JP6487294B2 - Compound charged particle beam system - Google Patents

Compound charged particle beam system Download PDF

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JP6487294B2
JP6487294B2 JP2015157298A JP2015157298A JP6487294B2 JP 6487294 B2 JP6487294 B2 JP 6487294B2 JP 2015157298 A JP2015157298 A JP 2015157298A JP 2015157298 A JP2015157298 A JP 2015157298A JP 6487294 B2 JP6487294 B2 JP 6487294B2
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高橋 春男
春男 高橋
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Hitachi High Tech Science Corp
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Description

本発明は複数の荷電粒子ビーム装置を統合した、複合荷電粒子ビーム装置に関するものである。   The present invention relates to a composite charged particle beam apparatus in which a plurality of charged particle beam apparatuses are integrated.

近年、半導体デバイスのパターン微細化に伴い、半導体デバイスの特定微小部を透過型電子顕微鏡(TEM:Transmission Electron Microscope)によって観察し、評価する技術の重要性が高まっている。このような特定微小部となる試料を作成するには、集束イオンビーム(FIB:Focused Ion Beam)装置が広く用いられているが、FIBによる試料作製は試料の表面の厚さ数nm〜数十nmが変質してしまう。この変質層をダメージ層と称する。薄片化試料に要求される厚みが小さくなるにつれて、試料全体の厚みに占めるこのダメージ層の割合が相対的に大きくなり、TEM観察の支障となる。そのため、TEM観察用薄片化試料表面のダメージ層を除去するための方法が必要とされている。   2. Description of the Related Art In recent years, with the miniaturization of semiconductor device patterns, the importance of techniques for observing and evaluating specific minute portions of a semiconductor device with a transmission electron microscope (TEM: Transmission Electron Microscope) is increasing. A focused ion beam (FIB) apparatus is widely used to prepare such a sample that becomes a specific minute portion. However, the sample preparation by FIB is performed with a thickness of several nanometers to several tens of nanometers on the surface of the specimen. nm is altered. This altered layer is referred to as a damaged layer. As the thickness required for the thinned sample decreases, the ratio of the damaged layer to the total thickness of the sample relatively increases, which hinders TEM observation. Therefore, a method for removing the damaged layer on the surface of the thinned sample for TEM observation is required.

特許文献1においては、上述した状況の解決策として、例えば、アルゴンなどの化学的活性の低い元素をイオン種とするイオンビームを数キロボルト以下の低い加速電圧で照射する方法が提案されている。また、このダメージ除去のプロセスを確実に、効率よく行うために、FIB鏡筒の軸と走査電子顕微鏡の軸とがそれぞれ試料ステージのユーセントリックチルト軸と実質的に直交し、かつFIB鏡筒の軸と気体イオンビーム鏡筒の軸と前記ユーセントリックチルト軸とが実用上一つの平面内にある位置関係に配置することが有効であることが、特許文献2において開示されている。これによりFIBで加工した試料面を適当な角度だけ傾けることで気体イオンビームを浅い角度で照射することが可能になり、かつ加工中の試料面を走査電子顕微鏡で観察することができる。   In Patent Document 1, as a solution to the above situation, for example, a method of irradiating an ion beam having an ion species of an element having low chemical activity such as argon with a low acceleration voltage of several kilovolts or less is proposed. In order to perform the damage removal process reliably and efficiently, the axis of the FIB column and the axis of the scanning electron microscope are substantially perpendicular to the eucentric tilt axis of the sample stage, and the FIB column It is disclosed in Patent Document 2 that it is effective to arrange the axis, the axis of the gas ion beam column, and the eucentric tilt axis in a practical relationship in one plane. Thus, it is possible to irradiate the gas ion beam at a shallow angle by tilting the sample surface processed by FIB by an appropriate angle, and the sample surface being processed can be observed with a scanning electron microscope.

特開平10−221227号公報JP-A-10-212227 特開2007−164992号公報JP 2007-164992 A

しかしながら、特許文献2で開示されている装置では、走査電子顕微鏡が試料と集束イオンビーム鏡筒に挟まれるように配置されているため、走査電子顕微鏡と試料との距離を短くできないという問題点がある。一般に走査電子顕微鏡は試料との距離が短いほど観察能力が向上する傾向がある。非常に微細な構造を含む極薄膜試料を確実に作製するためには、走査電子顕微鏡の観察能力の向上は非常に重要な課題である。   However, in the apparatus disclosed in Patent Document 2, since the scanning electron microscope is arranged so as to be sandwiched between the sample and the focused ion beam column, there is a problem in that the distance between the scanning electron microscope and the sample cannot be shortened. is there. In general, the scanning electron microscope tends to improve the observation capability as the distance from the sample is shorter. Improving the observation capability of a scanning electron microscope is a very important issue in order to reliably produce an extremely thin film sample having a very fine structure.

この発明は、このような事情を考慮してなされたもので、その目的は、集束イオンビーム装置でTEM観察用の薄片化試料を作製し、低加速電圧の気体イオンビーム装置で試料表面のダメージ層を除去する装置において、一連の工程で薄片化試料の状態を高分解能で観察するために、電子顕微鏡と試料との距離を短く配置可能な複合荷電粒子ビーム装置を提供することである。   The present invention has been made in view of such circumstances, and its purpose is to produce a thinned sample for TEM observation with a focused ion beam device and to damage the surface of the sample with a gas ion beam device with a low acceleration voltage. An object of the present invention is to provide a composite charged particle beam apparatus in which a distance between an electron microscope and a sample can be arranged short in order to observe a state of a sliced sample with high resolution in a series of steps in an apparatus for removing a layer.

上記の目的を達成するために、この発明は以下の手段を提供している。
本発明に係る複合荷電粒子ビーム装置は、集束イオンビームを照射して試料を薄膜化する集束イオンビーム鏡筒と、前記試料のダメージ層を除去する低加速電圧の気体イオンビームを照射する気体イオンビーム鏡筒と、前記集束イオンビームで前記試料を薄膜化しながら形成される薄膜化試料を垂直方向から観察する電子ビームを照射する走査電子顕微鏡筒と、を配置したことを特徴とする。
In order to achieve the above object, the present invention provides the following means.
A compound charged particle beam apparatus according to the present invention includes a focused ion beam column that irradiates a focused ion beam to thin a sample, and a gas ion that irradiates a gas ion beam having a low acceleration voltage for removing a damaged layer of the sample. A beam column and a scanning electron microscope column for irradiating an electron beam for observing a thinned sample formed while thinning the sample with the focused ion beam from a vertical direction are arranged.

本発明に係る複合荷電粒子ビーム装置は、集束イオンビーム鏡筒と、走査電子顕微鏡筒と、低加速電圧の気体イオンビーム鏡筒とを備え、前記集束イオンビーム鏡筒のビーム照射軸は、前記走査電子顕微鏡筒のビーム照射軸と略直交し、前記気体イオンビーム鏡筒のビーム照射軸は前記走査電子顕微鏡筒のビーム照射軸と90度より小さい角度で交わるように配置し、かつ、前記走査電子顕微鏡筒のビーム照射軸と前記気体イオンビーム鏡筒のビーム照射軸がなす角を、前記気体イオンビーム鏡筒のビーム照射軸を前記走査電子顕微鏡筒の軸と垂直な面に投影した線分と前記気体イオンビーム鏡筒のビーム照射軸がなす角よりも大きくなるようにして、集束イオンビームと電子ビームと気体ビームのそれぞれが、試料ステージに取り付けた試料に照射可能な位置に配置した複合荷電粒子ビーム装置であって、前記集束イオンビームで前記試料を薄膜化し、低加速電圧の気体イオンビームで薄膜化試料のダメージ層を除去する工程を、前記薄膜化試料を前記走査電子顕微鏡筒で垂直方向から観察しながら実施することを特徴とする。   A composite charged particle beam apparatus according to the present invention includes a focused ion beam column, a scanning electron microscope column, and a gas ion beam column with a low acceleration voltage, and a beam irradiation axis of the focused ion beam column includes: The beam irradiation axis of the scanning electron microscope tube is substantially orthogonal, the beam irradiation axis of the gas ion beam column is arranged to intersect the beam irradiation axis of the scanning electron microscope tube at an angle smaller than 90 degrees, and the scanning An angle formed by the beam irradiation axis of the electron microscope column and the beam irradiation axis of the gas ion beam column is a line segment obtained by projecting the beam irradiation axis of the gas ion beam column onto a plane perpendicular to the axis of the scanning electron microscope column. Each of the focused ion beam, electron beam, and gas beam is mounted on the sample stage so that the angle formed by the beam irradiation axis of the gas ion beam column is larger than the angle formed by the sample. A step of thinning the sample with the focused ion beam and removing a damaged layer of the thinned sample with a gas ion beam having a low acceleration voltage. It is characterized in that the measurement is performed while observing the sample from the vertical direction with the scanning electron microscope tube.

本発明によれば、電子顕微鏡と試料との距離を短くしてTEM観察用の薄片化試料の状態を観察しながら、集束イオンビーム装置で薄片化試料を作製し、低加速電圧の気体イオンビーム装置で試料表面のダメージ層を除去する一連の工程を実施可能な装置が実現され、微小な構造を観察するためのTEM観察用薄片化試料を確実に作製することができる。   According to the present invention, a thinned sample is produced by a focused ion beam device while observing the state of a thinned sample for TEM observation by shortening the distance between the electron microscope and the sample, and a gas ion beam having a low acceleration voltage is produced. An apparatus capable of performing a series of steps for removing a damaged layer on the sample surface with the apparatus is realized, and a thinned sample for TEM observation for observing a minute structure can be reliably produced.

本発明に係る複合荷電粒子ビーム装置の斜視図である。1 is a perspective view of a composite charged particle beam apparatus according to the present invention. 本発明に係る複合荷電粒子ビーム装置の(a)集束イオンビーム鏡筒の照射軸と気体イオンビーム鏡筒の照射軸を有する面の構成図、(b)集束イオンビーム鏡筒の照射軸と走査電子顕微鏡の照射軸を有する面の構成図である。(A) Configuration diagram of a surface having an irradiation axis of a focused ion beam column and an irradiation axis of a gas ion beam column, (b) an irradiation axis and scanning of the focused ion beam column of the composite charged particle beam apparatus according to the present invention. It is a block diagram of the surface which has the irradiation axis | shaft of an electron microscope. 本発明に係る複合荷電粒子ビーム装置の構成図である。It is a block diagram of the composite charged particle beam apparatus which concerns on this invention. 従来の複合荷電粒子ビーム装置の配置図である。It is a layout view of a conventional composite charged particle beam apparatus.

以下、本発明に係る複合荷電粒子ビーム装置の実施形態について説明する。なお、本実施形態の説明は例示であり、本発明の構成は以下の説明に限定されない。   Hereinafter, embodiments of the composite charged particle beam apparatus according to the present invention will be described. The description of the present embodiment is an exemplification, and the configuration of the present invention is not limited to the following description.

<実施形態1>
図1に本発明の実施形態を説明する図を示す。試料4は薄片化される厚み方向が走査電子顕微鏡の軸8と平行な方向になるように、試料ステージを用いて配置される。試料設置方法は、試料4の厚み方向に突起物がないような設置にする。試料4表面に対して、走査電子顕微鏡2を走査電子顕微鏡の軸8が垂直方向になるように配置する。更に試料4の位置で集束イオンビーム鏡筒の軸7が走査電子顕微鏡の軸8と直角に交わるように集束イオンビーム鏡筒1を配置する。このような配置とすることで、図4に示した従来装置の構成と比較して試料と走査電子顕微鏡の距離10を大幅に縮めることができる。それに伴い、装置で処理できる試料の大きさは制限されることになるが、TEM試料用の薄片試料は一般的には直径3mmの円盤より小さいので大きな制約とはならない。
<Embodiment 1>
FIG. 1 is a diagram illustrating an embodiment of the present invention. The sample 4 is arranged using a sample stage so that the thickness direction in which the sample 4 is thinned becomes a direction parallel to the axis 8 of the scanning electron microscope. The sample placement method is such that there is no protrusion in the thickness direction of the sample 4. The scanning electron microscope 2 is arranged with respect to the surface of the sample 4 so that the axis 8 of the scanning electron microscope is vertical. Further, the focused ion beam column 1 is arranged so that the axis 7 of the focused ion beam column intersects the axis 8 of the scanning electron microscope at a right angle at the position of the sample 4. With such an arrangement, the distance 10 between the sample and the scanning electron microscope can be significantly reduced as compared with the configuration of the conventional apparatus shown in FIG. Accordingly, the size of the sample that can be processed by the apparatus is limited. However, since a thin sample for a TEM sample is generally smaller than a disk having a diameter of 3 mm, it is not a great limitation.

図2(a)は、図1の複合荷電粒子ビーム装置の集束イオンビーム鏡筒の軸8と気体イオンビーム鏡筒の軸9を有する面の構成図である。また、図2(b)は、図1の複合荷電粒子ビーム装置の集束イオンビーム鏡筒の軸8と走査電子顕微鏡の軸8を有する面の構成図である。走査電子顕微鏡2は集束イオンビーム鏡筒1と試料4に挟まれることなく配置されるので、走査電子顕微鏡2の先端と試料4との距離を集束イオンビーム鏡筒1の先端や気体イオンビーム鏡筒3の先端よりも短くすることができる。   FIG. 2A is a configuration diagram of a surface having the axis 8 of the focused ion beam column and the axis 9 of the gas ion beam column of the composite charged particle beam apparatus of FIG. FIG. 2B is a configuration diagram of a surface having the axis 8 of the focused ion beam column and the axis 8 of the scanning electron microscope of the composite charged particle beam apparatus of FIG. Since the scanning electron microscope 2 is arranged without being sandwiched between the focused ion beam column 1 and the sample 4, the distance between the tip of the scanning electron microscope 2 and the sample 4 is determined based on the tip of the focused ion beam column 1 or the gas ion beam mirror. It can be made shorter than the tip of the tube 3.

図3は複合荷電粒子ビーム装置の構成図である。集束イオンビーム鏡筒1から集束イオンビーム21が、走査電子顕微鏡2から電子ビーム22が、気体イオンビーム鏡筒3から気体イオンビーム23が、それぞれ試料4に照射可能な位置に配置されている。試料4は、試料室30内の試料ステージ24に取り付けられている。また、試料4から発生する二次電子を検出する二次電子検出器26と、走査電子顕微鏡2から照射し試料4を透過する透過電子を検出する透過電子検出器25を備えている。それぞれの検出器で検出した検出信号は、制御部27に送られ、ビーム走査信号と組み合わせることにより観察像が形成される。観察像は表示部28に表示される。   FIG. 3 is a configuration diagram of the composite charged particle beam apparatus. A focused ion beam 21 from the focused ion beam column 1, an electron beam 22 from the scanning electron microscope 2, and a gaseous ion beam 23 from the gaseous ion beam column 3 are arranged at positions where the sample 4 can be irradiated. The sample 4 is attached to the sample stage 24 in the sample chamber 30. Further, a secondary electron detector 26 that detects secondary electrons generated from the sample 4 and a transmission electron detector 25 that detects transmission electrons irradiated from the scanning electron microscope 2 and transmitted through the sample 4 are provided. Detection signals detected by the respective detectors are sent to the control unit 27 and combined with the beam scanning signal, an observation image is formed. The observation image is displayed on the display unit 28.

集束イオンビーム鏡筒1を使用して試料4を薄片形状に加工していく。集束イオンビーム21による薄片化が終了した時点では試料4の表面にはダメージ層が形成されている。このダメージ層を除去するために、気体イオンビーム鏡筒3を用いて、加速電圧1kVの気体イオンビーム23を照射する。多くの場合、イオン化させる気体としては希ガスが用いられ、この例示においてはアルゴンを用いた。従来の例では、試料を回転させて気体イオンビームの照射角度を調節していた。しかし、本発明による構成では、走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6が小さいため試料4を大きく回転させることは困難であるため、予め試料4に対して角度をつけた位置に気体イオンビーム鏡筒3を配置する。   The sample 4 is processed into a thin piece shape using the focused ion beam column 1. A damaged layer is formed on the surface of the sample 4 at the time when the thinning by the focused ion beam 21 is completed. In order to remove the damaged layer, the gas ion beam 23 having an acceleration voltage of 1 kV is irradiated using the gas ion beam column 3. In many cases, a rare gas is used as a gas to be ionized, and argon is used in this example. In the conventional example, the irradiation angle of the gaseous ion beam is adjusted by rotating the sample. However, in the configuration according to the present invention, since the angle 6 formed by the axis of the scanning electron microscope and the axis of the gas ion beam column is small, it is difficult to rotate the sample 4 greatly. The gas ion beam column 3 is disposed at the position.

次に、取付けの角度の決定方法について以下に説明する。気体イオンビーム23を照射している面の変化を走査電子顕微鏡1で観察したいので走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6は90度より小さい必要がある。さらに、気体イオンビーム23の軌道が走査電子顕微鏡2の先端部に遮られない角度の範囲を選んで取り付ける必要がある。また、気体イオンビーム23の入射角度は照射面に対して大きすぎると、試料4の表面の平滑性を損ない、逆に角度が浅すぎると表面のダメージ層の除去に時間がかかりすぎる。そこで、走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6は60度以上かつ88度以下であることが好ましい。この例では走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6は60度で取り付けた。上記の理由から気体イオンビーム鏡筒3は、少なくとも走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6を気体イオンビーム鏡筒の軸と気体イオンビーム鏡筒の軸を走査電子顕微鏡の軸と垂直な面に投影した線分がなす角12よりも大きくなるように配置することが好ましい。   Next, a method for determining the mounting angle will be described below. Since it is desired to observe the change of the surface irradiated with the gas ion beam 23 with the scanning electron microscope 1, the angle 6 formed by the axis of the scanning electron microscope and the axis of the gas ion beam column needs to be smaller than 90 degrees. Furthermore, it is necessary to select and attach an angle range in which the trajectory of the gaseous ion beam 23 is not blocked by the tip of the scanning electron microscope 2. If the incident angle of the gas ion beam 23 is too large with respect to the irradiation surface, the smoothness of the surface of the sample 4 is impaired. Conversely, if the angle is too shallow, it takes too much time to remove the damaged layer on the surface. Therefore, the angle 6 formed by the axis of the scanning electron microscope and the axis of the gas ion beam column is preferably 60 degrees or more and 88 degrees or less. In this example, the angle 6 formed by the axis of the scanning electron microscope and the axis of the gas ion beam column is 60 degrees. For the above reasons, the gas ion beam column 3 has at least an angle 6 formed by the axis of the scanning electron microscope and the axis of the gas ion beam column. The axis of the gas ion beam column and the axis of the gas ion beam column are scanned by the scanning electron microscope. It is preferable to arrange such that it is larger than the angle 12 formed by the line segment projected on the plane perpendicular to the axis.

ここまでの工程は、全て試料と走査電子顕微鏡の距離10は走査電子顕微鏡2にとって最適である短い距離で使用できるため、非常に微細な変化や構造を観察しながら行うことができ、本発明の課題を達成している。   All the steps up to here can be performed while observing very minute changes and structures because the distance 10 between the sample and the scanning electron microscope can be used at a short distance that is optimal for the scanning electron microscope 2. The challenge has been achieved.

<実施形態2>
実施形態1においては、試料4に対しての気体イオンビーム23の入射角度は固定であったが、実際には試料の特性に応じて調節する必要がある場合もある。このような場合、集束イオンビーム鏡筒の軸7と走査電子顕微鏡の軸8の双方の交点付近に試料4を保持し、かつ双方に直交する軸によって試料を傾斜する第一の傾斜機構31を試料ステージ24に設けることで、気体イオンビーム23の試料4に対する入射角度を調節することができる。試料4を大きく傾けることは、走査電子顕微鏡2の観察能力に影響を及ぼすため、比較的小さな傾斜角度の範囲で実用的な入射角度を制御できることが望ましい。このような場合、実施形態1で説明したように予め角度をつけて気体イオンビーム鏡筒3を取り付けておくことで、比較的小さな角度の傾斜で実用的な範囲の角度を制御することができる。例として、気体イオンビーム鏡筒3と集束イオンビーム鏡筒1が走査電子顕微鏡2の方向から見た時に、60度の角度を持ち、かつ走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6を70度とすると、±10度の傾斜で入射角度をおよそ11度から29度の範囲で制御することができる。
これにより、実施形態1で説明した利点はそのままに、気体イオンビーム23の入射角度を制御することが可能となる。
<Embodiment 2>
In the first embodiment, the incident angle of the gaseous ion beam 23 with respect to the sample 4 is fixed, but in practice, it may be necessary to adjust it according to the characteristics of the sample. In such a case, the first tilting mechanism 31 that holds the sample 4 near the intersection of both the axis 7 of the focused ion beam column and the axis 8 of the scanning electron microscope and tilts the sample by the axis orthogonal to both is provided. By providing the sample stage 24, the incident angle of the gaseous ion beam 23 with respect to the sample 4 can be adjusted. Since tilting the sample 4 greatly affects the observation ability of the scanning electron microscope 2, it is desirable that the practical incident angle can be controlled within a relatively small tilt angle range. In such a case, the angle in a practical range can be controlled with a relatively small inclination by attaching the gas ion beam column 3 with an angle in advance as described in the first embodiment. . As an example, when the gas ion beam column 3 and the focused ion beam column 1 are viewed from the direction of the scanning electron microscope 2, they have an angle of 60 degrees, and the axis of the scanning electron microscope and the axis of the gas ion beam column are If the formed angle 6 is 70 degrees, the incident angle can be controlled within a range of approximately 11 degrees to 29 degrees with an inclination of ± 10 degrees.
Thereby, it is possible to control the incident angle of the gaseous ion beam 23 while maintaining the advantages described in the first embodiment.

<実施形態3>
実施形態2と同様の目的で、集束イオンビーム鏡筒1と走査電子顕微鏡2のビームの交点付近に試料4を保持し、かつ集束イオンビーム鏡筒1の軸と平行な回転軸により試料を傾斜させる第二の傾斜機構32を試料ステージ24に備えることで、気体イオンビームの入射角度を制御することが可能となる。例として、気体イオンビーム鏡筒3と集束イオンビーム鏡筒1が走査電子顕微鏡2の方向から見た時に、30度の角度を持ち、かつ走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角6を70度とすると、±10度の傾斜で入射角度をおよそ11度から29度の範囲で制御することができる。
<Embodiment 3>
For the same purpose as in the second embodiment, the sample 4 is held near the intersection of the beam of the focused ion beam column 1 and the scanning electron microscope 2, and the sample is tilted by a rotation axis parallel to the axis of the focused ion beam column 1. By providing the sample stage 24 with the second tilt mechanism 32 to be performed, the incident angle of the gaseous ion beam can be controlled. As an example, when the gas ion beam column 3 and the focused ion beam column 1 are viewed from the direction of the scanning electron microscope 2, they have an angle of 30 degrees, and the axis of the scanning electron microscope and the axis of the gas ion beam column are If the formed angle 6 is 70 degrees, the incident angle can be controlled within a range of approximately 11 degrees to 29 degrees with an inclination of ± 10 degrees.

<実施形態4>
気体イオンビーム鏡筒3を複数備えることも好ましい。一般に、試料4が複数の材料で構成されている場合、気体イオンビーム23による試料表面のエッチング速度は同じではない。一部にエッチングが進行しにくい材質を含む場合、気体イオンビーム23の入射方向から見て、削れにくい材質の後側に筋を引いたようにエッチングの進行が遅い部分ができてしまう。そこで、気体イオンビーム鏡筒3を複数設けて、複数の方位から気体イオンビームを照射することで、このような現象を抑制することができる。この例においても、上述した条件の範囲内で気体イオンビーム鏡筒3を配置することで、本発明の課題は達成することができる。
<Embodiment 4>
It is also preferable to provide a plurality of gas ion beam column 3. In general, when the sample 4 is composed of a plurality of materials, the etching rate of the sample surface by the gaseous ion beam 23 is not the same. When a part of the material that does not easily progress in etching is included, a part where etching progresses slowly is formed as if a line is drawn behind the material that is difficult to scrape when viewed from the incident direction of the gas ion beam 23. Therefore, such a phenomenon can be suppressed by providing a plurality of gas ion beam column 3 and irradiating the gas ion beam from a plurality of directions. Also in this example, the subject of this invention can be achieved by arrange | positioning the gaseous ion beam column 3 within the range of the conditions mentioned above.

1…集束イオンビーム鏡筒
2…走査電子顕微鏡
3…気体イオンビーム鏡筒
4…試料
5…走査電子顕微鏡の軸と集束イオンビーム鏡筒の軸がなす角
6…走査電子顕微鏡の軸と気体イオンビーム鏡筒の軸がなす角
7…集束イオンビーム鏡筒の軸
8…走査電子顕微鏡の軸
9…気体イオンビームの軸
10…試料と走査電子顕微鏡の距離
11…気体イオンビーム鏡筒の軸を走査電子顕微鏡の軸と垂直な面に投影した線分
12…気体イオンビーム鏡筒の軸と気体イオンビーム鏡筒の軸を走査電子顕微鏡の軸と垂直な面に投影した線分がなす角
21…集束イオンビーム
22…電子ビーム
23…気体イオンビーム
24…試料ステージ
25…透過電子検出器
26…二次電子検出器
27…制御部
28…表示部
30…試料室
31…第一の傾斜機構
32…第二の傾斜機構
DESCRIPTION OF SYMBOLS 1 ... Focusing ion beam column 2 ... Scanning electron microscope 3 ... Gas ion beam column 4 ... Sample 5 ... The angle which the axis | shaft of a scanning electron microscope and the axis | shaft of a focused ion beam column 6 ... Axis of a scanning electron microscope and gas ion Angle formed by the axis of the beam column 7 ... axis of the focused ion beam column 8 ... axis of the scanning electron microscope 9 ... axis of the gas ion beam 10 ... distance between the sample and the scanning electron microscope 11 ... the axis of the gas ion beam column Line segment projected on a plane perpendicular to the axis of the scanning electron microscope 12 ... Angle formed by a line segment projected on the plane perpendicular to the axis of the scanning electron microscope with the axis of the gas ion beam column and the axis of the gas ion beam column 21 ... focused ion beam 22 ... electron beam 23 ... gaseous ion beam 24 ... sample stage 25 ... transmission electron detector 26 ... secondary electron detector 27 ... control unit 28 ... display unit 30 ... sample chamber 31 ... first tilt mechanism 32 ... Second tilting mechanism

Claims (2)

集束イオンビームを照射して試料を薄膜化する集束イオンビーム鏡筒と、
前記試料のダメージ層を除去する低加速電圧の気体イオンビームを照射する気体イオンビーム鏡筒と、
前記集束イオンビームで前記試料を薄膜化しながら形成される薄膜化試料を垂直方向から観察する電子ビームを照射する走査電子顕微鏡筒と、
前記集束イオンビーム鏡筒のビーム照射軸と前記走査電子顕微鏡筒のビーム照射軸の交点付近に前記試料を保持する試料ステージと、を備え、
前記集束イオンビーム鏡筒のビーム照射軸は、前記走査電子顕微鏡筒のビーム照射軸と略直交し、
前記気体イオンビーム鏡筒のビーム照射軸は前記走査電子顕微鏡筒のビーム照射軸と90度より小さい角度で交わるように配置し、
前記試料ステージは、前記集束イオンビーム鏡筒のビーム照射軸と略平行な回転軸により、前記試料を傾斜させる傾斜機構を備え、
前記傾斜機構は前記集束イオンビーム鏡筒の直径よりも小さい直径を有することを特徴とする複合荷電粒子ビーム装置。
A focused ion beam column that irradiates the focused ion beam to thin the sample;
A gas ion beam column for irradiating a gas ion beam with a low acceleration voltage for removing a damaged layer of the sample;
A scanning electron microscope tube for irradiating an electron beam for observing a thinned sample formed while thinning the sample with the focused ion beam from a vertical direction;
A sample stage for holding the sample near the intersection of the beam irradiation axis of the focused ion beam column and the beam irradiation axis of the scanning electron microscope tube;
The beam irradiation axis of the focused ion beam column is substantially orthogonal to the beam irradiation axis of the scanning electron microscope tube,
The beam irradiation axis of the gas ion beam column is arranged to intersect with the beam irradiation axis of the scanning electron microscope column at an angle smaller than 90 degrees,
The sample stage, by the focused ion beam column substantially parallel to the rotation axis and the beam irradiation axis of, e Bei a tilting mechanism for tilting said specimen,
The tilting mechanism has a diameter smaller than the diameter of the focused ion beam column .
集束イオンビーム鏡筒と、走査電子顕微鏡筒と、低加速電圧の気体イオンビーム鏡筒と、前記集束イオンビーム鏡筒のビーム照射軸と前記走査電子顕微鏡筒のビーム照射軸の交点付近に試料を保持する試料ステージと、を備え、
前記集束イオンビーム鏡筒のビーム照射軸は、前記走査電子顕微鏡筒のビーム照射軸と略直交し、
前記気体イオンビーム鏡筒のビーム照射軸は前記走査電子顕微鏡筒のビーム照射軸と90度より小さい角度で交わるように配置し、かつ、前記走査電子顕微鏡筒のビーム照射軸と前記気体イオンビーム鏡筒のビーム照射軸がなす角を、前記気体イオンビーム鏡筒のビーム照射軸を前記走査電子顕微鏡筒の軸と垂直な面に投影した線分と前記気体イオンビーム鏡筒のビーム照射軸がなす角よりも大きくなるようにして、集束イオンビームと電子ビームと気体ビームのそれぞれが、前記試料ステージに取り付けた前記試料に照射可能な位置に配置した複合荷電粒子ビーム装置であって、
前記集束イオンビームで前記試料を薄膜化し、低加速電圧の気体イオンビームで薄膜化試料のダメージ層を除去する工程を、前記薄膜化試料を前記走査電子顕微鏡筒で垂直方向から観察しながら実施し、
前記試料ステージは、前記集束イオンビーム鏡筒のビーム照射軸と略平行な回転軸により、前記試料を傾斜させる傾斜機構を備え、
前記傾斜機構は前記集束イオンビーム鏡筒の直径よりも小さい直径を有することを特徴とする複合荷電粒子ビーム装置。
A sample is placed near the intersection of a focused ion beam column, a scanning electron microscope tube, a low acceleration voltage gas ion beam column, a beam irradiation axis of the focused ion beam column and a beam irradiation axis of the scanning electron microscope column. A sample stage to hold,
The beam irradiation axis of the focused ion beam column is substantially orthogonal to the beam irradiation axis of the scanning electron microscope tube,
The beam irradiation axis of the gas ion beam column is arranged to intersect the beam irradiation axis of the scanning electron microscope tube at an angle smaller than 90 degrees, and the beam irradiation axis of the scanning electron microscope tube and the gas ion beam mirror An angle formed by the beam irradiation axis of the tube is formed by a line segment obtained by projecting the beam irradiation axis of the gas ion beam column onto a plane perpendicular to the axis of the scanning electron microscope tube and the beam irradiation axis of the gas ion beam column. A charged particle beam apparatus in which each of a focused ion beam, an electron beam, and a gas beam is arranged at a position where the sample attached to the sample stage can be irradiated so as to be larger than an angle,
The step of thinning the sample with the focused ion beam and removing the damaged layer of the thinned sample with a gas ion beam of low acceleration voltage is performed while observing the thinned sample from the vertical direction with the scanning electron microscope tube. ,
The sample stage, by the focused ion beam column substantially parallel to the rotation axis and the beam irradiation axis of, e Bei a tilting mechanism for tilting said specimen,
The tilting mechanism has a diameter smaller than the diameter of the focused ion beam column .
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