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Published online before print
September 15, 2003, 10.1101/gr.623903 Genome Res. 13:2348-2352, 2003 ©2003 by Cold Spring Harbor Laboratory Press; ISSN 1088-9051/03 $5.00
Methods Microfabricated Fountain Pens for High-Density DNA ArraysDepartment of Applied Physics, California Institute of Technology, Pasadena, California 91125, USA
We used photolithographic microfabrication techniques to create very small stainless steel fountain pens that were installed in place of conventional pens on a microarray spotter. Because of the small feature size produced by the microfabricated pens, we were able to print arrays with up to 25,000 spots/cm2, significantly higher than can be achieved by other deposition methods. This feature density is sufficiently large that a standard microscope slide can contain multiple replicates of every gene in a complex organism such as a mouse or human. We tested carryover during array printing with dye solution, labeled DNA, and hybridized DNA, and we found it to be indistinguishable from background. Hybridization also showed good sequence specificity to printed oligonucleotides. In addition to improved slide capacity, the microfabrication process offers the possibility of low-cost mass-produced pens and the flexibility to include novel pen features that cannot be machined with conventional techniques.
DNA microarrays have proven to be powerful tools for the analysis of many biological and medical problems, from tumor typing (Golub et al. 1999
High-density DNA microarrays are currently produced via one of three technologies: photolithographic DNA synthesis, modified ink-jet systems, or precisely controlled robotic pens. Although the photolithographic technique (Lipshutz et al. 1999
These synthetic methods require prior knowledge of the genome sequence, and when this is not available, one must resort to methods of arraying isolated genetic material, such as cDNA. Techniques for the deposition of cDNA (or synthetic oligonucleotides), including bubble jet printers and robotically controlled pens, are capable of producing features as small as 70-75 microns (Okamoto et al. 2000
Traditionally, the individual fountain pens for cDNA arrayers have been machined by hand: Stainless steel or titanium rods are first ground to a sharp tip, and then a slot is cut in the tip. Miniature grinding wheels and saws were used to cut early slots, but most commercial pen manufacturers now use wire electrical discharge machining (EDM) or laser cutting methods to achieve slots as small as 10-40 microns in width (http://www.majerprecision.com/pins.htm
The dominant factor in spot size tends not to be the slot width but rather the much larger contact area of the pen with the substrate (Reese 2001
Pen Design High-resolution photolithography is a popular method to create micromechanical devices. In the past, this has been done by using standard silicon fabrication technologies and resulted in the very powerful techniques known as microelectromechanical device (MEMS) technologies (Petersen 1982 We fabricated the pens from stainless steel foil using optical lithography. Photomasks were made with a 3386-dpi laser printer on standard overhead transparencies. The minimum line spacing on these masks is roughly 25 microns, but the foil was only 12.7 microns thick, allowing us to produce pens with a rectangular cross-section in which one dimension is extremely small. Figure 1 shows a collection of pens of varying designs created using this technique, including features such as reservoirs and mechanical support struts. Conventional pens work by capillary action, which requires that the length of the slot be greater than the width (Dreyer 1994). Because this was impossible to achieve with the printer resolution, we designed a different geometry in which the two-walled slot was replaced with a three-walled trench. When the pen is coated with hydrophilic polyurethane, the trench provides enough capillary action to trap the liquid. The unique design of this pen creates a surprising result: The total tip size is no longer the dominant property in determining the droplet size. Instead, the trench size determines the droplet width. The length of each rectangular droplet is controlled by pen flexure.
The trench was etched to a depth of 6 microns in the 12.7-micron-thick stainless steel. At the tip, the side walls of the trench are 30 microns wide, and the trench itself has a width of 30 microns. Away from the tip, the trench width and the width of the side walls increase to 90 microns and 120 microns, respectively, to increase the sturdiness of the pen. Figure 2 shows a comparison of the microfabricated trench pen with a conventionally machined slot pen. Higher-resolution photomasks will allow further reduction of pen features. Indeed, smaller channel widths will increase capillation, thus making the pens even more effective.
Although delicate, there is no reason to expect mechanical failure of the pens during normal spotting or cleaning. Stainless steel is an excellent mechanical material, and we have observed no plastic deformation from the slight deflections the pens undergo during printing and sonication. When printing, the pens contact the printing surface at an angle of 20-30 degrees from perpendicular. Using a nonperpendicular angle serves two purposes. First, this allows greater predictability of pen tip positioning due to flexion of the tip. Second, it serves as a way of crudely managing height variations in the slide, because the pen itself bends as a cantilever beam. Although previous systems used springs as shock absorbers to manage height control, in this case the pen itself acts as a shock absorber. One benefit of this approach is that the pen does not dull; it bends but does not "break." In the experiments described here, the pen deflects <5% of its length. A second result from using a flexible pen is the characteristic rectangular shape of the footprints of the pen, which can be lengthened or shortened based on the amount of deflection.
Pen Testing
As array densities increase and spot sizes shrink, a concern is having enough material deposited to measure a signal. To prove that the printed arrays could be used to measure DNA hybridization, we spotted down two species of short DNA probes and then hybridized fluorescently labeled complementary oligonucleotides to them. The two different oligonucleotides were printed in blocks of 72 spots with a single microfabricated pen. The blocks were printed with six rows of 12 spots. While printing each row, the pen was loaded prior to each group of four spots, alternating between the two probes on each load. Scans of arrays hybridized with complement A showed successful binding only to probe A. To further illustrate the success of the hybridization, the same slide was washed so as to remove the hybridized target DNA, and a second successful hybridization was performed with complement B (Fig. 4).
Although the size of the rectangular spots in Figures 3 and 4 appears irregular in comparison with spots printed with conventional pens, in fact, we discovered that they are more regularthe variations are simply more noticeable because the spots are smaller. We analyzed the results of hybridization to several arrays on the same substratethree independently printed 72-spot arrays made by our stainless steel pens (one shown in Fig. 4, top), and one 72-spot array printed with a conventional pen (data not shown). For the three arrays printed with the new pens, we found the mean spot sizes to be 3500 ± 700, 3750 ± 400, and 3550 ± 550 µm2; the array printed with the conventional pen had a mean spot size of 28,300 ± 4000 µm2. The relative variation in the latter spots is slightly smaller, giving the appearance of more regular spot size, but in absolute terms, the arrays produced by the new pens have a significantly more consistent spot size and quantity of deposited DNA. We also compared the uniformity of the hybridization intensity to assess accuracy. The three arrays printed with the new pens were found to have mean signals of 122 ± 2, 119 ± 4, and 114 ± 5 fluorescence units (for the 36 spots of each array with sequence matching the hybridization target), showing an accuracy of better than 5% for all arrays. The mean fluorescence intensity for the array printed by the conventional pens was 140 ± 4 units. The higher brightness in this case can probably be attributed to the larger droplet that is deposited by conventional pens. Because larger droplets have more "height" when wet, the spots will have a higher areal density of DNA upon drying. By adjusting the concentration of the spotting solution, one can counteract this effect and achieve similar sensitivity between the two printing methods.
Conclusions
Pen Fabrication Pens were fabricated by using a two-exposure procedure to define a pattern into 12.7-micron-thick 300 series stainless steel shim-stock sheets. During the lithographic exposure, the metal sheet is patterned from both the front and the back surface and is subsequently etched from both sides. Masks for the front and back of the pen were designed with Adobe Photoshop, printed onto transparencies by using a 3386-dpi laser printer, cut out, and individually secured by their edges to glass plates with tape. The masks were designed to be larger than the stainless steel shim-stock sheets from which the pens were etched. Moreover, alignment marks were defined in mask areas that extended beyond the stainless steel sample edges. The stainless steel sheets were spin-coated with thin layers of Microposit S1818 photoresist on both sides, and a soft-bake was performed for 10 min at 90°C on each side. The foil was then cut into smaller pieces, each of which would ultimately become a separate set of pens. These smaller pieces were then attached to a back mask (mask 1) transparency with tape, and exposed with a front mask pattern (mask 2) in a Carl Suss MJB-3 contact mask aligner. The front mask (mask 2) pattern, which is used for the initial exposure, was registered to the back mask pattern (onto which the sample was attached) by using the alignment marks from the back mask that were defined beyond the edges of the stainless steel shim-stock pieces. In the second photolithography step, the sample was turned over and exposed from the rear with the attached back mask (mask 1) pattern. By using this method, the front and rear of the shim-stock could be lithographically patterned with very accurate aligned features. By performing lithography on both sides of the shim-stock, it was possible to etch through the 12.7-micron-thick steel layer in a single chemical etch, and it was also possible to define slightly different features on the front and back of the shim-stock sample. After both exposures were completed, the sample was developed in a Microposit CD-30 developer, followed by a 140°C hard-bake for 15 min. The photoresist-masked stainless steel shim-stock was subsequently immersed into a mixture of 40% HCl: 40% H2O: 20% HNO3 (v/v/v), which removed the unmasked areas of stainless steel. During the etch, the sample was gently shaken in the solution to avoid gas bubble formation on the steel surface and to ensure a uniformly etched surface. The etch time was typically 8 to 10 min, or until excess steel was completely separated from the base of the pen. The pens were finally cleaned in baths of acetone, isopropyl alcohol, and distilled water. Low-power ultrasonic cleaning was used to completely remove the photoresist mask layer, and the pens were dipped into a thinned polyurethane solution (1 part ebecryl CL 1039 acrylated urethane: 1 part ethyl alcohol: 1% Irgacure 500) and then inverted and exposed in a UV curing oven for 10 min. At this point, the pens were ready for use.
Mechanics of Printing
The cleaning process consists of two stations: a sonication wash station and a drying station. The sonicator used was a Koh-I-Noor Ultrasonic Cleaner 25K42. The drying station was converted from the original Stanford vacuum station to a heat reservoir. The heat reservoir was constructed of two nested aluminum sheet-metal boxes separated by an insulating layer of glass wool. The heat was produced by a heat gun on its low setting, delivered through a hole in the side of the reservoir and deflected upward by an internal shield. Pens dip into the reservoir through the top. The reservoir was preheated for 1 min before a print commenced and was reheated during each sonication. The heat reservoir was measured to maintain temperatures of
Slide Calibration Protocol
Hybridization Protocol
This work was supported by the Whittier Foundation. We are grateful to Barbara Wold, Brian Williams, James Brody, Chris Hart, Cary Gunn, and David Barsic for helpful discussions and technical assistance. The publication costs of this article were defrayed in part by payment of page charges. This article must therefore be hereby marked "advertisement" in accordance with 18 USC section 1734 solely to indicate this fact.
1 Present address: Department of Applied Physics, Yale University, New Haven, Connecticut 06520-8284, USA.
2 Corresponding author. Article and publication are at http://www.genome.org/cgi/doi/10.1101/gr.623903. Article published online before print in September 2003.
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Received July 12, 2002;
accepted in revised format July 28, 2003.
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