhedral shape and size (Fig. 2B). Occasionally the paracrystalline arrangement of particles could be recognized (Fig. 2B inset, enlargement of the square). These must be RuBisCO molecules in a carboxysome. The detailed structure of carboxysomes was even more clearly observed in accidentally ruptured cells (Fig. 2C, arrows pointing to carboxysomes). The rupture of the cell was possibly induced when excess water was removed by filter paper in the instant prior to freezing. The partial leakage of cellular material probably lowered the density of the cytoplasm, making it more suitable for visualization of structural details by HDC-TEM. It seems that with thick whole cells containing dense cytoplasm, differential contrast between cytoplasm and other structures is more difficult to obtain. Examples of carboxysomes observed in this way are presented in Fig. 3A to H. We conclude that the paracrystalline arrangement is the configuration of RuBisCO in carboxysomes in vivo.
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FIG. 2. (A) Conventional TEM image of an ice-embedded whole cyanobacterial cell. (Square) Carboxysome (enlarged in inset). (B) HDC-TEM image of the same whole ice-embedded cyanobacterium. (Square) Carboxysome with paracrystalline RuBisCO molecules (enlarged in inset). (C) HDC-TEM image of ice-embedded cyanobacterium ruptured in the instant before freezing. Arrows, carboxysomes. Bars, 100 nm.
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FIG. 3. (A to H) Three-hundred-kilovolt HDC-TEM images of carboxysomes in ruptured ice-embedded cyanobacterial cells. Arrowheads, carboxysome shell consisting of arrays of globular structures; thick arrows, regularly arranged structures at intervals of about 12 nm; thin arrows, regularly arranged structures at intervals of 6 nm. An asterisk indicates the portion of carboxysome which does not exhibit the regular arrangement of molecules. Bar, 100 nm.
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FIG. 4. (A to D) One-hundred-kilovolt conventional TEM images of carboxysomes in ultrathin sections of chemically fixed and resin-embedded cyanobacterial cells. RuBisCO molecules are vaguely recognized in a paracrystalline arrangement. The shell appears partially as disrupted lines. Bar, 100 nm.
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HDC-TEM with its extraordinary high contrast for unfixed, undehydrated, and unstained whole cyanobacterial cells will be a powerful tool for elucidating in vivo carboxysomes and other subcellular structures.
We are grateful to Andreas Holzenburg for discussion.
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