High precision size measurement of centromere 8 and the 8q24/c-myc gene region in metaphase and interphase human fibroblasts indicate differential condensation

The hypothesis that distinct chromatin domains expand and are remodelled differently when they undergo transcription, replication or cell cycle processes is well accepted. The condensation changes by which chromosomes are transformed at the metaphase-interphase transition are especially interesting and therefore extensively studied by light microscopy; however, quantitative information of the size on specific small chromatin domains during the cell cycle is scarce. In this respect, a serious problem is the determination of structural features close to the resolution limit. In this report we use a novel approach to quantify the lateral extent of the 8q24/c-myc gene domain and the centromeric region of chromosome 8 in doubly labelled normal human foreskin fibroblasts using confocal laser scanning microscopy (CLSM). The domains were analysed in both metaphase spreads and interphase nuclei. These high precision measurements revealed a somewhat smaller (few 10s of nm) lateral extension of the centromere region in metaphase compared to interphase. Surprisingly, within the same cells the lateral extension of the 8q24/c-myc region was significantly smaller in interphase than in metaphase. For comparison the centromere size was more condensed in metaphase than in interphase. This implies a different folding behaviour for specific chromatin domains with opposite condensation behaviour.

Cell type-specific quantitative predictions of radiation-induced chromosome aberrations: a computer model approach

A quantitative computer model was applied to simulate the three-dimensional (3D) spatial organization of chromatin in human cell nuclei under defined conditions of virtual irradiation to explore the implications of spatial organization on chromosome aberrations. To calibrate the virtual irradiation algorithm, a dose-dependent spectrum of radiation-induced chromosome aberrations such as dicentrics, translocations and centric rings was calculated for low-LET radiation doses ranging from 0.5 to 5 Gy. This was compared with the results from experimental studies. While the dose-response curves calculated from model simulations agree well with experimental dose-response curves for dicentrics and translocations, centric rings are significantly more frequent in the model simulation than in experiments despite taking into account exclusive arm territories in the applied Spherical 1 Mbp Chromatin Domain (SCD) computer model explicitly. Taking into account the non-random positioning of chromosome territories observed in lymphocyte cell nuclei (a so-called gene density-correlated arrangement of chromosome territories), aberration frequencies were calculated with the calibrated irradiation algorithm to investigate the impact of chromosome territory neighborhood effects (proximity effects). The absolute frequencies of pairwise exchanges agree well with those found in an experimental study. In conclusion, the results obtained using the computer model approach presented here based on only a few adjustable parameters correlated well with those of experimental studies of chromosome aberration frequencies. Thus the model may be a useful tool in radiation-induced cancer risk estimates in combination with epidemiological studies.

Radial arrangement of chromosome territories in human cell nuclei: a computer model approach based on gene density indicates a probabilistic global positioning code

Numerous investigations in the last years focused on chromosome arrangements in interphase nuclei. Recent experiments concerning the radial positioning of chromosomes in the nuclear volume of human and primate lymphocyte cells suggest a relationship between the gene density of a chromosome territory (CT) and its distance to the nuclear center. To relate chromosome positioning and gene density in a quantitative way, computer simulations of whole human cell nuclear genomes of normal karyotype were performed on the basis of the spherical 1 Mbp chromatin domain model and the latest data about sequence length and gene density of chromosomes. Three different basic assumptions about the initial distribution of chromosomes were used: a statistical, a deterministic, and a probabilistic initial distribution. After a simulated decondensation in early G1, a comparison of the radial distributions of simulated and experimentally obtained data for CTs Nos. 12, 18, 19, and 20 was made. It was shown that the experimentally observed distributions can be fitted better assuming an initial probabilistic distribution. This supports the concept of a probabilistic global gene positioning code depending on CT sequence length and gene density.

Virtual radiation biophysics: implications of nuclear structure

The non-random positioning of chromosome territories (CTs) in lymphocyte cell nuclei has raised the question whether systematic chromosome-chromosome associations exist which have significant influence on interchange rates. In such a case the spatial proximity of certain CTs or even of clusters of CTs is expected to increase the respective exchange yields significantly, in comparison to a random association of CTs. In the present study we applied computer simulated arrangements of CTs to calculate interchange frequencies between all heterologous CT pairs, assuming a uniform action of the molecular repair machinery. For the positioning of CTs in the virtual nuclear volume we assumed a) a statistical, and b) a gene density-correlated arrangement. The gene density-correlated arrangement regards the more experimentally observed interior localization of gene-rich and the more peripheral positioning of gene-poor CTs. Regarding one-chromosome yields, remarkable differences for single CTs were observed taking into account the gene density-correlated distribution of CTs.

Non-random radial higher-order chromatin arrangements in nuclei of diploid human cells

A quantitative comparison of higher-order chromatin arrangements was performed in human cell types with three-dimensionally (3D) preserved, differently shaped nuclei. These cell types included flat-ellipsoid nuclei of diploid amniotic fluid cells and fibroblasts and spherical nuclei of B and T lymphocytes from peripheral human blood. Fluorescence in-situ hybridization (FISH) was performed with chromosome paint probes for large (#1-5) and small (#17-20) autosomes, and for the two sex chromosomes. Other probes delineated heterochromatin blocks of numerous larger and smaller human chromosomes. Shape differences correlated with distinct differences in higher order chromatin arrangements: in the spherically shaped lymphocyte nuclei we noted the preferential positioning of the small, gene dense #17, 19 and 20 chromosome territories (CTs) in the 3D nuclear interior--typically without any apparent connection to the nuclear envelope. In contrast, CTs of the gene-poor small chromosomes #18 and Y were apparently attached at the nuclear envelope. CTs of large chromosomes were also preferentially located towards the nuclear periphery. In the ellipsoid nuclei of amniotic fluid cells and fibroblasts, all tested CTs showed attachments to the upper and/or lower part of the nuclear envelope: CTs of small chromosomes, including #18 and Y, were located towards the centre of the nuclear projection (CNP), while the large chromosomes were positioned towards the 2D nuclear rim. In contrast to these highly reproducible radial arrangements, 2D distances measured between heterochromatin blocks of homologous and heterologous CTs were strikingly variable. These results as well as CT painting let us conclude that nuclear functions in the studied cell types may not require reproducible side-by-side arrangements of specific homologous or non-homologous CTs. 3D-modelling of statistical arrangements of 46 human CTs in spherical nuclei was performed under the assumption of a linear correlation between DNA content of each chromosome and its CT volume. In a set of modelled nuclei, we noted the preferential localization of smaller CTs towards the 3D periphery and of larger CTs towards the 3D centre. This distribution is in clear contrast to the experimentally observed distribution in lymphocyte nuclei. We conclude that presently unknown factors (other than topological constraints) may play a decisive role to enforce the different radial arrangements of large and small CTs observed in ellipsoid and spherical human cell nuclei.

Arrangements of macro- and microchromosomes in chicken cells

Arrangements of chromosome territories in nuclei of chicken fibroblasts and neurons were analysed employing multicolour chromosome painting, laser confocal scanning microscopy and three-dimensional (3D) reconstruction. The chicken karyotype consists of 9 pairs of macrochromosomes and 30 pairs of microchromosomes. Although the latter represent only 23% of the chicken genome they containalmost 50% of its genes. We show that territories of microchromosomes in fibroblasts and neurons were clustered within the centre of the nucleus, while territories of the macrochromosomes were preferentially located towards the nuclear periphery. In contrast to these highly consistent radial arrangements, the relative arrangements of macrochromosome territories with respect to each other (side-by-side arrangements) were variable. A stringent radial arrangement of macro- and microchromosomes was found in mitotic cells. Replication labelling studies revealed a pattern of DNA replication similar to mammalian cell nuclei: gene dense, early replicating chromatin mostly represented by microchromosomes, was located within the nuclear interior, surrounded by a rim of late replicating chromatin. These results support the evolutionary conservation of several features of higher-order chromatin organization between mammals and birds despite the differences in their karyotypes.

Towards a dynamical approach for the simulation of large scale, cancer correlated chromatin structures

To understand the influence of geometrical constraints in the spatial distribution of cancer correlated "Double Minute chromosomes (DMs)" in human cell nuclei, we applied computer simulations of the nuclear 3D structure in combination with a voxel based segmentation algorithm. With this approach we determined the overlap volumes and intensities of the DMs with the chromatin free space in the simulated nucleus. For this purpose, beginning from a start configuration, simulated linear chromosome chains together with the DMs were relaxed according to the Monte Carlo process. The simulations predict a preferential positioning of DMs within the "peripheral" "Inter Chromatin Domain (ICD)" space.

Chromosome territories, interchromatin domain compartment, and nuclear matrix: an integrated view of the functional nuclear architecture

Advances in the specific fluorescent labeling of chromatin in fixed and living human cells in combination with three-dimensional (3D) and 4D (space plus time) fluorescence microscopy and image analysis have opened the way for detailed studies of the dynamic, higher-order architecture of chromatin in the human cell nucleus and its potential role in gene regulation. Several features of this architecture are now well established: 1. Chromosomes occupy distinct territories in the cell nucleus with preferred nuclear locations, although there is no evidence of a rigid suprachromosomal order. 2. Chromosome territories (CTs) in turn contain distinct chromosome arm domains and smaller chromatin foci or domains with diameters of some 300 to 800 nm and a DNA content in the order of 1 Mbp. 3. Gene-dense, early-replicating and gene-poor, middle-to-late-replicating chromatin domains exhibit different higher-order nuclear patterns that persist through all stages of interphase. In mitotic chromosomes early replicating chromatin domains give rise to Giemsa light bands, whereas middle-to-late-replicating domains form Giemsa dark bands and C-bands. In an attempt to integrate these experimental data into a unified view of the functional nuclear architecture, we present a model of a modular and dynamic chromosome territory (CT) organization. We propose that basically three nuclear compartments exist, an "open" higher-order chromatin compartment with chromatin domains containing active genes, a "closed" chromatin compartment comprising inactive genes, and an interchromatin domain (ICD) compartment (Cremer et al., 1993; Zirbel et al., 1993) that contains macromolecular complexes for transcription, splicing, DNA replication, and repair. Genes in "open," but not in "closed" higher-order chromatin compartments have access to transcription and splicing complexes located in the ICD compartment. Chromatin domains that build the "open" chromatin compartment are organized in a way that allows the direct contact of genes and nascent RNA to transcription and splicing complexes, respectively, preformed in the ICD compartment. In contrast, chromatin domains that belong to the "closed" compartment are topologically arranged and compacted in a way that precludes the accessibility of genes to transcription complexes. We argue that the content of the ICD compartment is highly enriched in DNA depleted biochemical matrix preparations. The ICD compartment may be considered as the structural and functional equivalent of the in vivo nuclear matrix. A matrix in this functional sense is compatible with but does not necessitate the concept of a 3D nuclear skeleton existing of long, extensively arborized filaments. In the absence of unequivocal evidence for such a structural matrix in the nucleus of living cells we keep an agnostic attitude about its existence and possible properties in maintaining the higher-order nuclear architecture. Quantitative modeling of the 3D and 4D human genome architecture in situ shows that such an assumption is not necessary to explain presently known aspects of the higher-order nuclear architecture. We expect that the interplay of quantitative modeling and experimental tests will result in a better understanding of the compartmentalized nuclear architecture and its functional consequences.

Three-dimensional spectral precision distance microscopy of chromatin nanostructures after triple-colour DNA labelling: a study of the BCR region on chromosome 22 and the Philadelphia chromosome

Topological analysis of the three-dimensional (3D) chromatin nanostructure and its function in intact cell nuclei implies the use of high resolution far field light microscopy, e.g. confocal laser scanning microscopy (CLSM). However, experimental evidence indicates that, in practice, under biologically relevant conditions, the spatial resolution of CLSM is limited to about 300 nm in the lateral direction and about 700 nm in the axial direction. To overcome this shortcoming, the use of a recently developed light microscopical approach, spectral precision distance microscopy (SPDM) is established. This approach is based on the precise localization of small labelling sites of a given target in spectrally differential images. By means of quantitative image analysis, the bary centres (intensity weighted centroid analogous to the centre of mass) of these independently registered labelling sites can be used as point markers for distance and angle measurements after appropriate calibration of optical aberrations (here, polychromatic shifts). In combination with specific labelling of very small chromatin target sites with dyes of different spectral signatures by fluorescence in situ hybridization (FISH), SPDM presently allows us to analyse the nuclear topology in three-dimensionally conserved nuclei with a 'resolution equivalent', many times smaller than the conventional optical resolution. Chronic myelogeneous leukaemia (CML) is genetically characterized by the fusion of parts of the BCR and ABL genes on chromosomes 22 and 9, respectively. In most cases, the fusion leads to a translocation t(9; 22) producing the Philadelphia chromosome. SPDM was applied to analyse the 3D chromatin structure of the BCR region on the intact chromosome 22 and the BCR-ABL fusion gene on the Philadelphia chromosome (Ph) by using a new triple-colour FISH protocol: two different DNA probes were used to detect the BCR region and the third DNA probe was used to identify the location of the ABL gene. Consistent 3D distance measurements down to values considerably smaller than 100 nm were performed. The angle distributions between the three labelled sites on the Philadelphia chromosome territory were compared to two state-of-the-art computer models of nuclear chromatin structure. Significant differences between measured and simulated angle distributions were obtained, indicating a complex and non-random angle distribution.

Reconstruction of axial tomographic high resolution data from confocal fluorescence microscopy: a method for improving 3D FISH images

Fluorescent confocal laser scanning microscopy allows an improved imaging of microscopic objects in three dimensions. However, the resolution along the axial direction is three times worse than the resolution in lateral directions. A method to overcome this axial limitation is tilting the object under the microscope, in a way that the direction of the optical axis points into different directions relative to the sample. A new technique for a simultaneous reconstruction from a number of such axial tomographic confocal data sets was developed and used for high resolution reconstruction of 3D-data both from experimental and virtual microscopic data sets. The reconstructed images have a highly improved 3D resolution, which is comparable to the lateral resolution of a single deconvolved data set. Axial tomographic imaging in combination with simultaneous data reconstruction also opens the possibility for a more precise quantification of 3D data. The color images of this publication can be accessed from http://www.esacp.org/acp/2000/20-1/heintzmann.++ +htm. At this web address an interactive 3D viewer is additionally provided for browsing the 3D data. This java applet displays three orthogonal slices of the data set which are dynamically updated by user mouse clicks or keystrokes.

Chromatin structure and chromosome aberrations: modeling of damage induced by isotropic and localized irradiation

Various models for the nuclear architecture in interphase cell nuclei have been presented, proposing a territorial or a non-territorial organization of chromosomes. To better understand the correlation between nuclear architecture and the formation of chromosomal aberrations, we applied computer simulations to model the extent of radiation induced chromosome damage under certain geometrical constraints. For this purpose, chromosomes were described by different models, which approximate the chromatin fiber by a polymer chain, folded in different ways. Corresponding to the different condensation levels, a territorial or a non-territorial organization of chromosomes was obtained. To determine the relative frequencies of radiation induced damage, the effects of isotropic ionizing radiation and of a focused laser UV-beam were studied. For isotropic ionizing radiation, the calculated translocation frequencies showed no differences between territorial and non-territorial models except for one special case. For localized irradiation, the results of both organizations were clearly different, with respect to the total number of damaged chromosomes per cell. The predictions agreed well with the experimental data available.