A new chromosome model

We present a new model of the three-dimensional structure of chromosomes. With DNA and protein staining it could be shown by high-resolution scanning electron microscopy that metaphase chromosomes are mainly composed of DNA packed in "chromomeres" (coiled solenoides) and a dynamic matrix formed of parallel protein fibers. In the centromeric region, the chromomeres are less densely packed, giving insight into the matrix fibers. We postulate that chromosome condensation is achieved by the binding of solenoids to matrix fibers which have contact sites to one another and move antiparallel to each other. As condensation progresses, loops of solenoids accumulate to form additional chromomeres, causing chromosomes to become successively shorter and thicker as more chromomeres are formed. For sterical reasons, a tension vertical to the axial direction forces the chromatids apart. The model can simply explain the enormous variety of chromosome morphology in plant and animal systems by varying only a few cytological parameters. Primary and secondary constrictions and deletions are defined as regions devoid of chromomeres. Even in the highly condensed metaphase, all genes would be easily accessible.     

Nuclear proteins : III. The fibrillar nature of the nuclear matrix

The nuclear matrix of mouse liver nuclei was examined after extraction of the chromatin with high salt, deoxyribonuclease and Triton X-100. The residual nuclear matrix is composed of a nuclear pore-lamina complex, fibrillar nucleoli, and intranuclear matrix. Whole mount electron microscopy shows that a portion of the nuclear matrix is composed of 20–30 Å protein fibers which we call matrixin. The fibers may associate to form larger 100–300 Å fibers. When mouse testicular cells were used, intact synaptonemal complexes and the sex vesicle were intimately associated with the matrix and we suggest these structures may be composed of matrixin. SDS gel electrophoresis of the matrix shows three major polypeptides of 65 000, 67 000 and 68 000 D. Several observations suggest DNA is attached to the matrix at many sites throughout the nucleus. The matrix may play a role in the arrangement of chromatin into the chromomeres of meiotic and mitotic chromosomes.     

Ultrastructural analysis of chromatin in meiosis I + II of rye (Secale cereale L.)

Scanning electron microscopy (SEM) proves to be an appropriate technique for imaging chromatin organization in meiosis I and II of rye (Secale cereale) down to a resolution of a few nanometers. It could be shown for the first time that organization of basic structural elements (coiled and parallel fibers, chromomeres) changes dramatically during the progression to metaphase I and II. Controlled loosening with proteinase K (after fixation with glutaraldehyde) provides an enhanced insight into chromosome architecture even of highly condensed stages of meiosis. By selective staining with platinum blue, DNA content and distribution can be visualized within compact chromosomes as well as in a complex arrangement of fibers. Chromatin interconnecting threads, which are typically observed in prophase I between homologous and non-homologous chromosomes, stain clearly for DNA. In zygotene transversion of chromatid strands to their homologous counterparts becomes evident. In pachytene segments of synapsed and non-synapsed homologs alternate. At synapsed regions pairing is so intimate that homologous chromosomes form one filament of structural entity. Chiasmata are characterized by chromatid strands which traverse from one homolog to its counterpart. Bivalents are characteristically fused at their telomeric regions. In metaphase I and II there is no structural evidence for primary and secondary constrictions.     

Differences in the structural organization of the G- and R-bands detectable during the differential decondensation of chromosomes

The ultrastructure of G- and R-bands in differentially decondensed chromosomes of Chinese hamster was studied with a gradual decrease in CaCl2 concentration in the medium. The gradual reduction of CaCl2 concentration leads to the decondensation of compact G-bands into chromonemes, chromomeres and further into DNP-fibrils. In the complete local decondensation zones (R-bands), the DNP-fibril orientation is parallel to the chromosome longitudinal axis. These zones have no lateral loops or chromomeres. Thus, different chromosome regions corresponding to G- and R-bands possess different sensibility to the decondensing action. Following the complete decondensation in the calcium-free medium chromosomes can be "reconstructed" by adding Ca2+. The data obtained permit to suggest a "fastener" model of the mitotic chromosome organization in which the chromosome represents an hierarchy of discrete structures--G-bands, chromomeres, nucleomeres (superbeads) and nucleosomes. The structural integrity of these levels is supported by specific protein "fasteners".     

Ultrastructure of the mitotic chromosomes in pig embryonic kidney cells during their reversible artificial decondensation in vivo

Using methods of in vivo observation and ultrathin sectioning, it is shown that chromosomes of metaphase PE cells, previously treated with diluted Henk's solutions (70, 30 and 15%), undergo some structural transitions resulting in the formation of micronuclei. At the early stages of hypotonic treatment chromosomes are seen considerably swollen and losing the higher levels of organization, including the chromonema and chromomeres. The chromosomal bodies are formed by DNP fibers 10-25 nm in diameter making loops radiating from the central part of the chromatids. Chromosomes are capable of recondensing from this state by consecutive reconstitution of G-bands, chromomeres and the chromonema. The subsequent secondary decondensation of chromosomes is analogous to telophase decondensation at the normal mitosis, but it results in the formation of a great number of small nuclei (micronuclei). The chromatin structure in micronuclei as well as their ability to synthesize RNA and to replicate DNA show these effects to be reversible. It has been suggested that the loop organization of DNP may be essential for sustaining the structural integrity of the mitotic chromosome.     

Chromosome condensation in mitosis and meiosis of rye (Secale cereale L.)

Structural investigation and morphometry of meiotic chromosomes by scanning electron microscopy (in comparison to light microscopy) of all stages of condensation of meiosis I + II show remarkable differences during chromosome condensation in mitosis and meiosis I of rye (Secale cereale) with respect to initiation, mode and degree of condensation. Mitotic chromosomes condense in a linear fashion, shorten in length and increase moderately in diameter. In contrast, in meiosis I, condensation of chromosomes in length and diameter is a sigmoidal process with a retardation in zygotene and pachytene and an acceleration from diplotene to diakinesis. The basic structural components of mitotic chromosomes of rye are "parallel fibers" and "chromomeres" which become highly compacted in metaphase. Although chromosome architecture in early prophase of meiosis seems similar to mitosis in principle, there is no equivalent stage during transition to metaphase I when chromosomes condense to a much higher degree and show a characteristic "smooth" surface. No indication was found for helical winding of chromosomes either in mitosis or in meiosis. Based on measurements, we propose a mechanism for chromosome dynamics in mitosis and meiosis, which involves three individual processes: (i) aggregation of chromatin subdomains into a chromosome filament, (ii) condensation in length, which involves a progressive increase in diameter and (iii) separation of chromatids.     

Organization of higher-level chromatin structures (chromomere,chromonema and chromatin block) examined using visible light-induced chromatin photo-stabilization

The method of chromatin photo-stabilization by the action of visible light in the presence of ethidium bromide was used for investigation of higher-level chromatin structures in isolated nuclei. As a model we used rat hepatocyte nuclei isolated in buffers which stabilized or destabilized nuclear matrix. Several higher-level chromatin structures were visualized: 100nm globules-chromomeres, chains of chromomeres-chromonemata, aggregates of chromomeres-blocks of condensed chromatin. All these structures were completely destroyed by 2M NaCl extraction independent of the matrix state, and DNA was extruded from the residual nuclei (nuclear matrices) into a halo. These results show that nuclear matrix proteins do not play the main role in the maintenance of higher-level chromatin structures. Preliminary irradiation led to the reduction of the halo width in the dose-dependent manner. In regions of condensed chromatin of irradiated nucleoids there were discrete complexes consisting of DNA fibers radiating from an electron-dense core and resembling the decondensed chromomeres or the rosette-like structures. As shown by the analysis of proteins bound to irradiated nuclei upon high-salt extraction, irradiation presumably stabilized the non-histone proteins. These results suggest that in interphase nuclei loop domains are folded into discrete higher-level chromatin complexes (chromomeres). These complexes are possibly maintained by putative non-histone proteins, which are extracted with high-salt buffers from non-irradiated nuclei.     

Elementary structures in polytene chromosomes of Drosophila melanogaster

Whole-mounted polytene chromosomes were isolated from nuclei by microdissection in 60% acetic acid and analyzed by electron microscopy. Elementary chromosome fibers in the interchromomeric regions and individual chromomeres can be distinguished in polytene chromosomes at low levels of polyteny (2⁶–2⁷ chromatids). Elementary fibers in the interbands are oriented parallel to the axis of the polytene chromosome. Their number roughly corresponds to the expected level of polyteny. These fibers have an irregular beaded structure, 100–300 Å in diameter, and there is no apparent lateral association between them in the interchromomeric regions. Most bands, in contrast, form continuous structures crossing the entire width of the chromosome. Polytene chromosomes isolated in 2% or 10% acetic acid can be reversibly dispersed in a solution for chromatin spreading. The spread chromosomes consist of long uniform deoxyribonucleoprotein (DNP) fibers with a nucleosome structure. This supports the notion that continuous DNA molecules extend through the entire length of a polytene chromosome and that the nucleosome structure exists both in bands and interbands. Analysis of the band shape and of the fibrillar pattern in the interbands emphasizes that the polytene chromosome assumes a ribbonlike structure from which the more complex three-dimensional structure of the polytene chromosome at higher levels of polyteny develops.     

High resolution detection of uncoated metaphase chromosomes by means of field emission scanning electron microscopy

HeLa metaphase chromosomes were exammed by means of in lens field emission scanning electron microscopy, which permits high resolution detection of uncoated biological samples. By using uncoated chromosomes as a model for comparison we report evidence of how traditional scanning electron microscopy techniques such as metal coating and conductive methods can generate errors in chromosome structure evaluation, since both give rise to morphological artifacts. By comparing the morphology of uncoated chromosomes obtained by two different isolation procedures, such as that utilized in standard cytogenetics and the polyamine method, we have drawn the following conclusions: (a) the standard cytogenetic method gives rise to a chromosome structure consisting of a flattened network of 10 nm fibers, in which higher order chromatin organization is absent. (b) Chromosomes obtained by the polyamine method show both three-dimensional profile and higher level folding of chromatin fibers, supporting the loop chromosome organization previously suggested by scanning electron microscopy observation of hexylene glycol isolated chromosomes.     

Selective cleaning of the cell debris in human chromosome preparations studied by scanning force microscopy

The chromosome structure is one of most challenging biological structures to be discovered. Most evidence about the structure comes from optical microscopy. Scanning force microscopy (SFM) can achieve molecular resolution and allows imaging in liquids. However, little information about the chromosome structure has been revealed by SFM. In this work, a mild enzymatic treatment is applied to the chromosomes to remove selectively the RNA and proteins coming from the cell. The resulting SFM images indicate that a protein film with embedded RNA molecules covers chromosomes in standard cytogenetic preparations. The thickness of the protein layer is 15-35 nm and the RNA adheres preferentially to the chromosome surface. The cell material film results in a quite smooth chromosome surface without evidence of any structural detail. After treatment, the chromosome was cleaned from cell residues and individual chromatin fibers at the surface were resolved. Furthermore, insights about the higher order structure of the chromosome can be inferred.     

Quantitative analysis of single-molecule force spectroscopy on folded chromatin fibers

Single-molecule techniques allow for picoNewton manipulation and nanometer accuracy measurements of single chromatin fibers. However, the complexity of the data, the heterogeneity of the composition of individual fibers and the relatively large fluctuations in extension of the fibers complicate a structural interpretation of such force-extension curves. Here we introduce a statistical mechanics model that quantitatively describes the extension of individual fibers in response to force on a per nucleosome basis. Four nucleosome conformations can be distinguished when pulling a chromatin fiber apart. A novel, transient conformation is introduced that coexists with single wrapped nucleosomes between 3 and 7 pN. Comparison of force-extension curves between single nucleosomes and chromatin fibers shows that embedding nucleosomes in a fiber stabilizes the nucleosome by 10 k_BT. Chromatin fibers with 20- and 50-bp linker DNA follow a different unfolding pathway. These results have implications for accessibility of DNA in fully folded and partially unwrapped chromatin fibers and are vital for understanding force unfolding experiments on nucleosome arrays.     

The visualization of large organized chromatin domains enriched in the H3K9me2 mark within a single chromosome in a single cell

Despite considerable efforts, our understanding of the organization of higher order chromatin conformations in single cells and how these relate to chromatin marks remains poor. We have earlier invented the Chromatin In Situ Proximity (ChrISP) technique to determine proximities between chromatin fibers within a single chromosome. Here we used ChrISP to identify chromosome 11-specific hubs that are enriched in the H3K9me2 mark and that project toward the nuclear membrane in finger-like structures. Conversely, chromosome 11-specfic chromatin hubs, visualized by the presence of either H3K9me1 or H3K9me3 marks, are chromosome-wide and largely absent at the nuclear periphery. As the nuclear periphery-specific chromatin hubs were lost in the induced reduction of H3K9me2 levels, they likely represent Large Organization Chromatin in Lysine Methylation (LOCK) domains, previously identified by ChIP-seq analysis. Strikingly, the downregulation of the H3K9me2/3 marks also led to the chromosome-wide compaction of chromosome 11, suggesting a pleiotropic function of these features not recognized before. The ChrISP-mediated visualization of dynamic chromatin states in single cells thus provides an analysis of chromatin structures with a resolution far exceeding that of any other light microscopic technique.     

The visualization of large organized chromatin domains enriched in the H3K9me2 mark within a single chromosome in a single cell

Despite considerable efforts, our understanding of the organization of higher order chromatin conformations in single cells and how these relate to chromatin marks remains poor. We have earlier invented the Chromatin In Situ Proximity (ChrISP) technique to determine proximities between chromatin fibers within a single chromosome. Here we used ChrISP to identify chromosome 11-specific hubs that are enriched in the H3K9me2 mark and that project toward the nuclear membrane in finger-like structures. Conversely, chromosome 11-specfic chromatin hubs, visualized by the presence of either H3K9me1 or H3K9me3 marks, are chromosome-wide and largely absent at the nuclear periphery. As the nuclear periphery-specific chromatin hubs were lost in the induced reduction of H3K9me2 levels, they likely represent Large Organization Chromatin in Lysine Methylation (LOCK) domains, previously identified by ChIP-seq analysis. Strikingly, the downregulation of the H3K9me2/3 marks also led to the chromosome-wide compaction of chromosome 11, suggesting a pleiotropic function of these features not recognized before. The ChrISP-mediated visualization of dynamic chromatin states in single cells thus provides an analysis of chromatin structures with a resolution far exceeding that of any other light microscopic technique.     

Microrheology for Hi-C Data Reveals the Spectrum of the Dynamic 3D Genome Organization

The one-dimensional information of genomic DNA is hierarchically packed inside the eukaryotic cell nucleus and organized in a three-dimensional (3D) space. Genome-wide chromosome conformation capture (Hi-C) methods have uncovered the 3D genome organization and revealed multiscale chromatin domains of compartments and topologically associating domains (TADs). Moreover, single-nucleosome live-cell imaging experiments have revealed the dynamic organization of chromatin domains caused by stochastic thermal fluctuations. However, the mechanism underlying the dynamic regulation of such hierarchical and structural chromatin units within the microscale thermal medium remains unclear. Microrheology is a way to measure dynamic viscoelastic properties coupling between thermal microenvironment and mechanical response. Here, we propose a new, to our knowledge, microrheology for Hi-C data to analyze the dynamic compliance property as a measure of rigidness and flexibility of genomic regions along with the time evolution. Our method allows the conversion of an Hi-C matrix into the spectrum of the dynamic rheological property along the genomic coordinate of a single chromosome. To demonstrate the power of the technique, we analyzed Hi-C data during the neural differentiation of mouse embryonic stem cells. We found that TAD boundaries behave as more rigid nodes than the intra-TAD regions. The spectrum clearly shows the dynamic viscoelasticity of chromatin domain formation at different timescales. Furthermore, we characterized the appearance of synchronous and liquid-like intercompartment interactions in differentiated cells. Together, our microrheology data derived from Hi-C data provide physical insights into the dynamics of the 3D genome organization.     

Ultrastructural analysis of maize pachytene karyotypes by three dimensional reconstruction of the synaptonemal complexes

Aldehyde fixation followed by staining with phosphotungstic acid produces differential contrast between the synaptonemal complex and the chromatin of maize pachytene bivalents. Centromeres, heterochromatic knobs and large chromomeres are easily recognised. With this and other staining techniques the nucleolus organizer region can be differentiated into two components. — Microsporocyte nuclei at pachytene were serially sectioned and all ten bivalents reconstructed in five nuclei. An idiogram was derived from the mean chromosome (= synaptonemal complex) lengths, the arm ratios, positions of knobs and the nucleolus organizer region. The idiogram agrees well with that published from light microscopic analyses. However, bivalent lengths are only two thirds of those observed by light microscopy of squash preparations. Many telomeres of the bivalents are connected via chromatin to the nuclear envelope, but a varying number of free bivalent ends are observed in all five reconstructed nuclei. — Bivalents heterozygous for inversion 3b were reconstructed. In the presence of abnormal chromosome 10 (K10) the lateral components of the synaptonemal complex of chromosome 3 formed a typical inversion loop, while in one of the nuclei having no K10 the two lateral components of the long arms of chromosome 3 remained unpaired in the region of inversion heterozygosity. The presence of K10, which increases crossing-over frequencies and promotes intimate pairing at the light microscopic level, was thus found to permit formation of complete synaptonemal complexes in the inverted region. The extra terminal portion of the K10 chromosome folded back on itself and formed a morphologically normal synaptonemal complex in this — possibly non-homologously paired — region. The chromatin of centromeres and knobs from different bivalents were sometimes found to fuse, but the synaptonemal complexes transversing the fused centromeres or knobs retained their individuality.     

The ultrastructure of R-banded chromosomes

Electron microscopy has been used to study the fine structural organization of R-banded chromosomes prepared by treatment of the chromosomes with a hot NaH₂PO₄ solution. The results indicate that there is a structural basis for R-banding with this technique. In comparison to untreated control chromosomes, the R-banded chromosomes had a greatly reduced electron density, suggesting that the heat treatment has a general adverse effect on chromosome structure. Chromatin fibers formed a coarse, irregular network throughout the chromosome and were often enlarged, probably as a result of the fusion of two or more native fibers. The chromatin fibers were more aggregated and had an increased electron density in the R-band regions of the chromosome than in the interbands. This indicates that the treatment has a differential effect on the structure of bands and interbands. A comparison of the ultrastructure of R- and G-banded chromosomes demonstrated that the distribution of aggregated chromatin was reversed by these two types of banding techniques; however, the treatments producing R-banding appeared to induce less extreme differences in the degree of chromatin condensation in band and interband regions than those giving rise to G-banding. It is suggested that alterations of DNA-protein interactions may arise from the differential denaturation of proteins and/or DNA in R-band and interband regions during the heat pretreatment. Such differential alterations in DNA-protein interactions may induce localized changes in the organization of chromatin and may account for the subtle morphological differences observed between the band and interband regions.