JP3173554B2 - Measurement method of high frequency characteristics of dielectric thin film - Google Patents
Measurement method of high frequency characteristics of dielectric thin filmInfo
- Publication number
- JP3173554B2 JP3173554B2 JP05509795A JP5509795A JP3173554B2 JP 3173554 B2 JP3173554 B2 JP 3173554B2 JP 05509795 A JP05509795 A JP 05509795A JP 5509795 A JP5509795 A JP 5509795A JP 3173554 B2 JP3173554 B2 JP 3173554B2
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- JP
- Japan
- Prior art keywords
- measurement
- electrode layer
- correction
- thin film
- lower electrode
- Prior art date
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- Expired - Lifetime
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- Measurement Of Resistance Or Impedance (AREA)
- Tests Of Electronic Circuits (AREA)
- Testing Or Measuring Of Semiconductors Or The Like (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、半導体基板上に形成さ
ている誘電体薄膜を有する半導体装置を製造する場合に
適用される、半導体基板上に形成される誘電体薄膜の高
周波特性を測定する誘電体薄膜の高周波特性測定法に関
する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention measures the high frequency characteristics of a dielectric thin film formed on a semiconductor substrate, which is applied to the manufacture of a semiconductor device having a dielectric thin film formed on a semiconductor substrate. The present invention relates to a method for measuring high-frequency characteristics of a dielectric thin film.
【0002】[0002]
【従来の技術】従来、半導体基板B上に形成される誘電
体薄膜Fの高周波特性Hを測定するにつき、図4に示す
ように、(a)半導体基板Bに対応している基板BB上
に形成されている測定用下部電極層ELMと(b)基板
BB上に、測定用下部電極層ELM上に延長して、半導
体基板B上に形成されている誘電体薄膜と材質上から
も、形状上からも同様に形成されている測定用誘電体薄
膜FMと(c)測定用誘電体薄膜FM上に、測定用下部
電極層ELMと対向するように延長して形成されている
測定用上部電極層EUMとを有する測定用素子DMを形
成し、そして、その測定用素子DMの測定用下部電極層
ELM及び測定用上部電極層EUM間でみた高周波特性
HMを測定し、その測定用素子DMの高周波特性HMの
測定結果を用いる、という誘電体薄膜の高周波特性測定
法が提案されている。2. Description of the Related Art Conventionally, when measuring a high frequency characteristic H of a dielectric thin film F formed on a semiconductor substrate B, as shown in FIG. The lower electrode layer for measurement ELM formed and (b) the shape extending from the lower electrode layer for measurement ELM on the substrate BB to the dielectric thin film formed on the semiconductor substrate B and the material. The upper electrode for measurement formed so as to extend on the dielectric thin film for measurement FM similarly formed from above and (c) the dielectric thin film for measurement FM so as to face the lower electrode layer for measurement ELM. A measurement element DM having a layer EUM is formed, and a high-frequency characteristic HM between the measurement lower electrode layer ELM and the measurement upper electrode layer EUM of the measurement element DM is measured. Using the measurement result of the high frequency characteristic HM, Frequency characteristic measuring method of the dielectric thin film say has been proposed.
【0003】この場合、測定用素子DMの高周波特性H
Mの測定は、測定用素子DMの測定用下部電極層ELM
及び測定用上部電極層EUM間でみたアドミタンスYA
の測定とし得る。In this case, the high frequency characteristic H of the measuring element DM
The measurement of M is performed by measuring the lower electrode layer ELM of the measuring element DM.
And admittance Y A between the upper electrode layers EUM for measurement
Measurement.
【0004】また、測定用素子DMの高周波特性HMの
測定結果の用い方は、測定用素子DMの高周波特性HM
の測定を、測定用素子DMの測定用下部電極層ELM及
び測定用上部電極層EUM間でみたアドミタンスYA の
測定とする場合、そのアドミタンスYA から、周波数f
に対する測定用下部電極層ELM及び測定用上部電極層
EUM間の容量Cの関係を求め、その求められた容量C
が周波数fのどのような値またはどのような範囲の値で
どのような値を呈するのかとか、測定されたアドミタン
スYA から測定用誘電体薄膜FMの誘電損失tanδを
求め、その誘電損失tanδがどのような値を呈してい
るのか、測定されたアドミタンスYA から測定用誘電体
薄膜FMの比誘電率εを求め、その比誘電率εがどのよ
うな値を呈するかなどの判知ができるように用い得る。The method of using the measurement result of the high frequency characteristic HM of the measuring element DM is described in the following.
If the measurement, a measurement of the admittance Y A viewed between measurements lower electrode layer of the measuring device DM ELM and measuring the upper electrode layer EUM, from the admittance Y A, the frequency f
Of the capacitance C between the lower electrode layer ELM for measurement and the upper electrode layer EUM for measurement with respect to
There determined Toka whether exhibiting any value by the value of the value or any range as the frequency f throat, the measured admittance Y from the A of the measuring dielectric thin film FM dielectric loss tan [delta, its dielectric loss tan [delta what values of and has a obtains the relative dielectric constant ε of the measuring dielectric thin FM from the measured admittance Y a, can determine knowledge, such as whether the relative dielectric constant ε exhibits what value Can be used.
【0005】以上が、従来提案されている誘電体薄膜の
高周波特性測定法である。[0005] The above is a method of measuring high-frequency characteristics of a dielectric thin film that has been conventionally proposed.
【0006】このような従来の誘電体薄膜の高周波特性
測定法によれば、測定用素子DMを、半導体装置を製造
するのに従来用いている方法によって、容易に形成する
ことができるので、半導体基板B上に形成される誘電体
薄膜Fの高周波特性Hを、容易に測定することができ
る。According to such a conventional method for measuring high-frequency characteristics of a dielectric thin film, the measuring element DM can be easily formed by a method conventionally used for manufacturing a semiconductor device. The high-frequency characteristics H of the dielectric thin film F formed on the substrate B can be easily measured.
【0007】[0007]
【発明が解決しようとする課題】図4に示す従来の誘電
体薄膜の高周波特性測定法の場合、測定用素子DMの高
周波特性HMの測定は、それを測定用素子DMの測定用
下部電極層ELM及び測定用上部電極層EUM間でみた
アドミタンスYA の測定とする場合、その測定用素子D
MのアドミタンスYA が、一般に、周波数fに対する測
定用下部電極層ELM及び測定用上部電極層EUM間の
容量CのアドミタンスYC だけからなる等価アドミタン
ス回路で表されず、図5に示すような、測定用下部電極
層ELM及び測定用上部電極層EUM間の容量Cのアド
ミタンスYC と、それと直列な寄生アドミタンスY
S と、アドミタンスYC と並列な寄生アドミタンスYP
とを有する等価アドミタンス回路で表されるので、測定
用素子DMの測定用下部電極層ELM及び測定用上部電
極層EUMでみたアドミタンスYM から周波数fに対す
る測定用下部電極層ELM及び測定用上部電極層EUM
間の容量Cの関係を求めるとすれば、その周波数fに対
する測定用下部電極層ELM及び測定用上部電極層EU
M間の容量Cが、測定用素子DMが容量Cのアドミタン
スYC だけからなる等価アドミタンス回路で表されると
すれば、例えば図6の線aに示すように、周波数fの5
0GHz以下の値において一定値であるとして得られる
にも拘らず、図6の線bに示すように、周波数fの10
GHzから50GHzの範囲の値において周波数fが高
くなるに従い大きくなる値を呈して得られる。In the conventional method for measuring the high-frequency characteristics of a dielectric thin film shown in FIG. 4, the measurement of the high-frequency characteristics HM of the measuring device DM is performed by measuring the high-frequency characteristics HM of the measuring device DM. If the ELM and measurement of admittance Y a viewed between measurements for the top electrode layer EUM, the measuring device D
Admittance Y A of M is, generally, not represented in the equivalent admittance circuit consisting of only admittance Y C of the capacitance C between the measuring lower electrode layer ELM and measured for the top electrode layer EUM for the frequency f, as shown in FIG. 5 Admittance Y C of capacitance C between lower electrode layer ELM for measurement and upper electrode layer EUM for measurement, and parasitic admittance Y in series therewith
S and parasitic admittance Y P in parallel with admittance Y C
Because represented by an equivalent admittance circuit with bets, measuring lower electrode layer ELM and the lower electrode layer ELM and measuring upper electrode for measurement for measuring the upper electrode layer EUM Demi was admittance Y M from a frequency f of the measurement element DM Layer EUM
If the relationship between the capacitances C is determined, the lower electrode layer ELM for measurement and the upper electrode layer EU for measurement with respect to the frequency f are obtained.
Assuming that the capacitance C between M is represented by an equivalent admittance circuit in which the measuring element DM includes only the admittance Y C of the capacitance C, for example, as shown by a line a in FIG.
Although obtained as a constant value at a value of 0 GHz or less, as shown in a line b of FIG.
It is obtained by exhibiting a value that increases as the frequency f increases in a value in the range of GHz to 50 GHz.
【0008】このようなことから、図4に示す従来の誘
電体薄膜の高周波特性測定法の場合、半導体基板B上に
形成される誘電体薄膜Fの高周波特性Hを、正確に測定
することができない、という欠点を有していた。For this reason, in the conventional method for measuring high-frequency characteristics of a dielectric thin film shown in FIG. 4, it is possible to accurately measure the high-frequency characteristics H of a dielectric thin film F formed on a semiconductor substrate B. There was a drawback that it was not possible.
【0009】よって、本発明は、上述した欠点のない新
規な誘電体薄膜の高周波特性測定法を提案せんとするも
のである。Therefore, the present invention proposes a novel method for measuring high-frequency characteristics of a dielectric thin film which does not have the above-mentioned disadvantages.
【0010】[0010]
【課題を解決するための手段】本発明による誘電体薄膜
の高周波特性測定法は、半導体基板上に形成される誘電
体薄膜の高周波特性を測定するにつき、図4で上述した
従来の誘電体薄膜の高周波特性測定法の場合と同様に、
(a)上記半導体基板に対応している基板上に形成され
ている測定用下部電極層と(b)上記基板上に、上記測
定用下部電極層上に延長して、上記半導体基板上に形成
されている上記誘電体薄膜と同様に形成されている測定
用誘電体薄膜と(c)上記測定用誘電体薄膜上に、上記
測定用下部電極層と対向するように延長して形成されて
いる測定用上部電極層とを有する測定用素子を形成し、
そして、上記測定用素子の上記測定用下部電極層及び上
記測定用上部電極層間でみた高周波特性を測定し、その
測定用素子の高周波特性の測定結果を用いる。The method for measuring the high-frequency characteristics of a dielectric thin film according to the present invention measures the high-frequency characteristics of a dielectric thin film formed on a semiconductor substrate. As in the case of the high-frequency characteristic measurement method,
(A) a lower electrode layer for measurement formed on a substrate corresponding to the semiconductor substrate; and (b) a lower electrode layer for measurement formed on the substrate, extending on the lower electrode layer for measurement. And (c) formed on the dielectric thin film for measurement so as to extend so as to face the lower electrode layer for measurement. Forming a measurement element having a measurement upper electrode layer,
Then, the high-frequency characteristics of the measurement element between the measurement lower electrode layer and the measurement upper electrode layer are measured, and the measurement results of the high-frequency characteristics of the measurement element are used.
【0011】しかしながら、本発明による誘電体薄膜の
高周波特性測定法は、このような誘電体薄膜の高周波特
性測定法において、(i)(a)上記基板上に、上記基
板上に形成されている上記測定用下部電極層と同様に形
成されている第1の補正用下部電極層と(b)上記基板
上に、上記測定用下部電極層上に延長している上記測定
用誘電体薄膜と同様に上記第1の補正用下部電極層上に
延長して、上記基板上に形成されている上記測定用誘電
体薄膜と同様に形成されている第1の補正用誘電体薄膜
と(c)上記第1の補正用誘電体薄膜上に、上記測定用
誘電体薄膜上に形成されている上記測定用上部電極層
と、それが上記測定用下部電極層と対向して延長してい
るようには上記第1の補正用下部電極層と対向するよう
に延長していないことを除いて、同様に形成されている
第1の補正用上部電極層とを有する第1の補正用素子を
形成し、そして、その第1の補正用素子の上記第1の補
正用下部電極層及び上記第1の補正用上部電極層間でみ
た高周波特性を、上記測定用素子の高周波特性の測定の
場合と同様に測定するとともに、(ii)(a)上記基
板上に、上記基板上に形成されている上記測定用下部電
極層と同様に形成されている第2の補正用下部電極層と
(b)上記基板上に、上記測定用下部電極層上に延長し
ている上記測定用誘電体薄膜と同様に上記第2の補正用
下部電極層上に延長して、上記基板上に形成されている
上記測定用誘電体薄膜と同様に形成されている第2の補
正用誘電体薄膜と(c)上記第2の補正用誘電体薄膜上
に、上記測定用誘電体薄膜上に形成されている上記測定
用上部電極層と、それが上記測定用下部電極層と対向し
て延長しているようには上記第2の補正用下部電極層と
対向して延長していないこと及び上記第2の補正用下部
電極層に連結していることを除いて、同様に形成されて
いる第2の補正用上部電極層とを有する第2の補正用素
子を形成し、そして、その第2の補正用素子の上記第2
の補正用下部電極層及び上記第2の補正用上部電極層間
でみた高周波特性を、上記測定用素子の高周波特性の測
定の場合と同様に測定し、(iii)上記測定用素子の
高周波特性の測定結果を、上記第1の補正用素子の高周
波特性の測定結果及び上記第2の補正用素子の高周波特
性の測定結果で補正し、その補正された上記測定用素子
の高周波特性の測定結果を、上記測定用素子の高周波特
性の測定結果として用いる。However, the method for measuring the high-frequency characteristics of a dielectric thin film according to the present invention is the same as the method for measuring the high-frequency characteristics of a dielectric thin film described above, except that (i) (a) is formed on the substrate on the substrate. A first correction lower electrode layer formed similarly to the measurement lower electrode layer, and (b) the same as the measurement dielectric thin film extending on the measurement lower electrode layer on the substrate. A first correction dielectric thin film formed in the same manner as the measurement dielectric thin film formed on the substrate by extending on the first correction lower electrode layer; On the first correction dielectric thin film, the measurement upper electrode layer formed on the measurement dielectric thin film and the measurement upper electrode layer are extended so as to face the measurement lower electrode layer. Make sure that it does not extend so as to face the first correction lower electrode layer. Except that a first correcting element having a first correcting upper electrode layer formed in the same manner as above is formed, and the first correcting lower electrode layer of the first correcting element is formed. And measuring the high-frequency characteristics between the first correction upper electrode layers in the same manner as in the measurement of the high-frequency characteristics of the measurement element, and (ii) (a) forming on the substrate and on the substrate; A second lower electrode layer for correction formed in the same manner as the lower electrode layer for measurement, and (b) the dielectric for measurement extending on the lower electrode layer for measurement on the substrate. Like the thin film, the second correcting dielectric thin film formed on the substrate and extending on the second correcting lower electrode layer and formed in the same manner as the measuring dielectric thin film formed on the substrate ( c) on the second dielectric thin film for correction, on the dielectric thin film for measurement The upper electrode layer for measurement, and the second upper electrode layer for correction is not extended so as to be opposed to the lower electrode layer for measurement. A second compensating element having a similarly formed second compensating upper electrode layer except that it is coupled to the second compensating lower electrode layer; and The second element of the correction element
The high-frequency characteristics between the lower electrode layer for correction and the second upper electrode layer for correction are measured in the same manner as in the measurement of the high-frequency characteristics of the measurement element, and (iii) the high-frequency characteristics of the measurement element are measured. The measurement result is corrected by the measurement result of the high-frequency characteristic of the first correction element and the measurement result of the high-frequency characteristic of the second correction element, and the corrected measurement result of the high-frequency characteristic of the measurement element is obtained. This is used as a result of measuring the high-frequency characteristics of the measuring element.
【0012】[0012]
【実施例】次に、図1を伴って、本発明による誘電体薄
膜の高周波特性測定法の実施例を述べよう。Next, an embodiment of a method for measuring high-frequency characteristics of a dielectric thin film according to the present invention will be described with reference to FIG.
【0013】図1において、図4との対応部分には同一
符号を付して示す。In FIG. 1, parts corresponding to those in FIG. 4 are denoted by the same reference numerals.
【0014】図1に示す本発明による誘電体薄膜の高周
波特性測定法の実施例は、半導体基板B上に形成される
誘電体薄膜Fの高周波特性Hを測定するにつき、図4に
示す従来の誘電体薄膜の高周波特性測定法の場合と同様
に、(a)半導体基板Bに対応している基板BB上に形
成されている測定用下部電極層ELと(b)基板BB上
に、測定用下部電極層ELM上に延長して、誘電体薄膜
Fが半導体基板B上に形成されているのと同様に形成さ
れている測定用誘電体薄膜FMと(c)測定用誘電体薄
膜FM上に、測定用下部電極層ELMと対向するように
延長して形成されている測定用上部電極層EUMとを有
する測定用素子DMを形成し、その測定用素子DMの測
定用下部電極層ELM及び測定用上部電極層EUM間で
みた高周波特性HMを測定し、その測定用素子DMの高
周波特性HMの測定結果を用いる。In the embodiment of the method for measuring the high frequency characteristics of a dielectric thin film according to the present invention shown in FIG. 1, the high frequency characteristics H of a dielectric thin film F formed on a semiconductor substrate B are measured. As in the case of the method of measuring the high frequency characteristics of a dielectric thin film, (a) a lower electrode layer EL for measurement formed on a substrate BB corresponding to the semiconductor substrate B and (b) a lower electrode layer for measurement on the substrate BB. Extending on the lower electrode layer ELM, the dielectric thin film F is formed on the semiconductor thin film B in the same manner as the dielectric thin film F is formed on the semiconductor substrate B and (c) on the dielectric thin film for measurement FM. Forming a measuring element DM having a measuring upper electrode layer EUM extending so as to face the measuring lower electrode layer ELM, and forming the measuring lower electrode layer ELM and the measuring element DM of the measuring element DM. -Frequency characteristics H viewed between upper electrode layers EUM It was measured, using the measurement results of the frequency characteristics HM the measuring device DM.
【0015】この場合、測定用素子DMの高周波特性H
Mの測定は、図4に示す従来の誘電体薄膜の高周波特性
測定法の場合と同様に、測定用素子DMの測定用下部電
極層ELM及び測定用上部電極層EUM間でみたアドミ
タンスYA の測定とし得る。In this case, the high frequency characteristic H of the measuring element DM
Measurement of M is of the conventional 4 as in the case of the dielectric thin film of the high-frequency characteristics measuring method, the admittance Y A viewed between measurements lower electrode layer of the measuring device DM ELM and measuring the upper electrode layer EUM It can be a measurement.
【0016】また、測定用素子DMの高周波特性HMの
測定結果の用い方は、図4に示す従来の誘電体薄膜の高
周波特性測定法の場合と同様に、測定用素子DMの高周
波特性HMの測定を、測定用素子DMの測定用下部電極
層ELM及び測定用上部電極層EUM間でみたアドミタ
ンスYA の測定とする場合、図4に示す従来の誘電体薄
膜の高周波特性測定法の場合に準じて、そのアドミタン
スYA の後述するように補正されたアドミタンスYA ′
から、周波数fに対する測定用下部電極層ELM及び測
定用上部電極層EUM間の容量Cの関係を求め、その求
められた容量Cが周波数fのどのような値またはどのよ
うな範囲の値でどのような値を呈するのかとか、補正さ
れたアドミタンスYA から測定用誘電体薄膜FMの誘電
損失tanδを求め、その誘電損失tanδがどのよう
な値を呈しているのか、補正されたアドミタンスYA ′
から測定用誘電体薄膜FMの比誘電率εを求め、その比
誘電率εがどのような値を呈するかなどの判知ができる
ように用いる。The method of using the measurement result of the high-frequency characteristic HM of the measuring element DM is the same as that of the conventional method of measuring the high-frequency characteristic of the dielectric thin film shown in FIG. the measurement, when the measurement of the admittance Y a viewed between measurements lower electrode layer ELM measuring element DM and measured for the upper electrode layer EUM, in the case of high frequency characteristics measuring method of the conventional dielectric thin film shown in FIG. 4 analogously, in its admittance Y a corrected admittance Y a as described later in '
The relationship between the capacitance C between the lower electrode layer ELM for measurement and the upper electrode layer EUM for measurement with respect to the frequency f is obtained, and the obtained capacitance C is determined at what value of the frequency f or in what range of the value of the frequency f. From the corrected admittance Y A , the dielectric loss tan δ of the dielectric thin film FM for measurement is determined, and the value of the dielectric loss tan δ is determined, and the corrected admittance Y A ′
Is used to determine the relative dielectric constant ε of the dielectric thin film FM for measurement and to know what value the relative dielectric constant ε exhibits.
【0017】図1に示す本発明による誘電体薄膜の高周
波特性測定法の実施例においては、上述した誘電体薄膜
の高周波特性測定法において、(i)(a)上述した測
定用素子DMを形成するのに用いている同じ基板BB上
に、基板BB上に形成されている測定用素子DMの測定
用下部電極層ELMと材質上からも、形状上からも同様
に形成されている第1の補正用下部電極層ELC1と
(b)基板BB上に、測定用素子MMの測定用下部電極
層ELM上に延長している測定用誘電体薄膜FMと形状
上からも同様に第1の補正用下部電極層ELC1に延長
して、基板BB上に形成されている測定用素子DMの測
定用誘電体薄膜FMと材質上からも、形状上からも同様
に形成されている第1の補正用誘電体薄膜FC1と
(c)その第1の補正用誘電体薄膜FC1上に、測定用
素子DMの測定用誘電体薄膜FM上に形成されている測
定用上部電極層EUMと、それが測定用下部電極層EL
Mと対向して延長しているようには第1の補正用下部電
極層ELC1と対向して延長していないことを除いて、
材質上からも、形状上からも同様に形成されている第1
の補正用上部電極層EUC1とを有する第1の補正用素
子DC1を形成し、そして、その第1の補正用素子DC
1の第1の補正用下部電極層ELC1及び第1の補正用
上部電極層EUC1間でみた高周波特性HC1を、測定
用素子DMの高周波特性HMの測定の場合と同様に測定
する。In the embodiment of the method for measuring the high-frequency characteristics of a dielectric thin film according to the present invention shown in FIG. 1, the method for measuring the high-frequency characteristics of a dielectric thin film described above includes the steps of: The first lower electrode layer ELM of the measuring element DM formed on the substrate BB is formed on the same substrate BB used for the measurement on the same material as the first lower electrode layer ELM. Similarly, on the correction lower electrode layer ELC1 and (b) on the substrate BB, from the shape of the measurement dielectric thin film FM extending on the measurement lower electrode layer ELM of the measurement element MM, the first correction Extending to the lower electrode layer ELC1, the first compensating dielectric film FM is formed in the same manner as the material and the shape of the measuring dielectric thin film FM of the measuring device DM formed on the substrate BB. Body thin film FC1 and (c) for its first correction On-collecting thin film FC1, and measuring the dielectric thin film FM measurement upper electrode layer is formed on the EUM of the measuring device DM, it lower electrode layer EL measurement
Except that it does not extend opposite to the first lower electrode layer for correction ELC1 so as to extend opposite to M.
The first formed similarly from the material and the shape
And a first correction element DC1 having the upper correction electrode layer EUC1.
The high-frequency characteristics HC1 between the first first correction lower electrode layer ELC1 and the first correction upper electrode layer EUC1 are measured in the same manner as in the measurement of the high-frequency characteristics HM of the measuring element DM.
【0018】この場合、第1の補正用素子C1の高周波
特性HC1の測定は、上述した測定用素子DMの高周波
特性HMの測定が、測定用素子DMの測定用下部電極層
ELM及び測定用上部電極層EUM間でみたアドミタン
スYA の測定であるとするとき、第1の補正用素子DC
1の第1の補正用下部電極層ELC1及び第1の補正用
上部電極層EUC1間でみたアドミタンスYB の測定と
し得る。In this case, the measurement of the high frequency characteristic HC1 of the first correction element C1 is based on the measurement of the high frequency characteristic HM of the measurement element DM described above. when as a measurement of the admittance Y a viewed between electrode layers EUM, first correction element DC
It may be a measure of the admittance Y B viewed between 1 of the first correction for the lower electrode layer ELC1 and first correction upper electrode layer EUC1.
【0019】また、(ii)(a)基板BB上に、基板
BB上に形成されている測定用下部電極層ELMと材質
上からも、形状上からも同様に形成されている第2の補
正用下部電極層ELC2と(b)基板BB上に、測定用
素子DMの測定用下部電極層ELM上に延長している測
定用誘電体薄膜FMと形状的にも同様に第2の補正用下
部電極層ELC2上に延長して、基板BB上に形成され
ている測定用素子DMの測定用誘電体薄膜FMと材質上
からも、形状上からも同様に形成されている第2の補正
用誘電体薄膜FC2と(c)その第2の補正用誘電体薄
膜FC2上に、測定用素子DMの測定用誘電体薄膜FM
上に形成されている測定用上部電極層EUMと、それが
測定用下部電極層ELMと対向して延長しているように
は第2の補正用下部電極層と対向して延長していないこ
と及び第2の補正用下部電極層ELC2に連結している
ことを除いて、材質上からも、形状上からも同様に形成
されている第2の補正用上部電極層EUC2とを有する
第2の補正用素子DC2を形成し、そして、その第2の
補正用素子DC2の第2の補正用下部電極層ELC2及
び第2の補正用上部電極層EUC2間でみた高周波特性
HC2を測定用素子DMの高周波特性HMの測定の場合
と同様に測定する。(Ii) (a) On the substrate BB, the lower correction layer ELM formed on the substrate BB and the second correction formed similarly from the material and the shape. The lower electrode layer ELC2 for measurement and (b) the second lower electrode for correction similarly to the dielectric thin film FM for measurement extending on the lower electrode layer ELM for measurement of the element for measurement DM on the substrate BB. The second correcting dielectric film extending from the electrode layer ELC2 to the measuring dielectric thin film FM of the measuring element DM formed on the substrate BB and formed similarly from the material and the shape. The body thin film FC2 and (c) the measuring dielectric thin film FM of the measuring element DM on the second correcting dielectric thin film FC2.
The upper measurement electrode layer EUM formed thereon and the second lower electrode layer for correction should not extend so as to extend opposite to the lower electrode layer for measurement ELM. And a second upper correction electrode layer EUC2 similarly formed from the material and the shape except that it is connected to the second lower electrode layer for correction ELC2. The correction element DC2 is formed, and the high-frequency characteristics HC2 viewed between the second correction lower electrode layer ELC2 and the second correction upper electrode layer EUC2 of the second correction element DC2 are measured. The measurement is performed in the same manner as the measurement of the high frequency characteristics HM.
【0020】この場合、第2の補正用素子C2の高周波
特性HC2の測定は、上述した測定用素子DMの高周波
特性HMの測定を、測定用素子DMの測定用下部電極層
ELM及び測定用上部電極層EUM間でみたアドミタン
スYA の測定であるとするとき、第2の補正用素子DC
2の第2の補正用下部電極層ELC2及び第2の補正用
上部電極層EUC2間でみたアドミタンスYD の測定と
し得る。In this case, the measurement of the high-frequency characteristic HC2 of the second correction element C2 is based on the measurement of the high-frequency characteristic HM of the measurement element DM described above, and the measurement of the lower electrode layer ELM and the upper measurement layer of the measurement element DM. when as a measurement of the admittance Y a viewed between electrode layers EUM, the second correction element DC
It may be a measure of the admittance Y D viewed between 2 of the second correction lower electrode layer ELC2 and second correction for the upper electrode layer EUC2.
【0021】そして、(iii)測定用素子DMの高周
波特性HMの測定結果を、第1の補正用素子DC1の高
周波特性HC1の測定結果及び第2の補正用素子DC2
の高周波特性HC2の測定結果で補正し、その補正され
た測定用素子DMの高周波特性HMの測定結果を、測定
用素子DMの高周波特性HMの測定結果として用いる。(Iii) The measurement result of the high frequency characteristic HM of the measuring element DM is compared with the measurement result of the high frequency characteristic HC1 of the first correcting element DC1 and the second correcting element DC2.
The measurement result of the high frequency characteristic HM of the measurement element DM is used as the measurement result of the high frequency characteristic HM of the measurement element DM.
【0022】この場合、測定用素子DMの高周波特性H
Mの測定結果の補正は、測定用素子DMの高周波特性H
Mの測定を上述したように測定用素子DMの測定用下部
電極層ELM及び測定用上部電極層EUM間でみたアド
ミタンスYA の測定とし、また第1の補正用素子DC1
の高周波特性HC1の測定を上述したように第1の補正
用素子DC1の第1の補正用下部電極層ELC1及び第
1の補正用上部電極層EUC1間でみたアドミタンスY
B の測定とし、さらに第2の補正用素子DC2の高周波
特性HC2の測定を上述したように第2の補正用素子D
C2の第2の補正用下部電極層ELC2及び第2の補正
用上部電極層EUC2間でみたアドミタンスYD の測定
とする場合、アドミタンスYA をアドミタンスYB 及び
YC を用いてアドミタンスYA ′に補正するものとし得
る。In this case, the high frequency characteristic H of the measuring element DM
The measurement result of M is corrected by the high-frequency characteristic H of the measuring element DM.
Measurement of M and the measurement of the admittance Y A viewed between measurements lower electrode layer ELM measuring element DM as described above and measured for the upper electrode layer EUM, also first correction element DC1
Of the high frequency characteristic HC1 of the first correction element DC1 between the first correction lower electrode layer ELC1 and the first correction upper electrode layer EUC1 as described above.
B , and the measurement of the high frequency characteristic HC2 of the second correction element DC2 is performed as described above.
If the measurement of the admittance Y D viewed between the second correcting lower electrode layer ELC2 and second correction for the upper electrode layer EUC2 of C2, the admittance Y A using admittance Y B and Y C admittance Y A ' To be corrected.
【0023】また、補正された測定用素子DMの高周波
特性HMの測定結果の用い方は、測定用素子DMの高周
波特性HMの測定結果を、上述したアドミタンスYA を
アドミタンスYA ′に補正するものとするとき、そのア
ドミタンスYA ′から、周波数fに対する測定用素子D
Mの測定用下部電極層ELM及び測定用上部電極層EU
M間の容量Cの関係を求め、その求められた容量Cが周
波数fのどのような値またはどのような範囲の値でどの
ような値を呈するのかとか、アドミタンスYA′から測
定用誘電体薄膜FMの誘電損失tanδを求め、その誘
電損失tanδがどのような値を呈しているのか、アド
ミタンスYA から測定用誘電体薄膜FMの比誘電率ε
を求め、その比誘電率εがどのような値を呈するかなど
の判知ができるように用い得る。Further, manner of using the measurement results of the frequency characteristics HM of the corrected measurement element DM is the measurement results of the frequency characteristics HM of the measuring device DM, corrects the admittance Y A described above in admittance Y A ' when the objects, from the admittance Y a ', measuring device D with respect to the frequency f
M lower electrode layer ELM and upper electrode layer EU for measurement
Obtained relation capacitance C between M, the the obtained capacitance C Toka whether exhibiting any value by the value of the value or any range as the frequency f throat, measuring dielectric from admittance Y A ' seeking a dielectric loss tanδ of the thin film FM, whether the dielectric loss tanδ are exhibited any value, the dielectric constant of the measuring dielectric thin FM from admittance Y a epsilon
Is obtained, and it can be used so that the value of the relative permittivity ε can be known.
【0024】以上が、本発明による誘電体薄膜の高周波
特性測定法の実施例である。The above is an embodiment of the method for measuring high-frequency characteristics of a dielectric thin film according to the present invention.
【0025】このような本発明による誘電体薄膜の高周
波特性測定法によれば、測定用素子DMを、図4に示す
従来の誘電体薄膜の高周波特性測定法の場合と同様に、
半導体装置を製造するのに従来用いている方法によっ
て、容易に形成することができるとともに、第1及び第
2の補正用素子DC1及びDC2も、測定用素子DMと
同様に且つ同時に、容易に形成することができるので、
半導体基板B上に形成される誘電体薄膜Fの高周波特性
Hを、容易に測定することができる。According to the method for measuring the high-frequency characteristics of a dielectric thin film according to the present invention, the measuring element DM is connected to the same as the conventional method for measuring the high-frequency characteristics of a dielectric thin film shown in FIG.
It can be easily formed by a method conventionally used for manufacturing a semiconductor device, and the first and second correction elements DC1 and DC2 can be easily formed at the same time as the measurement element DM. So you can
The high frequency characteristics H of the dielectric thin film F formed on the semiconductor substrate B can be easily measured.
【0026】また、図1に示す本発明による誘電体薄膜
の高周波特性測定法の場合、測定用素子DMの高周波特
性HMの測定を、上述したように測定用素子DMの測定
用下部電極層ELM及び測定用上部電極層EUM間でみ
たアドミタンスYA の測定とし、また、第1の補正用素
子DC1の高周波特性HC1の測定を上述したように第
1の補正用素子DC1の第1の補正用下部電極層ELC
1及び第1の補正用上部電極層EUC1間でみたアドミ
タンスYB の測定とし、さらに第2の補正用素子DC2
の高周波特性HC2の測定を上述したように第2の補正
用素子DC2の第2の補正用下部電極層ELC2及び第
2の補正用上部電極層EUC2間でみたアドミタンスY
D の測定とする場合、測定用素子DMのアドミタンスY
A が、一般に、周波数fに対する測定用下部電極層EL
M及び測定用上部電極層EUM間の容量Cのアドミタン
スYC だけからなる等価アドミタンス回路で表されな
く、図2A及び図5に示すような、測定用下部電極層E
LM及び測定用上部電極層EUM間の容量Cのアドミタ
ンスYC と、それと直列な寄生アドミタンスYS と、ア
ドミタンスYC と並列な寄生アドミタンスYP とを有す
る等価アドミタンス回路で表されるとしても、第1の補
正用素子C1の第1の補正用下部電極層ELC1及び第
1の補正用上部電極層EUC1間でみたアドミタンスY
B が、一般に、図2Bに示す図2AのアドミタンスYC
がオープンしている等価アドミタンス回路で表され、ま
た第2の補正用素子DC2の第2の補正用下部電極層E
LC2及び第2の補正用上部電極層EUC2間でみたア
ドミタンスYD が、一般に、図2Cに示す図2Aのアド
ミタンスYCがショートしている等価アドミタンス回路
で表されることから、アドミタンス回路YC を、 YC={(YA−YB)(YC−YB)/(YC−YA)}Y0
=G+iωC で求め(Y0 は定数)、そして、そのアドミタンスYC
を用いて、周波数fに対する測定用下部電極層ELM及
び測定用上部電極層EUM間の容量Cの関係を求めるよ
うにすれば、その周波数fに対する測定用下部電極層E
LM及び測定用上部電極層EUM間の容量Cが、測定用
素子DMが容量CのアドミタンスYC だけからなる等価
アドミタンス回路で表されるとする場合に得られる図3
及び図6の線aに示すように、周波数fの50GHz以
下の値において一定値であるとして得られる。In the method for measuring the high-frequency characteristics of the dielectric thin film according to the present invention shown in FIG. 1, the measurement of the high-frequency characteristics HM of the measuring device DM is performed by the same method as described above. and the measurement of the admittance Y a viewed between measurements for the top electrode layer EUM, also for the first correction of the first correction element DC1 measured frequency characteristics HC1 of the first correction element DC1 as described above Lower electrode layer ELC
The admittance Y B is measured between the first and first correction upper electrode layers EUC1, and the second correction element DC2
Of the high frequency characteristic HC2 of the second correction element DC2 as described above between the second correction lower electrode layer ELC2 and the second correction upper electrode layer EUC2.
When measuring D , the admittance Y of the measuring element DM
A is generally the lower electrode layer EL for measurement with respect to the frequency f.
It is not represented by an equivalent admittance circuit consisting of only the admittance Y C of the capacitance C between M and the upper electrode layer EUM for measurement.
Even if it is represented by an equivalent admittance circuit having an admittance Y C of the capacitance C between the LM and the measurement upper electrode layer EUM, a parasitic admittance Y S in series with the admittance Y S, and a parasitic admittance Y P in parallel with the admittance Y C , Admittance Y viewed between the first correction lower electrode layer ELC1 and the first correction upper electrode layer EUC1 of the first correction element C1.
B is generally the admittance Y C of FIG. 2A shown in FIG. 2B.
Are represented by an open equivalent admittance circuit, and the second correction lower electrode layer E of the second correction element DC2 is
Since the admittance Y D viewed between the LC2 and the second upper electrode layer for correction EUC2 is generally represented by an equivalent admittance circuit in which the admittance YC in FIG. 2A shown in FIG. 2C is short-circuited, the admittance circuit Y C is used. , Y C = {(Y A −Y B ) (Y C −Y B ) / (Y C −Y A )} Y 0
= G + iωC (Y0 is a constant), and its admittance YC
Is used to determine the relationship of the capacitance C between the lower electrode layer ELM for measurement and the upper electrode layer EUM for measurement with respect to the frequency f.
FIG. 3 is obtained when the capacitance C between the LM and the measurement upper electrode layer EUM is represented by an equivalent admittance circuit composed of only the admittance Y C of the capacitance C.
As shown in a line a in FIG. 6, the frequency f is obtained as a constant value at a value of 50 GHz or less.
【0027】以上のことから、図1に示す本発明による
誘電体薄膜の高周波特性測定法の場合、半導体基板B上
に形成される誘電体薄膜Fの高周波特性Hを、図4で前
述した従来の誘電体薄膜の高周波特性測定法の場合に比
し、正確に測定することができる。As described above, in the method of measuring high-frequency characteristics of a dielectric thin film according to the present invention shown in FIG. 1, the high-frequency characteristics H of a dielectric thin film F formed on a semiconductor substrate B are compared with those of the prior art shown in FIG. It can be measured more accurately than the method of measuring the high frequency characteristics of a dielectric thin film.
【0028】なお、上述においては、本発明による誘電
体薄膜の高周波特性測定法の1つの実施例を示したに留
まり、本発明の精神を脱することなしに種々の変型、変
更をなし得るであろう。In the above, only one embodiment of the method for measuring the high-frequency characteristics of a dielectric thin film according to the present invention has been described, and various modifications and changes can be made without departing from the spirit of the present invention. There will be.
【図1】本発明による誘電体薄膜の高周波特性測定法の
説明に供する、測定用素子、及び第1及び第2の補正用
素子を示す略線的平面図(図1A)及びそのb−b線上
の断面図(図1B)である。FIG. 1 is a schematic plan view (FIG. 1A) showing a measuring element and first and second correcting elements for explaining a high-frequency characteristic measuring method of a dielectric thin film according to the present invention, and bb thereof. It is sectional drawing on a line (FIG. 1B).
【図2】図1に示す本発明による誘電体薄膜の高周波特
性測定法の説明に供する、測定用素子、及び第1及び第
2の補正用素子の等価回路を示す図である。FIG. 2 is a diagram showing an equivalent circuit of a measurement element and first and second correction elements for explaining a method of measuring high-frequency characteristics of a dielectric thin film according to the present invention shown in FIG. 1;
【図3】図1に示す本発明による誘電体薄膜の高周波特
性測定法の説明に供する、測定用素子の高周波特性の測
定結果から求められる周波数fに対する容量(C)の関
係を示す図である。FIG. 3 is a diagram illustrating the relationship between the capacitance (C) and the frequency f obtained from the measurement result of the high-frequency characteristics of the measuring element, for explaining the method of measuring the high-frequency characteristics of the dielectric thin film according to the present invention shown in FIG. .
【図4】従来の誘電体薄膜の高周波特性測定法の説明に
供する、測定用素子を示す略線的平面図(図4A)及び
そのb−b線上の断面図(図4B)である。4A and 4B are a schematic plan view (FIG. 4A) showing a measuring element and a cross-sectional view taken along the line bb (FIG. 4B) for explaining a conventional method for measuring high-frequency characteristics of a dielectric thin film.
【図5】図4に示す従来の誘電体薄膜の高周波特性測定
法の説明に供する、測定用素子の等価回路を示す図であ
る。FIG. 5 is a diagram showing an equivalent circuit of a measuring element for explaining the conventional method for measuring high-frequency characteristics of a dielectric thin film shown in FIG.
【図6】図4に示す従来の誘電体薄膜の高周波特性測定
法の説明に供する、測定用素子の高周波特性の測定結果
から求められる周波数fに対する容量(C)の関係を示
す図である。FIG. 6 is a diagram illustrating the relationship between the capacitance (C) and the frequency f obtained from the measurement result of the high-frequency characteristics of the measuring element, for explaining the conventional method for measuring the high-frequency characteristics of the dielectric thin film shown in FIG.
B 半導体基板 BB、BC 基板 DC1、DC2 補正用素子 DM 測定用素子 EUM 測定用上部電極層 ELM 測定用下部電極層 EUC1、EUC2 補正用上部電極層 ELC1、ELC2 補正用下部電極層 F 誘電体薄膜 FC1、FC2 補正用誘電体薄膜 FM 測定用誘電体薄膜 B Semiconductor substrate BB, BC substrate DC1, DC2 Correction element DM measurement element EUM measurement upper electrode layer ELM measurement lower electrode layer EUC1, EUC2 Correction upper electrode layer ELC1, ELC2 Correction lower electrode layer F Dielectric thin film FC1 , FC2 Dielectric thin film for correction Dielectric thin film for FM measurement
フロントページの続き (56)参考文献 特開 平5−34388(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01R 27/26 H01L 21/66 Continuation of the front page (56) References JP-A-5-34388 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G01R 27/26 H01L 21/66
Claims (1)
高周波特性を測定するにつき、 (a)上記半導体基板に対応している基板上に形成され
ている測定用下部電極層と(b)上記基板上に、上記測
定用下部電極層上に延長して、上記半導体基板上に形成
されている上記誘電体薄膜と同様に形成されている測定
用誘電体薄膜と(c)上記測定用誘電体薄膜上に、上記
測定用下部電極層と対向するように延長して形成されて
いる測定用上部電極層とを有する測定用素子を形成し、
上記測定用素子の上記測定用下部電極層及び上記測定用
上部電極層間でみた高周波特性を測定し、その測定用素
子の高周波特性の測定結果を用いる誘電体薄膜の高周波
特性測定法において、 (i)(a)上記基板上に、上記基板上に形成されてい
る上記測定用下部電極層と同様に形成されている第1の
補正用下部電極層と(b)上記基板上に、上記測定用下
部電極層上に延長している上記測定用誘電体薄膜と同様
に上記第1の補正用下部電極層上に延長して、上記基板
上に形成されている上記測定用誘電体薄膜と同様に形成
されている第1の補正用誘電体薄膜と(c)上記第1の
補正用誘電体薄膜上に、上記測定用誘電体薄膜上に形成
されている上記測定用上部電極層と、それが上記測定用
下部電極層と対向して延長しているようには上記第1の
補正用下部電極層と対向するように延長していないこと
を除いて、同様に形成されている第1の補正用上部電極
層とを有する第1の補正用素子を形成し、その第1の補
正用素子の上記第1の補正用下部電極層及び上記第1の
補正用上部電極層間でみた高周波特性を、上記測定用素
子の高周波特性の測定の場合と同様に測定するととも
に、 (ii)(a)上記基板上に、上記基板上に形成されて
いる上記測定用下部電極層と同様に形成されている第2
の補正用下部電極層と(b)上記基板上に、上記測定用
下部電極層上に延長している上記測定用誘電体薄膜と同
様に上記第2の補正用下部電極層上に延長して、上記基
板上に形成されている上記測定用誘電体薄膜と同様に形
成されている第2の補正用誘電体薄膜と(c)上記第2
の補正用誘電体薄膜上に、上記測定用誘電体薄膜上に形
成されている上記測定用上部電極層と、それが上記測定
用下部電極層と対向して延長しているようには上記第2
の補正用下部電極層と対向して延長していないこと及び
上記第2の補正用下部電極層に連結していることを除い
て、同様に形成されている第2の補正用上部電極層とを
有する第2の補正用素子を形成し、その第2の補正用素
子の上記第2の補正用下部電極層及び上記第2の補正用
上部電極層間でみた高周波特性を、上記測定用素子の高
周波特性の測定の場合と同様に測定し、 (iii)上記測定用素子の高周波特性の測定結果を、
上記第1の補正用素子の高周波特性の測定結果及び上記
第2の補正用素子の高周波特性の測定結果で補正し、そ
の補正された上記測定用素子の高周波特性の測定結果
を、上記測定用素子の高周波特性の測定結果として用い
ることを特徴とする誘電体薄膜の高周波特性測定法。1. A high-frequency characteristic of a dielectric thin film formed on a semiconductor substrate is measured by: (a) a lower electrode layer for measurement formed on a substrate corresponding to the semiconductor substrate; A dielectric thin film for measurement formed on the substrate and extending on the lower electrode layer for measurement and formed in the same manner as the dielectric thin film formed on the semiconductor substrate; On the body thin film, to form a measurement element having a measurement upper electrode layer formed to extend so as to face the measurement lower electrode layer,
In the method for measuring high-frequency characteristics between the lower electrode layer for measurement and the upper electrode layer for measurement of the measurement element, and using the measurement result of the high-frequency characteristics of the measurement element, (A) a first correction lower electrode layer formed on the substrate in the same manner as the measurement lower electrode layer formed on the substrate; and (b) a measurement lower electrode layer formed on the substrate. Like the measurement dielectric thin film extending on the lower electrode layer, extending on the first correction lower electrode layer in the same manner as the measurement dielectric thin film formed on the substrate. A first correction dielectric thin film formed, and (c) an upper electrode layer for measurement formed on the dielectric thin film for measurement, on the first dielectric thin film for correction, and The above-described first electrode extends so as to face the lower electrode layer for measurement. A first correction element having a first correction upper electrode layer similarly formed except that the first correction element does not extend so as to face the first correction lower electrode layer; The high-frequency characteristics of the first correction lower electrode layer and the first correction upper electrode layer of the first correction element are measured in the same manner as in the measurement of the high-frequency characteristic of the measurement element. ii) (a) A second electrode formed on the substrate in the same manner as the lower electrode layer for measurement formed on the substrate.
And (b) extending on the second correction lower electrode layer on the substrate in the same manner as the measurement dielectric thin film extending on the measurement lower electrode layer. A second dielectric thin film for correction formed in the same manner as the dielectric thin film for measurement formed on the substrate, and (c) a second dielectric thin film for correction.
On the correction dielectric thin film, the upper electrode layer for measurement formed on the dielectric thin film for measurement, and the first electrode layer as described above so that it extends facing the lower electrode layer for measurement. 2
And the second correction upper electrode layer, which is formed in the same manner, except that it does not extend opposite to the correction lower electrode layer and is connected to the second correction lower electrode layer. Is formed, and the high-frequency characteristics of the second correction element viewed between the second correction lower electrode layer and the second correction upper electrode layer are compared with those of the measurement element. The measurement is performed in the same manner as the measurement of the high-frequency characteristics. (Iii) The measurement result of the high-frequency characteristics of the measuring element is
The measurement result of the high-frequency characteristic of the first correction element and the measurement result of the high-frequency characteristic of the second correction element are corrected, and the corrected measurement result of the high-frequency characteristic of the measurement element is used for the measurement. A method for measuring high-frequency characteristics of a dielectric thin film, which is used as a result of measuring the high-frequency characteristics of an element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP05509795A JP3173554B2 (en) | 1995-02-20 | 1995-02-20 | Measurement method of high frequency characteristics of dielectric thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP05509795A JP3173554B2 (en) | 1995-02-20 | 1995-02-20 | Measurement method of high frequency characteristics of dielectric thin film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08226941A JPH08226941A (en) | 1996-09-03 |
| JP3173554B2 true JP3173554B2 (en) | 2001-06-04 |
Family
ID=12989246
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP05509795A Expired - Lifetime JP3173554B2 (en) | 1995-02-20 | 1995-02-20 | Measurement method of high frequency characteristics of dielectric thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3173554B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4518680B2 (en) * | 2001-01-30 | 2010-08-04 | 京セラ株式会社 | Dielectric constant measurement method |
| JP4530951B2 (en) * | 2005-08-29 | 2010-08-25 | 京セラ株式会社 | Dielectric constant measurement method and open-ended half-wavelength coplanar line resonator |
| JP5263944B2 (en) * | 2008-09-16 | 2013-08-14 | 独立行政法人産業技術総合研究所 | Micro thin film capacitance element and thin film dielectric property measurement and evaluation method using the same |
-
1995
- 1995-02-20 JP JP05509795A patent/JP3173554B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH08226941A (en) | 1996-09-03 |
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