JP2016063280A - Manufacturing method of micromachine vibration structure - Google Patents

Manufacturing method of micromachine vibration structure Download PDF

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JP2016063280A
JP2016063280A JP2014187324A JP2014187324A JP2016063280A JP 2016063280 A JP2016063280 A JP 2016063280A JP 2014187324 A JP2014187324 A JP 2014187324A JP 2014187324 A JP2014187324 A JP 2014187324A JP 2016063280 A JP2016063280 A JP 2016063280A
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graphene
vibration structure
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JP6156881B2 (en
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浩司 山口
Koji Yamaguchi
浩司 山口
玲皇 米谷
Reo Kometani
玲皇 米谷
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Nippon Telegraph and Telephone Corp
University of Tokyo NUC
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Abstract

PROBLEM TO BE SOLVED: To make it possible to improve a Q-value of a micro-vibrator in use under a practical environment.SOLUTION: The manufacturing method of a micromachine vibration structure includes: forming a vibration structure composed of an atomic layer material capable of constituting in an atomic layer unit such as graphene on a substrate in a step S101, and making a fluorine compound gas to act on the vibration structure. For instance, a vibration structure made of graphene may be exposed in a XeFgas in a step S102.SELECTED DRAWING: Figure 1

Description

本発明は、グラフェンなどの原子層材料より構成した微小機械振動構造の作製方法に関する。   The present invention relates to a method for manufacturing a micro mechanical vibration structure made of an atomic layer material such as graphene.

近年、様々な微小物理量を高感度に検出できることから、NEMS(Nanoelectro mechanical systems)センサの構成要素として、微小機械振動子の研究開発が活発に行われている。微小物理量の最小検知量は、例えば、質量計測の場合(非特許文献1),振動子構造の軽量さとその共振特性(Q値)に依存する。このため、より高感度なセンシング達成に向け,振動子構造の軽量化と高Q値化が進められている。   In recent years, since various microphysical quantities can be detected with high sensitivity, research and development of micromechanical vibrators have been actively conducted as constituent elements of NEMS (Nanoelectro mechanical systems) sensors. For example, in the case of mass measurement (Non-Patent Document 1), the minimum detection amount of a minute physical quantity depends on the lightness of the vibrator structure and its resonance characteristic (Q value). For this reason, in order to achieve more sensitive sensing, lightening of the vibrator structure and high Q value are being promoted.

軽量化の観点では、近年、原子層材料であるグラフェンやシリセン(シリコンがハニカム格子状に結晶を組んだグラフェン状物質),h−BN,MoS2,RuO2などが、振動子の構造材料として注目されている。例えば、グラフェンは、機械的性質に優れ、極めて軽量な材料であり、振動子センサの構造材料として期待できる材料である。 In terms of weight reduction, in recent years, graphene and silicene (graphene-like substances in which silicon forms crystals in a honeycomb lattice), h-BN, MoS 2 , RuO 2, etc. are used as the structural material of the vibrator. Attention has been paid. For example, graphene is a material that has excellent mechanical properties and is extremely lightweight, and can be expected as a structural material of a vibrator sensor.

しかしながら、室温で動作するグラフェン振動子のQ値は総じて低く(非特許文献2,非特許文献3)、高感度センシング達成のためには、Q値を改善する必要がある。Q値の改善方法として、極低温環境で動作する高Q値グラフェン振動子の報告がある(非特許文献4)。   However, the Q value of graphene vibrators operating at room temperature is generally low (Non-Patent Document 2, Non-Patent Document 3), and it is necessary to improve the Q value in order to achieve high-sensitivity sensing. As a method for improving the Q value, there is a report of a high Q value graphene vibrator operating in a cryogenic environment (Non-Patent Document 4).

K. L. Ekinci et al. , "Ultrasensitive nanoelectromechanical mass detection", Applied Physics Letters, vol.84, no.22, pp.4469-4471,2004.K. L. Ekinci et al., "Ultrasensitive nanoelectromechanical mass detection", Applied Physics Letters, vol.84, no.22, pp.4469-4471, 2004. J. S. Bunch et al. , "Electromechanical Resonators from Graphene Sheets", Science, vol.315, pp.490-493,2007.J. S. Bunch et al., "Electromechanical Resonators from Graphene Sheets", Science, vol.315, pp.490-493, 2007. S. Shivaraman et al. , "Free-Standing Epitaxial Graphene", Nano Letters, vol.9, no.9, pp.3100-3105,2009.S. Shivaraman et al., "Free-Standing Epitaxial Graphene", Nano Letters, vol.9, no.9, pp.3100-3105,2009. Y. Xu et al. , "Radio frequency electrical transduction of graphene mechanical resonators", Applied Physics Letters, vol.97, 243111, 2010.Y. Xu et al., "Radio frequency electrical transduction of graphene mechanical resonators", Applied Physics Letters, vol.97, 243111, 2010.

しかしながら、上述した極低温を利用した高Q値化は、グラフェン振動子の室温という通常環境下での産業的利用を考えた場合、高Q値化手法として実用的ではない。このため、室温という通常環境で、グラフェンをはじめとする原子層材料を利用した振動子のQ値を向上させる手法が、求められている。   However, the above-described increase in the Q value using the cryogenic temperature is not practical as a technique for increasing the Q value in consideration of the industrial use in a normal environment of room temperature of the graphene vibrator. For this reason, a technique for improving the Q value of an oscillator using an atomic layer material such as graphene in a normal environment of room temperature is demanded.

本発明は、以上のような問題点を解消するためになされたものであり、実用的な環境における使用で微細な振動子のQ値が向上できるようにすることを目的とする。   The present invention has been made to solve the above problems, and an object of the present invention is to improve the Q value of a fine vibrator when used in a practical environment.

本発明に係る微小機械振動構造の作製方法は、原子層の単位で構成することが可能な原子層材料からなる振動構造を基板の上に形成する第1工程と、振動構造にフッ素化合物ガスを作用させる第2工程とを備える。第1工程では、グラフェンからなる振動構造を基板の上に形成し、第2工程では、XeF2のガスを振動構造に作用させればよい。 The manufacturing method of the micro mechanical vibration structure according to the present invention includes a first step of forming a vibration structure made of an atomic layer material that can be configured in units of atomic layers on a substrate, and a fluorine compound gas in the vibration structure. A second step to act. In the first step, a vibration structure made of graphene is formed on the substrate, and in the second step, XeF 2 gas may be applied to the vibration structure.

以上説明したように、本発明によれば、振動構造にフッ素化合物ガスを作用させるようにしたので、実用的な環境における使用で微細な振動子(振動構造)のQ値が向上できるようになるという優れた効果が得られる。   As described above, according to the present invention, since the fluorine compound gas is allowed to act on the vibration structure, the Q value of a fine vibrator (vibration structure) can be improved by use in a practical environment. An excellent effect is obtained.

図1は、本発明の実施の形態における微小機械振動構造の作製方法を説明するフローチャートである。FIG. 1 is a flowchart illustrating a method for manufacturing a micromechanical vibration structure according to an embodiment of the present invention. 図2は、原子層材料としてグラフェンを用いた本発明の実施の形態における微小機械振動構造の作製方法を説明するための各工程の状態を示す断面図である。FIG. 2 is a cross-sectional view showing the state of each step for explaining a method for manufacturing a micromechanical vibration structure in an embodiment of the present invention using graphene as an atomic layer material. 図3は、グラフェン振動子の走査電子顕微鏡写真である。FIG. 3 is a scanning electron micrograph of the graphene vibrator. 図4は、グラフェン振動子の共振特性を測定した結果を示す特性図である。FIG. 4 is a characteristic diagram showing the result of measuring the resonance characteristics of the graphene vibrator. 図5は、本発明が適用可能な微小機械振動構造の構成例を示す斜視図である。FIG. 5 is a perspective view showing a configuration example of a micro mechanical vibration structure to which the present invention is applicable. 図6は、本発明が適用可能な微小機械振動構造の構成例を示す斜視図である。FIG. 6 is a perspective view showing a configuration example of a micro mechanical vibration structure to which the present invention is applicable. 図7は、本発明が適用可能な微小機械振動構造の構成例を示す斜視図である。FIG. 7 is a perspective view showing a configuration example of a micro mechanical vibration structure to which the present invention is applicable. 図8は、本発明が適用可能な微小機械振動構造の構成例を示す斜視図である。FIG. 8 is a perspective view showing a configuration example of a micro mechanical vibration structure to which the present invention is applicable. 図9は、本発明が適用可能な微小機械振動構造の構成例を示す斜視図である。FIG. 9 is a perspective view showing a configuration example of a micro mechanical vibration structure to which the present invention is applicable.

以下、本発明の実施の形態について図を参照して説明する。図1は、本発明の実施の形態における微小機械振動構造の作製方法を説明するフローチャートである。   Hereinafter, embodiments of the present invention will be described with reference to the drawings. FIG. 1 is a flowchart illustrating a method for manufacturing a micromechanical vibration structure according to an embodiment of the present invention.

この作製方法は、まず、工程S101で、グラフェンなどの原子層の単位で構成することが可能な原子層材料からなる振動構造を基板の上に形成する。例えば、基板の上に支持体を形成し、この支持体に一端が固定された梁部を原子層材料から形成すれば、片持ち張りの振動構造とすることができる。   In this manufacturing method, first, in step S101, a vibration structure made of an atomic layer material that can be configured in units of atomic layers such as graphene is formed on a substrate. For example, if a support is formed on a substrate and a beam portion having one end fixed to the support is formed of an atomic layer material, a cantilever vibration structure can be obtained.

次に、工程S102で、振動構造にフッ素化合物ガスを作用させる。例えば、グラフェンからなる振動構造をXeF2ガス中に晒せばよい。 Next, in step S102, a fluorine compound gas is allowed to act on the vibration structure. For example, a vibration structure made of graphene may be exposed to XeF 2 gas.

次に、実施例を用いてより詳細に説明する。以下では、原子層材料としてグラフェンを用い、グラフェンによるメンブレン型の振動構造(グラフェン振動子)を作製した結果について説明する。   Next, it demonstrates in detail using an Example. Below, the result of producing a membrane type vibration structure (graphene vibrator) using graphene by using graphene as an atomic layer material will be described.

まず、図2の(a)に示すように、シリコン基板201の上の、厚さ280nmのSiO2層202の上に、レジストパターン203を形成した。レジストパターン203は、開口部204を備える。SiO2層202は、シリコン基板201の表面を熱酸化することで形成できる。また、以下に説明するように、公知のリソグラフィー技術によりレジストパターン203を形成すればよい。 First, as shown in FIG. 2A, a resist pattern 203 was formed on a SiO 2 layer 202 having a thickness of 280 nm on a silicon substrate 201. The resist pattern 203 includes an opening 204. The SiO 2 layer 202 can be formed by thermally oxidizing the surface of the silicon substrate 201. Further, as described below, a resist pattern 203 may be formed by a known lithography technique.

例えば、電子線レジストであるZEP−520A(日本ゼオン株式会社製)をスピンコート法により膜厚600nmの厚さで塗布してレジスト膜を形成し、溶剤等の除去のために180℃・1分の条件で加熱処理をする。   For example, ZEP-520A (manufactured by Nippon Zeon Co., Ltd.), which is an electron beam resist, is applied by spin coating to a thickness of 600 nm to form a resist film, and 180 ° C. for 1 minute to remove the solvent, etc. Heat treatment is performed under the following conditions.

次に、よく知られた電子ビーム露光技術を用いてレジスト膜に露光を行い、この後現像することで、開口部204を備えるレジストパターン203を形成する。なお、電子ビーム露光に用いた電子ビームの加速電圧は、50kV、ビーム電流は1nAとし、露光量は、150μC/cm2とすればよい。また、現像工程では、現像液としてo−キシレンを用い、リンス液としてIPA(Isopropyl alcohol)を用いればよい。 Next, the resist film is exposed using a well-known electron beam exposure technique, and then developed to form a resist pattern 203 having an opening 204. The acceleration voltage of the electron beam used for electron beam exposure may be 50 kV, the beam current may be 1 nA, and the exposure amount may be 150 μC / cm 2 . In the developing step, o-xylene may be used as a developing solution, and IPA (Isopropyl alcohol) may be used as a rinsing solution.

次に、図2の(b)に示すように、レジストパターン203をマスクとし、エッチングガスにCHF3,O2混合ガスを用い、SiO2層202を反応性イオンエッチング(Reactive Ion Etching;RIE)し、開口部205を形成した。このエッチング処理では、CHF3ガス流量を50sccmとし、また、O2ガス流量を3sccmとした。なお、sccmは流量の単位であり、0℃・1013hPaの流体が1分間に1cm3流れることを示す。また、エッチング時間は30分とした。 Next, as shown in FIG. 2B, the resist pattern 203 is used as a mask, CHF 3 and O 2 mixed gas is used as an etching gas, and the SiO 2 layer 202 is subjected to reactive ion etching (RIE). Then, an opening 205 was formed. In this etching process, the CHF 3 gas flow rate was 50 sccm, and the O 2 gas flow rate was 3 sccm. Note that sccm is a unit of flow rate, and indicates that a fluid at 0 ° C. and 1013 hPa flows 1 cm 3 per minute. The etching time was 30 minutes.

また、次に、O2ガスを利用したRIEにより、レジストパターン203を除去した。このO2ガスによるRIEでは、O2ガス流量を20sccmとし、圧力を1Paとし、RFパワーを500Wとし、バイアスパワーを38Wとした。また、処理時間は1分とした。 Next, the resist pattern 203 was removed by RIE using O 2 gas. In RIE using this O 2 gas, the O 2 gas flow rate was 20 sccm, the pressure was 1 Pa, the RF power was 500 W, and the bias power was 38 W. The processing time was 1 minute.

次に、図2の(c)に示すように、TMAH(Tetramethylammonium hydroxide)エッチング溶液「Pure Etch 160」(林純薬株式会社製)を用い、SiO2層202をマスクとしてシリコン基板201をウエットエッチングし、トレンチ構造206を形成した。ここで、エッチング液の温度は65℃とし、エッチング時間は10分とした。 Next, as shown in FIG. 2C, a silicon substrate 201 is wet etched using a TMAH (Tetramethylammonium hydroxide) etching solution “Pure Etch 160” (manufactured by Hayashi Junyaku Co., Ltd.) and using the SiO 2 layer 202 as a mask. Thus, the trench structure 206 was formed. Here, the temperature of the etching solution was 65 ° C., and the etching time was 10 minutes.

次に、図2の(d)に示すように、開口部205の端部に架設する状態にグラフェン207を配置し、グラフェン207によるメンブレン型のグラフェン振動子を作製した。例えば、Cu箔の上にCVD(Chemical Vapor Deposition)法によりグラフェンを成長し、このグラフェンを転写すればよい。例えば、Cu箔の上に形成したグラフェンを、PMMA(Polymethyl methacrylate)膜を用いて剥離する。次いで、このPMMA膜に貼り付いているグラフェンを、SiO2層202(開口部205)の上に配置する(貼り付ける)。この後、PMMA膜をアセトンで溶解すれば、開口部205に架設するグラフェン207が形成できる。 Next, as illustrated in FIG. 2D, the graphene 207 is disposed so as to be installed at the end of the opening 205, and a membrane-type graphene vibrator using the graphene 207 is manufactured. For example, graphene may be grown on a Cu foil by a CVD (Chemical Vapor Deposition) method, and the graphene may be transferred. For example, graphene formed on a Cu foil is peeled off using a PMMA (Polymethyl methacrylate) film. Next, the graphene attached to the PMMA film is disposed (attached) on the SiO 2 layer 202 (opening 205). Thereafter, if the PMMA film is dissolved with acetone, the graphene 207 to be installed in the opening 205 can be formed.

次に、図2の(e)に示すように、グラフェン207に、XeF2のガスを作用させ、グラフェン207に対してフッ化表面改質を実施した。例えば、XeF2ガスエッチング装置(BP−3F,SAMCO)を用い、本装置の処理室内でグラフェン207をXeF2ガスに30秒間晒した。この処理の後では、グラフェン207の各炭素原子に、フッ素原子208が結合していることが確認されている。 Next, as shown in FIG. 2E, XeF 2 gas was allowed to act on the graphene 207 to perform fluorination surface modification on the graphene 207. For example, using a XeF 2 gas etching apparatus (BP-3F, SAMCO), graphene 207 was exposed to XeF 2 gas for 30 seconds in the processing chamber of this apparatus. After this treatment, it has been confirmed that the fluorine atom 208 is bonded to each carbon atom of the graphene 207.

このようにして作製したグラフェン振動子について、走査型電子顕微鏡で観察した結果を図3に示す、図3は、作製したグラフェン振動子の走査電子顕微鏡写真である。図3の(b)は、図3の(a)の一部を拡大して示している。平面視の寸法が2μm×2μm程度のメンブレン型のグラフェン振動子が形成されていることが分かる。   FIG. 3 shows the result of observation of the graphene vibrator thus produced with a scanning electron microscope. FIG. 3 is a scanning electron micrograph of the produced graphene vibrator. FIG. 3B is an enlarged view of a part of FIG. It can be seen that a membrane-type graphene vibrator having a dimension in plan view of about 2 μm × 2 μm is formed.

次に、上述したグラフェン振動子の共振特性を評価した結果について説明する。共振特性の評価は、光ヘテロダイン振動計を用いて実施した。この評価では、まず、光ヘテロダイン振動計の試料室のステージに、グラフェン振動子が作製された基板を設置し、試料室内を真空度10-2Paにまで減圧排気する。この状態で、発振波長408nmの半導体レーザーを用い、基板上のグラフェン振動子を光励振法により加振(励振)し、共振特性を計測した。共振特性計測に用いたレーザーは、632.8nmのHe−Neレーザーである。また、共振特性計測環境の温度は、室温とした。 Next, the results of evaluating the resonance characteristics of the graphene vibrator described above will be described. Resonance characteristics were evaluated using an optical heterodyne vibrometer. In this evaluation, first, a substrate on which a graphene vibrator is manufactured is placed on the stage of the sample chamber of the optical heterodyne vibrometer, and the sample chamber is evacuated to a vacuum degree of 10 −2 Pa. In this state, using a semiconductor laser with an oscillation wavelength of 408 nm, the graphene vibrator on the substrate was vibrated (excited) by the optical excitation method, and the resonance characteristics were measured. The laser used for the resonance characteristic measurement is a 632.8 nm He—Ne laser. The temperature of the resonance characteristic measurement environment was room temperature.

上述した測定結果を図4に示す。図4は、グラフェン振動子の共振特性を測定した結果を示す特性図である。図4の(a)は、平面視の寸法が2μm×2μmの、単層のグラフェン振動子のフッ化表面改質前の共振特性計測結果である。また、図4の(b)は、平面視の寸法が2μm×2μmの、単層のグラフェン振動子のフッ化表面改質後の共振特性計測結果である。   The measurement results described above are shown in FIG. FIG. 4 is a characteristic diagram showing the result of measuring the resonance characteristics of the graphene vibrator. FIG. 4A shows a resonance characteristic measurement result before fluorination surface modification of a single-layer graphene vibrator having a dimension in plan view of 2 μm × 2 μm. FIG. 4B shows a resonance characteristic measurement result after modification of the fluorinated surface of a single-layer graphene vibrator having a dimension in plan view of 2 μm × 2 μm.

図4の(a)に示すように、フッ化表面改質前のグラフェン振動子のQ値は354である。これに対し、図4の(b)に示すように、フッ化表面改質後のグラフェン振動子のQ値は2722となり、フッ化表面改質を施すことによりQ値はおよそ7.7倍向上したことになる。   As shown in FIG. 4A, the Q value of the graphene vibrator before the fluorination surface modification is 354. In contrast, as shown in FIG. 4B, the Q value of the graphene vibrator after the fluorination surface modification is 2722, and the Q value is improved by about 7.7 times by applying the fluorination surface modification. It will be done.

以上に説明したように、炭素系の原子層材料であるグラフェン振動子に対し、フッ素化合物ガスであるXeF2ガスを活用した表面改質を実施することで、Q値を向上させることができる。また、この作製方法は、極めて簡単なプロセスで実施可能であり,また既存の半導体製造プロセス技術,MEMS(Micro Electro Mechanical Systems),NEMS製造プロセス技術と親和性が高い。このように、本発明は、グラフェンをはじめとする原子層材料からなる振動構造体を利用した様々な素子研究開発,製造へ適用可能であると考えられる。 As described above, the Q value can be improved by performing surface modification using XeF 2 gas, which is a fluorine compound gas, on the graphene vibrator, which is a carbon-based atomic layer material. In addition, this manufacturing method can be implemented by a very simple process, and has high affinity with existing semiconductor manufacturing process technology, MEMS (Micro Electro Mechanical Systems), and NEMS manufacturing process technology. As described above, the present invention is considered to be applicable to various element research and development and manufacturing using a vibrating structure made of an atomic layer material such as graphene.

ところで、微小機械振動構造は、例えば、図5に示すように、支持体501に支持された片持ちの梁502から構成してもよい。また、図6に示すように、支持体501および支持体503に架設して支持された両持ちの梁502から構成してもよい。また、図7に示すように、円形の開口を有する支持体504の上に形成された薄膜505による円形のメンブレンから構成してもよい。   By the way, the micro mechanical vibration structure may be composed of a cantilever beam 502 supported by a support body 501 as shown in FIG. Moreover, as shown in FIG. 6, you may comprise from the support body 501 and the beam 502 of the both ends supported by the support body 503. Moreover, as shown in FIG. 7, you may comprise from the circular membrane by the thin film 505 formed on the support body 504 which has circular opening.

また、微小機械振動構造は、図8に示すように、支持体501および支持体503を連結する連結支持構造506,507に、支持された両自由端振動部508から構成してもよい。また、図9に示すように、支持体501および支持体503に架設して支持された両持ちの2つの梁509,510を、連結構造511,512で連結した構造としてもよい。これらのように、微小機械振動構造の形状は、本発明の趣旨に基づいて,種々の変形・応用が可能である。   Further, as shown in FIG. 8, the micromechanical vibration structure may be configured by both free end vibration portions 508 supported by connection support structures 506 and 507 that connect the support body 501 and the support body 503. Moreover, as shown in FIG. 9, it is good also as a structure which connected the two beams 509 and 510 of the both ends supported by the support body 501 and the support body 503 by the connection structure 511,512. As described above, the shape of the micro mechanical vibration structure can be variously modified and applied based on the gist of the present invention.

以上に説明したように、本発明によれば、原子層材料からなる振動構造にフッ素化合物ガスを作用させるようにしたので、実用的な環境における使用で微細な振動子(振動構造)のQ値が向上できる。微小機械振動子は、高速応答特性,高感度特性から、センサ,演算回路等の作製にけるキーコンポーネントとして期待され、研究開発が行われている素子である。このような微小機械振動子を利用した次世代デバイス作製において、微小機械振動子の動特性(特にQ値)の改善手法は重要な要素技術である。なかでも、極めて軽量な特性,優れた機械的性質を有するグラフェンは、上記メカニカル素子の構造材料として期待される材料である。室温(常温)という通常環境でグラフェン振動子の動特性(Q値)を改善できる本発明によれば、上述した次世代デバイス実現の重要な要素技術となる可能性がある。   As described above, according to the present invention, since the fluorine compound gas is allowed to act on the vibration structure made of the atomic layer material, the Q value of a fine vibrator (vibration structure) can be used in a practical environment. Can be improved. A micro mechanical vibrator is an element that is expected to be a key component in the production of sensors, arithmetic circuits, and the like due to its high-speed response characteristics and high sensitivity characteristics, and is being researched and developed. In the production of next-generation devices using such micromechanical vibrators, a technique for improving the dynamic characteristics (particularly the Q value) of the micromechanical vibrators is an important elemental technology. Among them, graphene having extremely lightweight characteristics and excellent mechanical properties is a material expected as a structural material for the mechanical element. According to the present invention that can improve the dynamic characteristics (Q value) of a graphene vibrator in a normal environment of room temperature (room temperature), it may become an important elemental technology for realizing the next-generation device described above.

なお、本発明は以上に説明した実施の形態に限定されるものではなく、本発明の技術的思想内で、当分野において通常の知識を有する者により、多くの変形および組み合わせが実施可能であることは明白である。例えば、上述では、CVD法により作製したグラフェンを用いたが、テープ剥離法,SiCの熱分解などの手法により作製したグラフェンを振動構造体とする素子に対しても適用可能である。また、上述では、原子層材料としてグラフェンを例示したが、これに限るものではなく、カーボンナノチューブなどの炭素系材料であっても同様である。   The present invention is not limited to the embodiment described above, and many modifications and combinations can be implemented by those having ordinary knowledge in the art within the technical idea of the present invention. It is obvious. For example, in the above description, graphene produced by the CVD method is used. However, the present invention can also be applied to an element in which graphene produced by a technique such as a tape peeling method or thermal decomposition of SiC is used as a vibration structure. In the above description, graphene is exemplified as the atomic layer material. However, the present invention is not limited to this, and the same applies to carbon-based materials such as carbon nanotubes.

また、微小機械振動構造の形成は、電子ビーム露光技術,フォトリソグラフィー,ナノインプリント技術,ドライ・ウエットエッチング技術,蒸着・スパッタリング・化学気相成長などの既存の超微細加工技術を複数組み合わせて使用することでも可能である。原子層材料を利用した振動構造体,あるいはナノ・マイクロメートルオーダーの微小機械振動構造体の形成は、前述した説明に限定するものではない。また、ガス雰囲気を利用した表面改質を例示したが、光化学表面反応や低エネルギーイオンの利用,表面コーティングなどの表面改質手法を用いても同様の効果が期待できる。   In addition, the formation of the micro mechanical vibration structure is to use a combination of multiple existing ultra-fine processing technologies such as electron beam exposure technology, photolithography, nanoimprint technology, dry / wet etching technology, vapor deposition / sputtering / chemical vapor deposition. But it is possible. The formation of a vibration structure using an atomic layer material or a micro mechanical vibration structure on the order of nano / micrometers is not limited to the above description. In addition, although surface modification using a gas atmosphere has been exemplified, the same effect can be expected by using a surface modification technique such as photochemical surface reaction, use of low energy ions, or surface coating.

201…シリコン基板、202…SiO2層、203…レジストパターン、204…開口部、205…開口部、206…トレンチ構造、207…グラフェン、208…フッ素原子。 201 ... silicon substrate, 202 ... SiO 2 layer, 203 ... resist pattern, 204 ... opening, 205 ... opening, 206 ... trench structure 207 ... graphene, 208 ... fluorine atom.

Claims (2)

原子層の単位で構成することが可能な原子層材料からなる振動構造を基板の上に形成する第1工程と、
前記振動構造にフッ素化合物ガスを作用させる第2工程と
を備えることを特徴とする微小機械振動構造の作製方法。
A first step of forming on the substrate a vibration structure made of an atomic layer material that can be configured in units of atomic layers;
And a second step of causing a fluorine compound gas to act on the vibration structure.
請求項1記載の微小機械振動構造の作製方法において、
前記第1工程では、グラフェンからなる振動構造を基板の上に形成し、
前記第2工程では、XeF2のガスを前記振動構造に作用させる
ことを特徴とする微小機械振動構造の作製方法。
In the method for producing a micro mechanical vibration structure according to claim 1,
In the first step, a vibration structure made of graphene is formed on a substrate,
In the second step, a XeF 2 gas is allowed to act on the vibration structure.
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