Abstract

Indium tin oxide (ITO) is widely used as a substrate for fabricating chips because of its optical transparency, favorable chemical stability, and high electrical conductivity. However, the wettability of ITO surface is neutral (the contact angle was approximately 90°) or hydrophilic. For reagent transporting and manipulation in biochip application, the surface wettability of ITO-based chips was modified to the hydrophobic or nearly hydrophobic surface to enable their use with droplets. Due to the above demand, this study used a 355-nm ultraviolet laser to fabricate a comb microstructure on ITO glass to modify the surface wettability characteristics. All of the fabrication patterns with various line width and pitch, depth, and surface roughness were employed. Subsequently, the contact angle (CA) of droplets on the ITO glass was analyzed to examine wettability and electrical performance by using the different voltages applied to the electrode. The proposed approach can succeed in the fabrication of a biochip with suitable comb-microstructure by using the optimal operating voltage and time functions for the catch droplets on ITO glass for precision medicine application. The experiment results indicated that the CA of droplets under a volume of 20 μL on flat ITO substrate was approximately 92° ± 2°; furthermore, due to its lowest surface roughness, the pattern line width and pitch of 110 μm exhibited a smaller CA variation and more favorable spherical droplet morphology, with a side and front view CA of 83° ± 1° and 78.5° ± 2.5°, respectively, while a laser scanning speed of 750 mm/s was employed. Other line width and pitch, as well as scanning speed parameters, increased the surface roughness and resulted in the surface becoming hydrophilic. In addition, to prevent droplet morphology collapse, the droplet’s electric operation voltage and driving time did not exceed 5 V and 20 s, respectively. With this method, the surface modification process can be employed to control the droplet’s CA by adjusting the line width and pitch and the laser scanning speed, especially in the neutral or nearly hydrophobic surface for droplet transporting. This enables the production of a microfluidic chip with a surface that is both light transmittance and has favorable electrical conductivity. In addition, the shape of the microfluidic chip can be directly designed and fabricated using a laser direct writing system on ITO glass, obviating the use of a mask and complicated production processes in biosensing and biomanipulation applications.

Highlights

  • Microfluidics technology refers to the precision control and manipulation of fluids at the submillimeter scale

  • The results indicated that the microstructure of the glass microfluidic chip could be fabricated with high surface quality; the method can be applied to the mass production of glass fluidic chips

  • The droplet was placed on of the droplet on the surface of the indium tin oxide (ITO) glass, which relates to the wettability, was examthe ITO glass to acquire the droplet image by using the digital microscope; subsequently, ined using the developed image system measurement

Read more

Summary

Introduction

Microfluidics technology refers to the precision control and manipulation of fluids at the submillimeter scale. The laser system’s processing parameters and microstructure morphology (e.g., scanning speed and ablated line pitch and depth) were adjusted, and their effect on the surface roughness, depth, and conductivity of the ITO glass, as well as the CA of the droplet, was analyzed. In this manner, we determined the optimal laser-ablation parameters for the fabrication of a neutral (contact angle was approximately 90◦ ) or hydrophobic surface and the patterns that can withstand depth, and conductivity of the ITO glass, as well as the CA of the droplet, was analyzed. This process can expand the theITO precision medicine applicability and application field of ITO glass in biochips for the precision medicine field

Fundamental Theory
Schematic
Droplet
Materials
Pattern Fabrication
Surface
Experimental
Results and Discussion
Effect of Droplet Volume on CA
Effect
Effect of Line Pitch and Laser Scanning Speed on CA
Effect of Repetition Times on CA
Effect of Electric Field on CA
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.