WO2003052159A1 - Amorphous ferrosilicide film exhibiting semiconductor characteristics and method for producing the same - Google Patents
Amorphous ferrosilicide film exhibiting semiconductor characteristics and method for producing the same Download PDFInfo
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- WO2003052159A1 WO2003052159A1 PCT/JP2002/009242 JP0209242W WO03052159A1 WO 2003052159 A1 WO2003052159 A1 WO 2003052159A1 JP 0209242 W JP0209242 W JP 0209242W WO 03052159 A1 WO03052159 A1 WO 03052159A1
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/35—Sputtering by application of a magnetic field, e.g. magnetron sputtering
- C23C14/352—Sputtering by application of a magnetic field, e.g. magnetron sputtering using more than one target
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/06—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
- C23C14/0682—Silicides
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/3407—Cathode assembly for sputtering apparatus, e.g. Target
- C23C14/3414—Metallurgical or chemical aspects of target preparation, e.g. casting, powder metallurgy
Definitions
- the present invention relates to an amorphous iron silicide film exhibiting semiconductor characteristics and a method for manufacturing the same.
- 3— F e S i2 is a direct-transition semiconductor with a band gap of 0.85 eV, and is expected to be applied to solar cells and light emitting and receiving devices for communication.
- the present inventor has previously developed a method for depositing a three-phase FeSi 2 thin film while being deposited on a substrate by a laser ablation method (Patent Document 1: Japanese Patent Application Laid-Open No. 2000-178713). ). Disclosure of the invention
- a stable solid solution is formed when Si is in the range of 69 to 72.5 at%. It has been disclosed in Japanese Patent Publication No. 1133-1453 that the amorphous film of the FeSi 2 phase exhibits semiconductor characteristics. However, this amorphous film is manufactured by a cluster ion beam evaporation method in which Fe and Si are sprayed from separate hermetically sealed crucibles and vapor-deposited. The value of the degree ⁇ is 11 ⁇ — 1 cm— 1 at 590 ° ⁇ , and the band gap is 1.258 eV, which does not show characteristics close to 1 F e S i 2.
- amorphous structure film In order to obtain a good quality amorphous structure film, it is necessary to use It is necessary to allow the atomic particles to reach the substrate and quench them on a substrate that is not heated or cooled at a low temperature, such as cluster ion beam evaporation, molecular beam epitaxy, ion implantation, etc.
- the RF magnetron sputtering method which is considered to be the most suitable for obtaining an amorphous structure film compared to other existing methods, also requires that the plasma be in contact with the film being deposited. However, the film is damaged, and microcrystals are formed due to the effect of annealing, so that it is difficult to obtain a completely amorphous film. Not obtained until.
- the inventor of the present invention has obtained a very good quality FeSi 2 in an amorphous state by depositing a flat film that is not granular, that is, a continuous film by using a sputtering method capable of depositing particles with high energy. It has been found that FeSi 2 in the state shows semiconductor characteristics close to 3 — FeSi 2.
- the present invention is an amorphous iron silicide film exhibiting semiconductor characteristics comprising an amorphous FeSi 2 film having a band gap of 0.6 to 1.0 OeV obtained by a sputtering method.
- the present invention uses a FeSi 2 alloy target having a component atomic ratio of Fe to Si of 1: 2, at a low Ar gas pressure of 5 mTorr or less, and at a temperature of less than 400 ° C.
- Amorphous FeSi 2 can be obtained by low-pressure sputtering under a low Ar gas pressure of 5 mTorr or less.
- the opposing target sputtering method A high quality amorphous FeSi 2 film can be grown.
- FIG. 1 is a conceptual diagram showing the principle of the opposed target type DC sputtering method.
- the plasma is completely confined between the target 2 and the target 3 by the magnetic field B applied in parallel with the electric field E, and the plasma does not come into contact with the substrate 1 arranged vertically with the target 2 and the target 3.
- the substrate 1 arranged vertically with the target 2 and the target 3.
- only neutral particles are deposited on the substrate 1, and the grown film is not damaged by the plasma and does not receive an anneal effect, so that microcrystals are not generated and a better amorphous film is obtained.
- a continuous film (as-growth) can be grown because the surface temperature of the deposited film is small.
- the resulting film has a very small composition deviation from the target, and a FeSi 2 alloy target can be used similarly to the laser ablation method.
- low-pressure sputtering of 5 mTorr or less, preferably 1 mTorr or less, is possible, the emitted particles (atoms) from the target maintain high energy without substantially colliding with the Ar gas for sputtering. To reach.
- the above two improvements over the RF magnetron sputtering method enable the growth of higher quality amorphous iron silicide films.
- FIG. 1 is a conceptual diagram showing the principle of the facing target type DC sputtering method.
- (A) and (b) in FIG. 2 are photographs substituted for drawings showing surface SEM images of amorphous iron silicide and polycrystalline] 3 _FeSi 2 films produced by the method of the present invention, respectively.
- FIG. 3 shows an X-ray diffraction pattern of iron silicide produced by the method of the present invention.
- 6 is a graph showing substrate temperature dependence of a turn.
- FIG. 4 is a graph showing the substrate temperature dependence of the light absorption spectrum and absorption coefficient ⁇ of iron silicide produced by the method of the present invention.
- FIG. 5 is a graph showing the substrate temperature dependence of the optical absorption spectrum and the optical band gap E g of the iron silicide produced by the method of the present invention.
- FIG. 6 is a graph showing the substrate temperature dependence of the sheet resistance and specific resistance P of iron silicide produced by the method of the present invention.
- the sputtering was performed by the sputtering method.
- An iron silicide thin film having a thickness of about 240 ⁇ m was formed on a substrate in a temperature range from room temperature to 400 ° C.
- an iron silicide thin film was similarly prepared at a temperature range of 400 ° C or higher.
- the target used was a FeSi 2 alloy (99.99%) having a composition ratio of 1: 2.
- the sputtering chamber in one was evacuated to less 10- 4 P a with a turbo-molecular pump, the time of film formation gas pressure of 1. OmTorr flows into the A r gas 15. Osccm, applied voltage, current, respectively 95 OmV, 6.0 mA.
- the deposition rate was 1.0 nmZmin.
- FIG. 2 shows an SEM image showing a change in the surface shape of the iron silicide with respect to the substrate temperature.
- the sample surface is extremely smooth regardless of the substrate temperature.
- Figure 3 shows the substrate temperature dependence of the X-ray diffraction pattern. It can be seen that when the substrate temperature is lower than 400 ° C., amorphous Fe S i 2 is obtained, and when the substrate temperature is 400 ° C. or higher,] 3—F e S i 2 is obtained.
- Figure 4 shows the substrate temperature dependence of the light absorption spectrum and absorption coefficient.
- Figure 5 shows the substrate temperature dependence of the optical absorption spectrum and optical band gap Eg.
- the amorphous FeSi 2 film has a thickness of 0.64 to 0.82 eV
- the polycrystalline 3-FeSi 2 film has a thickness of 0.84 to 0.94 eV.
- FIG. 6 shows the substrate temperature dependence of the sheet resistance and the specific resistance p. Amorufasu F e S i 2 the resistivity p of the film, 3. a 2 ⁇ 7. 3 X 10- 3 Q cm
- the resistivity of the polycrystalline j3- F 6 3 12 film is from 1.0 to 3.2 it is an X 10- 1 ⁇ cm.
- the facing target sputtering method can easily realize the property improvement by adding another element which is effective for the amorphous film.
- a high-quality amorphous film can be obtained by preventing the plasma from coming into contact with the film being formed, thereby preventing the effect of the anneal from acting. Since the method is plasma-free, an amorphous film can be easily obtained. Therefore, lamination is easy. Suitable for large area, easy for industrial application.
- amorphous iron silicide has a magnetic semiconductivity by adding a magnetic element. It is possible to adjust the carrier concentration by solidification and hydrogenation.
- Iron silicide does not require a substrate heating mechanism because it grows at room temperature.
- the amorphous iron silicide film exhibiting the semiconductor characteristics of the present invention can be applied to a solar cell element and a communication light emitting / receiving element.
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Abstract
Description
明 細 書 半導体特性を示すアモルファス鉄シリサイド膜とその作製方法 技術分野 Description Amorphous iron silicide film showing semiconductor characteristics and fabrication method
本発明は、 半導体特性を示すアモルファス鉄シリサイド膜およびその作製方法 に関する。 背景技術 The present invention relates to an amorphous iron silicide film exhibiting semiconductor characteristics and a method for manufacturing the same. Background art
|3— F e S i2は 0. 85 e Vのバンドギャップを持つ直接遷移型の半導体で 太陽電池素子や通信用発受光素子への応用が期待されている。 本発明者は、 先に レーザーアブレーション法で基板上に堆積したままで ;3相の F e S i 2薄膜を堆 積する方法を開発した (特許文献 1 :特開 2000— 1 7871 3号公報) 。 発明の開示 | 3— F e S i2 is a direct-transition semiconductor with a band gap of 0.85 eV, and is expected to be applied to solar cells and light emitting and receiving devices for communication. The present inventor has previously developed a method for depositing a three-phase FeSi 2 thin film while being deposited on a substrate by a laser ablation method (Patent Document 1: Japanese Patent Application Laid-Open No. 2000-178713). ). Disclosure of the invention
S iが 69〜 72. 5 a t %の範囲で安定な固溶体を作る ζ— F e S i 2相の 非晶質膜が半導体特性を示すことが特公平 1一 3 1453号公報に開示されてい るが、 この非晶質膜は、 F eと S iを別々の密閉型坩堝から噴射させて蒸着する クラスターイオンビーム蒸着法で製作されており、 S iが 68 a t%のもので電 気伝導度 σの値は 590° Κで〜 1 Ω— 1 c m— 1であり、 バンドギヤップは 1. 258 e Vであり、 一 F e S i 2に近い特性を示していない。 A stable solid solution is formed when Si is in the range of 69 to 72.5 at%. It has been disclosed in Japanese Patent Publication No. 1133-1453 that the amorphous film of the FeSi 2 phase exhibits semiconductor characteristics. However, this amorphous film is manufactured by a cluster ion beam evaporation method in which Fe and Si are sprayed from separate hermetically sealed crucibles and vapor-deposited. The value of the degree σ is 11 Ω— 1 cm— 1 at 590 ° 、, and the band gap is 1.258 eV, which does not show characteristics close to 1 F e S i 2.
良質なアモルファス構造膜を得るには、 できるだけ高いエネルギー状態で、 か つ原子状の粒子を基板に到達させ、 加熱されていない、 あるいは冷却された低い 温度の基板にて急冷させる必要があるが、 クラスターイオンビーム蒸着法、 分子 線ェピタキシャル成長法、 イオン注入法などの他の既存の方法に比べて、 ァモル ファス構造膜を得るには最も適していると考えられている R Fマグネトロンスパ ッタリング法においても、 通常の方法では、 プラズマが堆積中の膜に接するため に、 膜が損傷を受けるとともにァニール的な効果を受けて微結晶が生成してしま い、 完全なアモルファス膜は得にくく、 一 F e S i 2に近い特性の半導体特性 を有するアモルファス鉄シリサイドはこれまで得られていない。 In order to obtain a good quality amorphous structure film, it is necessary to use It is necessary to allow the atomic particles to reach the substrate and quench them on a substrate that is not heated or cooled at a low temperature, such as cluster ion beam evaporation, molecular beam epitaxy, ion implantation, etc. The RF magnetron sputtering method, which is considered to be the most suitable for obtaining an amorphous structure film compared to other existing methods, also requires that the plasma be in contact with the film being deposited. However, the film is damaged, and microcrystals are formed due to the effect of annealing, so that it is difficult to obtain a completely amorphous film. Not obtained until.
本発明者は、 高エネルギーな粒子堆積が可能なスパッタリング法を用いること によって粒状でない平坦な膜、 すなわち連続膜を堆積することにより極めて良質 なアモルファス状態の F e S i 2が得られ、 該アモルファス状態の F e S i 2が 3 — F e S i 2に近い特性の半導体特性を示すことを見いだした。 The inventor of the present invention has obtained a very good quality FeSi 2 in an amorphous state by depositing a flat film that is not granular, that is, a continuous film by using a sputtering method capable of depositing particles with high energy. It has been found that FeSi 2 in the state shows semiconductor characteristics close to 3 — FeSi 2.
すなわち、 本発明は、 スパッタリング法により得られた 0 . 6〜1 . O e Vの バンドギャップを有するアモルファス F e S i 2膜からなる半導体特性を示すァ モルファス鉄シリサイド膜である。 That is, the present invention is an amorphous iron silicide film exhibiting semiconductor characteristics comprising an amorphous FeSi 2 film having a band gap of 0.6 to 1.0 OeV obtained by a sputtering method.
さらに、 本発明は、 F eと S iの成分原子比 1 : 2の F e S i 2合金ターゲッ トを用い、 5 m T o r r以下の低い A rガス圧力下で、 4 0 0 °C未満の基板上に スパッタリング法により F e S i 2を連続膜として堆積することにより 0 . 6〜 1 . 0 e Vのバンドギヤップを有する ]3— F e S i 2に近い特性の半導体特性を 示すアモルファス F e S i 2膜を作製する方法である。 Furthermore, the present invention uses a FeSi 2 alloy target having a component atomic ratio of Fe to Si of 1: 2, at a low Ar gas pressure of 5 mTorr or less, and at a temperature of less than 400 ° C. Has a band gap of 0.6 to 1.0 eV by depositing F e S i 2 as a continuous film on the substrate by sputtering.] 3- Shows semiconductor characteristics close to those of F e S i 2 This is a method for producing an amorphous FeSi2 film.
アモルファス F e S i 2は 5 mTorr以下の低い A rガス圧力下の低圧スパッタリ ング法により得られる。 特に、 対向ターゲット式スパッタリング法によって、 よ り良質なアモルファス F e S i 2膜を成長できる。 Amorphous FeSi 2 can be obtained by low-pressure sputtering under a low Ar gas pressure of 5 mTorr or less. In particular, the opposing target sputtering method A high quality amorphous FeSi 2 film can be grown.
第 1図は、 対向ターゲット式 D Cスパッタリング法の原理を示す概念図である。 この方法では、 電場 Eと並行に印加された磁場 Bによりプラズマがターゲット 2 およびターゲット 3間に完全に閉じ込められ、 ターゲット 2およびターゲット 3 と垂直方向に配置された基板 1にプラズマが接しないために、 中性粒子のみが基 板 1に堆積され、 成長膜がプラズマによる損傷を受けず、 ァニール的な効果を受 けないために微結晶が生成せず、 より良質なアモルファス膜が得られる。 また、 堆積膜の表面温度上昇が少ないために連続膜 (as- growth) が成長できる。 FIG. 1 is a conceptual diagram showing the principle of the opposed target type DC sputtering method. In this method, the plasma is completely confined between the target 2 and the target 3 by the magnetic field B applied in parallel with the electric field E, and the plasma does not come into contact with the substrate 1 arranged vertically with the target 2 and the target 3. However, only neutral particles are deposited on the substrate 1, and the grown film is not damaged by the plasma and does not receive an anneal effect, so that microcrystals are not generated and a better amorphous film is obtained. In addition, a continuous film (as-growth) can be grown because the surface temperature of the deposited film is small.
また、 プラズマ接触による再スパッタが起こらないために、 得られた膜はター ゲットからの組成ずれが極めて小さく、 レーザーアブレーション法と同様に、 F e S i 2合金ターゲットを使用できる。 さらに、 5 mTorr以下、 好ましくは l mTor r以下の低圧スパッタリングが可能なために、 ターゲットからの放出粒子 (原子) はスパッタ用の A rガスにほとんど衝突することなく高エネルギーを維持したま ま基板に到達する。 同じスパッタリング法でも、 R Fマグネトロンスパッタリン グ法に比べて以上の 2つの改善点により、 より良質なアモルファス鉄シリサイド 膜の成長が可能になる。 図面の簡単な説明 In addition, since re-sputtering due to plasma contact does not occur, the resulting film has a very small composition deviation from the target, and a FeSi 2 alloy target can be used similarly to the laser ablation method. Furthermore, since low-pressure sputtering of 5 mTorr or less, preferably 1 mTorr or less, is possible, the emitted particles (atoms) from the target maintain high energy without substantially colliding with the Ar gas for sputtering. To reach. Even with the same sputtering method, the above two improvements over the RF magnetron sputtering method enable the growth of higher quality amorphous iron silicide films. BRIEF DESCRIPTION OF THE FIGURES
第 1図は、 対向ターゲット式 D Cスパッタリング法の原理を示す概念図である。 第 2図の (a ) 、 ( b ) は、 それぞれ、 本発明の方法により作製したァモルファ ス鉄シリサイドおよび多結晶 ]3 _ F e S i 2膜の表面 S E M像を示す図面代用写 真である。 第 3図は、 本発明の方法により作製された鉄シリサイドの X線回析パ ターンの基板温度依存性を示すグラフである。 第 4図は、 本発明の方法により作 製された鉄シリサイドの光吸収スぺクトルと吸収係数 αの基板温度依存性を示す グラフである。 第 5図は、 本発明の方法により作製された鉄シリサイドの光吸収 スぺクトルと光学バンドギャップ E gの基板温度依存性を示すグラフである。 第 6図は、 本発明の方法により作製された鉄シリサイドのシート抵抗おょぴ比抵抗 Pの基板温度依存性を示すグラフである。 発明を実施するための最良の形態 FIG. 1 is a conceptual diagram showing the principle of the facing target type DC sputtering method. (A) and (b) in FIG. 2 are photographs substituted for drawings showing surface SEM images of amorphous iron silicide and polycrystalline] 3 _FeSi 2 films produced by the method of the present invention, respectively. . FIG. 3 shows an X-ray diffraction pattern of iron silicide produced by the method of the present invention. 6 is a graph showing substrate temperature dependence of a turn. FIG. 4 is a graph showing the substrate temperature dependence of the light absorption spectrum and absorption coefficient α of iron silicide produced by the method of the present invention. FIG. 5 is a graph showing the substrate temperature dependence of the optical absorption spectrum and the optical band gap E g of the iron silicide produced by the method of the present invention. FIG. 6 is a graph showing the substrate temperature dependence of the sheet resistance and specific resistance P of iron silicide produced by the method of the present invention. BEST MODE FOR CARRYING OUT THE INVENTION
(実施例 1 ) (Example 1)
対向ターゲット式 DCスパッタリング装置 ( (株) 薄膜ソフト社製、 ミラート ロンスパッタリング装置 MTS- L2000- 2T) を用いて、 パッタリング法により S i Using a facing target type DC sputtering device (Mitsurin Soft Co., Ltd., Millertron sputtering device MTS-L2000-2T), the sputtering was performed by the sputtering method.
(100) 、 (1 11) 基板上に室温から 400 °Cの温度範囲で膜厚約 240 η mの鉄シリサイド薄膜を作製した。 比較のため 400°C以上の温度範囲で同様に 鉄シリサイド薄膜を作製した。 ターゲットには組成比 1 : 2の F e S i 2合金 (9 9.99%) を使用した。 スパッタリングチャンバ一内はターボ分子ポンプを用いて 10—4P a以下まで排気し、 成膜時は 15. Osccmの A rガスを流入してガス圧 を 1. OmTorrとし、 印加電圧、 電流をそれぞれ 95 OmV、 6. 0mAとした。 堆積速度は 1. 0 nmZm i nであった。 (100), (111) An iron silicide thin film having a thickness of about 240 ηm was formed on a substrate in a temperature range from room temperature to 400 ° C. For comparison, an iron silicide thin film was similarly prepared at a temperature range of 400 ° C or higher. The target used was a FeSi 2 alloy (99.99%) having a composition ratio of 1: 2. The sputtering chamber in one was evacuated to less 10- 4 P a with a turbo-molecular pump, the time of film formation gas pressure of 1. OmTorr flows into the A r gas 15. Osccm, applied voltage, current, respectively 95 OmV, 6.0 mA. The deposition rate was 1.0 nmZmin.
作成膜の評価は S EM観察、 X線回折、 光吸収スぺク トル測定、 電気抵抗測定 により行った。 X線回折測定により基板温度が 400 °C未満ではァモルファスな 膜になっていることが分かった。 吸収スペク トル測定により、 アモルファス F e S i 2は 0. 6〜 0. 7 e 第 2図は、 鉄シリサイドの膜表面形状の基板温度に対する変化を示す SEM像 を示す。 基板温度に係わらず、 試料表面は極めて平滑である。 800°Cではわず かにうねりのような凹凸が観察された。 第 3図は、 X線回析パターンの基板温度 依存性を示す。 基板温度が 400 °C未満でァモルファス F e S i 2が得られ、 4 00°C以上では ]3— F e S i 2が得られることが分かる。 The prepared films were evaluated by SEM observation, X-ray diffraction, light absorption spectrum measurement, and electrical resistance measurement. X-ray diffraction measurement showed that the film was amorphous when the substrate temperature was less than 400 ° C. According to the absorption spectrum measurement, the amorphous FeSi2 was 0.6 to 0.7 e. FIG. 2 shows an SEM image showing a change in the surface shape of the iron silicide with respect to the substrate temperature. The sample surface is extremely smooth regardless of the substrate temperature. At 800 ° C, slight undulation-like irregularities were observed. Figure 3 shows the substrate temperature dependence of the X-ray diffraction pattern. It can be seen that when the substrate temperature is lower than 400 ° C., amorphous Fe S i 2 is obtained, and when the substrate temperature is 400 ° C. or higher,] 3—F e S i 2 is obtained.
第 4図は、 光吸収スペク トルと吸収係数ひの基板温度依存性を示す。 ァモルフ ァス F e S i 2膜は α = 1. 3〜1. 6 X 105 c m— 1、 多結晶 ]3— F e S i 2膜 は α = 5. 0〜7. 8 X 104 cm— 1である。 第 5図は、 光吸収スペク トルと光 学バンドギヤップ E gの基板温度依存性を示す。 アモルファス F e S i 2膜は 0. 64〜0. 82 e V、 多結晶 3— F e S i 2膜は 0. 84〜0. 94 eVである。 第 6図は、 シート抵抗および比抵抗 pの基板温度依存性を示す。 ァモルファス F e S i 2膜の抵抗率 pは、 3. 2〜7. 3 X 10— 3Q cmであり、 多結晶 j3— F 6 3 12膜の抵抗率 は、 1. 0〜3. 2 X 10— 1 Ω c mである。 Figure 4 shows the substrate temperature dependence of the light absorption spectrum and absorption coefficient. Α-Fe S i 2 film is α = 1.3 to 1.6 × 10 5 cm— 1 , polycrystalline] 3 — F e S i 2 film is α = 5.0 to 7.8 X 10 4 cm— one . Figure 5 shows the substrate temperature dependence of the optical absorption spectrum and optical band gap Eg. The amorphous FeSi 2 film has a thickness of 0.64 to 0.82 eV, and the polycrystalline 3-FeSi 2 film has a thickness of 0.84 to 0.94 eV. FIG. 6 shows the substrate temperature dependence of the sheet resistance and the specific resistance p. Amorufasu F e S i 2 the resistivity p of the film, 3. a 2~7. 3 X 10- 3 Q cm , the resistivity of the polycrystalline j3- F 6 3 12 film is from 1.0 to 3.2 it is an X 10- 1 Ω cm.
産業上の利用可能性 Industrial applicability
対向ターゲット式スパッタリング法は、 レーザーアブレーシヨン法と同様に、 アモルファス膜に有効な、 他の元素の添加による特性改善が容易に実現できる。 通常のスパッタリング法ではブラズマが成膜中の膜に接しないようにしてァニ ール的な効果が作用しないようにすることによって、 良質なァモルファス膜を得 ることができるが、 対向ターゲット式スパッタリング法ではプラズマフリーであ るために、 アモルファス膜が容易に得られる。 したがって、 積層化も容易である 。 大面積化にも適し、 工業的応用が容易である。 Similar to the laser ablation method, the facing target sputtering method can easily realize the property improvement by adding another element which is effective for the amorphous film. In a normal sputtering method, a high-quality amorphous film can be obtained by preventing the plasma from coming into contact with the film being formed, thereby preventing the effect of the anneal from acting. Since the method is plasma-free, an amorphous film can be easily obtained. Therefore, lamination is easy. Suitable for large area, easy for industrial application.
また、 アモルファス鉄シリサイドは、 磁性元素を添加することによる磁性半導 体化や、 水素化によるキャリア濃度の調整が可能である。 さらに、 In addition, amorphous iron silicide has a magnetic semiconductivity by adding a magnetic element. It is possible to adjust the carrier concentration by solidification and hydrogenation. further,
鉄シリサイドは、 室温で成長する為に、 基板加熱機構が不要である。 Iron silicide does not require a substrate heating mechanism because it grows at room temperature.
本発明の半導体特性を示すアモルファス鉄シリサイド膜は、 太陽電池素子や通 信用発受光素子へ応用できる。 The amorphous iron silicide film exhibiting the semiconductor characteristics of the present invention can be applied to a solar cell element and a communication light emitting / receiving element.
Claims
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| CA002470332A CA2470332A1 (en) | 2001-12-19 | 2002-09-10 | Amorphous iron-silicide film exhibiting semiconductor characteristics and method of preparing same |
| US10/499,091 US20050155675A1 (en) | 2001-12-19 | 2002-09-10 | Amorphous ferrosilicide film exhibiting semiconductor characteristics and method of for producing the same |
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| JP2001386824A JP4009102B2 (en) | 2001-12-19 | 2001-12-19 | Amorphous iron silicide film exhibiting semiconductor characteristics and fabrication method thereof |
| JP2001-386824 | 2001-12-19 |
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| JP2004265889A (en) * | 2003-01-16 | 2004-09-24 | Tdk Corp | Photoelectric conversion element, photoelectric conversion device, and iron silicide film |
| RU2458181C2 (en) * | 2010-08-17 | 2012-08-10 | Государственное образовательное учреждение высшего профессионального образования Московский государственный институт радиотехники, электроники и автоматики (Технический университет) (МИРЭА) | Method for obtaining ferromagnetic film from silicide nanoclusters on surface of silicone substrate |
| US9612521B2 (en) * | 2013-03-12 | 2017-04-04 | Applied Materials, Inc. | Amorphous layer extreme ultraviolet lithography blank, and manufacturing and lithography systems therefor |
| US9354508B2 (en) | 2013-03-12 | 2016-05-31 | Applied Materials, Inc. | Planarized extreme ultraviolet lithography blank, and manufacturing and lithography systems therefor |
| US20140272684A1 (en) | 2013-03-12 | 2014-09-18 | Applied Materials, Inc. | Extreme ultraviolet lithography mask blank manufacturing system and method of operation therefor |
| RU2607288C2 (en) * | 2015-03-25 | 2017-01-10 | Федеральное государственное бюджетное учреждение науки Институт сильноточной электроники Сибирского отделения Российской академии наук (ИСЭ СО РАН) | Method for gas-discharge sputtering of films |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4539054A (en) * | 1982-04-30 | 1985-09-03 | Futaba Denshi Kogyo K.K. | Amorphous film of transition element-silicon compound |
| JPS6447850A (en) * | 1987-08-14 | 1989-02-22 | Mitsubishi Heavy Ind Ltd | Manufacture of thermoelement |
| JPH1027927A (en) * | 1996-07-09 | 1998-01-27 | Hiroshi Ko | Amorphous thermoelectric device |
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| JP3348924B2 (en) * | 1993-08-04 | 2002-11-20 | 株式会社テクノバ | Thermoelectric semiconductor materials |
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2001
- 2001-12-19 JP JP2001386824A patent/JP4009102B2/en not_active Expired - Fee Related
-
2002
- 2002-09-10 US US10/499,091 patent/US20050155675A1/en not_active Abandoned
- 2002-09-10 WO PCT/JP2002/009242 patent/WO2003052159A1/en not_active Ceased
- 2002-09-10 CA CA002470332A patent/CA2470332A1/en not_active Abandoned
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4539054A (en) * | 1982-04-30 | 1985-09-03 | Futaba Denshi Kogyo K.K. | Amorphous film of transition element-silicon compound |
| JPS6447850A (en) * | 1987-08-14 | 1989-02-22 | Mitsubishi Heavy Ind Ltd | Manufacture of thermoelement |
| JPH1027927A (en) * | 1996-07-09 | 1998-01-27 | Hiroshi Ko | Amorphous thermoelectric device |
Non-Patent Citations (1)
| Title |
|---|
| Edited by Masao DOYAMA et al., "Zairyo Technology 9, Zairyo no Process Gijutsu", ÄIÜ Shohan, University of Tokyo Press, 30 November 1987, pages 135 to 136 * |
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| CA2470332A1 (en) | 2003-06-26 |
| JP4009102B2 (en) | 2007-11-14 |
| US20050155675A1 (en) | 2005-07-21 |
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