JP4388294B2 - Heat treatment method for single crystal substrate - Google Patents
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- JP4388294B2 JP4388294B2 JP2003077151A JP2003077151A JP4388294B2 JP 4388294 B2 JP4388294 B2 JP 4388294B2 JP 2003077151 A JP2003077151 A JP 2003077151A JP 2003077151 A JP2003077151 A JP 2003077151A JP 4388294 B2 JP4388294 B2 JP 4388294B2
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- single crystal
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Description
【0001】
【発明の属する技術分野】
本発明は、誘電体、磁性体、高温超電導体などの薄膜成長用基板や光触媒材料の発現機構解明のための材料などに適用される単結晶基板の熱処理方法に関するものである。
【0002】
【従来の技術】
良質なエピタキシャル膜の作製には、単結晶基板表面の原子レベルの平坦性が大きく影響されることは知られている。これまで、SrTiO3単結晶基板やサファイア単結晶基板については、極めて高い平坦度が得られる処理技術が開発され、その処理技術が例えば特許第3252052号特許公報、特許第3015261号特許公報及び特許第3244966号特許公報などにおいて提案されており、現在は超平坦化技術が確立されているのが実情である。
【0003】
【発明が解決しようとする課題】
一方、TiO2単結晶については、光触媒の発現機構の解明のために、また薄膜電子ディバイス応用のために、多くの研究が行われてきた。
しかしながら、発明者の知る限りではTiO2単結晶基板の表面の原子レベル制御についてはこれまで系統的に研究された例は見当たらない。
本願発明の目的は、TiO2ルチル単結晶基板(以下「ルチル単結晶基板」と略称する。)の表面を原子レベルでの高い平坦化を可能にすることにある。
【0004】
【課題を解決するための手段】
本発明において、選択した面方位のルチル単結晶基板を大気下約300°C〜約1,100°Cの加熱温度で電気炉などの加熱装置を用いて所定時間焼成して、上記ルチル単結晶基板の表面に約0.22nm〜約0.46nmの高さ原子ステップ及びテラス構造を得るようにする方法である。
熱処理の対象となる上記ルチル単結晶基板はその面方位が選択される。選択される面方位は、所望の高さの原子ステップ及びテラス構造を制御できる面方位か又はルチル単結晶基板上に成長させる異種物質の結晶格子に適合する格子定数を有する面方位である。面方位は、(110),(100),(001),(111)及び(101)の中から選択され、選択の範囲は最小で少なくとも1つ、最大ですべての面方位である。
加熱温度は約300°C〜約1,100°Cの範囲が望ましい。約300°Cより低温になると、上記ルチル単結晶基板の表面に所望のステップが得にくく、また約1,100°Cを越えて高温になると、ステップの高さが不均一となって高平坦性を有する基板が得にくくなるおそれがある。
加熱時間として上記加熱温度の範囲においては1時間程度で良いが、1時間未満又は1時間を越えても良い。もっとも、加熱時間については、加熱温度との関係で相対的に決定され、高温の場合には短時間の加熱処理が可能であり、また時間をかけることにより低温でも処理が可能である。
ルチル単結晶基板を焼成する段階において、前処理として基板表面を洗浄剤を用いて洗浄しておく場合と、洗浄することなく焼成する場合の双方があるが、前処理することは超平坦面であるテラス構造を得やすくするためには望ましい。前処理工程である洗浄工程では、洗浄剤例えば有機溶剤で洗浄し、ついで例えば酸性溶剤で洗浄すると、上記効果が高められる。有機溶剤としてはアセトン、エタノールなどが用いられ、また酸性溶剤としては塩酸、硝酸、硫酸、リン酸、フッ酸などが使用される。
【0005】
【作用】
選択した面方位(110),(100),(001),(111)又は(101)を持つ表面のルチル単結晶基板を所定温度で所定時間焼成することにより、上記ルチル単結晶基板表面には所望の高さの原子レベルのステップを有する超平坦面であるテラス構造が形成される。
【0006】
【実施例】
(実施例1)
面方位(110)であるルチル単結晶基板の表面をまず有機溶剤によって洗浄し、ついで酸性溶剤で洗浄処理した後、研磨仕上げされたルチル単結晶基板を電気炉内において大気中400°Cの加熱温度で1時間焼成した。
同様に、上記ルチル単結晶基板に対して異なった加熱温度すなわち、500°C、600°C、700°C、800°C、900°C及び1,000°Cのそれぞれの加熱温度でも1時間焼成した。
このように、上記の面方位で、かつ下限を400°C、上限を1,000°Cとして加熱温度を順次100°Cそれぞれ上昇させた7ケースについて、個別に焼成後、原子間力顕微鏡でルチル単結晶基板の表面を観察したところ、7ケースのいずれの加熱温度の場合でもその表面には高さ0.32nmのステップ及びテラス構造が形成されていた。テラス幅はルチル単結晶基板の表面の結晶軸精度すなわち面方位(110)からのずれ幅に依存して相対的に変化した。
この観察では、原子間力顕微鏡(AFM)としてSII社製のSPA300/SPI3800を使用した。観察範囲は1×1μm2である。
図1(A)及び図1(B)は、加熱温度が900°Cにおける焼成後の上記ルチル単結晶基板における配向面(110)のAFM像の斜視図及び同断面図である。ルチル単結晶基板の表面には高さ0.32nmのステップ2及びテラス幅が100nmを越えるテラス1を有する構造が形成されていた。
【0007】
(実施例2)
面方位(100)であるルチル単結晶基板の表面をまず有機溶剤によって洗浄し、ついで酸性溶剤で洗浄処理した後、研磨仕上げされたルチル単結晶基板を電気炉内において大気中400°Cの加熱温度で1時間焼成した。
同様に、上記ルチル単結晶基板に対して異なった加熱温度すなわち、500°C、600°C、700°C、800°C、900°C、1,000°C及び1,100°Cで個別毎に1時間焼成した。
このように、上記の面方位で、かつ下限を400°C、上限を1,100°Cとして加熱温度を順次100°Cそれぞれ上昇させた8ケースについて、焼成後、上記原子間力顕微鏡でルチル単結晶基板の表面を観察したところ、いずれの加熱温度の場合でもその表面には高さ0.46nmのステップ及びテラス構造が形成されていた。テラス幅はルチル単結晶基板の表面の結晶軸精度すなわち面方位(100)からのずれ幅に依存して相対的に変化した。観察範囲は1×1μm2である。
図2(A)及び図2(B)は、加熱温度が800°Cにおける焼成後の上記ルチル単結晶基板における配向面(100)のAFM像の斜視図及び同断面図である。ルチル単結晶基板の表面には高さ0.46nmのステップ2及びテラス幅が100nmを越えるテラス1を有する構造が形成されていた。
【0008】
(実施例3)
選択する面方位及び加熱温度を除いて、実施例1に示す条件と同一の条件でルチル単結晶基板の表面を熱処理した。
本例の面方位は(001)、加熱温度は800°C及び900°Cの2ケースであった。
焼成後のルチル単結晶基板の表面を上記原子間力顕微鏡で観察したところ、いずれの加熱温度の場合でもその表面には高さ0.30nmのステップ及びテラス構造が形成されていた。テラス幅はルチル単結晶基板の表面の結晶軸精度すなわち面方位(001)からのずれ幅に依存して相対的に変化した。観察範囲は1×1μm2である。
図3(A)及び図3(B)は加熱温度が900°Cにおける焼成後の上記ルチル単結晶基板における配向面(001)のAFM像の斜視図及び同断面図である。
ルチル単結晶基板の表面には高さ0.30nmのステップ2及びテラス幅が100nmを越えるテラス1を有する構造が形成されていた。
【0009】
(実施例4)
選択する面方位及び加熱温度を除いて、実施例1に示す条件と同一の条件でルチル単結晶基板の表面を熱処理した。
本例の面方位は(111)、加熱温度は500°C、600°C、700°C、800°C及び900°Cの5ケースであった。
焼成後のルチル単結晶基板の表面を上記原子間力顕微鏡で観察したところ、いずれのケース(加熱温度)でも上記ルチル単結晶基板の表面には高さ0.22nmのステップ及びテラス構造が形成されていた。テラス幅はルチル単結晶基板の表面の結晶軸精度すなわち面方位(111)からのずれ幅に依存して相対的に変化した。観察範囲は1×1μm2である。
図4(A)及び図4(B)は加熱温度が800°Cにおける焼成後の上記ルチル単結晶基板における配向面(111)のAFM像の斜視図及び同断面図である。ルチル単結晶基板の表面には高さ0.22nmのステップ2及びテラス幅が80nmを越えるテラス1を有する構造が形成されていた。
【0010】
(実施例5)
選択する面方位及び加熱温度を除いて、実施例1に示す条件と同一の条件でルチル単結晶基板の表面を熱処理した。
本例の面方位は(101)、加熱温度は600°C、700°C及び800°Cの3ケースであった。
焼成後のルチル単結晶基板の表面を上記原子間力顕微鏡で観察したところ、いずれのケース(加熱温度)においても、ルチル単結晶基板の表面には高さ0.25nmのステップ及びテラス構造が形成されていた。テラス幅はルチル単結晶基板の表面の結晶軸精度すなわち面方位(101)からのずれ幅に依存して相対的に変化した。観察範囲は1×1μm2である。
図5(A)及び図5(B)は加熱温度が800°Cにおける焼成後の上記ルチル単結晶基板における配向面(101)のAFM像の斜視図及び同断面図である。ルチル単結晶基板の表面には高さ0.25nmのステップ2及びテラス幅が50nmを越えるテラス1を有する構造が形成されていた。
【0011】
【発明の効果】
本発明によれば、ルチル単結晶基板の表面を原子レベルでの平坦化が可能となるから、光触媒の発現機構の解明用材料に応用でき、また性能の良い薄膜電子ディバイスに適用することができる。
【図面の簡単な説明】
【図1】(A)及び(B)はルチル単結晶基板における配向面(110)のAFM像の斜視図及び同断面図である。
【図2】(A)及び(B)はルチル単結晶基板における配向面(100)のAFM像の斜視図及び同断面図である。
【図3】(A)及び(B)はルチル単結晶基板における配向面(001)のAFM像の斜視図及び同断面図である。
【図4】(A)及び(B)はルチル単結晶基板における配向面(111)のAFM像の斜視図及び同断面図である。
【図5】(A)及び(B)はルチル単結晶基板における配向面(101)のAFM像の斜視図及び同断面図である。
【符号の説明】
1 テラス
2 ステップ[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a heat treatment method for a single crystal substrate applied to a thin film growth substrate such as a dielectric material, a magnetic material, and a high-temperature superconductor, or a material for elucidating the expression mechanism of a photocatalytic material.
[0002]
[Prior art]
It is known that the flatness at the atomic level on the surface of a single crystal substrate is greatly affected in the production of a high-quality epitaxial film. Until now, for SrTiO 3 single crystal substrates and sapphire single crystal substrates, a processing technique capable of obtaining extremely high flatness has been developed. For example, Japanese Patent No. 3252552, Japanese Patent No. 3015261, and Patent No. No. 3244966 is proposed, and the current situation is that an ultra-flattening technique has been established.
[0003]
[Problems to be solved by the invention]
On the other hand, with regard to the TiO 2 single crystal, many studies have been conducted for elucidation of the mechanism of the photocatalyst and for the application of thin film electronic devices.
However, as far as the inventor knows, there has been no systematic study so far on the atomic level control of the surface of the TiO 2 single crystal substrate.
An object of the present invention is to enable the surface of a TiO 2 rutile single crystal substrate (hereinafter abbreviated as “rutile single crystal substrate”) to be highly planarized at an atomic level.
[0004]
[Means for Solving the Problems]
In the present invention, the rutile single crystal substrate having a selected plane orientation is baked for a predetermined time using a heating device such as an electric furnace at a heating temperature of about 300 ° C. to about 1,100 ° C. in the atmosphere. A method of obtaining a height atomic step and terrace structure of about 0.22 nm to about 0.46 nm on the surface of the substrate.
The plane orientation of the rutile single crystal substrate to be heat-treated is selected. The selected plane orientation is a plane orientation that can control the atomic step and terrace structure at a desired height, or a plane orientation that has a lattice constant that matches a crystal lattice of a different material grown on a rutile single crystal substrate. The plane orientation is selected from among (110), (100), (001), (111) and (101), and the range of selection is at least one and at most all plane orientations.
The heating temperature is preferably in the range of about 300 ° C to about 1,100 ° C. When the temperature is lower than about 300 ° C, it is difficult to obtain a desired step on the surface of the rutile single crystal substrate, and when the temperature is higher than about 1,100 ° C, the step height becomes uneven and the surface is highly flat. It may be difficult to obtain a substrate having the property.
The heating time may be about 1 hour in the above heating temperature range, but may be less than 1 hour or more than 1 hour. However, the heating time is relatively determined in relation to the heating temperature, and when the temperature is high, the heat treatment can be performed for a short time, and the treatment can be performed at a low temperature by taking time.
In the stage of firing the rutile single crystal substrate, there are both a case where the substrate surface is washed with a cleaning agent as a pretreatment and a case where the substrate is baked without washing. It is desirable to make it easier to obtain a certain terrace structure. In the cleaning step, which is a pretreatment step, the above effect is enhanced by cleaning with a cleaning agent such as an organic solvent and then with an acidic solvent. As the organic solvent, acetone, ethanol or the like is used, and as the acidic solvent, hydrochloric acid, nitric acid, sulfuric acid, phosphoric acid, hydrofluoric acid or the like is used.
[0005]
[Action]
By firing the rutile single crystal substrate having the selected plane orientation (110), (100), (001), (111) or (101) at a predetermined temperature for a predetermined time, the surface of the rutile single crystal substrate is A terrace structure is formed that is an ultra-flat surface with atomic level steps of the desired height.
[0006]
【Example】
Example 1
The surface of the rutile single crystal substrate having the plane orientation (110) is first cleaned with an organic solvent, then cleaned with an acidic solvent, and then the polished rutile single crystal substrate is heated to 400 ° C. in the atmosphere in an electric furnace. Baked for 1 hour at temperature.
Similarly, different heating temperatures for the rutile single crystal substrate, i.e., 500 ° C, 600 ° C, 700 ° C, 800 ° C, 900 ° C, and 1,000 ° C, are also used for one hour. Baked.
As described above, with respect to 7 cases having the above-mentioned plane orientation, the lower limit set to 400 ° C., the upper limit set to 1,000 ° C., and the heating temperature sequentially increased to 100 ° C., individually fired and then subjected to an atomic force microscope. When the surface of the rutile single crystal substrate was observed, a step and terrace structure having a height of 0.32 nm was formed on the surface at any heating temperature in the seven cases. The terrace width changed relatively depending on the crystal axis accuracy of the surface of the rutile single crystal substrate, that is, the deviation from the plane orientation (110).
In this observation, SPA300 / SPI3800 manufactured by SII was used as an atomic force microscope (AFM). The observation range is 1 × 1 μm 2 .
1A and 1B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (110) in the rutile single crystal substrate after baking at a heating temperature of 900 ° C. On the surface of the rutile single crystal substrate, a
[0007]
(Example 2)
The surface of the rutile single crystal substrate having a plane orientation (100) is first cleaned with an organic solvent, then cleaned with an acidic solvent, and then the polished rutile single crystal substrate is heated to 400 ° C. in the atmosphere in an electric furnace. Baked for 1 hour at temperature.
Similarly, different heating temperatures for the rutile single crystal substrate, namely, 500 ° C, 600 ° C, 700 ° C, 800 ° C, 900 ° C, 1,000 ° C, and 1,100 ° C, respectively. Each was baked for 1 hour.
As described above, 8 cases having the above-mentioned plane orientation, the lower limit set to 400 ° C., the upper limit set to 1,100 ° C., and the heating temperature sequentially increased to 100 ° C. were each fired and then subjected to rutile using the atomic force microscope. When the surface of the single crystal substrate was observed, a step and terrace structure having a height of 0.46 nm was formed on the surface at any heating temperature. The terrace width relatively changed depending on the crystal axis accuracy of the surface of the rutile single crystal substrate, that is, the deviation from the plane orientation (100). The observation range is 1 × 1 μm 2 .
2A and 2B are a perspective view and a cross-sectional view of an AFM image of the orientation plane (100) in the rutile single crystal substrate after baking at a heating temperature of 800 ° C. On the surface of the rutile single crystal substrate, a
[0008]
(Example 3)
The surface of the rutile single crystal substrate was heat-treated under the same conditions as those shown in Example 1 except for the selected plane orientation and heating temperature.
In this example, the plane orientation was (001), and the heating temperature was two cases of 800 ° C and 900 ° C.
When the surface of the fired rutile single crystal substrate was observed with the atomic force microscope, a step and terrace structure having a height of 0.30 nm were formed on the surface at any heating temperature. The terrace width relatively changed depending on the crystal axis accuracy of the surface of the rutile single crystal substrate, that is, the deviation from the plane orientation (001). The observation range is 1 × 1 μm 2 .
FIGS. 3A and 3B are a perspective view and a cross-sectional view of an AFM image of the orientation plane (001) in the rutile single crystal substrate after baking at a heating temperature of 900 ° C. FIG.
On the surface of the rutile single crystal substrate, a structure having a
[0009]
(Example 4)
The surface of the rutile single crystal substrate was heat-treated under the same conditions as those shown in Example 1 except for the selected plane orientation and heating temperature.
In this example, the plane orientation was (111), and the heating temperature was 500 ° C, 600 ° C, 700 ° C, 800 ° C and 900 ° C.
When the surface of the rutile single crystal substrate after firing was observed with the atomic force microscope, a step and terrace structure having a height of 0.22 nm was formed on the surface of the rutile single crystal substrate in any case (heating temperature). It was. The terrace width relatively changed depending on the crystal axis accuracy of the surface of the rutile single crystal substrate, that is, the deviation width from the plane orientation (111). The observation range is 1 × 1 μm 2 .
4A and 4B are a perspective view and a cross-sectional view of an AFM image of the orientation plane (111) in the rutile single crystal substrate after baking at a heating temperature of 800 ° C. On the surface of the rutile single crystal substrate, a
[0010]
(Example 5)
The surface of the rutile single crystal substrate was heat-treated under the same conditions as those shown in Example 1 except for the selected plane orientation and heating temperature.
In this example, the plane orientation was (101), and the heating temperatures were 600 ° C, 700 ° C, and 800 ° C in three cases.
When the surface of the fired rutile single crystal substrate was observed with the atomic force microscope, a step and terrace structure with a height of 0.25 nm was formed on the surface of the rutile single crystal substrate in any case (heating temperature). It had been. The terrace width changed relatively depending on the crystal axis accuracy of the surface of the rutile single crystal substrate, that is, the deviation width from the plane orientation (101). The observation range is 1 × 1 μm 2 .
5A and 5B are a perspective view and a cross-sectional view of an AFM image of the orientation plane (101) in the rutile single crystal substrate after baking at a heating temperature of 800 ° C. On the surface of the rutile single crystal substrate, a
[0011]
【The invention's effect】
According to the present invention, since the surface of a rutile single crystal substrate can be flattened at the atomic level, it can be applied to a material for elucidating the mechanism of expression of a photocatalyst and can be applied to a thin film electronic device having good performance. .
[Brief description of the drawings]
FIGS. 1A and 1B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (110) in a rutile single crystal substrate, respectively.
FIGS. 2A and 2B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (100) in a rutile single crystal substrate, respectively.
3A and 3B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (001) in a rutile single crystal substrate, respectively.
4A and 4B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (111) in a rutile single crystal substrate, respectively.
FIGS. 5A and 5B are a perspective view and a cross-sectional view of an AFM image of an orientation plane (101) in a rutile single crystal substrate, respectively.
[Explanation of symbols]
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| JP6221572B2 (en) * | 2013-09-27 | 2017-11-01 | 株式会社デンソー | Temperature sensor |
| CN107890861B (en) * | 2017-11-30 | 2020-09-29 | 新疆维吾尔自治区产品质量监督检验研究院 | Preparation method of titanium dioxide lamella/graphene composite film with {001} crystal face |
| CN111172596A (en) * | 2020-01-20 | 2020-05-19 | 北京科技大学 | A kind of processing technology of rutile type 110-oriented TiO2 single crystal |
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