Randall E.
Burton‡
*,
Eric J.
White‡
,
Ted R.
Foss
,
Kevin M.
Phillips
,
Robert H.
Meltzer
,
Nanor
Kojanian
,
Lisa W.
Kwok
,
Alex
Lim
,
Nancy L.
Pellerin
,
Natalia V.
Mamaeva
and
Rudolf
Gilmanshin§
U. S. Genomics, Inc., 12 Gill St., Suite 4700, Woburn, MA, USA 01801. E-mail: rburton@usgenomics.com
First published on 14th January 2010
Many applications in pharmaceutical development, clinical diagnostics, and biological research demand rapid detection of multiple analytes (multiplexed detection) in a minimal volume. This need has led to the development of several novel array-based sensors. The most successful of these so far have been suspension arrays based on polystyrene beads. However, the 5 µm beads used for these assays are incompatible with most microfluidic chip technologies, mostly due to clogging problems. The challenge, then, is to design a detection particle that has high information content (for multiplexed detection), is compatible with miniaturization, and can be manufactured easily at low cost. DNA is a solid molecular wire that is easily produced and manipulated, which makes it a useful material for nanoparticles. DNA molecules are very information-rich, readily deformable, and easily propagated. We exploit these attributes in a suspension array sensor built from specialized recombinant DNA, Digital DNA, that carries both specific analyte-recognition units, and a geometrically encoded identification pattern. Here we show that this sensor combines high multiplexing with high sensitivity, is biocompatible, and has sufficiently small particle size to be used within microfluidic chips that are only 1 µm deep. We expect this technology will be the foundation of a broadly applicable technique to identify and quantitate proteins, nucleic acids, viruses, and toxins simultaneously in a minimal volume.
Here we introduce a novel suspension array technology using a specialized DNA molecule—Digital DNA—as a scaffold that carries both an identifier and receptors. Digital DNA molecules are identified by a graphical encoding scheme that permits a high degree of multiplexing and processed by a single-molecule reader previously used for DNA mapping (Fig. 1).14–16 Our current sample size is ∼20 µl, primarily due to the need for manual pipetting and cleanup on a macro-scale. The microfluidic analyzer processes a minute amount of liquid (∼5 nl for a 15 min run), potentially enabling assays on extraordinarily small samples, such as laser-capture tissue dissections or even single cells.
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Fig. 1 Suspension array based on Digital DNA. (a) Digital DNA molecules are built of two types of blocks: 1 and 0, generating many distinct bar codes. Identification fluorophores (green stars) and antibodies are attached to block 1. (b) Analytes (circles) bind to the DNA-bound antibodies and serve as bridges for the red-labeled secondary antibodies (red stars). (c) DNA is then stretched within the microfluidic device and interrogated with light beams I–IV. (d) Representative signals of a single capture unit, based on Digital DNA 111111111111. Traces 1 and 4 are produced by the DNA backbone. Traces 2 and 3 are generated by fluorophores of the identification tags and secondary antibodies, respectively. |
Conjugation control experiments required antibody modified with both SATA and Alexa 647. In this case, antibody was transferred into buffer #1 as described above, allowed to react for 30 min with a 4-fold molar excess of SATA, and then a 10-fold excess of Alexa 647 SE was added. The reaction was allowed to continue for another 30 min, and then the excess cross-linker and dye were removed from the antibody with a Sephadex G50 column as described above.
For hybridization, DNA was combined with bisPNA in buffer H at final concentrations of 32 µg ml−1 and 2 µM, respectively. This mixture was incubated for 1 h at 65 °C, placed on ice, and combined with an equal volume of 0.5 mM LC-SPDP (succinimidyl 6-[3′-(2-pyridyldithio)-propionamido] hexanoate, Pierce) in buffer #1. The reaction continued overnight at room temperature. Excess bisPNA and LC-SPDP were removed by 4 cycles of 10-fold concentration with a Microcon YM-30 centrifuge filter unit (Millipore, Billerica, MA) and addition of 10 mM NaHxPO4 (pH 7.2) buffer with 15 mM NaCl and 10 mM EDTA to the original volume.
Antibodies were conjugated to the DNA by combining 32 µg ml−1 SPDP-modified DNA with 2 µM SATA-modified antibody in buffer #1. This mixture was incubated at room temperature overnight, then excess antibody was removed from the DNA–antibody conjugate by dialysis on 0.1 micron pore size filter disks (Millipore, catalog #VCWP 025 00) against 10 mM NaHxPO4 (pH 7.2) buffer with 50 mM NaCl and 1 mM EDTA for 4–8 h, changing disk and buffer once.
Optical componenta | Detection channel | |||
---|---|---|---|---|
Blueb | Green | Red | ||
a Dichroic mirrors are not included in the table. The first dichroic mirror in the system is Z442/532/638rpc, which directs all excitation laser beams into the system and lets the fluorescence out. The second dichroic mirror 515dcxr reflects the POPO-1 emission from the blue spots to the corresponding detectors. The third dichroic mirror 625dcxr reflects the TMR emission from the green spot to the corresponding detector. All dichroic mirrors are products of Chroma Technologies (Rockingham, VT). b Blue excitation beam of single laser is separated into two spots of focused light to excite the fluorescence of DNA backbone. | ||||
Laser | Wavelength/nm | 445 | 532 | 635 |
Model | 56RCS/S2770 | Compass 215M-20 | Cube 635-25 | |
Manufacturer | Melles Griot | Coherent | Coherent | |
Bandpass excitation filter | Part number | FF01-438/24-25 | FF01-632/22-25 | |
Manufacturer | Semrock | Semrock | ||
Excitation power per spot/mW | 0.2–0.5 | 2–5 | 1–3 | |
Bandpass emission filter | Part number | HQ 480/40 | HQ 580/40 | HQ 680/40 |
Manufacturer | Chroma | Chroma | Chroma |
Digital DNA encoding is information-rich; each block can have a 0 or 1 value. As described below, we use a rigorous analysis of both the green bar code and the blue intercalator signal to discriminate between even closely related bar codes. Our longest molecule includes 20 blocks; at this length, multiplexing up to ∼2N−1 = 5.2 × 105 is possible (the use of 2N−1 corrects for sequences that are mirror images of one another). Up to 2000 unique identifiers are possible with the dodecameric Digital DNA described here, which is sufficient for many applications. If the DNA is designed for independent traces in two colors, up to ∼22N−1 = 8.4 × 106 unique identifiers are possible. In practice, the number of CUs is limited by library construction. However, we have produced over 40 Digital DNAs differing in sizes and bar codes with our simple modular approach. Once a Digital DNA is cloned, the plasmid is easily propagated in bacterial culture. CU assembly involves similar steps to those used to attach antibodies in any suspension array. Therefore, production of Digital DNA suspension arrays is no more complicated than production of current bead-based arrays, while offering significant advantages for increased multiplexing, compatibility with lab-on-chip devices and significantly lower batch to batch variability compared to polystyrene beads.
Digital DNA plasmids are constructed via stepwise ligation of the 0 and 1 blocks. The construction of these blocks and the plasmid vector used to propagate the DNA is described in detail in the ESI†. To add a block to the growing construct, the block was excised from its carrier plasmid with BamHI and XbaI restriction enzymes, then ligated to complementary 5′ overhangs in the Digital DNA plasmid, which was previously cut with BamHI and NheI (Fig. 2a). After ligation, the BamHI-specific site remained, but the NheI and XbaI sites were not present. Plasmids of the proper length were identified by pulsed-field gel electrophoresis with the Chef Mapper system (Biorad) (Fig. 2b). EcoRI digestion was used to confirm the proper sequence of block order, which also was confirmed by single-molecule analysis of bisPNA tagged DNA.
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Fig. 2 Assembly of Digital DNA. (a) Assembly schematic: a plasmid with several connected blocks 0 and 1 is cut with BamHI and NheI restriction endonucleases. The obtained overhangs hybridize with complementary overhangs of block 1 excised with BamHI and XbaI enzymes. The assembly is ligated to yield block 10 and ready for addition of the next block. The NheI and XbaI sites are lost after hybridization. (b) Control of sizes of assembled Digital DNAs. Every plasmid was cut either with XbaI restriction enzyme to linearize the circular plasmid (lanes 2, 4, 6, 8, 10, and 12) or with NheI and XbaI restriction enzymes to excise the vector (lanes 3, 5, 7, 9, 11, and 13). The analyzed samples are Digital DNAs 10011101 (lanes 2–5), 1001110110 (lanes 6–9), 100111010010 (lanes 10 and 11), and 100111011011 (lanes 12 and 13). Lanes 2, 3, 6, and 7 include 4-site series Digital DNA. Lanes 1 and 14 contain a size standard (low range PFG Marker, NEB). (c) Confirmation of sequence of the blocks in Digital DNA. A single EcoRI site is located in the carrier plasmid 31 bases away from the BamHI site. An additional EcoRI site is located in the identification segment of block 1 but is absent from block 0. Digestion of the Digital DNA constructs with EcoRI enables independent confirmation of their proper construction. Lane 1, size standard (1 kb extension ladder, Invitrogen); lane 2, Digital DNA 0111; lane 3, Digital DNA 00111; lane 4, Digital DNA 100111; lane 5, Digital DNA 100111010100; lane 6, Digital DNA 100111011011. Digested DNA was fractionated by pulsed-field gel electrophoresis and stained with SYBR Green I. |
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Fig. 3 Specificity of detection of botulinum toxoid A (BT) with (100111010100) Digital DNA. (a) Unoriented maps are a superposition of multiple head-first (HF) and tail-first (TF) single-molecule traces. (b–e) Unoriented maps of anti-BT CUs measured in green (identification) and red (secondary antibodies) channels either without targets (b), with 50 nM of BT (c and e) or 3 × 109 pfu of MS2 phage (d). The secondary antibodies (also referred to as signal units or SUs) were either anti-BT (b, d and e) or anti-MS2 (c). Every map is an average of 1600 to 4200 single traces. Signal intensity is plotted against the distance from the center of DNA molecule. |
We tested the sensor with a sandwich immunoassay for botulinum toxoid A (BT) against samples containing no antigen, the correct target (BT), or an incorrect antigen (bacteriophage MS2) (Fig. 3). In every case a correct (green) identification map was detected, as every CU carried these tags (Fig. 3b–e). However, the (red) assay map was only detected in the presence of the correct antigen and secondary antibody (Fig. 3e). In all other cases, the red signal was indistinguishable from background. Thus, a complete antibody sandwich can be formed only with correct antigen, attachment of the antibody to Digital DNA does not prevent binding, and the immuno-sandwich structure survives transport and stretching within the chip.
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Fig. 4 Discrimination of different DNA bar codes used to test single-molecule classification. Digital DNA (100111010100) was used to prepare both species. (a) To obtain group #1, bisPNA tag p2368 with TMR fluorophore was hybridized to the sites on the signal segments. (b) To obtain group #2, bisPNA tag p368 with TMR fluorophore was hybridized to the sites on the receptor segments. Since both block 0 and block 1 contain p368 sites, the resulting bar code is (111111111111). Alexa 647-labeled antibodies were conjugated to the bisPNA tag for group #2 molecules, generating a red bar code identical to the green identification bar code. |
In the simplest case, all molecules were included in the analysis; each molecule was assigned to either group #1 or #2 depending on which template was more correlated with the experimental bar code (Table 2). Because only group #2 molecules should have red signals, the classification performance could be independently verified. The molecule was considered incorrectly classified if either group #1 molecule carried at least one red peak >20 photons, or group #2 molecule carried no red peak above 20 photons. That way we determined that 148 molecules were misclassified, corresponding to 6.8% of the total.
No filtering | Backbone filtera | r > 0.5 filterb | Backbone and r > 0.5 filters | |
---|---|---|---|---|
a Backbone filter excluded molecules if the profile of the fluorescence signal from the backbone-bound intercalator indicated stretching anomalies, usually molecules with a hairpin conformation. b Pearson's linear correlation (r) between the observed bar code and the anticipated template. c Incorrectly classified group #1 molecules exhibited fluorescence in red channel. Incorrectly classified group #2 molecules exhibited no fluorescence in red channel. d This is the fraction of the total molecules that passed the backbone and/or classification quality filters. | ||||
Total events | 2165 | 2165 | 2165 | 2165 |
Backbone OK | 2165 | 1562 | 2165 | 1562 |
Classified as group #1 | 921 | 644 | 690 | 519 |
Classified as group #2 | 1244 | 918 | 833 | 660 |
Unclassified | 0 | 0 | 642 | 383 |
Group #1 with redc | 99 | 51 | 6 | 3 |
Group #2 without redc | 49 | 33 | 2 | 1 |
% Misclassified | 6.8 | 5.4 | 0.5 | 0.3 |
% Usable moleculesd | 100 | 72 | 70 | 54 |
To improve classification, we introduced extra criteria to eliminate poorly measured molecules. First, we applied a backbone filter, which excluded molecules if the fluorescence signal from the backbone-bound intercalator indicated stretching anomalies, caused by the inhomogeneous nature of DNA stretching in mixed elongational flow.16 The filter removed all molecules that contained any bins with fluorescence intensity exceeding the mean intercalator signal by at least 50%, eliminating molecules that have short folded-over regions on the DNA which are not big enough to affect the length measurement significantly, but could still affect classification of closely related bar codes. This filter removed 28% of the molecules. When the remaining traces were classified, the error dropped to 5.4%. In the second approach, we filtered out molecules with poor similarity to any of the expected bar codes; only traces with a correlation coefficient of at least 0.5 to one of the expected templates were kept for further analysis. This filter removed 30% of the observed molecules. When the remaining molecules were classified, the error rate dropped to 0.5%. Finally, if both filters were combined, 44% of the molecules were removed, and the classification error on the remainder was 0.3%. Ultimately, the fidelity of bar code classification depends on the efficiency and specificity of tag binding. BisPNA tags have proven to be extraordinarily versatile probes for detection of genomic DNA species, but they do bind reversibly and have significant affinity for single-mismatch sites. We have developed a new tagging technology based on photo-crosslinkable oligos that demonstrates excellent classification efficiency in a mixture of 12 different Digital DNA species.23 Work is ongoing to attach capture probes to these molecules to create a highly multiplexed assay.
To assess the assay performance in a mixture of antigens, we applied the mixture of CUs against BT and coat protein of the MS2 phage (anti-BT and anti-MS2, respectively) in various combinations (Fig. 5). We separated the signals by the number of the CU peaks (Fig. 5a). The sorted molecules exhibited correct green identification traces (Fig. 5b). Detection patterns for anti-BT and anti-MS2 CUs (Fig. 5c and d, respectively) were observed in the red channel only with correct antigens.
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Fig. 5 Multiplexed detection of botulinum toxoid (BT) and MS2 virus. A mixture of (100111010100)-anti-MS2 and (111111111111)-anti-BT was used for the assay. (a) Detected CUs were grouped by the number of green peaks. (b) Each group had the expected ID barcode. Average detection channel traces were measured for (c) anti-BT and (d) anti-MS2, CUs with BT (red), MS2 (blue), BT + MS2 (black), or blank (green). Assays used 63 pM of each CU; 25 nM of each secondary antibody; 25 nM of each antigen, when included. 800 to 2400 single traces were averaged in each map. Signal intensity is plotted as in Fig. 3b–e. |
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Fig. 6 Dependence of the FSH assay signal on the antigen concentration. The normalized signal of the red channel was measured at different antigen concentrations. The concentrations of capture units and signal antibodies were 0.03 and 5 nM, respectively. The threshold level (dashed line) is set at the average red background level plus two standard deviations. The average pattern of red signal on Digital DNA at selected FSH concentrations is shown in the insets. Between 3800 and 8500 molecules were averaged in each case. Results are reported for an FSH sandwich immunoassay cleaned up with either drop-dialysis (a), or in a custom mini-reactor (b). |
Further improvements in assay sensitivity will involve integration of sample preparation onto the microfluidic chip itself, as this will allow for smaller volumes and the use of a minimal amount of the CUs. We have performed preliminary experiments with an on-chip device called the DNA prism.20 This device was originally designed for efficient size-separation of long DNA (100's of kb), but also works extremely well as a mechanism for cleanup of uncomplexed secondary antibodies from our Digital DNA-based immunoassay. In this experiment, a 20 µl reaction was processed using an integrated microfluidic chip that combines DNA stretching, cleanup with a DNA prism, and concentration on acrylamide gel surfaces.28 Details of this device will be published elsewhere. The prism consists of a hexagonal array of posts that interact with long DNA molecules as they are pulled through the device with an alternating pair of electric fields (Fig. 7a). In the first phase, voltage is applied at an angle across the postfield, pulling DNA through the channel between posts. The field then switches to a horizontal direction. Long DNA (>100 kb) hooks on the adjacent posts, preventing these molecules from following the horizontal field. In contrast, short DNA molecules and antibodies are small enough to avoid the posts, and are diverted from the long DNA stream in the horizontal direction. Over many such pulses, the Digital DNA is separated from the free antibodies, ultimately shunted into a different exit port. The port containing the Digital DNA molecules is fluidically connected with the DNA-stretching funnel, where analysis occurs. As shown in Fig. 5b, the red bar code on Digital DNA is barely seen over the background of red signal from free detection antibodies in the original mixture, preventing detection. After sample cleanup in the DNA prism, the background red signal from free secondary antibodies disappears, leaving only the optical background signal. Further work is necessary to assess the benefits of on-chip sample processing on assay sensitivity, but this proof-of-principle experiment demonstrates that all of the fundamental steps can be performed with an integrated microfluidic chip.
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Fig. 7 On-chip removal of secondary antibodies with DNA prism. A 20 µl reaction mix containing 3 × 109 pfu of MS2 phage was prepared as described in Materials and Methods, then run through a chip containing the DNA prism (a) and DNA-stretching fluidics. A control reaction was prepared at the same time, but not cleaned up in the DNA prism. The red signal from the control sample (average of 304 molecules) run directly through the stretching funnel (b, red line) is obscured by the intense noise from the uncomplexed secondary antibodies. In contrast, the sample run through the DNA prism (b, purple line) has a clear red bar code (average of 21![]() |
Particle volume is a fundamental limit to assay sensitivity, as it affects both sample size and required excitation volume. Macro-scale solution handling necessitates ≥10 µl samples, and includes a huge excess of targets over capture agents.24,25,29 Microchip assays reduce this waste, and allow for integration and automation of the assay. We can manipulate and measure the DNA “bead” in 1 µm deep chips, where the DNA is stretched into a linear conformation, then excited with a diffraction-limited laser spot (d ≈ 0.5 µm diameter). For a bead assay, the whole bead must be illuminated to excite the fluorescence of the secondary antibody. As noise is proportional to illuminated volume,30 the limiting signal-to-noise ratio for a Digital DNA-based assay is (D/d)3 = 103 times higher than that for the D = 5 µm beads typically used.24 Finally, using negatively charged DNA obviates the need for pre-blocking capture agents to reduce background signal, as CU's do not self-associate or adhere to the chip walls (a major problem for submicron polystyrene beads). DNA can also be manipulated within the chip by electric field, enabling extraction and purification protocols similar to those employed with magnetic beads, which facilitates automation and miniaturization of analysis.
A critical feature of any suspension array is the read rate for the encoded particles. Our reader scans DNA in constant hydrodynamic flow, which offers significant throughput advantages over other DNA-encoding strategies that require immobilization prior to measurement.31 For the experiments reported here, we were focused on proof-of-principle demonstration, not speed. As such, we drove the DNA through the chip at relatively low concentrations (0.5 ng µl−1) and speeds (15 µm ms−1). Reliable detection of targets in the duplex assay described in Fig. 4 required acquisition times of ∼10 min. The acquisition time will scale with the multiplexing of the assay, since ∼1000 molecules of each type need to be read to achieve reasonable confidence that a target is or is not present in the sample. Therefore, a 12-plex assay (typical for suspension array assays) using the same parameters would require an hour of read time, which may not be acceptable for some applications. Assay throughput in the chip can be improved by increasing the stretching velocity and/or decreasing DNA length. We currently drive DNA at 20 µm ms−1, but we have designed microchips for velocities up to 50 µm ms−1. As both identification sites and secondary antibodies carry multiple fluorophores, measurements can be performed at this velocity without considerable loss of sensitivity. In addition, our Digital DNA blocks can be shrunk from 10 kb to 4.5 kb (3 µm) given our current optical resolution. Shorter molecules can be read at higher concentrations, while still avoiding overlaps between adjacent molecules. The required size to achieve a given multiplexing can also be reduced with double-color coding; a trimer is sufficient to code more than a dozen targets with a 2-color encoding, which gives the overall length of 9 µm for this minimal DNA. With a DNA occupancy of 1/3 to prevent overlap in the detection channel (corresponding to a concentration of ∼6 ng µl−1) and 103 CUs per target, the minimum reading time for a 12-plex assay will be ∼6.5 s, insignificant compared to the tens of minutes to hours needed for sample preparation and incubation.24,25,32
Footnotes |
† Electronic supplementary information (ESI) available: Details of Digital DNA construction and algorithms used to classify single molecule traces. See DOI: 10.1039/b922106a |
‡ These authors contributed equally to this work. |
§ All authors are currently or were employed by US Genomics, Inc. and involved in research on its behalf. R.E.B., E.J.W., T.R.F., R.H.M., N.V.M. and R.G. hold stock and/or stock options in U.S. Genomics, Inc. |
This journal is © The Royal Society of Chemistry 2010 |