Single-molecule magnetic sequencing

The DNA molecule of interest must be incorporated into a hairpin, and attached to a magnetic bead on one end and to an immobile glass surface on the other end. The hairpin is attached to the glass surface via a digoxigenin-antidigoxigenin bond.[1] The magnetic bead is attached to the opposite end via biotin-streptavidin interaction.[1] Such DNA hairpin setup can be made in two ways:

1) In the case of double-stranded DNA molecules (for whole genome sequencing, or targeted sequencing), the DNA fragment is ligated to a DNA loop at one end and a DNA fork structure, labeled with biotin and digoxigenin at the two ends.[1]

2) For RNA-seq, the mRNA can be trapped on a poly-T-coated bead, where reverse transcription reaction is performed on the bead to generate a cDNA hairpin.[1]

Electromagnets are placed above the sample slide,[6] and an inverted microscope is placed below.[7] The image is captured via a CCD camera and transferred to a computer, where the three-dimensional positions of the magnetic beads are determined. The position of the bead within the horizontal plane of the glass slide, x and y, are determined by real-time correlation of the bead images.[8] The vertical length of the hairpin, measured by the vertical position of the attached magnetic bead, is measured by the bead’s diffraction ring diameter, which increases with distance.[7]

A constant magnetic force is applied to unzip the DNA hairpin, and reducing the force allows the hairpin to rezip.[9] Prior to performing the downstream applications several unzipping and rezipping cycles are performed. While the magnetic force required to unzip and rezip may vary depending on the DNA sequence and hairpin length, their absolute values are not critical as long as they are consistent within a sequencing run.[1]

When the DNA hairpin is unzipped into single-strand, oligonucleotides complementary to the hairpin sequence are allowed to hybridize. During the time course of the rezipping process, the bound oligonucleotides cause transient blockages.[1] The time course measurement of hairpin length allows for the determination of the exact position of the hybridization, as well as the presence of mismatches between the oligonucleotide and the hairpin.[1]

Steps involved in magnetic sequencing by hybridization

Hybridization is one way to determine the sequence of a DNA strand from detecting the changes in the length of a hairpin. When a probe hybridizes to an open hairpin, complete refolding of the hairpin is stalled, and the position of the hybridized probe can be inferred. Thus the sequence of a DNA fragment of interest can be inferred from overlapping the positions of probes sets, which are allowed to hybridize one by one.[10]

First, a DNA fragment can be converted into a new sequence in which each original nucleotide is encoded by a specific 8-nt sequence (A8, T8, G8 and C8)[11] and then ligated to a hairpin.

After applying a magnetic force, in the unzipped state of the hairpin, a small number of discriminating nucleotides can hybridize to the new individual complementary sequences on the hairpin which can transiently block the refolding of the hairpin.

Identification of the blockage positions of the hairpin produced by the hybridization of the discriminating nucleotides can be observed as the pauses in the time course of the hairpin distance measurement. The complete sequence can be reconstructed by the overlapping fragments.

Steps involved in magnetic sequencing by ligation

Another application for the magnetic sequencing is using the hairpin end-to-end distance to detect the successive ligation of oligonucleotide.[12] First step of sequencing by ligation is using a primer to extend a DNA fragment. Extension is first attempted with a fragment starting with adenine, which can only be ligated if the next nucleotide on the opposite strand is a thymine. Then fragments starting with cytosine, guanine and thymine are attempted in turn, and the cycle is repeated. The magnetic field is released after each ligation, and then the length of the extended primer is measured. Upon ligation the primer is extended by seven bases, which is resulting in a detectable increase in the hairpin’s end to end distance. RNase cleavage at position 2 is followed by the ligation for the preparation of the next ligation cycle, so that the next ligation is positioned just ahead of the previous one.[10]

7-nt primer library, 5′-NNNNNNrX-3′, are used in the ligation of a short degenerate oligonucleotide fragmentin, in which N represents any of the four deoxyribonucleotides and Nr represents any of the four ribonucleotides, X is the tested base(A,G,C,T). The ligation to a primer strand of each of the four tested bases in hairpin opening and closing cycles are tested.[1]

7-nt primer ligates in the open state of the hairpin, which will block rezipping of the last seven nucleotides and increase the distance between the surface and the magnetic bead by ~5 nm.[1] If the ligation is not successful, no change in the hairpin length is observed.

RNase cleavage of the last six nucleotides is the next step following the ligation, ultimately extending the primer strand by a single base. Such cleavage allows rezipping of 6 nucleotides of the hairpin, signaled by a decrease in hairpin length of ~4 nm.[1] Therefore, an incorporation of a complementary nucleotide is indicated by an increase in 7 nucleotides (+5 nm) followed by a decrease in 6 nucleotides (-4 nm).[1]

After the RNase cleavage of the last six nucleotides, the next step is phosphorylation of the 5'-end via Kinase. Then the next cycle of ligation can be repeated.

Many of the competitive single-molecule sequencing methods rely on the incorporation of fluorescently labeled nucleotides.[4][5] In next-generation sequencing, the fluorescence signal of clusters can be easily detected. However, when the same concept is applied to single-molecule sequencing, the largest complication results from the high error rates. Because it is difficult to detect single labeled molecules, these platforms suffer from low signal-to-noise ratios, often resulting in misdetection or non-detection of fluorescent signals.[13] In the case of magnetic sequencing, the signal measured is the changes in distance between two ends of a hairpin. Such signal can be readily detected with standard cameras. Thus, the signals are easier to detect, even without the use of expensive imaging devices.

In addition to the nature of the detected signal, other implementations in this platform allows for an even higher signal-to-noise ratio. In the case of magnetic sequencing by hybridization, a set of overlapping tiles is used such that the sequence of each nucleotide is determined by the hybridization of an 8-mer.[1] Therefore, the instrument only requires the sensitivity to detect a change of ~ 6 nm (the length of 8 nucleotides). Similarly, for sequencing by ligation cycles, successful incorporation is characterized by a ~5 nm increase (ligation of a 7-mer) followed by a ~ 4 nm decrease (RNase cleavage of 6-mer) in hairpin length.[1] In this case, the decrease in length in the second step provides additional confirmation for the obtained signal.

With the current methods, the instrumental error in the measured hairpin length is 1-1.5 nm.[1] The length of a basepair, or 2 extended single-stranded nucleotides, is approximately 0.85 nm.[1] Therefore, the resolution of the system is at a few nucleotides. The sources of noise arise from length-dependent Brownian motion of the bead anchored by the extended hairpin, statistical error in bead position determination, and slow mechanical drifts.[1] However, as mentioned earlier, such resolution is sufficient for the current sequencing method because changes in >4 nm are being measured.

Through the use of magnetic traps,[6] constant magnetic force can be applied to millions of DNA hairpin-tethered magnetic beads in parallel. The magnetic force can be easily adjusted by changing the distance between the trap and the magnetic beads. The number of eads that can be simultaneously monitored, which determines the read throughput of this platform, is limited by the bead size, length of the tethered DNA hairpin, and the optical resolution limit.[1] Currently, a density of 750 K/mm² (comparable to an Illumina HiSeq 2000)[14] can be achieved.[1]

As mentioned above, the noise due to the Brownian fluctuations of the bead increases with length. Robust sequencing tests have yet to be performed to determine the maximum read length of this system. However, the ligation of a 7-mer in the middle of a 1241 nucleotide-long hairpin was successfully detected, suggesting that the current system is sufficient to sequence up to ~500 bp.[1]

The rate of sequencing or imaging is dependent on the mechanical movement speed of the magnetic beads, which is limited by drag force.[1] Currently, it is possible to measure 10 hairpin open-close cycle per second.[1] Additional complications include the existence of a secondary hairpin structure in the DNA of interest. In such a case the DNA loop to be ligated must be designed such that it its closing is favored over the closing of the endogenous loop in the DNA of interest.[1]