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JP6967239B2 - Electron beam transmission membrane and electronic device - Google Patents
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JP6967239B2 - Electron beam transmission membrane and electronic device - Google Patents

Electron beam transmission membrane and electronic device Download PDF

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JP6967239B2
JP6967239B2 JP2017075503A JP2017075503A JP6967239B2 JP 6967239 B2 JP6967239 B2 JP 6967239B2 JP 2017075503 A JP2017075503 A JP 2017075503A JP 2017075503 A JP2017075503 A JP 2017075503A JP 6967239 B2 JP6967239 B2 JP 6967239B2
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electron beam
substrate
recess
transmitting film
thickness
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JP2018181471A (en
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洋志 菅
諒 狩野
淳 宮脇
哲夫 清水
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National Institute of Advanced Industrial Science and Technology AIST
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本発明は、電子線透過膜及び電子デバイスに関する。 The present invention relates to an electron beam transmitting membrane and an electronic device.

電子線透過膜は、様々な用途で用いられている。例えば電子デバイスの動作を原子レベルで解明する際に用いられている。電子デバイスは一般に基板上に形成されるが、基板の厚みが厚すぎると電子線は透過できない。そのため、基板の一部を薄く加工し、電子線透過膜を形成することで、透過型電子顕微鏡を用いた電子デバイスの動作の測定が可能となる。 Electron beam transmission membranes are used for various purposes. For example, it is used to elucidate the operation of electronic devices at the atomic level. Electronic devices are generally formed on a substrate, but if the thickness of the substrate is too thick, electron beams cannot pass through. Therefore, by thinly processing a part of the substrate to form an electron beam transmitting film, it is possible to measure the operation of the electronic device using a transmission electron microscope.

また電子線透過膜は、生体分子やウィルスの反応機構を解明する際にも用いられている。生体分子やウィルスは、高真空下では死滅のおそれがある。そこで高真空領域で発生した電子線を、電子線透過膜を介して生体分子やウィルスに照射することで、これらの反応機構の解明が行われている。 The electron beam permeable membrane is also used to elucidate the reaction mechanism of biomolecules and viruses. Biomolecules and viruses can die under high vacuum. Therefore, the reaction mechanism of these reactions has been elucidated by irradiating biomolecules and viruses with electron beams generated in a high vacuum region via an electron beam permeable membrane.

電子線透過膜としては様々なものが知られている。電子デバイスの動作を測定する場合は、基板を加工して電子線透過膜を作製する。基板の加工方法としては、集束イオンビーム(FIB)加工(非特許文献1)、フォトリソグラフィー法を用いたウェットエッチング加工(特許文献1)等が知られている。またこの他、メンブレンを電子線透過膜として使用することも行われている(特許文献2)。 Various electron beam transmission films are known. When measuring the operation of an electronic device, the substrate is processed to produce an electron beam transmitting film. As a method for processing a substrate, focused ion beam (FIB) processing (Non-Patent Document 1), wet etching processing using a photolithography method (Patent Document 1), and the like are known. In addition, the membrane is also used as an electron beam transmitting membrane (Patent Document 2).

特開2010−61812号公報Japanese Unexamined Patent Publication No. 2010-61812 特開2006−219314号公報Japanese Unexamined Patent Publication No. 2006-219314

L. A Giannuzzi, and F. A. Stevie, A review of focused ion beam milling techniques for TEM specimen preparation, Micron 30 (1999) 197-204.L. A Giannuzzi, and F. A. Stevie, A review of focused ion beam milling techniques for TEM specimen preparation, Micron 30 (1999) 197-204.

しかしながら、上記の方法はいずれも電子線透過膜を作製するための加工時間が長いという問題がある。またいずれの方法も、加工のために大掛かりな設備が必要であり、設備投資が必要となる。フォトリソグラフィー法を用いた方法は、加工プロセスが多く煩雑であり、マスクとして用いるレジスト等による汚染の可能性もある。 However, all of the above methods have a problem that the processing time for producing the electron beam transmitting film is long. In addition, both methods require large-scale equipment for processing and require capital investment. The method using the photolithography method has many processing processes and is complicated, and there is a possibility of contamination by a resist or the like used as a mask.

本発明は上記問題に鑑みてなされたものであり、簡便に作製可能で低コストな電子線透過膜を提供することを目的とする。 The present invention has been made in view of the above problems, and an object of the present invention is to provide an electron beam transmitting membrane that can be easily manufactured and is inexpensive.

本発明者らは、鋭意検討の結果、局所プラズマエッチング技術を用いることで、簡便かつ低コストに電子線透過膜を得ることができることを見出した。また局所プラズマエッチング技術を用いて作製した構造体を電子線透過膜として用いることができることを見出した。
本発明は、上記課題を解決するため、以下の手段を提供する。
As a result of diligent studies, the present inventors have found that an electron beam transmitting film can be obtained easily and at low cost by using a local plasma etching technique. It was also found that the structure prepared by using the local plasma etching technique can be used as an electron beam transmitting film.
The present invention provides the following means for solving the above problems.

(1)第1の態様にかかる電子線透過膜は、基基板の第1面から対向する第2面に向かって形成された凹部を有し、前記凹部は湾曲面を有し、前記凹部の最底部と前記第2面との厚みが、電子線が透過可能な厚み以下である。 (1) The electron beam transmitting film according to the first aspect has a recess formed from the first surface of the base substrate toward the facing second surface, the recess has a curved surface, and the recess has a curved surface. The thickness of the bottom portion and the second surface is equal to or less than the thickness through which the electron beam can pass.

(2)上記態様にかかる電子線透過膜において、前記凹部の最底部と前記第2面との厚みが200nm以下であってもよい。 (2) In the electron beam transmitting film according to the above aspect, the thickness of the bottommost portion of the recess and the second surface may be 200 nm or less.

(3)上記態様にかかる電子線透過膜において、前記基板が、前記第2面側に絶縁体層を有する半導体基板であってもよい。 (3) In the electron beam transmitting film according to the above aspect, the substrate may be a semiconductor substrate having an insulator layer on the second surface side.

(4)上記態様にかかる電子線透過膜において、前記絶縁体層が酸化シリコン又は窒化シリコンであり、前記半導体基板がシリコン基板であってもよい。 (4) In the electron beam transmission film according to the above embodiment, the insulator layer may be silicon oxide or silicon nitride, and the semiconductor substrate may be a silicon substrate.

(5)第2の態様にかかる電子デバイスは、上記態様にかかる電子線透過膜と、前記電子線透過膜の凹部が形成されていない第2面に設けられた素子部と、を備える。 (5) The electronic device according to the second aspect includes the electron beam transmitting film according to the above aspect and an element portion provided on the second surface on which the recess of the electron beam transmitting film is not formed.

上記態様にかかる電子線透過膜は、簡便に作製でき、低コストである。 The electron beam permeable membrane according to the above aspect can be easily produced and is low in cost.

本実施形態にかかる電子線透過膜の断面模式図である。It is sectional drawing of the electron beam transmission membrane which concerns on this embodiment. 本実施形態にかかる電子線透過膜の製造過程を模式的に示した図である。It is a figure which showed schematically the manufacturing process of the electron beam transmission film which concerns on this embodiment. フォトリソグラフィー法を用い、ウェットエッチングで作製された凹部を有する電子線透過膜の断面図である。It is sectional drawing of the electron beam transmission film which has the recess made by wet etching using the photolithography method. 本実施形態にかかる電子デバイスの断面模式図である。It is sectional drawing of the electronic device which concerns on this embodiment. 実施例1で作製した電子線透過膜の写真である。It is a photograph of the electron beam transmission film produced in Example 1. 実施例1において電子線透過膜を介して金属配線Mを観察した図である。It is a figure which observed the metal wiring M through an electron beam transmission film in Example 1. FIG.

以下、添付図面を参照しながら本発明の実施形態を詳細に説明する。 Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings.

「電子線透過膜」
図1は、本実施形態にかかる電子線透過膜の断面模式図である。図1に示す電子線透過膜10は、凹部4が形成された基板1である。凹部4は、基板1の第1面1aから対向する第2面1bに向かって形成されている。凹部4は、お椀状の湾曲面4aを有する。図1において基板1は、半導体基板2と絶縁体層3とからなる。絶縁体層3は、基板1の第2面1b側に設けられている。
"Electron beam transmission membrane"
FIG. 1 is a schematic cross-sectional view of an electron beam transmitting membrane according to the present embodiment. The electron beam transmitting film 10 shown in FIG. 1 is a substrate 1 on which a recess 4 is formed. The recess 4 is formed from the first surface 1a of the substrate 1 toward the facing second surface 1b. The recess 4 has a bowl-shaped curved surface 4a. In FIG. 1, the substrate 1 is composed of a semiconductor substrate 2 and an insulator layer 3. The insulator layer 3 is provided on the second surface 1b side of the substrate 1.

本実施形態にかかる電子線透過膜10は、局所プラズマエッチング技術によって作製されたものである。凹部4の湾曲面4aは、局所プラズマエッチング技術で作製されたものに特有の構造である。 The electron beam transmission film 10 according to the present embodiment is manufactured by a local plasma etching technique. The curved surface 4a of the recess 4 has a structure peculiar to that manufactured by the local plasma etching technique.

局所プラズマエッチング技術とは、プラズマを利用して試料に残渣を残すことなく、サブミリメーター径の局所加工を行うことが可能な技術である。またこの方法は、加工対象の温度上昇を抑え、ダメージを少なくできるという利点も有する。 The local plasma etching technique is a technique that can perform local processing with a submillimeter diameter by using plasma without leaving a residue on the sample. This method also has an advantage that the temperature rise of the object to be processed can be suppressed and damage can be reduced.

図2は、本実施形態にかかる電子線透過膜10の製造過程を模式的に示した図である。局所プラズマエッチング技術は、高周波を印加できる電極を有するキャピラリを準備する工程と、このキャピラリの一端を加工対象に近接させる工程と、キャピラリ内にエッチングガスを導入し、高周波を印加することでプラズマを発生させる工程と、を有する。以下、具体的に説明する。 FIG. 2 is a diagram schematically showing the manufacturing process of the electron beam transmitting film 10 according to the present embodiment. Local plasma etching technology has a process of preparing a capillary having an electrode that can apply high frequency, a process of bringing one end of this capillary close to the processing target, and a process of introducing etching gas into the capillary and applying high frequency to plasma. It has a step of generating it. Hereinafter, a specific description will be given.

まず図2に示すように、交流を印加できる電源13に接続された円筒状の電極11を有するキャピラリ12を準備する。キャピラリ12は、アルミナ等を用いることができる。 First, as shown in FIG. 2, a capillary 12 having a cylindrical electrode 11 connected to a power source 13 to which alternating current can be applied is prepared. Alumina or the like can be used for the capillary 12.

次いで、このキャピラリの第1端12aを加工対象である基板1の第1面1aに近接させる。キャピラリ12内には、エッチングガスを導入し、キャピラリ12の第2端12b側に吸引する。すなわち、エッチングガスはキャピラリ12の第1端12aから第2端12bに向かうガス流が生み出される。図2ではガス流の流れを矢印として図示した。 Next, the first end 12a of the capillary is brought close to the first surface 1a of the substrate 1 to be processed. Etching gas is introduced into the capillary 12 and sucked into the second end 12b side of the capillary 12. That is, the etching gas produces a gas flow from the first end 12a of the capillary 12 toward the second end 12b. In FIG. 2, the flow of the gas flow is shown as an arrow.

電源13により電極11に電流を加えると高周波が発生する。高周波が印加されたキャピラリ12内のエッチングガスは、プラズマ化する。生じたプラズマPの一部は、ガス流に逆らってキャピラリ12の第1端12aから浸み出し、基板1の第1面1aを局所エッチングする。 When a current is applied to the electrode 11 by the power supply 13, a high frequency is generated. The etching gas in the capillary 12 to which a high frequency is applied is turned into plasma. A part of the generated plasma P seeps out from the first end 12a of the capillary 12 against the gas flow, and locally etches the first surface 1a of the substrate 1.

局所エッチングは、基板1の第1面1aから原子を1層ずつ剥ぎ取るように進行する。そのため、エッチングの過程でできる角部は徐々に無くなり、お椀状の湾曲面4aが形成される。エッチングの進行状態は、カメラ14で確認する。プラズマ発光で生じた光のうち特定の波長の光をカメラで検出したところでエッチングを終了する。プラズマ発光で生じた光は、長波長の光から順にカメラで検出される。そのため、何れの波長を検出した際にエッチングを止めるかを設定することで、凹部4の深さを自由に設定できる。 The local etching proceeds so as to strip the atoms one layer at a time from the first surface 1a of the substrate 1. Therefore, the corners formed in the etching process gradually disappear, and a bowl-shaped curved surface 4a is formed. The progress of etching is confirmed by the camera 14. Etching ends when the camera detects light of a specific wavelength among the light generated by plasma emission. The light generated by plasma emission is detected by the camera in order from the long wavelength light. Therefore, the depth of the recess 4 can be freely set by setting which wavelength is detected when the etching is stopped.

局所エッチング法を用いると、500μm程度の厚みのSi基板を20分程度で貫通させることができ、凹部4を極めて簡便かつ素早く形成できる。凹部4の形成速度は、エッチングガス種、エッチングガスの供給速度、印加する高周波の強度、処理環境の真空度等を調整することで、自由に設計できる。 When the local etching method is used, a Si substrate having a thickness of about 500 μm can be penetrated in about 20 minutes, and the recess 4 can be formed extremely easily and quickly. The formation speed of the recess 4 can be freely designed by adjusting the etching gas type, the etching gas supply speed, the intensity of the applied high frequency, the degree of vacuum in the processing environment, and the like.

図3は、フォトリソグラフィー法を用い、ウェットエッチングで作製された凹部を有する電子線透過膜の断面図である。図3に示す電子線透過膜20は、半導体基板22と絶縁体層23とを備える基板21の第1面21aから第2面21bに向かって形成された凹部24を有する点は、図1に示す本実施形態にかかる電子線透過膜10と同様である。一方で、凹部24の断面視形状は台形状であり、凹部24を形成する面24aが湾曲面ではない点が異なる。 FIG. 3 is a cross-sectional view of an electron beam transmitting film having recesses produced by wet etching using a photolithography method. The point that the electron beam transmission film 20 shown in FIG. 3 has a recess 24 formed from the first surface 21a to the second surface 21b of the substrate 21 including the semiconductor substrate 22 and the insulator layer 23 is shown in FIG. It is the same as the electron beam transmission membrane 10 which concerns on this embodiment shown. On the other hand, the cross-sectional view shape of the recess 24 is trapezoidal, and the difference is that the surface 24a forming the recess 24 is not a curved surface.

フォトリソグラフィー法では、凹部24を開けたい部分以外の場所にレジスト等の保護膜を設け、エッチング処理を行う。レジストの開口部内におけるエッチング速度は、レジスト近傍を除き、略一定である。そのため、フォトリソグラフィー法を用いると、凹部24の形状は原則台形状になり、図1に示す凹部4の湾曲面4aは形成されない。 In the photolithography method, a protective film such as a resist is provided at a place other than the portion where the recess 24 is desired to be opened, and the etching process is performed. The etching rate in the opening of the resist is substantially constant except in the vicinity of the resist. Therefore, when the photolithography method is used, the shape of the recess 24 is in principle trapezoidal, and the curved surface 4a of the recess 4 shown in FIG. 1 is not formed.

フォトリソグラフィー法は、レスストの塗布、露光、現像、レジスト剥離等の種々の工程が必要である。そのため、凹部24を形成するために長時間が必要であり、高コストである。 The photolithography method requires various steps such as coating, exposure, development, and resist peeling. Therefore, a long time is required to form the recess 24, which is high cost.

上述のように、本実施形態にかかる電子線透過膜10の凹部4は、製造方法に特有の湾曲面4aを有する。電子線透過膜10は湾曲面4aを有するということは換言すると、電子線透過膜10の最薄部がアーチ形状の基板1で支持されていることを意味する。橋脚の形状に見られるように、アーチ形状が最も効率よく上方から下方への荷重を支えることができる構造であり、最薄部のたわみを抑制することができる。最薄部のたわみが抑制されると、最薄部の面積を広くすることができる。電子線透過膜10として最も重要なのは最薄部であり、最薄部の面積を広くできることは、電子線透過膜において極めて重要である。 As described above, the recess 4 of the electron beam transmitting film 10 according to the present embodiment has a curved surface 4a peculiar to the manufacturing method. In other words, the fact that the electron beam transmitting film 10 has a curved surface 4a means that the thinnest portion of the electron beam transmitting film 10 is supported by the arch-shaped substrate 1. As seen in the shape of the pier, the arch shape is the structure that can most efficiently support the load from above to below, and can suppress the deflection of the thinnest part. When the deflection of the thinnest part is suppressed, the area of the thinnest part can be increased. The thinnest part is the most important as the electron beam transmitting film 10, and it is extremely important in the electron beam transmitting film that the area of the thinnest part can be widened.

また電子線は、電子線透過膜10の凹部4と第2面2bの間を透過する。そのため、図1に示すように、凹部4の最底部4bと基板1の第2面2bとの間の厚みdは、電子線が透過可能な厚み以下である。電子線が透過可能な厚みは、照射する電子線の強度等によっても変わる。 Further, the electron beam passes between the recess 4 of the electron beam transmitting film 10 and the second surface 2b. Therefore, as shown in FIG. 1, the thickness d between the bottommost portion 4b of the recess 4 and the second surface 2b of the substrate 1 is equal to or less than the thickness through which the electron beam can pass. The thickness through which the electron beam can pass varies depending on the intensity of the irradiated electron beam and the like.

凹部4の最底部4bと基板1の第2面2bとの間の厚みdは、具体的には200nm以下であることが好ましく、150nm以下であることがより好ましく、120nm以下であることがさらに好ましい。また厚みdが薄すぎると電子線透過膜10の強度が低下するため、厚みdは10nm以上であることが好ましく、30nm以上であることがより好ましく、50nm以上であることがさらに好ましい。 Specifically, the thickness d between the bottommost portion 4b of the recess 4 and the second surface 2b of the substrate 1 is preferably 200 nm or less, more preferably 150 nm or less, and further preferably 120 nm or less. preferable. Further, if the thickness d is too thin, the strength of the electron beam transmitting film 10 is lowered, so that the thickness d is preferably 10 nm or more, more preferably 30 nm or more, still more preferably 50 nm or more.

凹部4の最底部4bと基板1の第2面2bとの間の厚みdは、レーザー顕微鏡を用いて測定することができる。レーザー顕微鏡を用いて凹部4を観察すると光干渉膜が見られる。光干渉膜は、凹部4の湾曲面4aで反射する光と、基板1の第2面1bで反射する光の干渉によって生じる。入射光の波長をλ、基板1の屈折率をn、回折時数をmとすると、明環部における厚みdはd=(m+1/2)×λ/2nで求められ、暗環部における厚みdはd=m×λ/2nで求められる。 The thickness d between the bottommost portion 4b of the recess 4 and the second surface 2b of the substrate 1 can be measured using a laser microscope. When the concave portion 4 is observed using a laser microscope, an optical interference film can be seen. The optical interference film is generated by the interference between the light reflected by the curved surface 4a of the recess 4 and the light reflected by the second surface 1b of the substrate 1. Assuming that the wavelength of the incident light is λ, the refractive index of the substrate 1 is n, and the diffraction time is m, the thickness d L in the bright ring portion is obtained by d L = (m + 1/2) × λ / 2n, and the dark ring portion is obtained. The thickness d D in is obtained by d D = m × λ / 2n.

また凹部4の最底部4bと基板1の第2面2bとの間の厚みdは、作製時にカメラ14に入射する透過光の強度から求めてもよい。透過光の強度と厚みdとの関係は、波長ごとの透過率を事前に測定して求められる。一般に透過光の強度をI、入射光の強度をI、基板1の吸収係数をα、膜厚をdとすると、I=I―αdの関係が成り立つ。 Further, the thickness d between the bottommost portion 4b of the recess 4 and the second surface 2b of the substrate 1 may be obtained from the intensity of the transmitted light incident on the camera 14 at the time of fabrication. The relationship between the intensity of the transmitted light and the thickness d is obtained by measuring the transmittance for each wavelength in advance. Generally, if the intensity of transmitted light is I, the intensity of incident light is I 0 , the absorption coefficient of substrate 1 is α, and the film thickness is d, the relationship of I = I 0 e − αd holds.

凹部4の最底部4bの位置は、任意に設定できる。電子線の透過しやすさの観点では、凹部4の最底部4bは絶縁体層3まで到達していることが好ましい。異なる屈折率の物質を電子線が透過すると、界面で電子線の屈折が生じるためである。一方で、電子線透過膜10の強度を高める観点では、凹部4の最底部4bは絶縁体層3まで到達していないことが好ましい。半導体基板2が除去されると、残った絶縁体層3の圧縮応力が開放され、座屈する場合がある。 The position of the bottommost portion 4b of the recess 4 can be arbitrarily set. From the viewpoint of ease of electron beam transmission, it is preferable that the bottommost portion 4b of the recess 4 reaches the insulator layer 3. This is because when an electron beam is transmitted through a substance having a different refractive index, the electron beam is refracted at the interface. On the other hand, from the viewpoint of increasing the strength of the electron beam transmitting film 10, it is preferable that the bottommost portion 4b of the recess 4 does not reach the insulator layer 3. When the semiconductor substrate 2 is removed, the compressive stress of the remaining insulator layer 3 is released, and buckling may occur.

基板1は、図1に示す半導体基板2と絶縁体層3とからなるものに限られない。例えば、単層の基板でもよいし、2層以上の複数層の基板でもよい。また半導体、絶縁体に限られず、金属層を有してもよい。一方で、電子線の散乱を抑制するという観点では、金属層は含まない方が好ましい。 The substrate 1 is not limited to the semiconductor substrate 2 shown in FIG. 1 and the insulator layer 3. For example, it may be a single-layer substrate or a multi-layer substrate having two or more layers. Further, the present invention is not limited to semiconductors and insulators, and may have a metal layer. On the other hand, from the viewpoint of suppressing the scattering of electron beams, it is preferable not to include the metal layer.

図1に示すように基板1が半導体基板2と絶縁体層3とを有すると、電子線透過膜10を電子デバイスに組み込みやすくなる。半導体基板2は、例えばSi基板のような公知の半導体を用いることができる。また絶縁体層3は、基板がシリコンの場合は、酸化シリコン(SiO)、窒化シリコン(SiN)等を用いることができる。 As shown in FIG. 1, when the substrate 1 has the semiconductor substrate 2 and the insulator layer 3, the electron beam transmission film 10 can be easily incorporated into the electronic device. As the semiconductor substrate 2, a known semiconductor such as a Si substrate can be used. When the substrate is silicon, silicon oxide (SiO 2 ), silicon nitride (SiN), or the like can be used for the insulator layer 3.

上述のように、本実施形態にかかる電子線透過膜10は、局所プラズマエッチング技術を用いて簡便に作製でき、低コストである。また電子線透過膜10の凹部4が湾曲面4aを有することで、最薄部のたわみを抑制することができる。 As described above, the electron beam transmission film 10 according to the present embodiment can be easily manufactured by using a local plasma etching technique, and is low in cost. Further, since the concave portion 4 of the electron beam transmitting film 10 has the curved surface 4a, the deflection of the thinnest portion can be suppressed.

「電子デバイス」
図4は、本実施形態にかかる電子デバイスの断面模式図である。図4に示す電子デバイス100は、図1に示す電子線透過膜10と、電子線透過膜10の凹部4が形成されていない第2面1bに設けられた素子部30と、を備える。
"Electronic device"
FIG. 4 is a schematic cross-sectional view of the electronic device according to the present embodiment. The electronic device 100 shown in FIG. 4 includes an electron beam transmitting film 10 shown in FIG. 1 and an element portion 30 provided on a second surface 1b in which a recess 4 of the electron beam transmitting film 10 is not formed.

図4に示す素子部30は、ソース電極31と、ドレイン電極32と、半導体領域33と、ゲート電極34と、を備えるトランジスタである。ソース電極31とドレイン電極32間の半導体領域33内に流れる電子をゲート電極34で制御する。 The element unit 30 shown in FIG. 4 is a transistor including a source electrode 31, a drain electrode 32, a semiconductor region 33, and a gate electrode 34. The gate electrode 34 controls the electrons flowing in the semiconductor region 33 between the source electrode 31 and the drain electrode 32.

図4に示す電子デバイス100は、半導体領域33の動的な変化を、電子線透過膜10の第1面1a側から透過型電子線顕微鏡を用いて観察できる。電子顕微鏡では、観察対象に対して電子線を当てる。電子線透過膜10は、凹部4を有することで電子線が透過できる。そのため電子線は、電子線透過膜10を有していても、半導体領域33の動的な変化を観察できる。 In the electronic device 100 shown in FIG. 4, the dynamic change of the semiconductor region 33 can be observed from the first surface 1a side of the electron beam transmitting film 10 by using a transmission type electron beam microscope. In an electron microscope, an electron beam is applied to the observation target. Since the electron beam transmitting film 10 has the recess 4, the electron beam can be transmitted through the electron beam transmitting film 10. Therefore, even if the electron beam has the electron beam transmitting film 10, the dynamic change of the semiconductor region 33 can be observed.

図4に示す電子デバイス100の場合、半導体領域33への外部からの影響からの影響を避けるために、基板1の第2面2bには絶縁体層3を設けることが好ましい。 In the case of the electronic device 100 shown in FIG. 4, it is preferable to provide the insulator layer 3 on the second surface 2b of the substrate 1 in order to avoid the influence from the outside on the semiconductor region 33.

上述のように、本実施形態にかかる電子デバイス100は、電子線透過膜10を有するため、電子線透過膜10を介して素子部30の状態を観察できる。 As described above, since the electronic device 100 according to the present embodiment has the electron beam transmitting film 10, the state of the element unit 30 can be observed via the electron beam transmitting film 10.

以上、本発明の好ましい実施の形態について詳述したが、本発明は特定の実施の形態に限定されるものではなく、特許請求の範囲内に記載された本発明の要旨の範囲内において、種々の変形・変更が可能である。 Although the preferred embodiments of the present invention have been described in detail above, the present invention is not limited to the specific embodiments and varies within the scope of the gist of the present invention described in the claims. Can be transformed / changed.

例えば、素子部30は図4に示すトランジスタに限られず、任意の素子を用いることができる。例えば、MEMS、センサ、電池、アクチュエタ、マイクロポンプ、バイオチップ、マイクロ流路、マイクロ発電、振動発電素子、メモリー、分析電極等を用いることができる。 For example, the element unit 30 is not limited to the transistor shown in FIG. 4, and any element can be used. For example, MEMS, sensors, batteries, actuators, micropumps, biochips, microchannels, micropower generation, vibration power generation elements, memories, analysis electrodes and the like can be used.

また生体分子やウィルスの反応機構を解明するための隔壁として電子線透過膜10を利用する場合は、電子線透過膜10を単体で用いてもよい。 When the electron beam permeable membrane 10 is used as a partition wall for elucidating the reaction mechanism of a biomolecule or a virus, the electron beam permeable membrane 10 may be used alone.

「実施例1」
まず表面に280nm厚のSiO膜を有する380μm厚のSi基板を準備する。SiO膜は、熱酸化により作製する。
"Example 1"
First, a 380 μm-thick Si substrate having a 280 nm-thick SiO 2 film on the surface is prepared. The SiO 2 film is produced by thermal oxidation.

また図2に示すように、第1端12aを内径1mmに絞ったアルミナ製のキャピラリ12を準備する。キャピラリ12には、交流を印加できる電源13に接続された円筒状の電極11が設けられている。そして、キャピラリ12の第1端12aを、準備したSi基板から0.1mm程度の近接した位置に設置する。 Further, as shown in FIG. 2, an alumina capillary 12 having a first end 12a narrowed to an inner diameter of 1 mm is prepared. The capillary 12 is provided with a cylindrical electrode 11 connected to a power source 13 to which alternating current can be applied. Then, the first end 12a of the capillary 12 is installed at a position close to the prepared Si substrate by about 0.1 mm.

マスフローコントロラーを用いてエッチングガスをチャンバー内に供給する。エッチングガスは、フッ化炭素を用いた。フッ化炭素はAr等の希ガスを用いて混合希釈してもよいが、ここでは希釈せずに用いた。キャピラリ12は、第2端12b側から排気され、第1端12aから第2端12bへ向かうガス流が形成される。 Etching gas is supplied into the chamber using a mass flow controller. Fluorocarbon was used as the etching gas. Fluorocarbon may be mixed and diluted with a rare gas such as Ar, but here, it is used without dilution. The capillary 12 is exhausted from the second end 12b side, and a gas flow from the first end 12a to the second end 12b is formed.

次いで、電極11に13.56MHzの高周波を印加して、エッチングガスをプラズマ化した。プラズマは、キャピラリの第1端12aと準備したSi基板との間に、第1端12aの内径程度の範囲で局在化し、局在エッチングが進行する。 Next, a high frequency of 13.56 MHz was applied to the electrode 11 to turn the etching gas into plasma. The plasma is localized between the first end 12a of the capillary and the prepared Si substrate within a range of about the inner diameter of the first end 12a, and the localized etching proceeds.

エッチングの進行状態は、SiO面をショートパスフィルターを通してカメラ14でモニターした。そして、プラズマ発光のうち440nm以下の波長のみが一定の強度で透過した時点で、エッチングを止めた。エッチング加工に要した時間は約20分であった。 The progress of etching was monitored by the camera 14 on the two sides of the SiO through a short pass filter. Then, when only the wavelength of 440 nm or less of the plasma emission was transmitted with a constant intensity, the etching was stopped. The time required for the etching process was about 20 minutes.

図5は、実施例1で作製した電子線透過膜の写真である。図5(a)は、凹部を斜め方向から撮影した全体像であり、図5(b)は電子線透過膜の断面を走査型電子顕微鏡(SEM)で撮影した画像である。凹部の開口径は、1.2mmであり、深さは約380μmであった。 FIG. 5 is a photograph of the electron beam transmitting membrane produced in Example 1. FIG. 5A is an overall image of the recess taken from an oblique direction, and FIG. 5B is an image of a cross section of the electron beam transmitting film taken with a scanning electron microscope (SEM). The opening diameter of the recess was 1.2 mm, and the depth was about 380 μm.

また凹部の最底部と基板の非加工面との間の厚みを、レーザー顕微鏡で観察される光干渉膜から求めた。はっきり認識できる明環及び暗環から求められる凹部の最底部と基板の非加工面との間の厚みは、69nm〜120nmであった。 Further, the thickness between the bottom of the recess and the unprocessed surface of the substrate was determined from the optical interference film observed with a laser microscope. The thickness between the bottom of the recesses, which can be clearly recognized from the bright and dark rings, and the unprocessed surface of the substrate was 69 nm to 120 nm.

またラマン顕微鏡(励起波長488nm)及びエネルギー分散型X線(EDX)分析器を用いて、凹部近傍の元素分析も行った。その結果、直径50μmの範囲で、SiOの存在が確認された。SiOが確認されたということは、Si基板が除去されていることを示す。すなわちこの結果は、凹部の深さ及び凹部の最底部と基板の非加工面との間の厚みの結果と整合している。 Elemental analysis in the vicinity of the recess was also performed using a Raman microscope (excitation wavelength 488 nm) and an energy dispersive X-ray (EDX) analyzer. As a result, the presence of SiO 2 was confirmed within the range of 50 μm in diameter. The fact that SiO 2 is confirmed indicates that the Si substrate has been removed. That is, this result is consistent with the result of the depth of the recess and the thickness between the bottom of the recess and the unprocessed surface of the substrate.

そして金属配線を作製した基板上に作製した電子線透過膜を設置し、走査型電子顕微鏡で観察した。図6(a)は、電子線透過膜を介して金属配線Mを作製した基板を可視光で観察した図であり、図6(b)は、電子線透過膜を介して金属配線Mを作製した基板を電子線で観察したSEM図である。 Then, the prepared electron beam transmission film was placed on the substrate on which the metal wiring was made, and observed with a scanning electron microscope. FIG. 6A is a view of observing a substrate on which a metal wiring M is manufactured via an electron beam transmitting film with visible light, and FIG. 6B is a diagram in which a metal wiring M is manufactured via an electron beam transmitting film. It is an SEM diagram which observed the substrate with an electron beam.

Si基板は可視光を透過できるため、図6(a)に示すように金属配線Mが何れの場所でも確認できる。これに対して電子線は、凹部が設けられた部分において金属配線Mが確認できている。換言すると、実施例1で作製した構造体は、凹部において電子線を透過することができ、電子線透過膜として利用できる。 Since the Si substrate can transmit visible light, the metal wiring M can be confirmed at any place as shown in FIG. 6A. On the other hand, in the electron beam, the metal wiring M can be confirmed in the portion where the recess is provided. In other words, the structure produced in Example 1 can transmit an electron beam in the recess and can be used as an electron beam transmitting film.

1,21…基板、1a,21a…第1面、1b,21b…第2面、2,22…半導体基板、3,23…絶縁体層、4,24…凹部、4a…湾曲面、24a…面、4b…最底部、11…電極、12…キャピラリ、12a…第1端、12b…第2端、13…電源、14…カメラ、30…素子部、31…ソース電極、32…ドレイン電極、33…半導体領域、34…ゲート電極、P…プラズマ、M…金属配線 1,21 ... Substrate, 1a, 21a ... First surface, 1b, 21b ... Second surface, 2,22 ... Semiconductor substrate, 3,23 ... Insulator layer, 4,24 ... Recessed, 4a ... Curved surface, 24a ... Surface, 4b ... bottom, 11 ... electrode, 12 ... capillary, 12a ... first end, 12b ... second end, 13 ... power supply, 14 ... camera, 30 ... element part, 31 ... source electrode, 32 ... drain electrode, 33 ... semiconductor area, 34 ... gate electrode, P ... plasma, M ... metal wiring

Claims (4)

半導体基板と絶縁体層とを備える基板を有し、
前記基板は、前記基板の第1面から対向する第2面に向かって形成された凹部を有し、
前記凹部は湾曲面を有し、
前記湾曲面は、前記半導体基板から前記絶縁体層に亘って形成され、
前記凹部の最底部と前記第2面との厚みが、電子線が透過可能な厚み以下である、電子線透過膜。
It has a substrate with a semiconductor substrate and an insulator layer,
The substrate has a recess formed from the first surface of the substrate toward the facing second surface.
The recess has a curved surface and has a curved surface.
The curved surface is formed from the semiconductor substrate to the insulator layer.
An electron beam transmitting film in which the thickness of the bottommost portion of the recess and the second surface is equal to or less than the thickness through which an electron beam can pass.
前記凹部の最底部と前記第2面との厚みが200nm以下である、請求項1に記載の電子線透過膜。 The electron beam transmitting film according to claim 1, wherein the thickness of the bottommost portion of the recess and the second surface is 200 nm or less. 前記絶縁体層が酸化シリコン又は窒化シリコンであり、前記半導体基板がシリコン基板である、請求項2に記載の電子線透過膜。 The electron beam transmission film according to claim 2, wherein the insulator layer is silicon oxide or silicon nitride, and the semiconductor substrate is a silicon substrate. 子線透過膜と、
前記電子線透過膜の凹部が形成されていない第2面に設けられた素子部と、を備え
前記電子線透過膜は、基板の第1面から対向する第2面に向かって形成された凹部を有し、
前記凹部は湾曲面を有し、
前記凹部の最底部と前記第2面との厚みが、電子線が透過可能な厚み以下である、電子デバイス。
And electron-ray transparent film,
The element portion provided on the second surface on which the concave portion of the electron beam transmitting film is not formed is provided .
The electron beam transmitting film has a recess formed from the first surface of the substrate toward the facing second surface.
The recess has a curved surface and has a curved surface.
An electronic device in which the thickness of the bottommost portion of the recess and the second surface is equal to or less than the thickness through which an electron beam can pass.
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