Forming tiny 3D structures for micro- and nanofluidics
Forming tiny 3D structures for micro- and nanofluidics
复制标题
形成微纳米流体的微小 3D 结构
DOI:
10.1117/2.1200612.0510
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发表时间:
2007
期刊:
影响因子:
--
通讯作者:
S. Juodkazis
中科院分区:
文献类型:
--
作者:
S. Juodkazis
Three-dimensional structures with predesigned optical functions such as waveguides, photonic crystals, and micromechanical parts can be combined into single microdevices with a number of functions. Researchers have made microfluidic devices and sensors that combine optical and microfluidic functions. For practical implementation of these devices, however, the current efficiency of production needs to be increased for 3D laser microfabrication and nanofabrication methods. We expect that a two-step approach—similar to the photographic process of exposure and development—will offer the most effective solution: first, subjecting the sample to a maskless exposure by interference and/or direct laser writing to record the structure, then wet processing to retrieve the written 3D structure. This fabrication route is compliant with batch processing, which is usually required for any practical implementation. To localize a light-matter interaction with high sub-wavelength spatial resolution for 3D structuring of materials, we need a laser source that provides a high irradiance per pulse. It became obvious long ago that femtosecond laser pulses are indispensable for this task, due to their ability to create a huge irradiance(of about a terawatt per square centimeter) with a small pulse energy, while limiting the thermally affected region around the irradiation spot. Fluidic microdevices and micro total analysis systems (μTAS) are expected to find an increasing number of applications in biomedical research and diagnostics. 3D architectures allow more integration and compactness, as well as increased sensitivity due to the small amount of analyte necessary to reliably recognize specific compounds and molecules. The function and versatility of μTAS devices can be augmented by combining optical, electrical, and fluidic systems. Thus, high optical transmissivity—especially to UV light, which can excite fluorescence of an analyte—is required. For electrophoretic applications, the host medium must have high electrical resistivity Figure 1. A confocal 3D image of photoluminescence from a rhodamine solution within a spiral structure.3 The spiral was written in the synthetic quartz Viosil by 3D direct laser writing at tight focusing conditions, using an objective lens of a numerical aperture of 1.35. Using 800nm irradiation with 180fs pulses, the volume was scanned with a separation of 200nm between pulse locations, at pulse energy equal to the two thresholds of an observable photomodification. Then the modified areas were etched with an aqueous solution of HNO3 and HF.4 The spiral depth spans 0− 62μm.