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Published online before print
August 3, 2007, 10.1101/gr.6522707 Genome Res. 17:1296-1303, 2007 ©2007 by Cold Spring Harbor Laboratory Press; ISSN 1088-9051/07 $5.00
Letter Architectures of somatic genomic rearrangement in human cancer amplicons at sequence-level resolution1 Wellcome Trust Sanger Institute, Hinxton, Cambridge, CB10 1SA, United Kingdom; 2 Department of Pathology, University of Cambridge, Hutchinson/MRC Research Centre, Cambridge, CB2 2XZ, United Kingdom; 3 Institute of Cancer Research, Sutton, Surrey, SM2 5NG, United Kingdom
For decades, cytogenetic studies have demonstrated that somatically acquired structural rearrangements of the genome are a common feature of most classes of human cancer. However, the characteristics of these rearrangements at sequence-level resolution have thus far been subject to very limited description. One process that is dependent upon somatic genome rearrangement is gene amplification, a mechanism often exploited by cancer cells to increase copy number and hence expression of dominantly acting cancer genes. The mechanisms underlying gene amplification are complex but must involve chromosome breakage and rejoining. We sequenced 133 different genomic rearrangements identified within four cancer amplicons involving the frequently amplified cancer genes MYC, MYCN, and ERBB2. The observed architectures of rearrangement were diverse and highly distinctive, with evidence for sister chromatid breakage–fusion–bridge cycles, formation and reinsertion of double minutes, and the presence of bizarre clusters of small genomic fragments. There were characteristic features of sequences at the breakage–fusion junctions, indicating roles for nonhomologous end joining and homologous recombination-mediated repair mechanisms together with nontemplated DNA synthesis. Evidence was also found for sequence-dependent variation in susceptibility of the genome to somatic rearrangement. The results therefore provide insights into the DNA breakage and repair processes operative in somatic genome rearrangement and illustrate how the evolutionary histories of individual cancers can be reconstructed from large-scale cancer genome sequencing.
Gene amplification may be defined as a somatically acquired increase in copy number of a restricted genomic region and is often found in cancer cells as a mechanism of increasing the transcript and therefore protein levels of dominantly acting cancer genes (Schwab 1999
The processes underlying the development of gene amplification are incompletely understood. One approach to understanding the genesis of amplicons in cancer cells is to characterize their genomic structure. At the level of resolution of light microscopy, amplified regions may exist as extrachromosomal DNA (double minutes) or as large contiguous stretches of amplified DNA (homogenously staining regions, HSRs) (Schwab 1999
Studies of amplicon structure have thus far been conducted at the microscopic level of analysis using FISH and thus have limited resolution. Volik et al. (2003
Cell lines HCC1954 is an immortal cell line derived from an invasive ductal carcinoma of the breast diagnosed in a 61-yr-old woman; NCI-H2171 is an immortal cell line derived from a metastatic small cell lung cancer in a pleural effusion from a 50-yr-old male Caucasian smoker; and NCI-H1770 is a lung neuroendocrine neoplasm arising in a 57-yr-old male Caucasian non-smoker.
Copy number analysis
Spectral karyotype and FISH analysis The spectral karyotype of HCC1954 was pseudotetraploid (http://www.path.cam.ac.uk/~pawefish; M. Grigorova, unpubl.). FISH using BACs from the amplified region on chromosome 17q that includes ERBB2 showed that this amplicon was constituted as two extended HSRs. Multicolor FISH using BACs from the chromosome 5p15.33, 5q35.2-q35.3, and 8q24.21-q24.22 (MYC) regions of amplification revealed two chimeric amplicons where all three signals co-localized. Multicolor FISH further demonstrated that these chimeric amplicons were physically separate from the chromosome 17q HSRs that include ERBB2 (Supplemental Fig. 2). The spectral karyotype of NCI-H2171 was hypodiploid. (http://www.path.cam.ac.uk/~pawefish). Multicolor FISH showed that all the amplified regions in this cell line from chromosomes 8, 11, 12, and 14 (Table 1) mapped to one chimeric amplicon (Supplemental Fig. 2).
The spectral karyotype of NCI-H1770 was pseudotetraploid and showed a large HSR of chromosome 2 origin inserted into chromosome 12 (Grigorova et al. 2005
End sequencing of bacterial artificial chromosome (BAC) libraries A subset of BACs from each library was not co-linear with the reference genome sequence. These putatively rearranged BACs were also over-represented in regions of amplification with 46.7%, 36.7%, and 23.2% mapping to amplicons in HCC1954, NCI-H2171, and NCI-H1770 respectively. The proportion of BACs that were rearranged in amplified regions was also elevated: 12.5%, 17.4%, and 18.0% of BACs were rearranged within the amplicons of HCC1954, NCI-H2171, and NCI-H1770 compared to 2.0%, 1.8%, and 1.3% in the whole genome (Table 1). Thus, there is a higher prevalence of genomic rearrangements in amplicons.
Sequence analysis of BACs showing evidence of rearrangement Nine rearranged BACs were from the 17q amplicon in HCC1954 that includes ERBB2. In each of these BACs, only a single BFJ was present, and these joined sequences located within the 17q amplicon. One rearrangement was observed in seven independent BACs and mapped telomeric to ERBB2. The seven BACs carrying the identical rearrangement appear to be different recombinant clones as the genome–vector ligation junctions were different in each case. Two further rearrangements were each present in a single BAC. These mapped centromeric to ERBB2. Thus only three unique BFJs were identified in this amplicon (Fig. 1), and the differing frequency of the three BFJs is likely to reflect different levels of amplification of the three rearrangements. The sequences either side of each of the three BFJs were in inverted orientation with respect to each other. Moreover, in each instance the sequences to either side of each BFJ aligned to essentially the same position in the reference genome, although there were small gaps of 4567, 1556, and 1462 bp between the two ends. These rearrangements therefore are inverted duplications with small amounts of sequence missing at the BFJ.
Twelve rearranged BACs from the chimeric chromosome 5/8 amplicon in HCC1954 contained 57 unique BFJs. Eighteen BFJs bridged chromosomes, joining regions from chromosome 8q to regions on chromosome 5. Fifteen BFJs joined pairs of regions on chromosome 5 and 24 joined pairs of regions on chromosome 8 (Supplemental Table 1). Twenty-two intrachromosomal rearrangements were inverted, and 17 were noninverted. No inverted duplications were observed. In several BACs with multiple BFJs, the junctions were not distributed randomly throughout the BAC. Instead, the BFJs appear to cluster, with several small fragments of genome ranging from 72 bp to a few kb in length strung end to end (Supplemental material Table 1, Fig. 1). The 24 BACs from the chimeric amplicon of NCI-H2171 contained a total of 64 different somatically acquired BFJs. Nineteen were interchromosomal, and 45 were intrachromosomal rearrangements, of which 23 were noninverted and 22 were inverted. One BAC (9g20) contained a large inverted duplication, which results in duplication of two BFJs (Supplemental material Table 1, Fig. 1). As was the case for the 5/8 amplicon in HCC1954, there were several BACS with clustering of several small fragments of genome (Supplemental material Table 1, Fig. 1). Eight recombinant BACs from the chromosome 2 amplicon in NCI-H1770 were sequenced, yielding nine unique BFJs (Fig. 1). All were intrachromosomal and connected genomic areas within the chromosome 2 amplicon. Five were in noninverted orientation to each other, and four were inverted. No inverted duplications were observed. One BFJ (Supplemental Table 1, no. 130) was identified in two sequenced BACs as well as two additional BACs in which the junction was predicted from the BAC end-sequence data and confirmed by PCR. This BFJ was the most commonly observed and therefore the most highly amplified BFJ in this line. The structure of this BFJ bears the hallmarks expected of a double-minute chromosome (see Discussion).
DNA sequences at breakage–fusion junctions
A different pattern was observed at three BFJs in HCC1954 (Supplemental Table 1, BFJs nos. 121, 71, and 74). These were characterized by relatively long microhomologies (10, 15, and 32 bp) and were within inverted Alu repeats (Fig. 2). Beyond the region of sequence identity in the microhomology, there was a much longer region of >80% sequence similarity either side of the BFJ. This extended sequence similarity was not observed at BFJs with shorter microhomologies. This pattern corresponds more closely to that expected for a double-strand break repair mechanism using nonallelic homologous recombination.
The remaining 26/133 (19%) of the BFJs could not be aligned to the reference genome without allowing insertion of a short DNA sequence from 1 to 64 bp in size between two putative breakpoints that did not align to the reference human genome as part of either flanking sequence or to a unique location elsewhere in the genome. Five of these insertions were longer than 20 bp. One of these gave no significant alignment to the reference human genome using BLASTN (http://www.ncbi.nlm.nih.gov/genome/seq/BlastGen/BlastGen.cgi?taxid=9606) or BLAT (no. 60 [24-bp insertion]). The remaining four (no. 20 [25-bp insertion], no. 36 [37-bp insertion], no. 5 [44-bp insertion], and no. 78 [64-bp insertion]) contained short regions that mapped to multiple locations in the genome and that did not account for the full length of the insertion. These inserted sequences may represent nontemplated DNA synthesis, clusters of very short DNA fragments, or, conceivably in some cases, unique sequences containing SNPs (see Discussion; Table 2; Supplemental Tables 1, 3).
We have explored the underlying mechanisms of gene amplification in human cancer by identifying somatic genomic rearrangements in cancer amplicons and using the observed patterns to reconstruct the breakage and fusion processes involved. To achieve this, we end-sequenced more than 13,000 BACs and obtained finished shotgun sequences from 57, thus characterizing 133 unique somatic BFJs (derived from fusion of 266 somatic breakpoints) (Fig. 1; Supplemental Table 1), several fold more than have been previously reported in solid tumor genomes. A total of 30 genes were affected by the somatic breakpoints identified, and in 19 BFJs the rearrangement fused part of the genomic sequences of two genes. However, none of the BFJs apposed coding sequence from the gene pair in the correct orientation while maintaining the translational frame, indicating that a functional fusion gene is unlikely to have been created. Nevertheless, the results illustrate how this strategy, particularly when coupled with the application of new sequencing technologies, could be implemented to identify fusion genes in cancer.
Three unique inverted duplications, and no other rearrangements, were observed among the nine rearranged BACs from the 17q21.1 amplicon in HCC1954 that includes ERBB2 (Fig. 1A; Table 1; Supplemental Table 1). The architecture of rearrangements in this amplicon recapitulates remarkably well the structural features predicted by a classical breakage–fusion–bridge cycle involving sister chromatids, as originally proposed by Barbara McClintock (1941)
The model predicts that the sequences either side of each BFJ should be identical. We found, however, that there appears to have been a few kilobases of erosion leading to differences in the lengths of the sister chromatids prior to fusion. This erosion has previously been observed in an inverted duplication created as a result of sister chromatid breakage–fusion–bridge cycles during amplification of the DHFR gene in methotrexate-treated Chinese hamster cells (Okuno et al. 2004 The simplest model of the sister chromatid breakage–fusion–bridge cycle has two further predictions: (1) that the first inverted duplication will occur telomeric to the amplified cancer gene while all subsequent inverted duplications will be centromeric (see Supplemental Fig. 4); (2) that the amplified cancer gene will be present at approximately twice the copy number of the first inverted duplication, which itself will be at twice the copy number of the second BFJ. In HCC1954, the highest copy number inverted duplication in the ERBB2 amplicon (which is therefore likely to have been the first that occurred) mapped telomeric of ERBB2 and was present at about half the copy number of ERBB2 (Supplemental Table 4). The other inverted duplications were at lower copy numbers and were centromeric. Therefore, the ERBB2 amplicon in HCC1954 bears all the architectural hallmarks at the sequence level of a classical sister chromatid breakage–fusion–bridge process, the first time that this has been demonstrated in human cancer.
Rearrangements in the chromosome 2 amplicon of NCI-H1770 that includes MYCN exhibited a different pattern (Fig. 1D). Although the rearrangements were restricted to the region surrounding MYCN, there were both inverted and noninverted BFJs and inverted duplications were not observed. Four independent BACs contained an identical noninverted rearrangement (Supplemental Table 1, no. 130), which provides a clue to the processes involved in the formation of this amplicon. The particular orientation, structure, and breakpoint locations of this BFJ are compatible with looping out and excision of DNA to form a double-minute chromosome. This double minute would encompass the amplified region and bring the ends of the region, which are The patterns of rearrangement found in the chimeric amplicons of HCC1954 and NCI-H2171 (Fig. 1B,C) were considerably more complex than the two previously described. Several BACs carried multiple BFJs, many of which formed interchromosomal in addition to inverted and noninverted intrachromosomal rearrangements. Notably, in many BACs from these two amplicons, the BFJs were not randomly distributed (see Supplemental material Table 1, Fig. 1). Instead, they appear to cluster, with several small fragments of genome, ranging from 20 bp to a few kilobases in length, strung end to end.
The derivation of these bizarre accretions of genomic shards is not clear. However, the small fragments almost always originate from within amplified regions. Moreover, their genomic origins are usually tightly clustered within a few kilobases of each other, often around the position of a chromosomal break (Fig. 3). We therefore propose that a cascade of small DNA fragments is sometimes generated in the vicinity of a chromosomal double strand break (either by physical or enzymatic processes). Each fragment is subsequently fused to an available free end, with a string of fragments sequentially extending during a single cell cycle, until a DNA segment with a telomere terminates the progression. This process, if true, may be similar to the capture of DNA fragments seen during double-strand break repair in model systems (Little and Chartrand 2004
Although these unusual structures in the two chimeric amplicons bear many similarities, there are subtle differences. For example, genomic fragments from the NCI-H2171 and HCC1954 amplicons have significantly different mean lengths of 5797 and 3954 bp, respectively (P = 0.006), indicative either of distinct processes or of processes occurring at different rates. Indeed, in both amplicons the distributions of fragment lengths have significantly greater variation than a simple random breakage model (P < 0.0001), suggesting that more than one breakage process is operative in each. The markedly different patterns of structural rearrangement found in the chromosome 17q21.1 ERBB2 amplicon and the chimeric chromosome 5/8 amplicon (Fig. 1A,B) co-exist in HCC1954 cells, albeit physically isolated from each other. The results therefore illustrate how different evolutionary paths, probably relying on different processes of breakage and repair, can be followed in the same cancer genome.
The DNA sequence at many BFJs showed overlapping microhomologies (Fig. 2; Table 2; Supplemental Tables 1, 3). These are believed to be influential in apposing fragments to be joined and are characteristic of nonhomologous end-joining mechanisms of double-strand break repair (Cahill et al. 2006 There were also traces of DNA breakage and repair processes that are more cryptic to interpretation. Twenty-six BFJs showed insertion of short (1–64 bp) DNA segments between the chromosomal breakpoints that could not be aligned to the reference genome as part of either flanking sequence or to a unique location elsewhere in the genome (Supplemental Table 1). Five of these insertions were longer than 20 bp. One of these gave no significant alignment to the reference human genome, and the remaining four contained short regions that mapped to multiple locations in the genome but that did not account for the full length of the insertion. These insertions may represent clusters of such small DNA fragments that their origin in the reference genome cannot be unambiguously ascertained. Alternatively, they may be the result of nontemplate-dependent DNA synthesis or a combination of the two processes. Twenty-two such insertions were observed in NCI-H2171 and only three in HCC1954 (Fig. 1; Table 2), suggesting that the variant of breakage or repair processes that this pattern represents is more active in NCI-H2171.
The large number of breakpoints detected in this study further allows us to investigate whether there are structural features of the genome that are particularly prone to breakage or repair (Abeysinghe et al. 2003
We recently described the variation in prevalence and pattern of somatic point mutations in human cancer genomes (Greenman et al. 2007
Cell culture and copy number analysis The HCC1954, NCI-H2171, and NCI-H1770 cell lines were obtained from the American Type Culture Collection. Copy number analysis was carried out using the Affymetrix 10K SNP array as previously described (Bignell et al. 2004
BAC library construction
BAC end sequencing and clone selection
Sequencing of BACs and breakpoint analysis
Quantitative PCR
Fluorescence in situ hybridization and spectral karyotyping
Statistical analysis
Modeling breakages as a Poisson process will lead to shard lengths with exponential distributions. Goodness-of-fit to an exponential distribution was assessed as follows. If s represents the set of n shard lengths, the test distribution P(s) =
s = n . We can then simulate any test statistic using this distribution without requiring knowledge of the nuisance parameter . One hundred thousand simulations were used in the application. The test statistic used was the sample standard deviation, providing a goodness-of-fit test sensitive to distributions with variances either greater or smaller than that of an exponential distribution.
The studies were supported by the Wellcome Trust, Cancer Research, United Kingdom, and the Michael and Betty Kadoorie Cancer Genetics Research Programme.
4 Corresponding authors. E-mail mrs{at}sanger.ac.uk; fax +44-(0)1223-494809.
E-mail paf{at}sanger.ac.uk; fax +44-(0)1223-494809. [Supplemental material is available online at www.genome.org.] Article published online before print. Article and publication date are at http://www.genome.org/cgi/doi/10.1101/gr.6522707
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Received March 20, 2007; accepted in revised format June 18, 2007.
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