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* Department of Physics and Astronomy and
Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287;
Division of Basic Sciences, Arizona College of Osteopathic Medicine, Midwestern University, Glendale, Arizona 85308;
Laboratory of Receptor Biology and Gene Expression, National Cancer Institute, National Institutes of Health, Bethesda, Maryland 20892; and ¶ Biodesign Institute, Arizona State University, Tempe, Arizona 85287
Correspondence: Address reprint requests to Stuart Lindsay, Physics Department, Arizona State University, Tempe, AZ 85287-1604. Tel.: 480-965-4691; Fax: 480-965-7954; E-mail: stuart.lindsay{at}asu.edu.
| ABSTRACT |
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| INTRODUCTION |
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Several different types of ATP-dependent nucleosome remodeling complexes have been identified (Becker and Horz, 2002
; Tsukiyama, 2002
). Of these, the Swi-Snf family of complexes has probably been the most extensively studied (Becker and Horz, 2002
; Narlikar et al., 2002
; Martens and Winston, 2003
). They have been shown to cause alterations in vitro that include enhanced accessibility of nucleosomal DNA to nuclease cleavage, histone octamer movement in cis (nucleosome sliding) or in trans (transfer between DNA molecules), formation of specific dinucleosome structures, and decreased levels of nucleosome-restrained supercoiling. Precisely how remodeling complexes carry out these alterations remains uncertain, but current models have converged on a mechanism in which the action of the remodeling complex triggers the release of a localized bulge of DNA that is propagated around the nucleosome, perhaps by DNA twisting or translocation activities inherent in the complex (Flaus and Owen-Hughes, 2001
; Becker and Horz, 2002
; Narlikar et al., 2002
; Martens and Winston, 2003
). This mechanism is proposed to account for most of the effects produced by these enzymes.
Single molecule approaches offer tremendous advantages for the study of complex and (apparently) heterogeneous processes such as nucleosome remodeling. However, to date, remodeling studies have been dominated by ensemble-average biochemical approaches, except for two single molecule analyses (Bazett-Jones et al., 1999
; Schnitzler et al., 2001
). In both cases, remodeling reactions were carried out in solution, and then the remodeled molecules were deposited for imaging. Thus, different molecules were analyzed before and after remodeling, and remodeling changes were assessed by comparing the two populations. In the work described here, we apply a single molecule atomic force microscopy (AFM) technique, first demonstrated by Kasas et al. (1997)
, which can detect events on individual molecules by imaging the same molecules before and after a process is activated. To apply this approach to nucleosome remodeling, chromatin arrays that had been preincubated with the remodeling complex human Swi-Snf (hSwi-Snf) under inactivating (no ATP) conditions are deposited and imaged in a flow cell linked to the AFM. After activation of hSwi-Snf by the addition of ATP, the same fields are reimaged. In this way, it is possible to study remodeling on individual chromatin molecules. Imaging is done in solution, which enhances the biological relevance of the results, and the system is physiologically relevant because single-copy mouse mammary tumor virus (MMTV) promoter nucleosomal arrays reconstituted with human histones (Bash et al., 2003
) are remodeled by the same complex that remodels this promoter in vivo during nuclear receptor mediated transcription activation (Yoshinaga et al., 1992
; Muchardt and Yaniv, 1993
; Fryer and Archer, 1998
).
In an approach such as this one, the process takes place while the molecules are on the imaging surface, an environment that can inhibit enzyme activity (Kasas et al., 1997
). However, for remodeling reactions carried out by hSwi-Snf, we find that many of the observed chromatin changes are more dramatic in scale than those previously suggested from biochemical or from single molecule studies. The changes are, however, consistent in nature with the types of remodeling outcomes suggested from those studies. The changes observed involve several novel DNA-mediated alterations in chromatin structure, including one that suggests an unanticipated mode of hSwi-Snf action.
| MATERIALS AND METHODS |
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Nucleosomal arrays containing the MMTV promoter region were salt reconstituted to various subsaturated levels of nucleosome occupation with HeLa histones exactly as previously described (Bash et al., 2003
) and then glutaraldehyde (GD) fixed, to prevent the loss of nucleosomes that occurs during solution imaging (Wang et al., 2002
). Arrays were preincubated with hSwi-Snf, to avoid potential difficulties arising from diffusion-limited binding rates at these low sample concentrations, at stoichiometries ranging from 2.5 to 12 chromatin molecules per hSwi-Snf molecule for 20 min in a solution of 5 mM NaCl, 5 mM NaH2PO4 buffer (pH 7.5), and then deposited on GD-aminopropyltriethoxysilane (APTES); (Facci et al., 2002
), derivatized at 1-µM levels with GD (substantially lower than in previous studies; Wang et al., 2002
) and allowed to adsorb for a period of 40 min. After deposition, fields are scanned twice. The second scan assesses the effect of the AFM scanning process on chromatin structure and thus provides the background level of change. Thus, this important control is carried out on the same samples that will be analyzed for remodeling. Then a solution of 1 mM MgCl2 and 1 mM ATP is flowed into the cell, and remodeling is allowed to take place for 30 min. Then the same fields (and the same set of tethered molecules) are scanned again, to determine the changes induced by hSwi-Snf remodeling. Other reaction times were tried, but 30 min was judged to be optimal. Note that since the Mg2+ and ATP are equimolar, there will be little free Mg2+ present (to affect chromatin structure). For imaging, the prepared sample is mounted into a scanning probe microscopy (SPM) liquid flow cell (Molecular Imaging, Phoenix, AZ.). Imaging was carried out with a Macmode PicoSPM (Molecular Imaging) equipped with Silicon Cantilevers (Maclevers type II, Molecular Imaging) with a spring constant of 2.8 N/m. Measurements were performed at
25 kHz driving frequency. The scanning rate was 1.78 Hz.
Data analysis
Pairs of images taken before and after ATP addition were compared by digital subtraction after alignment to compensate for instrumental drift. The difference images flagged changes that were then quantified using Scanning Probe Image Processor software (SPIP v3.0, Image Metrology, www.imagmet.com). Background levels of change were determined by comparing pairs of images taken in samples before ATP addition. Image pairs (pre- and post-ATP addition) were adjusted to approximately the same contrast scale, so that changes in the apparent width and height of features on ATP addition are real. These local changes are not analyzed here for two reasons. a), They may be produced by a trivial process such as changes in the AFM tip caused by picking up material freed during remodeling. b), Many of the distinctive local changes in the size of protein-like features may well reflect compositional changes on remodeling, but they cannot be identified without a means for identifying the proteins during imaging, a problem we are currently addressing.
The samples clearly lose rigidity during remodeling, and continuous scanning induces a higher level of scan-induced artifacts than this before and after imaging. Thus we cannot continuously track the remodeling process.
| RESULTS |
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Inspection of the images in Fig. 1 demonstrates that the method can reliably compare the same nucleosomal arrays before (Fig. 1 a) and after (Fig. 1 b) ATP is introduced into the flow cell. Indeed, the majority of molecules in the two images look exactly the same before and after ATP introduction. This lack of change could reflect the absence of remodeling or changes that are too subtle to be detectable by AFM; note that modest changes have been suggested from many previous remodeling studies (Becker and Horz, 2002
; Narlikar et al., 2002
). However, the +ATP images do contain array molecules that have clearly undergone significant alteration (compare the numbered molecules in the ATP and +ATP scans; Fig. 1, a and b, respectively). Eight changes are marked on the full scans, and five examples of these are shown magnified to the right of the full scans. These images demonstrate that after ATP introduction array molecules show alterations in the free DNA path (1, 2, and 48), in the length of free DNA in particular regions (13 and 68), and in protein (nucleosome) size and position (2, 3, and 68). The changes we observe will be discussed in more detail below.
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These major changes are found in a minority of molecules, at least under the conditions used here (modest hSwi-Snf/chromatin ratios and tethered molecules). However, they are not rare, occurring in up to 10% of the molecules in a field. The frequency with which we observe them increases with increasing hSwi-Snf/chromatin ratios (solid circles, Fig. 2). On the other hand, chromatin changes resulting from the technique itself (tip induced movement in the sample during scanning, etc.) show no hSwi-Snf dose dependence (open circles, Fig. 2).
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This variety of major chromatin changes that are observed after hSwi-Snf activation not only takes place within a single chromatin sample but even occurs in individual molecules that are in close spatial proximity (cf. Fig. 3, a and c, and Supplemental Fig. 1, c and d), thus demonstrating that hSwi-Snf is inherently capable of producing different types of remodeling outcomes.
Modest remodeling events (Fig. 3 a, white arrowhead) also occur in molecules that lie close to molecules undergoing major changes, indicating that variability in remodeling extent is also a characteristic of hSwi-Snf action. Such heterogeneity makes single molecule techniques particularly appropriate for studying the process of nucleosome remodeling. We did not analyze the more modest remodeling changes because some of them could result from scanning-induced changes (see Materials and Methods) and because the large-scale changes are the most novel.
The arrays shown in Figs. 1 and 3 contain an average of 4.4 nucleosomes per template. More highly loaded MMTV arrays (averaging 7.6 nucleosomes per template) undergo remodeling changes that are quite similar to those shown above (data not shown), but the changes are more difficult to analyze due to the higher nucleosome density on the arrays. In addition, these samples show an increased incidence of large and highly compacted structures (Fig. 4). These structures result from the presence of hSwi-Snf (they are not observed without hSwi-Snf and are present in both plus and minus ATP); similar structures were detected in the ex situ AFM studies of Schniztler et al. (2001)
. The structures show evidence of remodeling changes (Fig. 4) but they are impossible to analyze by AFM. For the above reasons, the less highly loaded array samples (nav = 4.4) were used for the detailed quantitative analyses presented below. The similarity in the types of remodeling changes observed in both the highly loaded arrays (in the uncompacted molecules) and less highly loaded arrays argues that the changes we observe are characteristic of chromatin at any occupation level.
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25-fold molar excess of nucleosomes over hSwi-Snf molecules on a per nucleosome basis, yet 510% of the nucleosomes in a given field undergo major changes, in addition to many (unscored) minor changes. These changes do not reverse when ATP is removed (data not shown), which is also consistent with catalytic action of hSwi-Snf (Imbalzano et al., 1996The relative frequencies of each of the four classes of major remodeling changes are shown in Fig. 5 a. DNA unwrapping (DU) and chromatin rewiring (R) are the two most common changes observed (dotted bars) but these two are not observed at all in the background (ATP) scans (solid gray bars). Thus, they must result from ATP-dependent hSwi-Snf remodeling. In addition, PM and especially DM changes occur more frequently after hSwi-Snf activation. The R and DU frequencies shown are a minimal estimate because they were only scored as R and DU events if changes were unambiguous. For example, some PM events could in fact be R events, and many changes were unscored because the exact nature of the change was ambiguous.
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6597 basepairs (bp) (Fig. 5 b, 2030 nm bin). This length corresponds roughly to one turn of nucleosomal DNA (80 bp). Thus, hSwi-Snf apparently has a preference for unwrapping a complete turn of nucleosomal DNA during remodeling. That the DNA (loops) were directly removed from the nucleosome itself rather than additional DNA being pulled or otherwise propagated through flanking nucleosomes is indicated by the observation that the paths of DNA on each side of the event (i.e., the DNA stretches that are adjacent to the released segment) typically show no change (e.g., Fig. 3, c and d); it seems unlikely that DNA could be pulled through neighboring tethered nucleosomes without changing the DNA path somewhere within the array. The release of such fairly significant amounts of DNA from nucleosomes by hSwi-Snf is consistent with other observations: remodeling changes across large regions of the nucleosome (Aoyagi et al., 2002| DISCUSSION |
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The analysis detects a significant incidence of DNA-mediated remodeling changes: DNA transfer in cis or trans, DNA unwrapping from nucleosomes, and DNA movement. Although the tendency of hSwi-Snf to carry out these types of reactions may be exaggerated by surface tethering of the histones, the observations do demonstrate that remodeling complexes like hSwi-Snf are capable of carrying out major alterations directly through DNA. This is consistent with their proven ability to break histone-DNA contacts although not affecting histone octamer structure (Bazett-Jones et al., 1999
). An ability to carry out alterations directly via nucleosomal DNA would provide an easy, direct, and potentially quite reversible way for Swi-Snf complexes to alter chromatin organization to facilitate DNA access and could prove useful in various types of in vivo genomic processes.
The observed preference of hSwi-Snf to remove a complete turn of nucleosomal DNA is particularly intriguing. Current models (Flaus and Owen-Hughes, 2001
; Becker and Horz, 2002
; Narlikar et al., 2002
; Martens and Winston, 2003
) propose that remodeling complexes work by propagating a bulge of released DNA around the nucleosome, acting via its 5-nm DNA-containing face (Fig. 6 a) and possibly initiating their action at the nucleosomal DNA entry/exit sites. However, this mechanism seems unlikely to produce a preference for releasing complete 80-bp turns of DNA. On the other hand, hSwi-Snf acting through the 11-nm histone surface of the nucleosomal disc (Fig. 6 b), perhaps lifting off a turn of DNA, could produce such a preference. The likely tendency of nucleosomes to lie flat on the imaging surface would preferentially expose the 11-nm face and thus might enhance this mode of approach in our studies; however, this approach mechanism is also consistent with solution observations. For example, H3-H4 tetramer-DNA complexes are not as efficiently remodeled as complete nucleosomes (Boyer et al., 2000
). Tetramer complexes lack H2A and H2B, which are significant features of the 11-nm face of the complete nucleosome (Luger et al., 1997
) and thus ought to be viewed differently by remodeling complexes that approach via this surface. An electron microscopy imaging model of yeast Swi-Snf shows the complex to be oblate in shape with a cavity capable of accommodating the 11-nm nucleosome face (Smith et al., 2003
). This approach mechanism is consistent with the ability of Swi-Snf to remodel nucleosomal DNA containing nicks (Aoyagi and Hayes, 2002
) that should compromise DNA torsion-dependent remodeling mechanisms. Nucleosomes can contact each other via the 11-nm surface (Luger et al., 1997
). Other factors that interact with nucleosomes might also use this mode of contact; for example, H2A-H2B dimers would be readily accessible on the 11-nm surface for mobilization by FACT, a complex that facilitates chromatin transcription (Belotserkovskaya et al., 2003
).
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| SUPPLEMENTARY MATERIAL |
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| ACKNOWLEDGEMENTS |
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Submitted on March 12, 2004; accepted for publication April 30, 2004.
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