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Address correspondence to Victor G. Corces, Department of Biology, Johns Hopkins University, 3400 N. Charles St., Baltimore, MD 21218. Tel.: (410) 516-8749. Fax: (410) 516-5456. email: corces{at}jhu.edu
| Abstract |
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Key Words: insulator; chromatin; transcription; nucleus; retrotransposon
| Introduction |
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500 binding sites for the Su(Hw) and Mod(mdg4) proteins that are presumed to be endogenous insulators; out of the multiple isoforms encoded by the mod(mdg4) gene, only the Mod(mdg4)2.2 protein appears to be present at the gypsy insulator (Mongelard et al., 2002). We will refer to the insulator present in the gypsy retrotransposon as the gypsy insulator, whereas we will use "endogenous Su(Hw) binding sites" to designate genomic binding sites for the Su(Hw) protein that do not contain copies of the gypsy retrotransposon but might act as insulators, although this property has not yet been demonstrated experimentally. We have previously shown that Su(Hw) and Mod(mdg4)2.2 colocalize in large foci, named insulator bodies, located mostly at the nuclear periphery of diploid cells. These insulator bodies are presumed to be formed by multiple individual insulator sites coming together at restricted nuclear locations. This hypothesis is supported by observations indicating that the presence of the gypsy insulator at two distant chromosomal sites causes the DNA containing these gypsy sequences to come together at the nuclear periphery (Gerasimova et al., 2000). If insulator bodies bring together individual insulator sites, the intervening DNA should form a loop. These loops might then represent functionally separate chromatin domains that allow independent regulation of transcription within each domain. Indirect molecular evidence for the possibility that the formation of chromatin loops might serve as a basis for insulator function comes from results obtained during a screen for proteins with boundary function in yeast (Ishii et al., 2002). Proteins involved in nucleo-cytoplasmic transport or components of the nuclear pore complex (NPC) were found to be able to buffer a flanked reporter gene from heterochromatic silencing effects. These results suggest that boundary activity can be accomplished by attachment of both sides of the insulated DNA to a solid substrate, in this case the NPC, in a perinuclear compartment. Although not directly shown in this work, attachment is likely to result in the formation of a small loop with its base at the NPC, and this loop might be functionally similar to the ones hypothesized to mediate gypsy insulator activity.
In spite of the widespread discussion of the loop domain model in the context of insulator function, neither the existence of these loops nor the basis for their location at the nuclear periphery has been demonstrated directly. Using FISH analysis of high saltextracted nuclei, we show here that DNA sequences located between two insulators form a loop in the interphase nucleus. The formation of this loop is dependent on functional insulator proteins and an intact nuclear matrix. The results suggest that insulators might regulate nuclear organization by controlling the formation of higher-order domains of chromatin structure.
| Results |
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7% of nuclear proteins) from Drosophila embryos ranging in age from 6 to 18 h postegg laying. Fig. 1 shows the results of Western analyses of different protein fractions. Lamin, as expected, is predominantly located in the nuclear matrix fraction. In contrast, histones are extracted in previous steps and are not present in this fraction (Oegema et al., 1997; Ma et al., 1999). Both gypsy insulator components, Su(Hw) and Mod(mdg4)2.2, copurify almost entirely with the nuclear matrix fraction (Fig. 1). As a control, we tested whether the Ultrabithorax (Ubx) transcription factor is also present in the nuclear matrix fraction; the Ubx protein is extracted from nuclei under the same conditions as histones and, therefore, is not associated with the nuclear matrix (Fig. 1). The same association of Su(Hw) and Mod(mdg4)2.2 was found using a different nuclear matrix isolation protocol that involves precipitation with ammonium sulfate (unpublished data). These results suggest that the gypsy insulator associates with the nuclear matrix and provides a biochemical foundation for the observed formation of insulator bodies in the nuclear periphery.
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95% of nuclear proteins are extracted with this technique; however, lamin and other known matrix-associated proteins remain (Fey et al., 1986; Ma et al., 1999). We then performed immunofluorescence light microscopy on nuclei that were either untreated or extracted with 2 M NaCl using antibodies to Mod(mdg4)2.2 and lamin. As expected from previous results with paraformaldehyde-fixed nuclei (Gerasimova et al., 2000), Mod(mdg4)2.2 is present in insulator bodies formed by the aggregation of multiple individual insulator sites in intact nuclei (Fig. 2, BE). To confirm that the insulator bodies are associated with the nuclear matrix, we stained nuclei extracted with 2 M NaCl with antibodies to lamin and Mod(mdg4)2.2 (Fig. 2, FI). The Mod(mdg4)2.2 protein, which marks the localization of gypsy insulator bodies, remains associated with the lamin-containing nuclear matrix core. We then extracted nuclei with 2 M NaCl and stained them with antibodies to both insulator proteins, Su(Hw) and Mod(mdg4)2.2, as well as DAPI to visualize the DNA (Fig. 2, JM). Extraction with such high salt concentrations that remove 95% of nuclear proteins did not disrupt the interaction between the two insulator proteins or their interaction with the nuclear matrix. It has been previously shown that the nuclear matrix, although not composed of one repeating protein unit, is composed of ribonucleoprotein complexes and, thus, is susceptible to destruction by RNase (He et al., 1990; Ma et al., 1999). To test whether disruption of nuclear matrix integrity would affect the formation of gypsy insulator bodies, we treated 2 M NaCl-extracted nuclei from wild-type larvae with RNase A. Under these conditions, the nuclear matrix appears fragmented and disorganized. In addition, the insulator bodies are destroyed, as determined by the localization of Su(Hw) and Mod(mdg4)2.2 proteins (Fig. 2, NQ). This result strongly suggests that the formation of insulator bodies requires the existence of an intact nuclear matrix.
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To ensure that the formation of an additional loop was due to the presence of a new functional gypsy insulator, we examined 2 M NaCl-extracted nuclei from male larvae of the genotype ct6; su(Hw)V, which carry the gypsy retrotransposon in the ct locus but lack Su(Hw) protein. Nuclei from these larvae failed to show DNA structures with the characteristic V shape in the region complementary to probe B (Fig. 4 R). The number of nuclei showing a V structure, scored as described above, is 19%, which is significantly different (P < 0.001, chi-squared test) when compared with nuclei carrying the ct6 mutation but wild type for su(Hw) (Table I). The formation of a V structure by probes A and C is also disrupted in nuclei from ct6; su(Hw)V mutant male larvae. In these nuclei, the DNA complementary to probes A and C only occasionally appears as a straight line going from the central region toward the surrounding halo; instead, the DNA appears disorganized in the nuclear halo region surrounding the residual nuclear matrix core (Fig. 4, QS). The number of times the V structure was observed in nuclei from ct6; su(Hw)V larvae is significantly lower (P < 0.001, chi-squared test) than wild type (Table I). In the absence of Su(Hw) protein, both the insulator present in the gypsy retrotransposon in the ct locus as well as the putative insulators present at endogenous Su(Hw) binding sites are not functional. The disorganized appearance of the DNA in nuclei from ct6; su(Hw)V male larvae implies that the lack of Su(Hw) protein results in the absence of loop structures, probably because of a failure to form functional insulators, suggesting that the insulators serve as attachment points of the DNA to the nuclear matrix. Similar experiments were also performed with nuclei from male larvae of the genotype ct6; mod(mdg4)u1. The results were comparable to those obtained with the ct6; su(Hw)V (unpublished data), suggesting that both proteins, Su(Hw) and Mod(mdg4)2.2, are required for the formation of a functional insulator capable of attaching the DNA to the nuclear matrix.
Loop formation requires an intact nuclear matrix
As these results suggest the requirement of the nuclear matrix for the formation of DNA loops in the nucleus, we then examined the effect of destroying the nuclear matrix, with RNase, on the organization of the DNA flanked by endogenous Su(Hw) binding sites. Nuclei from wild-type male larvae were extracted with 2 M NaCl, treated with RNase A, and then labeled with probes A, B, and C. The DNA complementary to probes A and C fails to form the characteristic V structure with the vertex attached to the nuclear matrix (Fig. 4, compare V with G). The frequency of the V structure in the RNase-treated nuclei is significantly lower (P < 0.001, chi-squared test) when compared with wild-type nuclei that were not RNase treated using probes A and C or to ct6 nuclei using probe B (Table I). This result suggests that the nuclear matrix is important for the attachment of the DNA and the establishment of the loop structures.
The formation of DNA loops should require not only attachment to the nuclear matrix, but also interactions between individual Su(Hw) binding sites to form insulator bodies. We have previously shown that the heat shock response causes gypsy insulator bodies to fall apart, as a brief increase in temperature to 37°C results in the disappearance of the typical punctate pattern of Su(Hw) and Mod(mdg4) observed in imaginal disk cells (Gerasimova et al., 2000). Under these conditions, the insulator bodies disappear, and, instead, Su(Hw) and Mod(mdg4) proteins are diffusely spread throughout the nucleus; this is accompanied by changes in the subnuclear localization of insulator-containing sequences, suggesting a dissociation of the chromatin loops (Gerasimova et al., 2000). To confirm the effect of heat shock on insulator body structure and distribution under the assay conditions used in the experiments described above, we performed immunolocalization experiments using Su(Hw) and Mod(mdg4) 2.2 antibodies on 2 M NaCl-extracted nuclei from imaginal disk cells of ct6 male larvae. The typical distribution of insulator bodies observed in cells grown at normal temperature (Fig. 3) is dramatically affected by heat shock. Nuclei from heat-shocked cells do not show large insulator bodies; instead, the Su(Hw) and Mod(mdg4)2.2 proteins are distributed throughout the nucleus and do not appear to be located in the nuclear periphery (Fig. 5, AD). This result suggests that heat shock interferes with the ability of individual Su(Hw) binding sites to come together at specific nuclear locations to form insulator bodies. If this is the case, heat shock should also interfere with the formation of DNA loops, which are presumed to be caused by interactions between Su(Hw) binding sites. To test this prediction, we performed in situ hybridizations with probes A and B to 2 M NaCl-extracted nuclei from ct6 male larvae. As we have described above, nuclei from these larvae should show the formation of an asymmetric V structure by DNA homologous to probe B (Fig. 4, LN). Instead, in most nuclei from cells subjected to heat shock, the DNA homologous to probe B appears disorganized and located in the halo region of the extracted nuclei, away from the darkly stained core (Fig. 5, EH). The number of times the V structure was observed in nuclei from heat-shocked ct6 male larvae is significantly lower (P < 0.005, chi-squared test) than in nonheat-shocked animals (Table I). These results suggest that interactions between Su(Hw) binding sites, which are disrupted by heat shock, are normally required for the formation of the V structure and, therefore, for the formation of a loop mediated by the gypsy insulator present in the ct locus of ct6 flies.
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| Discussion |
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Although the insulator DNA and associated proteins remain in the nuclear matrix fraction, the intervening DNA is extruded from the nucleus by high salt extraction and is found in the form of a large loop. The DNA contained within this loop appears only as a small dot after FISH analysis of unextracted nuclei. These two observations suggest that the chromatin fiber present in the loop formed by two insulators is not completely decondensed during interphase and only becomes extended after extraction of histones and other associated proteins. This suggests that the loop formed by two insulators might represent a domain of higher-order chromatin structure. This higher-order structure might be established and/or maintained by specific covalent modifications of histone tails. For example, it has been found that the chicken ß-globin locus, which is flanked by two CTC-binding factor insulators, contains histones H3 and H4, acetylated in various lysine residues (Litt et al., 2001; Mutskov et al., 2002). Covalent modification of histone tails might modulate internucleosome interactions, which, in turn, determine the degree of higher-order chromatin structure (Tse and Hansen, 1997).
The existence of chromatin insulator-induced domains would explain their unusual gene regulatory property of preventing an enhancer from activating a promoter in a different domain while not preventing the same enhancer from activating a promoter located in its own domain. The ability of the insulator, when flanking a transgene, to provide position-independent expression of the transgene is also consistent with the formation of a loop domain. This domain appears to be created by the interaction of flanking insulators with each other and the nuclear matrix. In fact, recent experiments by Ishii et al. (2002) have shown that boundary function in yeast can be elicited by tethering boundary-associated proteins to the NPC. This tethering would presumably result in the formation of a loop, similar to the ones we observe here, by the DNA located between the two boundary elements, which would attach the base of the loop to the NPC. In the case of Drosophila, the requirement for interactions between individual Su(Hw) binding sites for the formation of the loops is underscored by the observation that a brief heat shock interferes both with the formation of insulator bodies and with the ability of the gypsy retrotransposon to form a new loop when inserted in the ct locus.
The organization of the chromatin fiber into loops has also been shown for the Drosophila specialized chromatin structures (scs) and scs' boundary sequences. The proteins that interact with these elements have been shown to interact with each other both in vitro and in vivo. Consistent with the idea that interaction between the two proteins might facilitate pairing of boundary elements and formation of chromatin loops, sequences corresponding to the scs and scs' elements can be found in close proximity to each other in Drosophila nuclei (Blanton et al., 2003). The formation of similar loops by the gypsy insulator could also explain results by Cai and Shen (2001) and Muravyova et al. (2001), who demonstrated that two gypsy insulators inserted between an enhancer and promoter have no enhancer-blocking effect. These results could be explained in the context of the loop organization observed here by assuming that two closely linked insulators, due to their proximity, may preferentially interact with each other. This interaction would take place at the expense of interactions with other insulators, and it would result in the formation of a minidomain within a larger domain. Enhancers located within the larger domain would then be free to activate transcription from promoters in the same domain (Mongelard and Corces, 2001). The ability of the gypsy insulator to establish these chromatin loops raises the question of whether insulators/boundary elements are functionally equivalent to MARs/SARs. These sequences have been defined biochemically, based on their ability to attach to the nuclear matrix protein fraction in vitro. In some cases, MARs/SARs have also been shown to possess boundary activity using in vivo assays (McKnight et al., 1992; Namciu et al., 1998), although most MARs lack this activity (Poljak et al., 1994; van der Geest and Hall, 1997). It is possible that insulators and MARs have similar properties but play very different roles in the cell. MARs might have a fixed structural function in establishing chromatin organization within the nucleus. MARs might only be functional during mitosis, when the interphase to metaphase and back to interphase transition requires orderly changes in chromosome condensation and organization. Alternatively, MARs might create a scaffold of proteins and DNA that is more or less permanent during cell differentiation and among various cell types. Insulators, on the other hand, might act at a different level by creating an organization superimposed to that of MARs. Contrary to MARs, insulator activity might be regulatable, allowing this organization to change during development as cells differentiate and different patterns of gene expression are established.
Functional analyses of genome-wide expression patterns in yeast, Drosophila, and mammals also support the idea of the compartmentalization of the chromatin fiber into domains of gene expression (Cohen et al., 2000; Caron et al., 2001; Lercher et al., 2002; Spellman and Rubin, 2002). Studies in this diverse group of organisms have shown that genes located together in the same chromosomal region are transcriptionally coregulated. Although coregulation has not been shown to depend on insulator function, the existence of these transcriptional domains could have a structural basis in the formation of chromatin loops in which gene expression is globally regulated.
| Materials and methods |
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Nuclear matrix preparations
Nuclear matrices were prepared from wild-type, Oregon R, D. melanogaster embryos 618 h old, following the protocol described by Fisher et al. (1982), except that 2 M NaCl was used for the final fractionation step. Western analysis was performed according to standard protocols. Nuclear halos were prepared according to Gerdes et al. (1994), except that the cells were obtained by dissecting and manually disrupting imaginal disk cells from third instar larvae with dissecting needles and spun onto coverslips at 350 g for 15 min. Samples that were treated with RNase were extracted with 2 M NaCl, as before, and then were incubated with 200 µg/ml of RNase A for 1 h at 4°C.
Immunocytochemistry and FISH analysis
Antibodies against Su(Hw) and Mod(mdg4)2.2 were prepared as previously described (Gerasimova and Corces, 1998; Mongelard et al., 2002). Antibodies against Mod(mdg4)2.2 recognize only this isoform, which is the only one present in the gypsy insulator (Mongelard et al., 2002). Monoclonal antibodies against lamin were obtained from P. Fisher (The State University of New York at Stony Brook, Stony Brook, NY), H. Saumweber (Humboldt Universitaet Berlin, Berlin, Germany), and Y. Gruenbaum (The Hebrew University of Jerusalem, Jerusalem, Isreal); Ubx antibodies were obtained from J. Botas (Bayer College of Medicine, Houston, TX). Immunolocalization of proteins on nuclear halos was performed as follows: coverslips with samples were incubated 3 x 20 min in 1% BSA, 0.1% TX-100, 1x PBS (BBST) and then incubated in 1:100 dilution of primary antibody overnight at 4°C in a humidified chamber. Samples were then washed 3 x 1 min and 3 x 15 min in 1x BBST and then incubated in 1:500 FITC- or Texas redconjugated secondary antibody in 1x BBST for 1 h at 37°C in a humidified chamber. The samples were then washed 3 x 1 min and then 3 x 15 min in 1x BBST without BSA, coated with DAPI-containing Vectashield (Vector Laboratories), and then visualized with a Carl Zeiss MicroImaging, Inc. fluorescence light microscope using MetaMorph (Universal Imaging Corp.) imaging software. For FISH analysis, probes A, B, and C were made from DNA from BAC clones 20K1, 35A, and 26L11 respectively representing the X chromosome at subdivisions 7B27B8. BAC clones were obtained from BACPAC Resources, and DNA was prepared following their protocol. Probes were synthesized using DIG-UTP or Biotin-UTP following a protocol from Boehringer. FISH on the untreated and 2 M NaCl-extracted halos was performed following protocols established by Gerdes et al. (1994) with the following exceptions. The probes were denatured for 5 min at 95°C. Washes after 16 h incubation with probe were 3 x 5 min in 2x SSC at 42°C, 3 x 5 min in 0.1x SSC at 60°C, and 2 x 30 min in 4x SSC with 1.5% BSA at 37°C. The samples were then incubated in 1:500 secondary antibody in 4x SSC with 1.5% BSA at 37°C in a humidified chamber for 1 h. The samples were washed 3 x 1 min in 4x SSC, 1 x 10 min in 4x SSC, 1 x 10 min in 4x SSC with 0.1% TX-100, 1 x 10 min in 4x SSC, 3 x 5 min in 1x PBS with 0.1% TX-100, and then 3 x 1 min in 1x PBS. The samples were then coated with Vectashield and visualized as described above. Chi-squared analyses were done using Statistica 4.0 (Statsoft Inc.). Polytene chromosomes for immunostaining and FISH were prepared as previously described (Gerasimova and Corces, 1998) with the following exceptions. Before immunostaining, FISH was performed by placing the liquid nitrogenfrozen slides in -70°C 95% EtOH at RT for 3 h. Then the samples were air dried, incubated in 2x SSC at 65°C for 1 h, incubated in 65°C 70% EtOH at RT 3 x 10 min, incubated in 95% EtOH at RT 2 x 10 min, denatured in 0.14 M NaOH for 3 min, rinsed in 2x SSC for 5 min, rinsed in 70% EtOH three times, rinsed in 95% EtOH two times, and then air dried. Probes were prepared and denatured as above and added to each slide, covered with coverslips, sealed with rubber cement, and incubated in humidified chambers overnight at 37°C. After hybridization, the rubber cement was removed, and the slides were placed in 2x SSC at 37°C for 2 min, washed 2 x 10 min in 2x SSC at 37°C, 1 x 5 min in 1x SSC at 30°C, 1 x 10 min in 0.1x SSC, 2 x 5 min in 1x PBS, 0.1% TX-100, and then rinsed 1 x 5 min in 1x PBS at room temperature. Immunostaining was performed as previously described (Gerasimova and Corces, 1998).
| Acknowledgments |
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The work reported here was supported by United States Public Health Service Award GM35463 from the National Institutes of Health.
Submitted: 2 May 2003
Accepted: 8 July 2003
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