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Daniel T Chiu

Publications and source records attributed to Daniel T Chiu.

At least 19 recordsLinked to original sources

Vortex-trap-induced fusion of femtoliter-volume aqueous droplets.

This paper describes the use of an optical vortex trap for the transport and fusion of single femtoliter-volume aqueous droplets. Individual droplets were generated by emulsifying water in acetophenone with SPAN 80 surfactant. We demonstrate the ability of optical vortex traps to position trapped droplets precisely while excluding surrounding aqueous droplets from entering the trap, thereby preventing unwanted cross contamination by other nearby droplets. Additionally, the limitation of optical vortex traps for inducing droplet fusion is illustrated, and a remedy is provided through modulation of the spatial intensity profile of the optical vortex beam. Spatial modulation was achieved by translating the computer-generated hologram (CGH) with respect to the input Gaussian beam, thereby shifting the location of the embedded phase singularity (dark core) within the optical vortex beam. We present both simulated and experimentally measured intensity profiles of the vortex beam caused by translation of the CGH. We further describe the use of this technique to achieve controlled and facile fusion of two aqueous droplets.

Acetophenones↗

Accurate sizing of nanoparticles using confocal correlation spectroscopy.

The ability to accurately size low concentrations of nanoscale particles in small volumes is useful for a broad range of disciplines. Here, we characterize confocal correlation spectroscopy (CCS), which is capable of measuring the sizes of both fluorescent and nonfluorescent particles, such as quantum dots, gold colloids, latex spheres, and fluorescent beads. We accurately measured particles ranging in diameter from 11 to 300 nm, a size range that had been difficult to probe, owing to a phenomenon coined biased diffusion that causes diffusion times, or particle size, to deviate as a function of laser power. At low powers, artifacts mimicking biased diffusion are caused by saturation of the detector, which is especially problematic when probing highly fluorescent or highly scattering nanoparticles. However, at higher powers (>1 mW), autocorrelation curves in both resonant and nonresonant conditions show a structure indicative of an increased contribution from longer correlation times coupled with a decrease in shorter correlation times. We propose that this change in the autocorrelation curve is due to the partial trapping of the particles as they transit the probe volume. Furthermore, we found only a slight difference in the effect of biased diffusion when comparing resonant and nonresonant conditions. Simulations suggest the depth of trapping potential necessary for biased diffusion is > 1 k(B)T. Overcoming artifacts from detector saturation and biased diffusion, CCS is particularly advantageous due to its ability to size particles in the small volumes characteristic of microfluidic channels and aqueous microdroplets. We believe the method will find increasing use in a wide range of applications in measuring nanoparticles and macromolecular systems.

Computer Simulation↗

Capillary electrophoresis separation in the presence of an immiscible boundary for droplet analysis.

This paper demonstrates the ability to use capillary electrophoresis (CE) separation coupled with laser-induced fluorescence for analyzing the contents of single femtoliter-volume aqueous droplets. A single droplet was formed using a T-channel (3 microm wide by 3 microm tall) connected to microinjectors, and then the droplet was fluidically moved to an immiscible boundary that isolates the CE channel (50 microm wide by 50 microm tall) from the droplet generation region. Fusion of the aqueous droplet with the immiscible boundary effectively injects the droplet content into the separation channel. In addition to injecting the contents of droplets, we found aqueous samples can be introduced directly into the separation channel by reversibly penetrating and resealing the immiscible partition. Because droplet generation in channels requires hydrophobic surfaces, we have also investigated the advantages to using all hydrophobic channels versus channel systems with patterned hydrophobic and hydrophilic regions. To fabricate devices with patterned surface chemistry, we have developed a simple strategy based on differential wetting to deposit selectively a hydrophilic polymer (poly(styrenesulfonate)) onto desired regions of the microfluidic chip. Finally, we applied our device to the separation of a simple mixture of fluorescein-labeled amino acids contained within a approximately 10-fL droplet.

Electrophoresis, Capillary↗

Microfluidic and optical systems for the on-demand generation and manipulation of single femtoliter-volume aqueous droplets.

This paper describes a fluidic and optical platform for the generation and manipulation of single femtoliter-volume aqueous droplets. Individual droplets were generated on-demand using a microfluidic chamber that confers environmental flow stability. Optical vortex traps were implemented to manipulate and transport the generated droplets, which have a lower refractive index than the immiscible medium in which the droplets are immersed and thus cannot be trapped using conventional optical tweezers. We also demonstrated the ability to shrink and increase the refractive index of the generated droplet, thereby permitting its facile fusion with another droplet using an optical tweezer. To illustrate the versatility of this platform, we have performed both fast (<1 s) and slow (>1 h) chemical reactions in these femtoliter-volume aqueous droplets.

Journal Article↗

Effects of ultrasmall orifices on the electrogeneration of femtoliter-volume aqueous droplets.

The ability to generate individual picoliter- and femtoliter-volume aqueous droplets on demand is useful for encapsulating and chemically manipulating discrete chemical and biological samples. This paper characterizes the effects of orifice dimensions and material choices on generating such droplets in an immiscible oil phase by using single high-voltage pulses with various amplitudes and durations. We have examined microfluidic orifices as small as 1.7 microm in equivalent radii and found that the electrohydrodynamic jet lengths and the subsequent formation of droplets are affected by the axial aspect ratios of the orifices (length of an orifice divided by its equivalent radius). As higher voltages were used to compensate for the increased capillary pressure and hydrodynamic resistance in ultrasmall orifices, we observed secondary jet protrusions and droplet formations that were not of classical electrohydrodynamic origin. The droplets generated from secondary jets traveled at relatively lower velocities as compared to those of electrohydrodynamic origin, and these slow individual droplets are potentially more useful for applications in microscale chemical reactions.

Electrochemistry↗

Proton permeation into single vesicles occurs via a sequential two-step mechanism and is heterogeneous.

This article describes the first single-vesicle study of proton permeability across the lipid membrane of small (approximately 100 nm) uni- and multilamellar vesicles, which were composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC). To follow proton permeation into the internal volume of each vesicle, we encapsulated carboxyfluorescein, a pH-sensitive dye whose fluorescence was quenched in the presence of excess protons. A microfluidic platform was used for easy exchange of high- and low-pH solutions, and fluorescence quenching of single vesicles was detected with single-molecule total internal reflection fluorescence (TIRF) microscopy. Upon solution exchange and acidification of the extravesicular solution (from pH 9 to 3.5), we observed for each vesicle a biphasic decay in fluorescence. Through single-vesicle analysis, we found that rate constants for the first decay followed a Poisson distribution, whereas rate constants for the second decay followed a normal distribution. We propose that proton permeation into each vesicle first arose from formation of transient pores and then transitioned into the second decay phase, which occurred by the solubility-diffusion mechanism. Furthermore, for the bulk population of vesicles, the decay rate constant and vesicle intensity (dependent on size) correlated to give an average permeability coefficient; however, for individual vesicles, we found little correlation, which suggested that proton permeability among single vesicles was heterogeneous in our experiments.

Cell Membrane Permeability↗

Real-time sizing of nanoparticles in microfluidic channels using confocal correlation spectroscopy.

This Communication reports real-time sizing of nanoparticles in microfluidic systems using confocal correlation spectroscopy (CCS). CCS can be used to measure the size of both fluorescent and nonfluorescent particles at low concentrations (<nanomolar) and in small volumes (<femtoliters). With advances in nonfluorescent modes of single-particle and single-molecule detection, we anticipate CCS will find broad use in the real-time measurements of nanoparticles and macromolecules.

Fluorescent Dyes↗

Layered polyelectrolyte-silica coating for nanocapsules.

This paper demonstrates the ability to grow silica directly on a deposited surface of polyelectrolyte. Using this strategy, we describe the deposition of layered polyelectrolyte-silica coating on negatively charged surfaces of polystyrene particles and latex nanocapsules, which could not be coated directly with silica alone. By etching away the underlying polystyrene bead, we were able to form polyelectrolyte-silica capsules that were mechanically robust. Using scanning and transmission electron microscopy, we imaged and studied the coating after the deposition of each layer of polyelectrolyte and silica. We then applied this new coating to latex nanocapsules that were loaded with fluorescein molecules. We found that the coating procedure did not cause the loaded molecules to leak out from the capsules, and we determined that the variation in the number of loaded molecules among capsules arose from differences in the volume of the nanocavities and was not caused by the loading and coating of the capsules. This layered architecture permits the thickness of the coating to be controlled in principle over a wide dynamic range, but more importantly, this coating could act as an effective seal to prevent undesired leakage from nanocapsules and thus increase the long-term storability of loaded capsules. Over a 30-day period, we determined that leakage from uncoated capsules was significant but negligible for ones that were coated with two layers of polyelectrolyte-silica. Using single-pulse UV photolysis of individual nanocapsules, we demonstrate that the molecules contained within coated capsules could be released effectively and on demand with a single laser pulse.

Journal Article↗

Microfluidic technologies in drug discovery.

Microfluidic systems are increasingly used as tools in various stages of the drug discovery process. Microscale systems offer several obvious advantages, such as low sample consumption and significantly reduced analysis or experiment time. These technologies raise the possibility of massive parallelization and concomitant reduction in cost per acquired data point. In addition, fluids in confined spaces display unique behaviors that can be used to acquire information not accessible using macroscopic systems. This article will focus on the implementation of microfluidic systems and technologies in the process of drug discovery.

Chemistry, Pharmaceutical↗

Determination of the encapsulation efficiency of individual vesicles using single-vesicle photolysis and confocal single-molecule detection.

This paper describes a new method to measure the encapsulation efficiency of individual lipid vesicles. Single vesicles were first optically trapped (with a CW Nd:YAG laser at 1064 nm) and then photolyzed with a single 3-ns UV laser pulse (from a N(2) laser at 337 nm) to release the molecules encapsulated within the vesicle; confocal detection with single-molecule sensitivity (laser excitation at 488 nm from a CW Ar(+) laser) was used to measure the number of released molecules. By placing the confocal probe volume a few micrometers from the vesicle and by monitoring the transit times and the number of released molecules that crossed this probe volume, we could calculate the total number of molecules released from the vesicle using a three-dimensional diffusion equation. Unlike traditional definitions of encapsulation efficiencies based on bulk assays, because we can measure the contents of and release from individual vesicles, we can define the encapsulation efficiency by dividing the concentration of molecules encapsulated in each vesicle over the original concentration of the molecules present in the loading solution. We characterized the encapsulation efficiency of carboxyfluorescein for vesicles prepared by rotary evaporation and found oligolamellar vesicles have an encapsulation efficiency of 36.3 +/- 18.9%, while multilamellar vesicles have an encapsulation efficiency of 17.5 +/- 8.9%.

1,2-Dipalmitoylphosphatidylcholine↗

Selective encapsulation of single cells and subcellular organelles into picoliter- and femtoliter-volume droplets.

This paper describes a method, which combines optical trapping and microfluidic-based droplet generation, for selectively and controllably encapsulating a single target cell or subcellular structure, such as a mitochondrion, into a picoliter- or femtoliter-volume aqueous droplet that is surrounded by an immiscible phase. Once the selected cell or organelle is encased within the droplet, it is stably confined in the droplet and cannot be removed. We demonstrate in droplet the rapid laser photolysis of the single cell, which essentially "freezes" the state that the cell was in at the moment of photolysis and confines the lysate within the small volume of the droplet. Using fluorescein di-beta-d-galactopyranoside, which is a fluorogenic substrate for the intracellular enzyme beta-galactosidase, we also assayed the activity of this enzyme from a single cell following the laser-induced lysis of the cell. This ability to entrap individual selected cells or subcellular organelles should open new possibilities for carrying out single-cell studies and single-organelle measurements.

Animals↗

Disposable microfluidic devices: fabrication, function, and application.

This review article describes recent developments in microfluidics, with special emphasis on disposable plastic devices. Included is an overview of the common methods used in the fabrication of polymer microfluidic systems, including replica and injection molding, embossing, and laser ablation. Also described are the different methods by which on-chip operations--such as the pumping and valving of fluid flow, the mixing of different reagents, and the separation and detection of different chemical species--have been implemented in a microfluidic format. Finally, a few select biotechnological applications of microfluidics are presented to illustrate both the utility of this technology and its potential for development in the future.

Biosensing Techniques↗

Fast initiation of chemical reactions with laser-induced breakdown of a nanoscale partition.

This letter describes a new strategy for initiating a chemical reaction that is based on the laser-induced breakdown of a nanoscopic barrier, which physically separates the reactants in space. Because the breakdown of the barrier is fast ( approximately 0.3 micros) and owing to the nanometer dimension of the barrier, the reactants can be brought together and the reaction can be initiated rapidly. The time scale most suited for this method (from microseconds to tens of milliseconds) bridges nicely between the faster time scales that are accessible mostly with laser-based triggering experiments and the slower time scales that are studied most frequently with flow-based devices.

Kinetics↗

Rapid prototyping of thermoset polyester microfluidic devices.

This paper presents a simple procedure for the fabrication of thermoset polyester (TPE) microfluidic systems and discusses the properties of the final devices. TPE chips are fabricated in less than 3 h by casting TPE resin directly on a lithographically patterned (SU-8) silicon master. Thorough curing of the devices is obtained through the combined use of ultraviolet light and heat, as both an ultraviolet and a thermal initiator are employed in the resin mixture. Features on the order of micrometers and greater are routinely reproduced using the presented procedure, including complex designs and multilayer features. The surface of TPE was characterized using contact angle measurements and X-ray photoelectron spectroscopy (XPS). Following oxygen plasma treatment, the hydrophilicity of the surface of TPE increases (determined by contact angle measurements) and the proportion of oxygen-containing functional groups also increases (determined by XPS), which indicates a correlated increase in the charge density on the surface. Native TPE microchannels support electroosmotic flow (EOF) toward the cathode, with an average electroosmotic mobility of 1.3 x 10(-4) cm(2) V(-1) s(-1) for a 50-microm square channel (20 mM borate at pH 9); following plasma treatment (5 min at 30 W and 0.3 mbar), EOF is enhanced by a factor of 2. This enhancement of the EOF from plasma treatment is stable for days, with no significant decrease noted during the 5-day period that we monitored. Using plasma-treated TPE microchannels, we demonstrate the separation of a mixture of fluorescein-tagged amino acids (glycine, glutamic acid, aspartic acid). TPE devices are up to 90% transparent (for approximately 2-mm-thick sample) to visible light (400-800 nm). The compatibility of TPE with a wide range of solvents was tested over a 24-h period, and the material performed well with acids, bases, alcohols, cyclohexane, n-heptane, and toluene but not with chlorinated solvents (dichloromethane, chloroform).

Microfluidic Analytical Techniques↗

Synthesis, loading, and application of individual nanocapsules for probing single-cell signaling.

This paper describes the synthesis and loading of silica and polystyrene-acrylic based nanocapsules with small molecules. The nanocapsules are used for delivering defined packages of stimuli to single cells with both high spatial and temporal resolutions. To introduce molecules into the capsules, we characterized two approaches. The first approach is based on a base-swell process in which the shell of the capsule is swelled so small molecules can diffuse into the interior of the capsule and be trapped inside once the capsules are de-swelled. The second approach is based on a dry-swell-dry process in which the solution containing the molecules of interest and the nanocapsules is physically dried to promote more molecules to enter into the interior of the capsule. We characterized both methods by monitoring the content of and the release from individual capsules with confocal microscopy and wide-field imaging. To illustrate the biological applications of such nanocapsules, we used optical trapping to position a single carbachol-loaded capsule adjacent to a single CHO cell that has been transfected with muscarinic acetylcholine (M1) receptors, released the carbachol from the capsule with a single 3-ns N2 laser pulse, and then monitored the subsequent intracellular signaling triggered by the binding of carbachol to the M1 receptors.

Animals↗

Direct manipulation and observation of the rotational motion of single optically trapped microparticles and biological cells in microvortices.

This paper describes a method for manipulating and monitoring the rotational motion of single, optically trapped microparticles and living cells in a microvortex. To induce rotation, we placed the microparticle at the center of rotation of the vortex and used the recirculating fluid flow to drive rotation. We have monitored the rotation of single beads (which ranged in diameter from a few micrometers to tens of micrometers) and living cells in a microvortex. To follow the rotation of a smooth and symmetrically shaped bead, we first ablated a small region ( approximately 1 microm) on the bead. An Ar(+) laser was then tightly focused ( approximately 0.5-microm spot size) onto the bead, and rotation was tracked by recording changes in the level of backscattered laser light as the ablated region repeatedly transited the laser focus. Using this method, we have followed bead rotation that varied in frequency from 0.15 to 100 Hz and have studied the effect of bead diameter on the rate of rotation at a given fluid flow rate. To monitor the rotation of single living cells, we selectively stained portions of B-lymphocytes with the fluorescent dye DiOC(6). We observed rotation by following changes in the fluorescence signal as the dye-stained region transited the laser focal volume. This technique provides a simple and sensitive method for controlling and monitoring the rotational motion of microparticles in a microfluidic environment.

Animals↗