JPH04238203A - Probe for scanning type capacity microscope and manufacture thereof - Google Patents
Probe for scanning type capacity microscope and manufacture thereofInfo
- Publication number
- JPH04238203A JPH04238203A JP523791A JP523791A JPH04238203A JP H04238203 A JPH04238203 A JP H04238203A JP 523791 A JP523791 A JP 523791A JP 523791 A JP523791 A JP 523791A JP H04238203 A JPH04238203 A JP H04238203A
- Authority
- JP
- Japan
- Prior art keywords
- metal
- probe
- tip
- sample
- film
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
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- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】本発明は走査型容量顕微鏡の探針
及びその製造方法に関する。Binning 及びRo
hrerにより発明された走査型トンネル顕微鏡(ST
M) は圧電素子とそれに取付けた探針を用いて、試料
と探針間に流れるトンネル電流をとらえ表面の構造を原
子スケールの分解能で観察するものである。これを改良
したものに走査型容量顕微鏡(SCM) がある。この
走査型容量顕微鏡は試料と探針間の容量を測定して試料
の表面を観察するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a probe for a scanning capacitance microscope and a method for manufacturing the same. Binning and Ro
The scanning tunneling microscope (ST
M) uses a piezoelectric element and a probe attached to it to capture the tunneling current flowing between the sample and the probe and observe the surface structure with atomic-scale resolution. An improved version of this is the scanning capacitance microscope (SCM). This scanning capacitance microscope measures the capacitance between the sample and the probe to observe the surface of the sample.
【0002】0002
【従来の技術】図4は従来の走査型トンネル顕微鏡及び
走査型容量顕微鏡を説明するための図である。同図にお
いて、1は圧電素子であり、2は圧電素子により上下に
駆動される探針、3は被測定試料である。そして試料3
と探針2の間に電圧を印加しておき、探針2で試料表面
を走査する。このとき走査型トンネル顕微鏡では探針2
と試料との間に流れる電流を一定(1nA程度)となる
ように圧電素子1に電流を流し、その電流の変化により
試料表面の凹凸を測定することができる。これに対し走
査型容量顕微鏡では探針2と試料間の容量が一定となる
ように圧電素子1を駆動し、その電流から試料表面の凹
凸を測定するようになっている。2. Description of the Related Art FIG. 4 is a diagram for explaining a conventional scanning tunneling microscope and a scanning capacitance microscope. In the figure, 1 is a piezoelectric element, 2 is a probe that is driven up and down by the piezoelectric element, and 3 is a sample to be measured. and sample 3
A voltage is applied between the probe 2 and the probe 2, and the probe 2 scans the surface of the sample. At this time, in the scanning tunneling microscope, the probe 2
A current is passed through the piezoelectric element 1 so that the current flowing between the piezoelectric element 1 and the sample is constant (about 1 nA), and the irregularities on the sample surface can be measured by changes in the current. On the other hand, in a scanning capacitance microscope, the piezoelectric element 1 is driven so that the capacitance between the probe 2 and the sample is constant, and the unevenness of the sample surface is measured from the current.
【0003】0003
【発明が解決しようとする課題】上記の走査型トンネル
顕微鏡では、そのトンネル電流は図5に曲線Aで示すよ
うに、試料3と探針2間の距離の指数に比例して急速に
減少するため、数Å以下の分解能が得られる。一方走査
型容量顕微鏡では図6に示すように試料3と探針2間の
電界4をとらえており、これは図5に曲線Bで示すよう
に距離の二乗に比例して減少する。従って走査型容量顕
微鏡では走査型トンネル顕微鏡のような高分解能は得ら
れず 250Å程度が限界であった。[Problems to be Solved by the Invention] In the above scanning tunneling microscope, the tunneling current rapidly decreases in proportion to the index of the distance between the sample 3 and the probe 2, as shown by curve A in FIG. Therefore, a resolution of several Å or less can be obtained. On the other hand, the scanning capacitance microscope captures the electric field 4 between the sample 3 and the probe 2, as shown in FIG. 6, and this decreases in proportion to the square of the distance, as shown by curve B in FIG. Therefore, a scanning capacitance microscope cannot achieve the high resolution of a scanning tunneling microscope, and its limit is about 250 Å.
【0004】本発明は走査型容量顕微鏡の解像度を向上
可能とした探針を実現しようとする。The present invention attempts to realize a probe capable of improving the resolution of a scanning capacitance microscope.
【0005】[0005]
【課題を解決するための手段】本発明の走査型容量顕微
鏡の探針においては、金属針と、該金属針の先端部以外
の部分に被覆された金属酸化膜と、該金属酸化膜上に被
覆された金属膜とにより構成されたことを特徴とする。
また本発明の走査型容量顕微鏡の探針の製造方法におい
ては、金属針の先端部を電界蒸発させて尖鋭化する工程
と、該金属針を加熱して全面に金属酸化膜を形成する工
程と、該金属酸化膜の上に金属を蒸着して金属膜を形成
する工程と、先端部の前記金属膜及び金属酸化膜を電界
蒸発させて除去し、金属針の先端を露出させる工程とを
含んで成ることを特徴とする。[Means for Solving the Problems] A probe for a scanning capacitance microscope according to the present invention includes a metal needle, a metal oxide film coated on a portion other than the tip of the metal needle, and a metal oxide film coated on the metal oxide film. It is characterized by being composed of a coated metal film. Further, the method for manufacturing a probe for a scanning capacitance microscope of the present invention includes a step of sharpening the tip of the metal needle by electric field evaporation, and a step of heating the metal needle to form a metal oxide film on the entire surface. , a step of depositing a metal on the metal oxide film to form a metal film, and a step of removing the metal film and the metal oxide film at the tip by electric field evaporation to expose the tip of the metal needle. It is characterized by consisting of.
【0006】[0006]
【作用】図1の如く金属膜14をアースに接続すれば、
先端の針先のみ電界18が発生し、先端以外の容量の影
響が無くなるため、従来に比して高い分解能が得られる
。[Operation] If the metal film 14 is connected to the ground as shown in FIG.
Since the electric field 18 is generated only at the tip of the tip of the needle, and the influence of capacitance other than the tip is eliminated, higher resolution can be obtained than in the past.
【0007】[0007]
【実施例】図1は本発明の走査型容量顕微鏡の探針の実
施例を試料と共に示す断面図である。同図において、1
0は探針、11は被測定試料である。探針10は金属製
の針12の針先を除いた部分に金属酸化膜13が被覆さ
れ、さらにその上に金属膜14が被覆されている。なお
金属針12及び金属膜14にはタングステン等の金属が
用いられ、金属酸化膜13としては、金属針がタングス
テンの場合はタングステンオキザイドが用いられる。ま
た金属針の材料として不純物をイオン注入等で高濃度に
ドープしたシリコンを使用すれば金属酸化膜として信頼
性の高い絶縁膜であるSiO2が得られる。DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a sectional view showing an embodiment of the probe of a scanning capacitance microscope according to the present invention together with a sample. In the same figure, 1
0 is a probe, and 11 is a sample to be measured. The probe 10 includes a metal needle 12 whose portion other than the tip is coated with a metal oxide film 13, and further coated with a metal film 14 thereon. Note that metal such as tungsten is used for the metal needle 12 and the metal film 14, and tungsten oxide is used for the metal oxide film 13 when the metal needle is tungsten. Furthermore, if silicon doped with impurities at a high concentration by ion implantation or the like is used as the material of the metal needle, SiO2, which is a highly reliable insulating film, can be obtained as a metal oxide film.
【0008】このように構成された本実施例の探針は図
2の如き測定回路に接続されて用いられる。図は試料1
1としてSiO2膜が形成されたSi を用い、そのS
iO2膜の容量を求める例である。探針10は圧電素子
15に固定され、且つその金属針12は容量センサ16
に接続され、金属膜14はアースに接続されている。ま
た金属針12と試料11との間にはVb =V+ΔV(
ω2)で振動している電圧が印加されており、この間の
容量変化分を容量センサ16でとらえる。The probe of this embodiment constructed as described above is used by being connected to a measuring circuit as shown in FIG. The figure shows sample 1
Using Si on which a SiO2 film was formed as 1, the S
This is an example of determining the capacity of an iO2 film. The probe 10 is fixed to a piezoelectric element 15, and the metal needle 12 is connected to a capacitive sensor 16.
The metal film 14 is connected to ground. Also, between the metal needle 12 and the sample 11, Vb = V + ΔV (
A voltage oscillating at ω2) is applied, and the capacitance sensor 16 captures the capacitance change during this period.
【0009】そして測定時には圧電素子15をx方向に
移動させるのであるが、このとき探針10と試料11の
距離を一定に保つ必要がある。このために、圧電素子1
5に交流電圧をかけて探針10をω1 で上下に振動さ
せる。探針10と試料11間の容量Cair はCai
r =ε0S/d(x)であり、電圧振動による容量の
変化ΔCair は、ΔCair =−ε0S/d2(
x)で変化する。そしてΔCair が一定になるよう
に圧電素子15にフィードバックをかけてやればdは一
定になる。一方試料11に印加された電圧をω2(≠ω
1)で振動させ、これを容量センサ16を通してロック
インアンプ17でキャッチすれば、試料内の容量変化分
(dc/dVb)を測定することができる。さらにこ
れを電圧で積分すればSiO2膜の容量Cs が計算で
きる。[0009] During measurement, the piezoelectric element 15 is moved in the x direction, but at this time it is necessary to keep the distance between the probe 10 and the sample 11 constant. For this purpose, piezoelectric element 1
An alternating current voltage is applied to 5 to cause the probe 10 to vibrate up and down at ω1. The capacitance Cair between the probe 10 and the sample 11 is Cai
r = ε0S/d(x), and the change in capacitance due to voltage oscillation ΔCair is ΔCair = -ε0S/d2(
x). Then, if feedback is applied to the piezoelectric element 15 so that ΔCair becomes constant, d becomes constant. On the other hand, the voltage applied to the sample 11 is ω2(≠ω
1), and by passing it through the capacitance sensor 16 and catching it with the lock-in amplifier 17, it is possible to measure the capacitance change (dc/dVb) in the sample. Furthermore, by integrating this with respect to voltage, the capacitance Cs of the SiO2 film can be calculated.
【0010】なお探針10の内側の金属針12と外側の
金属膜14との間に容量Ct があるが、これは容量セ
ンサ16が交流変化分のみキャッチするのでCt は除
かれる。以上の本実施例によれば、図1の如く金属針1
2の先端以外からは電界が発生せず、先端のみに電界1
8が発生するため従来に比してより高い分解能が得られ
る。次に本発明の走査型容量顕微鏡の探針の製造方法を
図3により説明する。Although there is a capacitance Ct between the metal needle 12 on the inside of the probe 10 and the metal film 14 on the outside, this Ct is excluded because the capacitance sensor 16 catches only the alternating current change. According to the present embodiment described above, the metal needle 1 as shown in FIG.
No electric field is generated from any part other than the tip of 2, and the electric field 1 is generated only at the tip.
8 is generated, higher resolution can be obtained than in the past. Next, a method for manufacturing a probe for a scanning capacitance microscope according to the present invention will be explained with reference to FIG.
【0011】先ず図3(a)の如くタングステンの金属
針12を電界蒸発で先端12aを尖鋭にする。電界蒸発
は数+KV、2〜3分間で良い。次に図3(b)の如く
空気中で加熱し、表面に金属酸化膜13として厚さ 1
00Å程度のタングステンオキサイドを形成する。次に
図3(c)の如く金属酸化膜(タングステンオキサイド
)13の上にタングステンを厚さ1μm程度蒸着し金属
膜14を形成する。最後に図3(d)の如く電界蒸発に
より先端の金属膜14及び金属酸化膜13を除去し、金
属針12の先端部12aを 100Å程度露出させ尖鋭
にするのである。First, as shown in FIG. 3(a), a tungsten metal needle 12 is made sharp at its tip 12a by electric evaporation. Field evaporation may be performed at several KV for 2 to 3 minutes. Next, as shown in FIG. 3(b), it is heated in air to form a metal oxide film 13 on the surface with a thickness of 1.
Tungsten oxide with a thickness of about 0.00 Å is formed. Next, as shown in FIG. 3C, tungsten is deposited on the metal oxide film (tungsten oxide) 13 to a thickness of about 1 μm to form a metal film 14. Finally, as shown in FIG. 3(d), the metal film 14 and metal oxide film 13 at the tip are removed by electric field evaporation, and the tip 12a of the metal needle 12 is exposed to a thickness of about 100 Å and made sharp.
【0012】以上の本実施例によれば高い分解能が得ら
れる探針を容易に作成することができる。According to the present embodiment described above, a probe capable of obtaining high resolution can be easily produced.
【0013】[0013]
【発明の効果】本発明によれば、金属針の先端のみを露
出させ、他の部分を絶縁膜を介して金属膜で被覆するこ
とにより、走査型容量顕微鏡に用いたとき、先端のみか
ら電界が発生し、他の部分からは発生しないため、従来
に比して高い分解能が得られる。According to the present invention, only the tip of the metal needle is exposed and the other part is covered with a metal film via an insulating film, so that when used in a scanning capacitance microscope, an electric field is generated only from the tip. is generated and not generated from other parts, so higher resolution can be obtained than in the past.
【図1】本発明の走査型容量顕微鏡の探針の実施例を被
測定試料と共に示す断面図である。FIG. 1 is a sectional view showing an embodiment of a probe of a scanning capacitance microscope according to the present invention together with a sample to be measured.
【図2】本発明の走査型容量顕微鏡の探針の使用状態を
示す図である。FIG. 2 is a diagram showing how the probe of the scanning capacitance microscope of the present invention is used.
【図3】本発明の走査型容量顕微鏡の探針の製造方法を
説明するための図である。FIG. 3 is a diagram for explaining a method of manufacturing a probe for a scanning capacitance microscope according to the present invention.
【図4】従来の走査型トンネル顕微鏡及び走査型容量顕
微鏡を説明するための図である。FIG. 4 is a diagram for explaining a conventional scanning tunneling microscope and a scanning capacitance microscope.
【図5】従来の走査型トンネル顕微鏡と走査型容量顕微
鏡の特性曲線を示す図である。FIG. 5 is a diagram showing characteristic curves of a conventional scanning tunneling microscope and a scanning capacitance microscope.
【図6】従来の走査型容量顕微鏡の探針と試料間の電界
を示す図である。FIG. 6 is a diagram showing an electric field between a probe and a sample of a conventional scanning capacitance microscope.
10…探針 11…試料 12…金属針 13…金属酸化膜 14…金属膜 15…圧電素子 16…容量センサ 17…ロックインアンプ 18…電界 10... Probe 11...Sample 12...Metal needle 13...Metal oxide film 14...Metal film 15...Piezoelectric element 16...capacitance sensor 17...Lock-in amplifier 18...Electric field
Claims (3)
の先端部以外の部分に被覆された金属酸化膜(13)と
、該金属酸化膜(13)上に被覆された金属膜(14)
とにより構成されたことを特徴とする走査型容量顕微鏡
の探針。[Claim 1] A metal needle (12) and the metal needle (12)
A metal oxide film (13) coated on a portion other than the tip of the metal oxide film (13), and a metal film (14) coated on the metal oxide film (13).
A probe for a scanning capacitance microscope characterized by comprising:
度にドープしたシリコンを用いたことを特徴とする請求
項1の走査型容量顕微鏡の探針。2. The probe for a scanning capacitance microscope according to claim 1, wherein silicon doped with impurities at a high concentration is used for the metal needle (12).
電界蒸発させて尖鋭化する工程と、該金属針(12)を
加熱して全面に金属酸化膜(13)を形成する工程と、
該金属酸化膜(13)の上に金属を蒸着して金属膜(1
4)を形成する工程と、先端部の前記金属膜(14)及
び金属酸化膜(13)を電界蒸発させて除去し、金属針
(12)の先端部(12a)を露出させる工程、とを含
んで成ることを特徴とする走査型容量顕微鏡の探針の製
造方法。3. A step of sharpening the tip (12a) of the metal needle (12) by electric field evaporation, and a step of heating the metal needle (12) to form a metal oxide film (13) on the entire surface. ,
A metal is deposited on the metal oxide film (13) to form a metal film (1).
4) and a step of removing the metal film (14) and metal oxide film (13) at the tip by electric field evaporation to expose the tip (12a) of the metal needle (12). A method of manufacturing a probe for a scanning capacitance microscope, comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP523791A JPH04238203A (en) | 1991-01-21 | 1991-01-21 | Probe for scanning type capacity microscope and manufacture thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP523791A JPH04238203A (en) | 1991-01-21 | 1991-01-21 | Probe for scanning type capacity microscope and manufacture thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04238203A true JPH04238203A (en) | 1992-08-26 |
Family
ID=11605592
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP523791A Withdrawn JPH04238203A (en) | 1991-01-21 | 1991-01-21 | Probe for scanning type capacity microscope and manufacture thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04238203A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5509300A (en) * | 1994-05-12 | 1996-04-23 | Arizona Board Of Regents Acting For Arizona State University | Non-contact force microscope having a coaxial cantilever-tip configuration |
| US6888135B2 (en) | 2000-10-18 | 2005-05-03 | Nec Corporation | Scanning probe microscope with probe formed by single conductive material |
-
1991
- 1991-01-21 JP JP523791A patent/JPH04238203A/en not_active Withdrawn
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5509300A (en) * | 1994-05-12 | 1996-04-23 | Arizona Board Of Regents Acting For Arizona State University | Non-contact force microscope having a coaxial cantilever-tip configuration |
| US6888135B2 (en) | 2000-10-18 | 2005-05-03 | Nec Corporation | Scanning probe microscope with probe formed by single conductive material |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A300 | Application deemed to be withdrawn because no request for examination was validly filed |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 19980514 |