Digital microfluidic (DMF) devices use independent electrodes to propel, split, and join droplets in a confined environment, thereby providing a “lab-on-a-chip.” Digital microfluidic devices are alternatively referred to as electrowetting on dielectric, or “EWoD,” to further differentiate the method from competing microfluidic systems that rely on electrophoretic flow and/or micropumps.
Typically, EWoD devices include a stack of a conductor, an insulator dielectric layer, and a hydrophobic layer. A droplet is placed on the hydrophobic layer, and the stack, once actuated, can cause the droplet to deform and wet or de-wet from the surface depending on the applied voltage. Most of the literature reports on EWoD involve so-called “passive matrix” devices (a.k.a. “segmented” devices), whereby ten to twenty electrodes are directly driven with a controller. While segmented devices are easy to fabricate, the number of electrodes is limited by space and driving constraints. Accordingly, it is not possible to perform massive parallel assays, reactions, etc. in passive matrix devices. In comparison, “active matrix” devices (a.k.a. active matrix EWoD, a.k.a. AM-EWoD) devices can have many thousands, hundreds of thousands or even millions of addressable electrodes. The electrodes are typically switched by thin-film transistors (TFTs) and droplet motion is programmable so that AM-EWoD arrays can be used as general purpose devices that allow great freedom for controlling multiple droplets and executing simultaneous analytical processes.
In biological and chemical applications, the content of the water droplet (e.g., proteins, DNA) can have a major impact on its wetting properties on the hydrophobic layer, specifically related to the resting contact angle of the particular droplet formulation. Thus, it is often required to electrically actuate droplets differently depending on what their contents are. Given that in certain applications it is possible to generate a wide range of droplet formulations that can span several tens of degrees of contact angle for various concentrations/constituents, it would be desirable to provide conditions to accommodate this variability. While the changes in contact angle can partially be done with the addition of surfactant, but is not feasible in many cases to add substantial quantities of surfactant to a reaction liquid with biological molecules because the surfactant may cause damage to the biological molecules.
In a first aspect, there is provided a digital microfluidic device, comprising: a substrate comprising a plurality of driving electrodes coupled to a set of thin-film-transistors, and including a dielectric layer covering both the plurality of driving electrodes and the set of thin-film-transistors; a controller operatively coupled to the set of thin-film-transistors and configured to provide a driving voltage to at least a portion of the plurality of driving electrodes, and a spatially variable wettability layer covering the dielectric layer. In one embodiment, the spatially variable wettability layer comprises a first portion having a first contact angle, and a second portion having a second contact angle. A difference between the first contact angle and the second contact angle may be in the range from least 20° to at most 160°. Alternatively, a difference between the first contact angle and the second contact angle may be in the range of at least 50° to at most 140°. In another, non-exclusive embodiment, the spatially variable wettability layer comprises at least a portion having a contact angle gradient. A difference in contact angle between a first end of the gradient and a second end of the gradient may be in the range from at least 20° to at most 160°. Alternatively, a difference in contact angle between a first end of the gradient and a second end of the gradient may be from at least 50° to at most 140°. The contact angle gradient may be located at an inlet or reservoir entry point for introducing liquids from an external source into the digital microfluidic device. In one embodiment, the device further includes a singular top electrode, a top hydrophobic layer covering the singular top electrode and a spacer separating the variable wettability layer and top hydrophobic layer and creating a microfluidic region between the variable wettability and top hydrophobic layers. In one embodiment, the top hydrophobic layer covering the singular top electrode is a spatially variable wettability layer. The spatially variable wettability layer covering the singular top electrode may include a first portion having a first contact angle, and a second portion having a second contact angle. The spatially variable hydrophobic layer covering the singular top electrode may include at least a portion having a contact angle gradient. In a further, non-exclusive embodiment, the singular top electrode includes at least one light-transmissive region. The light-transmissive region may be at least 10 mm2 in area. In an additional embodiment, the electrodes of the device are arranged in an array.
In another aspect, there is provided a method of manufacturing a microfluidic device, the method including: coupling a substrate comprising a plurality of driving electrodes to a set of thin-film-transistors; forming a dielectric layer covering the plurality of driving electrodes and the set of thin-film-transistors; operatively coupling a controller to the set of thin-film-transistors, wherein the controller is configured to provide a driving voltage to at least a portion of the plurality of driving electrodes, and forming a spatially variable wettability layer covering the dielectric layer. In one embodiment, the forming a spatially variable wettability layer includes: depositing a first material having a first contact angle to form a first zone of the spatially variable wettability layer, and depositing a second material having a second contact angle to form a second zone of the spatially variable wettability layer. A difference between the first contact angle and the second contact angle may be in the range from at least 20° to at most 160°. Alternatively, a difference between the first contact angle and the second contact angle may be in the range from at least 50° to at most 140°. In one embodiment, the forming a spatially variable wettability layer includes: depositing a mixture comprising a hydrophilic material and a hydrophobic material, to form a layer precursor covering the dielectric layer; placing a mask over the surface of the layer precursor, to protect a selected region of the surface, and exposing the surface to a treatment that removes a portion of the hydrophobic material to expose a portion of the hydrophilic material in the unprotected region. The treatment that removes a portion of the hydrophobic material may include exposing the unprotected region to electromagnetic radiation inducing photodegradation of the hydrophobic material. In a number of embodiments, the forming a spatially variable wettability layer includes forming a contact angle surface gradient. In one embodiment, the forming the contact angle surface gradient includes: forming a precursor surface covering the dielectric layer, and covalently binding a hydrophobic molecule to the dielectric layer, to form a density gradient along the precursor surface. In another embodiment, the forming the contact angle surface gradient includes: forming a hydrophobic precursor layer covering the dielectric layer, and irradiating the hydrophobic precursor layer with a spatially variable laser dose. In a further embodiment, the forming the contact angle surface gradient includes: forming a hydrophobic precursor layer covering the dielectric layer, and irradiating the hydrophobic precursor layer with vacuum ultraviolet light, through a filter or photomask, to induce patterned photodegradation. A difference in contact angle between a first end of the gradient and a second end of the gradient may be in the range from at least 20° to at most 160°. Alternatively, a difference in contact angle between a first end of the gradient and a second end of the gradient may be in the range from at least 50° to at most 140°.
In a first aspect, the present invention provides an active matrix electrowetting on dielectric (AM-EWoD) device including a substrate, a dielectric layer, and a variable wettability layer covering the dielectric layer. As depicted herein, the substrate includes a plurality of electrodes actuated by thin-film transistors (TFT) to propel various droplets through a microfluidic region. Though wettability gradients and spatial variation in hydrophobic layers have been investigated in the prior art, these concepts have not made their way to digital microfluidics systems relying on electrode actuation, nor have the specific utilities for such spatial variation been specifically developed to address challenges in DMF systems.
In some instances, surfactants are used to tune the contact angle; however, there are other instances where the presence of a surfactant is incompatible with the chemistry of the application at hand. In such situations, variations in wettability on the coating surface may enable different aqueous formulations to have similar contact angles, thus allowing for the same electrical driving scheme across the entire surface of an array and for simpler, more reliable and straightforward electrical actuation.
Additionally, an aqueous droplet will tend to preferentially migrate toward an area of lower contact angle if exposed to a hydrophobic gradient. This tendency can be useful for preferentially causing droplets to migrate in a chosen direction in a digital microfluidics device, for example to ensure proper droplet migration from reservoir and inlet entry points where liquids are introduced from an external source.
The fundamental operation of an exemplary EWoD device is illustrated in the sectional image of
While it is possible to have a single layer for both the dielectric and hydrophobic functions, such layers typically require thick inorganic layers (to prevent pinholes) with resulting low dielectric constants, thereby requiring more than 100V for droplet movement. To achieve low voltage actuation, it is usually better to have a thin inorganic layer for high capacitance and to be pinhole free, topped by a thin organic hydrophobic layer. With this combination it is possible to have electrowetting operation with voltages in the range +/−10 to +/−50V, which is in the range that can be supplied by conventional TFT arrays.
When a voltage differential is applied between adjacent electrodes, the voltage on one electrode attracts opposite charges in the droplet at the dielectric-to-droplet interface, and the droplet moves toward this electrode, as illustrated in
As shown in
As shown in
The TFT may be constructed by creating alternating layers of differently-doped Si structures along with various electrode lines, with methods know to those of skill in the art. The dielectric should be thin enough and have a dielectric constant compatible with low voltage AC driving, such as available from conventional image controllers for LCD displays. For example, the dielectric layer may comprise a layer of approximately 20-40 nm SiO2 topped over-coated with 200-400 nm plasma-deposited silicon nitride. Alternatively, the dielectric may comprise atomic-layer-deposited Al2O3 between 2 and 100 nm thick, preferably between 20 and 60 nm thick.
Hydrophobic materials may be formed into coatings by deposition onto the surface of the dielectric via suitable techniques, to form hydrophobic layers. Depending on the hydrophobic material to be applied, example deposition techniques include spin coating, molecular vapor deposition, and chemical vapor deposition. Hydrophobic layers may be more or less wettable as usually defined by their respective contact angles. Unless otherwise specified, the term “contact angle” is understood to refer to the contact angle of a surface in relation to a droplet of deionized (DI) water. If water has a contact angle between 0<θ<90°, then the surface is classed as hydrophilic, whereas a surface producing a contact angle between 90°<θ<180° is considered hydrophobic. Usually, moderate contact angles are considered to fall in the range from about 90° to about 120°, while high contact angles are typically considered to fall in the range from about 120° to about 160°. In instances where the contact angle is 160°<θ, then the surface is commonly known as superhydrophobic or ultrahydrophobic. Surface wettabilities may be measured by analytical methods well known in the art, for instance by dispensing a droplet on the surface and performing contact angle measurements using a contact angle goniometer. Anisotropic hydrophobicity may be examined by tilting substrates with gradient surface wettability along the transverse axis of the pattern and examining the minimal tilting angle that can move a droplet. A greater discussion of contact angle can be found at http://en.wikipedia.org/wiki/Contact_angle (last accessed Nov. 17, 2020), which is incorporated by reference.
Hydrophobic layers of moderate contact angle typically include one or a blend of fluoropolymers, such as PTFE (polytetrafluoroethylene), FEP (fluorinated ethylene propylene), PVF (polyvinylfluoride), PVDF (polyvinylidene fluoride), PCTFE (polychlorotrifluoroethylene), PFA (perfluoroalkoxy polymer), FEP (fluorinated ethylene-propylene), ETFE (polyethylenetetrafluoroethylene), and ECTFE (polyethylenechlorotrifluoroethylene). Commercially available fluoropolymers include Cytop® (AGC Chemicals, Exton, PA) and Teflon® AF (Chemours, Wilmington, DE). An advantage of fluoropolymer films is that they can be highly inert and can remain hydrophobic even after exposure to oxidizing treatments such as corona treatment and plasma oxidation.
Coatings having higher contact angles may be fabricated one or more superhydrophobic materials. As anticipated above, contact angles on superhydrophobic materials typically exceed 160°, meaning that only a small percentage of a droplet base is in contact with the surface. This imparts an almost spherical shape to the water droplet. Certain fluorinated silanes, perfluoroalkyls, perfluoropolyethers and RF plasma-formed superhydrophobic materials have found use as coating layers in electrowetting applications and render it relatively easier to slide along the surface. Some types of composite materials are characterized by chemically heterogeneous surfaces where one component provides roughness and the other provides low surface energy so as to produce a coating with superhydrophobic characteristics. Biomimetic superhydrophobic coatings rely on a delicate micro or nano structure for their repellence, but care should be taken as such structures are apt to be easily damaged by abrasion or cleaning.
In a representative embodiment, a given layer may be partitioned in two or more portions characterized by differing contact angles. Each portion is broad enough such that a droplet deposited on the portion may come to rest onto an area isotropic in wettability.
Alternatively, at least a portion of a layer may exhibit a gradual rather than step-wise variation in wettability in the form of a hydrophobic gradient whereby the contact angle with water increases or decreases along a given direction. In a gradient, areas having a given contact angle may be sufficiently narrow such that a droplet deposited on a more hydrophobic area will tend to migrate towards a less hydrophobic area, as illustrated in Langmuir 2005, 21, 11844-11849.
When establishing the parameters of a gradient, one needs to bear in mind that to move the droplet along desired directions, the surface wettability should be within an appropriate range. If the surface is too hydrophilic, the droplet may stick on the substrate. If the surface is too hydrophobic, the droplet may move out of the pattern. In a representative embodiment, the overall Δθ in contact angle between two ends of a gradient is chosen from within the range 20°≤Δθ≤160°. In another embodiment, the range is 20°≤Δθ≤135°. In further embodiments, the range may be 20°≤Δθ≤120°, 20°≤Δθ≤90°, or 20°≤Δθ≤60°, respectively. Other gradients where the range may be 160°≤Δθ≤180°, 120°≤Δθ≤180°, 90°≤Δθ≤180°, or 50°≤Δθ≤140° are also contemplated.
Also, the droplet may move from the more hydrophobic to the more hydrophilic area of a surface with a velocity that depends at least in part on the steepness of the gradient. The steeper the gradient, the faster a droplet may be expected to move, and the quasi-steady speed of the drop in a wettability gradient can be predicted, as illustrated in Langmuir 2005, 21, 11844-11849.
A layer partitioned in two or more portions characterized by different contact angles may be accomplished by covering each portion with a specific coating composition having the contact angle intended for such portion, resulting in a hydrophobic layer partitioned with a variable wettability as desired. In another method, the entirety of the layer is covered with the same coating, for example a hydrophobic polymer, then one or more portions of the surface undergo a treatment that removes portions of the polymer, thus forming a patterned surface where the untreated portions have preserved the highest degree of hydrophobicity while the treated portions are more hydrophilic. Unless otherwise specified, the term “covering” in relation to a layer covering a given item is not to be interpreted as necessarily implying that the layer and item are in physical contact; rather, and depending on the requirements of the application at hand, one or more additional, intermediate layers may be interposed between the covering layer and the item. In addition, the covering layer is not required to cover the absolute entirety of the item; rather, there may be gaps or uncovered sections to suit the requirements of the application at hand.
In another embodiment, and as exemplified in U.S. Pat. No. 6,352,758, a hydrophilic material, for instance inorganic oxide particles such as colloidal silica, is dispersed in a polymer matrix that is formed into a layer precursor covering the dielectric layer. A mask such as a screen is then placed over the surface of the layer precursor such that the mask protects selected regions of the surface while unprotected regions of the surface are exposed to further treatment steps. The surface is then exposed to a treatment that selectively removes a portion of the polymer matrix to expose an intended amount of the hydrophilic material in the unprotected region. The region that is protected by the screen maintains its original hydrophobicity. Thus, this method produces a patterned surface matching the pattern of the screen.
Several methods for preparing gradient surfaces, including thermal, vapor-phase diffusion, electrochemical, photolithographic, gradual immersion, photoinitiator-mediated photopolymerization, corona treatment, contact printing, microfluidic device, and microstructured approaches have been devised, and these techniques are usually based on a generation process, as illustrated in Langmuir 2007, 23, 1845-1850.
In one example generation process reported in Langmuir 2006, 22, 4483-4486, a relatively dilute first solution of a hydrophobic thiol molecule, for example HS(CH2)11CH3 0.05 mmol/L, was found to bind to a gold substrate at a density that can be controlled by varying the immersion time. Slowly adding the dilute solution to the container holding the rough gold substrate will lead to a density gradient along the surface. After the complementary adsorption of HS(CH2)10CH2OH, where the —OH moiety imparts a hydrophilic character to its point of attachment, the surface exhibits a gradient from superhydrophobicity to superhydrophilicity. The slope of the gradient can be conveniently tuned by varying the speed of addition.
Conversely, gradients may also be formed by treating one or more zones of a layer following deposition of a hydrophobic or superhydrophobic material, as seen in Adv. Mater. Interfaces 2018, 1801247. In some techniques, the layer may be treated with an injection of energy inducing change in surface topography, surface chemistry, or both, for example by degradation induced by heat, electromagnetic radiation, electron beam, plasma, and the like. In one embodiment, the electromagnetic radiation source is a laser and irradiation with spatially varied laser dose may be accomplished by changing operating parameters of the laser source, such as gray scale (GS), raster intensity (RI), number of engraving cycles (n), laser spot size, lateral traveling speed, laser repetition rate, and laser spatial resolution. In one configuration disclosed in Lab Chip, 2019, 19, 223, GS and RI allow independent control of the laser power in temporal and spatial domains, n determines the total laser dose, and the other operating parameters are kept constant, although other configurations may be chosen depending on the application at hand. In another embodiment, and as seen in Langmuir 2007, 23, 1845-1850 and U.S. Pat. No. 7,902,680 the gradient surface may be prepared by patterned photodegradation obtained with vacuum ultraviolet light (VUV) or other frequencies suited to the application at hand through a filter or photomask, to create a smooth or coarse gradient as needed.
In one exemplary application, the surface pattern features linear cascades of rectangular areas, the gradient being along either the long or short edge of the rectangles. By increasing the dose of photodegradation-inducing light in a gradual fashion, for example during laser or VUV etching, two or more increasingly hydrophilic areas can be formed. As such, a pattern may be formed with a first area at the more hydrophobic edge within the pattern, a more hydrophilic edge at the opposite side of the pattern, and a pattern center characterized by intermediate wettability.
It will be apparent to those skilled in the art that numerous changes and modifications can be made in the specific embodiments of the invention described above without departing from the scope of the invention. Accordingly, the whole of the foregoing description is to be interpreted in an illustrative and not in a limitative sense.
An EWoD may be manufactured by coupling a substrate 600 including driving electrodes to a set of thin-film-transistors. A controller for providing a driving voltage to the driving electrodes may be operatively coupled to the thin-film-transistors, and driving electrodes and thin-film-transistors can be covered with a dielectric layer. The dielectric layer may be coated with a spatially variable wettability layer. The spatially variable wettability layer may partitioned on the backplane 600 as illustrated in the diagram of
Each material may be deposited on its respective zone while the other zones are masked off, thereby generating differences in relative hydrophobicity along the surface. Specifically, Zone 3 of the liquid inlet may coated with a superhydrophobic nanoparticle/polymer blend having a contact angle 150°<θ1<180°. Zone 1 may be instead coated with a moderately hydrophobic material characterized by a contact angle 90°<θ2<120°, for example one or more fluoropolymers such as those commercially available as Teflon® and Cytop®. The wettability differential between the two zones would lead aqueous droplets placed on the surface of the inlet to migrate away from Zone 3. Each material may be deposited on its respective zone while the other areas are masked off, thereby generating differences in relative hydrophobicity along the surface.
A singular top electrode 700 covered by one or more top hydrophobic layers (705, 710) may also be added to the assembly, with spacers 715, thereby creating a microfluidic workspace 720 as exemplified in the schematic diagram of
Alternatively, or in addition to partitioning the variable wettability layer into discrete patches, a wettability gradient may be established where the contact angle is at a maximum θ1 at the inlet and gradually declines until the moderate contact angle θ2 of Zone 1 is reached. As such, each inlet may be fitted with a gradient characterized by an overall drop in wettability Δθ=θ1−θ2 that is specifically suited to the types of fluid to be introduced through the inlet. For example, the Δθ=θ1−θ2 value may be in the range from about 20° to 90° depending on the characteristics such as the ionic strength, pH, and concentration of the fluid introduced via the inlet. The gradient may also be steeper or milder depending on the speed that is to be imparted to fluid droplets traveling along the gradient.
This application claims priority to U.S. Provisional Application No. 62/937,897, filed Nov. 20, 2019. All references, patents, and patent applications disclosed herein are incorporated by reference in their entireties.
Number | Name | Date | Kind |
---|---|---|---|
3813519 | Jochin et al. | May 1974 | A |
5311337 | McCartney, Jr. | May 1994 | A |
5964995 | Nikiforov et al. | Oct 1999 | A |
6352758 | Huang et al. | Mar 2002 | B1 |
6565727 | Shenderov | May 2003 | B1 |
6773566 | Shenderov | Aug 2004 | B2 |
6911132 | Pamula et al. | Jun 2005 | B2 |
6967489 | Brooks et al. | Nov 2005 | B2 |
6977033 | Becker et al. | Dec 2005 | B2 |
7052244 | Fouillet et al. | May 2006 | B2 |
7053009 | Conley, Jr. et al. | May 2006 | B2 |
7163612 | Sterling et al. | Jan 2007 | B2 |
7215306 | Lo | May 2007 | B2 |
7328979 | Decre et al. | Feb 2008 | B2 |
7420549 | Jacobson et al. | Sep 2008 | B2 |
7458661 | Kim et al. | Dec 2008 | B2 |
7504709 | Masuda et al. | Mar 2009 | B2 |
7531072 | Roux et al. | May 2009 | B2 |
7547380 | Velev | Jun 2009 | B2 |
7641779 | Becker et al. | Jan 2010 | B2 |
7733559 | Kawase et al. | Jun 2010 | B2 |
7767069 | Lee et al. | Aug 2010 | B2 |
7902680 | Tano et al. | Mar 2011 | B2 |
7976795 | Zhou et al. | Jun 2011 | B2 |
8093064 | Shah et al. | Jan 2012 | B2 |
8128798 | Adachi et al. | Mar 2012 | B2 |
8159644 | Takatori | Apr 2012 | B2 |
8173000 | Hadwen et al. | May 2012 | B1 |
8187864 | Wheeler et al. | May 2012 | B2 |
8319759 | Jacobson et al. | Nov 2012 | B2 |
8349276 | Pamula et al. | Jan 2013 | B2 |
8388909 | Pollack et al. | Mar 2013 | B2 |
8409417 | Wu | Apr 2013 | B2 |
8460528 | Pollack et al. | Jun 2013 | B2 |
8514479 | Bae et al. | Aug 2013 | B2 |
8525966 | Takatori | Sep 2013 | B2 |
8529743 | Kim et al. | Sep 2013 | B2 |
8547111 | Hadwen et al. | Oct 2013 | B2 |
8587513 | Ozawa | Nov 2013 | B2 |
8593438 | Komatsu et al. | Nov 2013 | B2 |
8603413 | Fouillet | Dec 2013 | B2 |
8653832 | Hadwen et al. | Feb 2014 | B2 |
8764958 | Wang | Jul 2014 | B2 |
8791891 | Van Dijk et al. | Jul 2014 | B2 |
8810882 | Heikenfeld et al. | Aug 2014 | B2 |
8815070 | Wang et al. | Aug 2014 | B2 |
8834695 | Wang et al. | Sep 2014 | B2 |
8858772 | Crane et al. | Oct 2014 | B2 |
8926811 | Wu | Jan 2015 | B2 |
8936708 | Feiglin et al. | Jan 2015 | B2 |
8940147 | Bartsch et al. | Jan 2015 | B1 |
8958044 | Takatori | Feb 2015 | B2 |
8993348 | Wheeler et al. | Mar 2015 | B2 |
8994705 | Jacobson et al. | Mar 2015 | B2 |
9061262 | Vann et al. | Jun 2015 | B2 |
9216414 | Chu | Dec 2015 | B2 |
9266076 | Kim et al. | Feb 2016 | B2 |
9458489 | Lim et al. | Oct 2016 | B2 |
9458543 | Hadwen | Oct 2016 | B2 |
9476811 | Mudrik et al. | Oct 2016 | B2 |
9594056 | Fobel et al. | Mar 2017 | B2 |
9610582 | Kapur et al. | Apr 2017 | B2 |
9623407 | Delamarche et al. | Apr 2017 | B2 |
9649632 | Van Dam et al. | May 2017 | B2 |
9714463 | White et al. | Jul 2017 | B2 |
9815056 | Wu et al. | Nov 2017 | B2 |
9915631 | Hoffmeyer et al. | Mar 2018 | B2 |
9983169 | Bramanti | May 2018 | B2 |
10018828 | Massard | Jul 2018 | B2 |
10486156 | Campbell et al. | Nov 2019 | B2 |
10543466 | Wu | Jan 2020 | B2 |
10646454 | Liu et al. | May 2020 | B2 |
10695737 | Lammertyn et al. | Jun 2020 | B2 |
10882042 | French | Jan 2021 | B2 |
20060039823 | Yamakawa et al. | Feb 2006 | A1 |
20070023292 | Kim et al. | Feb 2007 | A1 |
20080124252 | Marchand et al. | May 2008 | A1 |
20080135411 | Whitehead et al. | Jun 2008 | A1 |
20100032293 | Pollack et al. | Feb 2010 | A1 |
20100225611 | Lee et al. | Sep 2010 | A1 |
20110005931 | Zhe | Jan 2011 | A1 |
20110220505 | Wang et al. | Sep 2011 | A1 |
20110247934 | Wang et al. | Oct 2011 | A1 |
20120273702 | Culbertson et al. | Nov 2012 | A1 |
20130161193 | Jacobs et al. | Jun 2013 | A1 |
20150377831 | Wheeler et al. | Dec 2015 | A1 |
20160199832 | Jamshidi et al. | Jul 2016 | A1 |
20160312165 | Lowe, Jr. et al. | Oct 2016 | A1 |
20170315090 | Wheeler et al. | Nov 2017 | A1 |
20180085756 | Kosaka | Mar 2018 | A1 |
20180311671 | Cook | Nov 2018 | A1 |
20190092623 | Ding | Mar 2019 | A1 |
20190210026 | Jebrail et al. | Jul 2019 | A1 |
20200064705 | Kayal et al. | Feb 2020 | A1 |
20200089035 | Tsai et al. | Mar 2020 | A1 |
20200114135 | Paolini, Jr. et al. | Apr 2020 | A1 |
20200347840 | Paolini, Jr. et al. | Nov 2020 | A1 |
20200348576 | Visani et al. | Nov 2020 | A1 |
Number | Date | Country |
---|---|---|
102389840 | Mar 2012 | CN |
108393101 | Aug 2018 | CN |
108452853 | Aug 2018 | CN |
2013076739 | Apr 2013 | JP |
200911375 | Mar 2009 | TW |
200916823 | Apr 2009 | TW |
201244824 | Nov 2012 | TW |
201632261 | Sep 2016 | TW |
2007120241 | Oct 2007 | WO |
2017075295 | May 2017 | WO |
Entry |
---|
Taiwan Search Report for Application No. 109140736, dated Feb. 2, 2022, 1 page. |
https://en.wikipedia.org/wiki/Contact_angle, printed Dec. 16, 2020. 2020. |
Choi, Kihwan et al., “Digital Microfluidics”, Annu. Rev. Anal. Chem. 5:413-40 (2012). Apr. 9, 2012. |
Qi, Lin et al., “Mechanical-activated digital microfluidics with gradient surface wettability”, Lab Chip, vol. 19, pp. 223-232, (2019). Dec. 4, 2019. |
Subramanian, R. Shankar et al., “Motion of a Drop on a Solid Surface Due to a Wettability Gradient”, Langmuir, vol. 12, pp. 11844-11849, (2005). Nov. 4, 2005. |
Yu, Xi et al., “Surface Gradient Material: From Superhydrophobicity to Superhydrophilicity”, Langmuir, vol. 22, pp. 4483-4486, (2006). Apr. 7, 2006. |
Ito, Yoshihiro et al., “The Movement of a Water Droplet on a Gradient Surface Prepared by Photodegradation”, Langmuir, vol. 23, pp. 1845-1850, (2007). Dec. 22, 2006. |
Nemani, Srinivasa Kartik et al., “Surface Modification of Polymers: Methods and Applications”, Advanced Materials Interfaces, vol. 5, Issue 24, p. 1801247, Dec. 21, 2018. Dec. 21, 2018. |
Abdelgawad, Mohamed et al., “The Digital Revolution: A New Paradigm for Microfluidics”, Advanced Materials, vol. 21, pp. 920-925,(2009). Jan. 1, 2009. |
Bhattacharjee, Biddut, “Study of Droplet Splitting in an Electrowetting Based Digital Microfluidic System”, The University of British Columbia, Sep. 2012. Sep. 1, 2012. |
Cho, Sung Kwon et al., “Creating, Transporting, Cutting, and Merging Liquid Droplets by Electrowetting-Based Actuation for Digital Microfluidic Circuits”, Journal of Microelectromechanical Systems, vol. 12, No. 1, Feb. 2003. Feb. 1, 2003. |
Nikapitiya, N. Y. Jagath B.et al., “Accurate, consistent, and fast droplet splitting and dispensing in electrowetting on dielectric digital microfluidics”, Mirco and Nano Systems Letters, vol. 5, No. 24, Jun. 2017. Jun. 16, 2017. |
Hadwen, B et al., “Programmable large area digital microfluidic array with integrated droplet sensing for bioassays”, Lab on a Chip, Issue 18, (2012). May 22, 2012. |
Cooney, Christopher G. et al., “Electrowetting droplet microfluidics on a single planar surface”, Microfluisics and Nanofluidics, vol. 2, Issue 5, pp. 435-446 (Sep. 2006). Sep. 1, 2006. |
Fouillet, Y. et al., “EWOD Digital Microfluidics for Lab on a Chip”, International Conference on Nanochannels, Microchannels, and Minichannels, Paper No. ICNMM2006-96020, pp. 1255-1264, (Sep. 2008). Sep. 15, 2008. |
Hlitzbleck, Martina et al., “Reagents in microfluidics: an ‘in’ and ‘out’ challenge”, Chem. Soc. Rev., vol. 42, p. 8494, (2013). Mar. 27, 2013. |
Walker, Shawn W. et al., “Modeling the Fluid Dynamics of Electro-Wetting On Dielectric (EWOD)”, Journal of Microelectromechanical Systems, vol. 15, No. 4, pp. 986-1000, (Aug. 2006). Aug. 2006. |
Li, Yiyan et al., “Improving the performance of electrowetting on dielectric microfluidics using piezoelectric top plate control”, Sensors and Actuators B, vol. 229, pp. 63-74 (2016). 2016. |
Barbulovic-Nad, Irena et al., “Digital microfluidics for cell-based assays”, Lab Chip, vol. 8, pp. 519-526 (2008). Feb. 25, 2008. |
Newman, Sharon et al., “High density DNA storage library via dehydration with digital microfluidic retrieval”, Nature Communications, vol. 10, No. 1706 (2019). Apr. 12, 2019. |
Dhindsa, Manjeet et al., “Virtual electrowetting channels: electronic liquid transport with continuous channel functionality”, Lab on a Chip, Issue 7, pp. 832-836, (2010). Feb. 26, 2010. |
International Preliminary Report on Patentability for Application No. PCT/US2020/061270, dated Jun. 2, 2022, 6 pages. |
Korean Intellectual Property Office, PCT/US2020/061270, International Search Report and Written Opinion, dated Mar. 12, 2021. |
Yong, K.W. et al., “Sliding behavior of droplet on a hydrophobic surface with hydrophilic cavities: A simulation study”, Phys. Fluids 30, 122006 (2018). |
Wu, Huaping et al., “Smart design of wettability-patterned gradients on substrate-independent coated surfaces to control unidirectional spreading of droplets”, Soft Matter, vol. 13, p. 2995 (2017). |
European Office Action for Application No. 20890019.1, dated Nov. 24, 2023, 7 pages. |
Number | Date | Country | |
---|---|---|---|
20210149184 A1 | May 2021 | US |
Number | Date | Country | |
---|---|---|---|
62937897 | Nov 2019 | US |