106 research outputs found

    Stretching the limits of dynamic range, shielding effectiveness, and multiband frequency response

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    In this dissertation, an RF MEMS variable capacitor suitable for applications requiring ultrawide capacitive tuning ranges is reported. The device uses an electrostatically tunable liquid dielectric interface to continuously vary the capacitance without the use of any moving parts. As compared to existing MEMS varactors in literature, this device has an extremely simple design that can be implemented using simple fabrication methods that do not necessitate the use of clean room equipment. In addition, this varactor is particularly suited for incorporating a wide range of liquid dielectric materials for specific tuning ratio requirements. Additionally, the shielding effectiveness performance of graphene-doped ABS thin films is investigated. The use of graphene as a replacement for metal fillers in composite EMI shielding materials is quickly becoming a widely-investigated field in the electromagnetic compatibility community. By replacing conventional metal-based shielding methods with graphene-doped polymers, low-weight, field-use temporary shielding enclosures can be implemented that do not suffer from mechanical unreliability and corrosion/oxidation like a traditional metal enclosure. While the performance of composite EMI shielding materials has not yet surpassed metals, the advantages of polymer-based shielding methods could find usage in a variety of applications. Finally, mutliband pre-fractal antennas fabricated via 3D printing are reported. These devices are the first to incorporate the advantages of 3D printing (rapid prototyping, fabrication of complex geometries otherwise unobtainable) with the advantages of self-similar antennas (increased gain and multiband performance) in a single device. The Sierpinski tetrahedron-based antenna design was both computationally modeled and physically realized to illustrate its potential as a solution to enable true multiband communication platforms

    Piezo-Electrochemical Transducer Effect (PECT) Intercalated Graphite Micro-Electromechanical Actuators

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    The purpose of this research is to investigate the Piezo-Electrochemical Transducer (PECT) effect in intercalated graphite as a possible mechanism of actuation for micro-electromechanical systems (MEMS). This dissertation presents the results of research into the PECT effect in H2SO4-intercalated graphitized carbon fibers, including both electrical and mechanical characteristics of this effect. PECT fibers achieve up to 1.7% strain at 1.4 V of applied potential. In contrast, the piezoelectric material polyvinylidene difluoride (PVDF) generates only 0.01% strain and polysilicon thermal expansion between 0.02 and 0.06% strain depending on the thermal conductivity of the particular polysilicon that the actuators are fabricated in. This work concludes that PECT carbon fiber actuators achieve two orders of magnitude better strain than PVDF piezoelectric actuators and polysilicon thermal expansion in the same voltage range of operation. In addition to this highly improved strain, the devices, after an initial peak power consumption of 227 micronW, a PECT device uses only 260 nW to hold actuation. Although slow operation and unpractical intercalants are serious drawbacks to PECT actuators, the characteristics of strain and power consumption presented in this dissertation prove that PECT actuators, given some minor modifications, prove to be a competitive alternative to current MEMS actuators

    Versatile High Performance Photomechanical Actuators Based on Two-dimensional Nanomaterials

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    The ability to convert photons into mechanical motion is of significant importance for many energy conversion and reconfigurable technologies. Establishing an optical-mechanical interface has been attempted since 1881; nevertheless, only few materials exist that can convert photons of different wavelengths into mechanical motion that is large enough for practical import. Recently, various nanomaterials including nanoparticles, nanowires, carbon nanotubes, and graphene have been used as photo-thermal agents in different polymer systems and triggered using near infrared (NIR) light for photo-thermal actuation. In general, most photomechanical actuators based on sp bonded carbon namely nanotube and graphene are triggered mainly using near infra-red light and they do not exhibit wavelength selectivity. Layered transition metal dichalcogenides (TMDs) provide intriguing opportunities to develop low cost, light and wavelength tunable stimuli responsive systems that are not possible with their conventional macroscopic counterparts. Compared to graphene, which is just a layer of carbon atoms and has no bandgap, TMDs are stacks of triple layers with transition metal layer between two chalcogen layers and they also possess an intrinsic bandgap. While the atoms within the layers are chemically bonded using covalent bonds, the triple layers can be mechanically/chemically exfoliated due to weak van der Waals bonding between the layers. Due to the large optical absorption in these materials, they are already being exploited for photocatalytic, photoluminescence, photo-transistors, and solar cell applications. The large breaking strength together with large band gap and strong light- matter interaction in these materials have resulted in plethora of investigation on electronic, optical and magnetic properties of such layered ultra-thin semiconductors. This dissertation will go in depth in the synthesis, characterization, development, and application of two- dimensional (2D) nanomaterials, with an emphasis on TMDs and molybdenum disulfide (MoS2), when used as photo-thermal agents in photoactuation technologies. It will present a new class of photo-thermal actuators based on TMDs and hyperelastic elastomers with large opto-mechanical energy conversion, and investigate the layer-dependent optoelectronics and light-matter interaction in these nanomaterials and nanocomposites. Different attributes of semiconductive nanoparticles will be studied through different applications, and the possibility of globally/locally engineering the bandgap of such nanomaterials, along with its consequent effect on optomechanical properties of photo thermal actuators will be investigated. Using liquid phase exfoliation in deionized water, inks based on 2D- materials will be developed, and inkjet printing of 2D materials will be utilized as an efficient method for fast fabrication of functional devices based on nanomaterials, such as paper-graphene-based photo actuators. The scalability, simplicity, biocompatibility, and fast fabrication characteristics of the inkjet printing of 2D materials along with its applicability to a variety of substrates such as plastics and papers can potentially be implemented to fabricate high-performance devices with countless applications in soft robotics, wearable technologies, flexible electronics and optoelectronics, bio- sensing, photovoltaics, artificial skins/muscles, transparent displays and photo-detectors

    Lateral bending liquid crystal elastomer beams for microactuators and microgrippers

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    With the rapid development of microsystems in the last few decades, there is a requirement for high precision tools for micromanipulation and transportation of micro-objects, such as microgrippers, for applications in microassembly, microrobotics, life sciences and biomedicine. Polymer based microgrippers and microrobots executing various tasks have been of significant interest as an alternative to the traditional silicon and metal based counterparts due to the advantages of low cost fabrication, low actuation temperature, biocompatibility, and sensitivity to various stimuli. The exceptional actuation properties of liquid crystal elastomers (LCE) have made these materials highly attractive for various emerging applications in the last two decades. Large programmable deformations and the benefits offered by the elastic, thermal and optical properties of LCEs are suitable for implementing stimuli-responsive microgrippers as well as various biomimetic motion in soft robots. In this thesis, a method and the associated processes for fabrication and molecular alignment in LCE were developed, which enabled new functionality and improved performance of the LCE based microactuators and microgrippers, providing controlled response by thermal and remote photothermal actuation, and allowing easy integration of the LCE end-effectors into robotic systems for automated operation. Lateral bending actuation has been demonstrated in LCE microbeams of 900 ยตm of length and 40 ยตm of thickness, owing to the new monolithic micromolding technique using vertical patterned walls for alignment. The effects of parameters such as the beam width, the size of the microgrooves, and the surface treatment method on the behavior of the microactuators were studied; the internal alignment pattern of liquid crystals in the structure was investigated by different microscopy methods. An efficient method for finite element modeling of the bending LCE actuators was developed and experimentally verified, based on the gradient of equivalent thermal expansion in the multi-layer structure, which was able to predict the bending behavior of the actuators in a large range of thicknesses as well as rolling behavior of the actuators of tapered thickness. The novel LCE microgripper with in-plane operation showed efficient thermal and photothermal actuation, achieving the gripping stroke of 64 ยตm under the light intensity of 239 mW/cm2 for the gripper length of 900 ยตm, which is more efficient than the typical SU-8 polymer based microgrippers of the same dimensions. The LCE gripper was successfully demonstrated for the application in manipulation of the objects of tens to hundreds of micrometers in size. Therefore, the novel LCE microgripper bridges the gap in the LCE-based gripper technologies for typical object size in applications for systems microassembly, biological and cell micromanipulation. The lateral bending functionality enabled by the proposed method expands design opportunities for thermal and photothermal LCE microactuators, providing an effective route toward realization of new modes of gripping, locomotion, and cargo transportation in soft microrobotics and micromanipulation

    CMOS-MEMS Scanning Microwave Microscopy

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    This thesis presents the design, fabrication and experimental validation of an integrated dual-mode scanning microwave microscopy (SMM)/Atomic Force Microscopy (AFM) system that does not require the use of a conventional laser-based AFM or external scanners. Microfabricated SMM probes are collocated with strain-based piezoresistive AFM probes in a CMOS-MEMS process, and are actuated by integrated electrothermal scanners. Integration of AFM enables dual-mode imaging (topography and electrical properties); it also enables control over tip-sample distance, which is crucial for accurate SMM imaging. The SMM (also known as Scanning Near-field Microwave Microscope and Scanning Evanescent Microwave Microscope) is the most well-known type of Scanning Probe Microscopes (SPM) that can quantify local dielectric and conductivity of materials. It has emerged as the most promising means for the fast, non-contact, and non-destructive study of materials and semiconductor devices. The CMOS-MEMS SMM devices are fabricated by using a standard foundry CMOS process, followed by an in-house mask-less post-processing technique to release them. Single-chip SMM/AFM devices with integrated 1-D and 3-D actuation are introduced. The CMOS-MEMS fabrication process allows external bulky scanners to be replaced with integrated MEMS actuators that are small and immune to vibration and drift. In this work, electrothermal MEMS actuators are utilized to scan the tip over the sample in 3 degrees of freedom, over a 13 ยตm x 13 ยตm x 10 ยตm scan range in the x, y, and z directions, respectively. Furthermore, the availability of polysilicon layers on the CMOS processes allows for on-chip integrated piezoresistive position sensing that obviates the need for the laser system. Vertical tip-sample distance control of a few nanometers is achieved with the integrated piezoresistive position sensors. These devices are used to modulate the tip-sample separation to underlying samples with a periodic signal, improving immunity to long-term system drifts. To improve the sensitivity of the CMOS-MEMS SMM, different types of matching networks for SMMs are thoroughly analyzed and closed form formulas are presented for each type. Based on the analyses, the stub matching method is selected to match the high tip-to-sample impedance to the 50 ohm characteristic impedance of the system. After that, with the help of lumped models and EM simulations, different sections of the CMOS-MEMS SMM system are analyzed and suggestions for selecting the best micro-transmission line and bonding-pad transmission lines are given. A measurement circuit for SMM is then presented and explained, showing how this measurement system can improve the output-signal-to-noise ratio and hence the sensitivity of microwave imaging. Calculations for the entire SMM system indicate that sub-attofarad tip-sample impedance can be measured. It is noteworthy that most of the analyses and suggestions given in this thesis can be applied to any Scanning Microwave Microscopes or, even more generally, to any microwave system that needs to sense a small signal. Finally, the measurement results for the fabricated CMOS-MEMS SMM are presented to verify the proposed methods. Several samples with sub-micron and nanometer feature sizes are imaged. A special test sample with no topography but with buried dielectric materials in grid and stripes is also designed and measured

    DEVELOPMENT OF NANO/MICROELECTROMECHANICAL SYSTEM (N/MEMS) SWITCHES

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    Ph.DDOCTOR OF PHILOSOPH

    MEMS Devices for Circumferential-scanned Optical Coherence Tomography Bio-imaging

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    Ph.DDOCTOR OF PHILOSOPH

    ์‚ฐ์†Œ ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ •์„ ์ด์šฉํ•œ ์‘๋ ฅ ๊ตฌ๋ฐฐ MEMS ์™ธํŒ”๋ณด๊ฐ€ ์žˆ๋Š” Ka๋ฐด๋“œ ๋Œ€์—ญ ๊ฐ€๋ณ€ํ˜• ๋ฉ”ํƒ€๋ฌผ์งˆ ํก์ˆ˜์ฒด

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022. 8. ๊น€์šฉ๊ถŒ.This dissertation proposes and realizes the first Ka-band frequency tunable metamaterial absorber with stress-induced MEMS cantilever with oxygen plasma ashing process. To employ a MEMS-driven actuator for LC resonance frequency tuning method in the GHz regime, the split-ring resonator (SRR) structure of the metamaterial unit cell is designed to have a sub-mm scale cantilever as a capacitor element of the unit cell. To enlarge capacitance change, the MEMS cantilever is released with a large out-of-plane deflection by the plasma ashing process. This MEMS cantilever with stress gradient is arranged at four parts of a symmetrical SRR unit cell, and the two cells compose the absorber sample as an array structure. The overall cantilevers of the absorber actuate from the initial bent upward state to pulled down state when the electrostatic voltage is applied. The decrease of deflection reduces the gap between cantilevers and bottom electrodes to increase capacitance for frequency tuning to lower frequency. To verify and improve the uniformity of the mechanical behavior of the absorber, this research proposes and demonstrates 3 different design types of releasing on stress-induced cantilevers. First, the array design of 12 cantilevers with 400 ฮผm in length and 50 ฮผm widths is modified from a cantilever with 400 ฮผm in length and 800 ฮผm widths. To overcome the limitation on the mechanical behavior of cantilever arrays due to their nonuniformity, further modification on etching hole rearrangement is reflected in the 2nd type of rectangular cantilever. The space length of etch hole varies depending on the position from the open end of cantilevers. This incremental space length between 8 ฮผm etch holes from the open end enables sequential releasing of cantilevers during photoresist oxygen plasma ashing. The cyclic process was performed in the ashing process to lower the distribution of fabrication results. Finally, the last design to have a semicircle shape with incremental space length between etching holes to improve the uniformity of the cantilever to prevent such drawbacks of a wrinkled profile which the previous design shows. Also, our last design is driven by a digital drive creating 5 different reconfiguration states. With full-wave simulations, the performance of the proposed absorber demonstrates experimentally in each of 5 different reconfiguration states. The initially measured deflection of the cantilever beam is 51.8 ฮผm on average. At the initial state, the resonant frequency and the absorptivity are 32.95 GHz and 80.95%. When all the cantilevers are pulled down, the frequency shifts a total of 4.08 GHz from the initial state showing a tuning ratio of 12.29 %. The error between the measured value and the simulation value came within 0.39 GHz in all five states. This dissertation demonstrated the potential of MEMS as a tuning method for Ka-band absorbers.์ด ๋…ผ๋ฌธ์€ ์‚ฐ์†Œ ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ •์„ ์‚ฌ์šฉํ•˜์—ฌ ์‘๋ ฅ๊ตฌ๋ฐฐ MEMS ์™ธํŒ”๋ณด๋ฅผ ์‚ฌ์šฉํ•œ ์ตœ์ดˆ์˜ Ka ๋Œ€์—ญ ์ฃผํŒŒ์ˆ˜ ๊ฐ€๋ณ€ ๋ฉ”ํƒ€๋ฌผ์งˆ ํก์ˆ˜์ฒด๋ฅผ ์ œ์•ˆํ•˜๊ณ  ๊ฒ€์ฆํ•˜์˜€๋‹ค. GHz ์˜์—ญ์—์„œ LC ๊ณต์ง„ ์ฃผํŒŒ์ˆ˜ ๊ฐ€๋ณ€ ๋ฐฉ์‹์— MEMS ์•ก์ถ”์—์ดํ„ฐ๋ฅผ ๊ตฌ๋™ํ•˜๊ธฐ ์œ„ํ•ด ๋ฉ”ํƒ€๋ฌผ์งˆ ๋‹จ์œ„ ์…€์ธ ๋ถ„ํ• ๋ง๊ณต์ง„๊ธฐ ๊ตฌ์กฐ๋Š” mm ์Šค์ผ€์˜ ์™ธํŒ”๋ณด๋ฅผ ์ •์ „์šฉ๋Ÿ‰์˜ ์š”์†Œ๋ฅผ ๊ฐ–๋„๋ก ์„ค๊ณ„ํ•˜์˜€๋‹ค. ์ •์ „์šฉ๋Ÿ‰ ๋ณ€ํ™”๋ฅผ ์ตœ๋Œ€ํ™”ํ•˜๊ธฐ ์œ„ํ•ด MEMS ์™ธํŒ”๋ณด๋Š” ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ •์— ์˜ํ•ด ์ˆ˜์ง ๋ฐฉํ–ฅ์œผ๋กœ ํฐ ํŽธํ–ฅ์ฐจ๋ฅผ ๊ฐ–๋„๋ก ์„ค๊ณ„ํ•˜์˜€๋‹ค. ์‘๋ ฅ๊ตฌ๋ฐฐ MEMS ์™ธํŒ”๋ณด๋Š” ๋Œ€์นญ์˜ ๋ถ„ํ• ๋ง ๊ณต์ง„๊ธฐ ๊ตฌ์กฐ์˜ ๋‹จ์œ„ ์…€ 4๊ณณ์— ๋ฐฐ์—ด๋˜๊ณ  ๋‘ ์…€์€ ๋ฐฐ์—ด๊ตฌ์กฐ๋กœ ์„ค๊ณ„๋˜์—ˆ๋‹ค. ์ด ๋•Œ, ํ’€์ธ ์ „์•• ์ด์ƒ์˜ ๋†’์€ ์ „์••์„ ์ธ๊ฐ€ ์‹œ ์™ธํŒ”๋ณด๋Š” ๋ฐ”๋‹ฅ์ „๊ทน์— ๋ถ™๊ฒŒ ๋˜์–ด ์ •์ „์šฉ๋Ÿ‰์„ ํ‚ค์šฐ๊ณ  LC ๊ณต์ง„ ์ฃผํŒŒ์ˆ˜๋ฅผ ๋‚ฎ์ถ˜๋‹ค. ํก์ˆ˜์ฒด์˜ ๊ธฐ๊ณ„์  ๊ฑฐ๋™์— ๋Œ€ํ•œ ๊ท ์ผ์„ฑ์„ ๊ฐœ์„ ํ•˜๊ธฐ ์œ„ํ•ด ์ด 3๊ฐ€์ง€ ๋‹ค๋ฅธ ๋ชจ์–‘์˜ ์™ธํŒ”๋ณด๋ฅผ ์„ค๊ณ„ํ•˜์˜€๋‹ค. ๋จผ์ € ๊ธธ์ด 400ฮผm, ๋„ˆ๋น„ 50ฮผm์ธ ์™ธํŒ”๋ณด๋ฅผ 12๊ฐœ์˜ ๋ฐฐ์—ด์ƒํƒœ๋กœ ์„ค๊ณ„ํ•˜์—ฌ ์ปดํ“จํ„ฐ ์‹œ๋ฎฌ๋ ˆ์ด์…˜๊ณผ ์ธก์ •๊ฐ’์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ฒซ ๋ฒˆ์งธ ํก์ˆ˜์ฒด์˜ ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ •์„ ํ†ตํ•œ ์™ธํŒ”๋ณด ๊ตฌํ˜„ ๊ณต์ •์˜ ๊ฒฐ๊ณผ, 96๊ฐœ์˜ ์™ธํŒ”๋ณด์˜ ํ‰๊ท  ๊ฐ’์€ 41.5 ฮผm์ด๊ณ  ํ‘œ์ค€ ํŽธ์ฐจ๋Š” 15.4 ฮผm์˜€๋‹ค. ์ฒซ ๋ฒˆ์งธ ํก์ˆ˜์ฒด์˜ ๊ฒฝ์šฐ ์ œ์ž‘ ์™ธํŒ”๋ณด์˜ ์‚ฐํฌ๊ฐ€ ์ƒ๋‹นํžˆ ํผ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , 15 V๊นŒ์ง€ ์•„๋‚ ๋กœ๊ทธ ํŠœ๋‹์„ ํ•˜์—ฌ, ์ดˆ๊ธฐ ์ƒํƒœ์˜ 28 GHz์˜ ๊ณต์ง„์ฃผํŒŒ์ˆ˜์—์„œ 25.5 GHz์˜ ๊ณต์ง„์ฃผํŒŒ์ˆ˜ ๋ณ€ํ™”ํ•˜์—ฌ ์ด 2.5 GHz์˜ ์ฃผํŒŒ์ˆ˜ ๊ฐ€๋ณ€๋ฒ”์œ„๋ฅผ ๋„๋‹ฌํ•˜์˜€๋‹ค. ๋ฐ˜์‚ฌ๊ณ„์ˆ˜๋Š” ์ดˆ๊ธฐ -5.68 dB์—์„œ -33.60 dB๊นŒ์ง€ ๋ณ€ํ™”ํ•˜์˜€๊ณ , ํˆฌ๊ณผ ๊ณ„์ˆ˜์˜ ๊ฒฝ์šฐ -40์—์„œ -60 dB๋ฅผ ์œ ์ง€ํ•˜์˜€๋‹ค. ํก์ˆ˜์œจ ๊ณ„์‚ฐ ๊ฒฐ๊ณผ, ๊ฐ ๊ณต์ง„ ์ฃผํŒŒ์ˆ˜์—์„œ์˜ ํก์ˆ˜์œจ์€ 0 V์ผ ๋•Œ 72.9%์—์„œ ๊ณ„์† ์ฆ๊ฐ€ํ•˜๋ฉฐ 15 V์ผ๋•Œ 99.9%์˜ ํก์ˆ˜์œจ์„ ๋„๋‹ฌํ•˜์˜€๋‹ค. ๊ทธ๋Ÿผ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , ์™ธํŒ”๋ณด ์–ด๋ ˆ์ด ๊ฐ–๋Š” ๋„“์€ ํŽธํ–ฅ๊ฐ’ ์‚ฐํฌ๊ฐ€ ์ปดํ“จํ„ฐ ์‹œ๋ฎฌ๋ ˆ์ด์…˜๊ณผ์˜ ๊ดด๋ฆฌ๊ฐ€ ์žˆ์–ด ๊ฐœ์„ ๋œ ์„ค๊ณ„๋ฅผ ๋‹ค์‹œ ์‹œ๋„ํ•˜์˜€๋‹ค. ์•ž์„  ์„ค๊ณ„์˜ ๋‹จ์ ์„ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์ ์ง„์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜๋Š” ํŒจํ„ด์˜ ์‹๊ฐ ๊ตฌ๋ฉ์„ ์™ธํŒ”๋ณด์— ์ ์šฉํ•˜์˜€๋‹ค. ์ด ๋‘ ๋ฒˆ์งธ ๊ตฌ์กฐ ๋˜ํ•œ ์ œ์ž‘, ์ปดํ“จํ„ฐ ๊ณ„์‚ฐ ๋ฐ ์‹คํ—˜ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ์‹๊ฐ ๊ตฌ๋ฉ ํŒจํ„ด์€ ์™ธํŒ”๋ณด๋ฅผ ์‚ฐ์†Œ ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ •์œผ๋กœ ๊ตฌํ˜„ ์‹œ, ์ œ์ž‘ ๊ท ์ผ์„ฑ์„ ํฌ๊ฒŒ ์ฆ๊ฐ€์‹œํ‚จ๋‹ค. ๋‚˜์•„๊ฐ€ ํ”Œ๋ผ์ฆˆ๋งˆ ์• ์‹ฑ ๊ณต์ • ๋˜ํ•œ ์‹œ๊ฐ„์„ ๋ถ„ํ• ํ•˜์—ฌ ์ œ์ž‘ํ•จ์œผ๋กœ์จ ๊ท ์ผ๋„๋ฅผ ํฌ๊ฒŒ ์ฆ๊ฐ€์‹œํ‚จ๋‹ค. ๋˜ํ•œ ๋‘๋ฒˆ์งธ ์„ค๊ณ„๋ถ€ํ„ฐ๋Š” ์‘๋ ฅ ๊ตฌ๋ฐฐ๋กœ ์ธํ•œ ํฐ ํŽธํ–ฅ์„ ๊ฐ–๋Š” ์™ธํŒ”๋ณด๊ฐ€ ๊ฐ–๋Š” ๋น„ํ‰ํ˜• ๊ตฌ๋™ ๋ฐฉ์‹์˜ ํ•ด์„ ์–ด๋ ค์›€์— ๋”ฐ๋ผ ์ „์••์„ ๊ฐœ๋ณ„์ ์œผ๋กœ ์ธ๊ฐ€ํ•˜๋ฉฐ on/off ํ˜•ํƒœ์˜ ๋””์ง€ํ„ธ ๊ตฌ๋™๋ฐฉ์‹์œผ๋กœ๋งŒ ๊ตฌ๋™ํ•˜๊ฒŒ๋” ์‹œ์Šคํ…œ ๊ตฌ๋™๋ฐฉ์‹์„ ๋ณ€๊ฒฝํ•˜์˜€๋‹ค. 2๊ฐœ์˜ ๋ฉ”ํƒ€๋ฌผ์งˆ ๋‹จ์œ„ ๊ตฌ์กฐ์— 4๊ฐœ์˜ ์ „๊ทน์„ ๋ถ„๋ฆฌํ•˜์—ฌ ์ด 5๊ฐœ์˜ ๊ตฌ์กฐ์ ์œผ๋กœ ๋‹ค๋ฅธ ์ƒํƒœ๋ฅผ ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ๋ชจ๋“  ์™ธํŒ”๋ณด๊ฐ€ ์œ„๋กœ ํœ˜์–ด์ง„ ์ƒํƒœ์—์„œ ์ „๊ทน์— ์ „์••์„ ์ˆœ์ฐจ์ ์œผ๋กœ ์ธ๊ฐ€ํ•˜์—ฌ 2๊ฐœ์”ฉ ๋ฐ”๋‹ฅ์— ๋ถ™๊ฒŒ ํ•˜์—ฌ ์ตœ์ข…์ ์œผ๋กœ ๋ชจ๋“  ์™ธํŒ”๋ณด๊ฐ€ ๋ฐ”๋‹ฅ์— ๋ถ™๊ฒŒ ํ•˜์˜€๋‹ค. ๋‘ ๋ฒˆ์งธ ํก์ˆ˜์ฒด์˜ ๊ฒฝ์šฐ, ์™ธํŒ”๋ณด ๊ตฌํ˜„์ด ํฌ๊ฒŒ ๊ฐœ์„ ๋จ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ  ์ดˆ๊ธฐ 32.24 GHz์˜ ๊ณต์ง„ ์ฃผํŒŒ์ˆ˜ ๊ฐ’์—์„œ 2.14 GHz๋งŒ ๋ณ€ํ™”ํ•˜์—ฌ ์ตœ์ข… 30.10 GHz์˜ ๊ณต์ง„์ฃผํŒŒ์ˆ˜ ์ธก์ • ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€๋‹ค. ํก์ˆ˜์œจ์˜ ๊ฒฝ์šฐ์—๋„ ์ดˆ๊ธฐ 83.59%์—์„œ ์ตœ์ข… 90.75%์˜ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€์ง€๋งŒ ์ปดํ“จํ„ฐ ๊ณ„์‚ฐ๊ณผ ๋งŽ์€ ์ฐจ์ด๋ฅผ ๋ณด์˜€๋‹ค. ์ตœ์ข…์ ์œผ๋กœ ์•ž์„  2๊ฐœ์˜ ์„ค๊ณ„๋ฅผ ๋ณด์™„ํ•œ, ์ตœ์ข… ์ง„ํ™”ํ•œ ํ˜•ํƒœ์ธ, ๋ฐ˜์›ํ˜• ์‘๋ ฅ ๊ตฌ๋ฐฐ ์™ธํŒ”๋ณด๋ฅผ ๊ฐ–๋Š” ํก์ˆ˜์ฒด๋ฅผ ์„ค๊ณ„, ์ œ์ž‘, ๋ฐ ์‹คํ—˜ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ํŠนํžˆ, ์™ธํŒ”๋ณด๊ฐ€ ๊ฐ–๋Š” ๋ถˆ์•ˆ์ •ํ•œ ๊ธฐ๊ณ„์  ๊ฑฐ๋™์„ ๋‹จ์ˆœํ™”ํ•˜์—ฌ ๋””์ง€ํ„ธ ๊ตฌ๋™์„ ํ•˜๊ฒŒ๋” ํก์ˆ˜์ฒด๋ฅผ ์„ค๊ณ„ํ•˜์˜€๋‹ค. ์‹๊ฐ ํŒจํ„ด์˜ ๊ฑฐ๋ฆฌ๋ฅผ 2 ฮผm์”ฉ ๋Š˜๋ฆฌ๋ฉฐ ๋ฐ˜์› ํ˜•ํƒœ์˜ ์™ธ๊ณฝ์œผ๋กœ๋ถ€ํ„ฐ ์„ค๊ณ„ํ•œ ๊ฒฐ๊ณผ ์žฌํ˜„์„ฑ๊ณผ ๊ท ์ผ์„ฑ์ด ๋งค์šฐ ํฌ๊ฒŒ ๊ฐœ์„ ๋˜์—ˆ๋‹ค. ํŠนํžˆ ๋ฐ˜์› ํ˜•ํƒœ์˜ ์™ธํŒ”๋ณด์˜ ๊ฒฝ์šฐ ์ตœ๊ณ ์  ํŽธํ–ฅ ๋†’์ด๊ฐ€ ํ•ญ์ƒ ๋ฐ˜์› ์ค‘๊ฐ„์—์„œ ๊ตฌํ˜„๋˜๊ธฐ ๋•Œ๋ฌธ์— ๋ฐ˜์›ํ˜• ์™ธํŒ”๋ณด ๊ฐ„์˜ ๋ชจ์–‘์ด ๊ท ์ผํ•˜๊ฒŒ ์œ ์ง€๋œ๋‹ค. ์ œ์ž‘๋œ 18๊ฐœ ํก์ˆ˜์ฒด ์ƒ˜ํ”Œ์—์„œ 144๊ฐœ์˜ ์™ธํŒ”๋ณด๋ฅผ ์ธก์ •ํ•œ ๊ฒฐ๊ณผ ํ‰๊ท  ํŽธํ–ฅ ๋†’์ด์˜ ํ‰๊ท  ๊ฐ’์ด 51.8 ฮผm์˜€์œผ๋ฉฐ ํ‘œ์ค€ ํŽธ์ฐจ๋Š” 3.1ฮผm์˜€๋‹ค. 4๊ฐœ์˜ ์ „๊ทน์—์„œ ๊ธฐ๋ฐ˜ํ•œ 5๊ฐœ ์ƒํƒœ์˜ ์„œ๋กœ ๋‹ค๋ฅธ ๊ตฌ์กฐ์— ๋”ฐ๋ฅธ ๋ฐ˜์‚ฌ ๊ณ„์ˆ˜์™€ ํˆฌ๊ณผ ๊ณ„์ˆ˜๋ฅผ ๋„ํŒŒ๊ด€ ์ธก์ •์œผ๋กœ ์‹คํ—˜ ๊ฐ’์„ ์–ป์—ˆ๋‹ค. ์ƒ์šฉ ์œ ํ•œ์š”์†Œ๋ฒ• ์ปดํ“จํ„ฐ ๊ณ„์‚ฐ๊ณผ ๋น„๊ต ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ดˆ๊ธฐ ์ƒํƒœ์—์„œ ๊ณต์ง„ ์ฃผํŒŒ์ˆ˜๋Š” 32.95 GHz์˜€๊ณ , ๋ชจ๋“  ์™ธํŒ”๋ณด๊ฐ€ ํ’€์ธ ์ „์•• ์ธ๊ฐ€๋กœ ์ธํ•ด ๋ฐ”๋‹ฅ ์ „๊ทน์— ๋ถ™์œผ๋ฉด ํ•˜๋ฉด ์ฃผํŒŒ์ˆ˜ 28.87 GHz๊ฐ€ ๋˜์–ด ์ด 4.08GHz ์ด๋™ํ•˜์—ฌ 12.29%์˜ ์ฃผํŒŒ์ˆ˜ ๊ฐ€๋ณ€์œจ์„ ๊ฐ–๋Š”๋‹ค. ์ธก์ •๊ฐ’๊ณผ ์œ ํ•œ์š”์†Œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๊ฐ’์˜ ์˜ค์ฐจ๋Š” 5๊ฐœ ์ƒํƒœ ๋ชจ๋‘์—์„œ 0.39GHz ์ด๋‚ด์˜€๋‹ค. ํก์ˆ˜์œจ์˜ ๊ฒฝ์šฐ ๊ฐ ์ƒํƒœ์—์„œ 80.95 %, 88.17 %, 86.29 %, 99.21 %, and 86.51% ๊ฐ’์„ ๋ณด์˜€๋‹ค. ์ด ๋…ผ๋ฌธ์€ Ka-๋Œ€์—ญ ํก์ˆ˜์ฒด์˜ ํŠœ๋‹ ๋ฐฉ๋ฒ•์œผ๋กœ์„œ MEMS์˜ ๊ฐ€๋Šฅ์„ฑ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค.CHAPTER 1. Introduction 1 1.1 Background 1 1.1.1 Advent of metamaterial 1 1.1.2 Application of metamaterial 2 1.1.3 Physics of metamaterial 3 1.1.4 Meta-atom 10 1.1.5 Electromagnetic absorber to metamaterial absorber 14 1.1.6 Reconfigurable metamaterial 17 1.1.7 MEMS reconfigurable metamaterial 21 1.1.8 Tunable metamaterial absorber 24 1.1.9 MEMS reconfigurable metamaterial absorber 27 1.1.10 Tunable metamaterial absorber for Ka-band 29 1.2 Originality and contribution 32 1.3 Document structure 33 CHAPTER 2. Stress-induced sub-mm scale cantilever 34 2.1 Initial design 34 2.2 Cantilever arrays with stress gradient 37 2.2.1 Preliminary experiment 37 2.2.2 Design 38 2.2.2 Fabrication results 39 2.3 Rectangular shape sub-mm scale cantilever with incremental etch hole spacing 40 2.3.1 Preliminary experiment 40 2.3.2 Design 42 2.4 Semicircular sub-mm scale cantilever with incremental etch hole 49 2.4.1 Design of semicircular sub-mm scale cantilever with incremental etch hole 49 2.4.2 Fabrication 52 CHAPTER 3. The 1st design of MEMS tunable metamaterial absorber with cantilever arrays for continuous tuning 57 3.1 General overview 57 3.2 Design 59 3.2.1 Split ring resonator and simulation 61 3.2.2 Capacitance of cantilever with stress gradient 64 3.2.3 Electrostatic driving of cantilever 67 3.2.4 Stress analysis & PR ashing 69 3.3 Fabrication 71 3.3.1 Fabrication process 71 3.3.2 Fabrication results 74 3.4 Simulation 77 3.5 Experiment 81 3.5.1 Experiment setup 81 3.5.2 Experiment results 84 3.6 Summary 86 CHAPTER 4. The 2nd design of MEMS tunable metamaterial absorber with rectangular shape sub-mm scale stress-induced cantilever with an incremental etch hole spacing for digital driving 87 4.1 General overview 87 4.2 Design 90 4.3 Fabrication 93 4.4 Simulation 98 4.5 Experiment 100 4.6 Summary 102 CHAPTER 5. The 3rd design of MEMS tunable metamaterial absorber with semicircular sub-mm scale stress-induced cantilever with an incremental etch hole spacing for digital driving 103 5.1 General overview 103 5.2 Design 107 5.2.1 Electromagnetic properties 107 5.2.2 Design parameter 109 5.3 Fabrication 112 5.4 Simulation 119 5.4.1 Simulation setup 119 5.4.2 Simulation results 122 5.5 Experiment 126 5.5.1 Experiment setup 126 5.5.2 Preliminary experiment 130 5.5.2 Experiment results 133 5.6 Further Analysis 137 5.6.1 The waveguide simulation 137 5.6.2 The periodic metamaterial unit cell simulation 141 5.6.3 Analysis on the surface current 148 5.7 Summary 152 5.7.1 Summary of the 1st, 2nd, and 3rd design 152 5.7.2 Comparison with MEMS tunable metamaterial absorber 155 5.7.3 Comparison with Ka-band tunable metamaterial absorber 157 CHAPTER 6. Conclusion 159 Bibliography 161 ์ดˆ๋ก (๊ตญ๋ฌธ) 180๋ฐ•

    Thermal- and Piezo-Tunable Flexural-Mode Resonator with Piezoelectric Actuation and Sensing

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