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JP4383418B2 - Thin film production apparatus and thin film production method - Google Patents
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JP4383418B2 - Thin film production apparatus and thin film production method - Google Patents

Thin film production apparatus and thin film production method Download PDF

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JP4383418B2
JP4383418B2 JP2006053875A JP2006053875A JP4383418B2 JP 4383418 B2 JP4383418 B2 JP 4383418B2 JP 2006053875 A JP2006053875 A JP 2006053875A JP 2006053875 A JP2006053875 A JP 2006053875A JP 4383418 B2 JP4383418 B2 JP 4383418B2
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thin film
chamber
substrate
etched
precursor
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JP2007231359A (en
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浩一 佐々木
直樹 八幡
仁志 坂本
一雅 笠木
裕 利根川
謙 小椋
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Nagoya University NUC
Canon Anelva Corp
Tokai National Higher Education and Research System NUC
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Canon Anelva Corp
Tokai National Higher Education and Research System NUC
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Description

本発明は、金属成分を成膜する薄膜作製装置及び薄膜作製方法に関し、環境や成膜履歴に拘わらず処理時間を長くすることなく均一な薄膜が作製できるようにしたものである。   The present invention relates to a thin film manufacturing apparatus and a thin film manufacturing method for forming a metal component, and is capable of manufacturing a uniform thin film without increasing the processing time regardless of the environment and the film forming history.

現在、半導体等の製造においては、プラズマCVD(Chemical Vapor Deposition)装置を用いた成膜が知られている。プラズマCVD装置とは、チャンバ内に導入した膜の材料となる有機金属錯体等のガスを、高周波アンテナから入射する高周波によりプラズマ状態にし、プラズマ中の活性な励起原子によって基板表面の化学的な反応を促進して金属薄膜等を成膜する装置である。   Currently, in the manufacture of semiconductors and the like, film formation using a plasma CVD (Chemical Vapor Deposition) apparatus is known. A plasma CVD apparatus is a plasma reaction of a gas such as an organometallic complex that becomes a material of a film introduced into a chamber by a high frequency incident from a high frequency antenna, and a chemical reaction on the substrate surface by active excited atoms in the plasma. Is a device for forming a metal thin film or the like by promoting the above.

これに対し、本発明者等は、高蒸気圧ハロゲン化物を作る金属成分であって、成膜を望む金属成分からなる被エッチング部材をチャンバに設置し、ハロゲンガスをプラズマ化して被エッチング部材をハロゲンのラジカルによりエッチングすることで金属成分のハロゲン化物である前駆体を生成させるとともに、前駆体の金属成分のみを基板上に成膜するプラズマCVD装置(以下、新方式のプラズマCVD装置という)および成膜方法を開発した(例えば、下記、特許文献1参照)。   On the other hand, the present inventors installed a member to be etched, which is a metal component for producing a high vapor pressure halide, and made of a metal component desired to be formed in a chamber, and converted the halogen gas into plasma to form the member to be etched. A plasma CVD apparatus (hereinafter referred to as a new type of plasma CVD apparatus) that forms a precursor, which is a halide of a metal component, by etching with a halogen radical and deposits only the metal component of the precursor on a substrate; A film forming method was developed (for example, see Patent Document 1 below).

上記新方式のプラズマCVD装置では、成膜される金属源となる被エッチング部材の温度に対して基板の温度が低くなるように制御して基板に当該金属膜を成膜している。例えば、被エッチング部材の金属をM、ハロゲンガスをCl2とした場合、被エッチング部材を高温(例えば300℃〜700℃)に、また基板を低温(例えば200℃程度)に制御することにより、前記基板にM薄膜を形成することができる。これは、次のような反応によるものと考えられる。 In the above-described plasma CVD apparatus of the new type, the metal film is formed on the substrate by controlling the temperature of the substrate to be lower than the temperature of the member to be etched which is a metal source to be formed. For example, when the metal of the member to be etched is M and the halogen gas is Cl 2 , the member to be etched is controlled to a high temperature (for example, 300 ° C. to 700 ° C.) and the substrate is controlled to a low temperature (for example, about 200 ° C.) An M thin film can be formed on the substrate. This is thought to be due to the following reaction.

(1)プラズマの解離反応;Cl2→2Cl*
(2)エッチング反応;M+Cl*→MCl(g)
(3)基板への吸着反応;MCl(g)→MCl(ad)
(4)成膜反応;MCl(ad)+Cl* →M+Cl2
ここで、Cl*はClのラジカルであることを、(g)はガス状態であることを、(ad)は吸着状態であることをそれぞれ表している。
(1) Plasma dissociation reaction; Cl 2 → 2Cl *
(2) Etching reaction; M + Cl * → MCl (g)
(3) Adsorption reaction to the substrate; MC1 (g) → MC1 (ad)
(4) Film formation reaction; MCl (ad) + Cl * → M + Cl 2
Here, Cl * represents a Cl radical, (g) represents a gas state, and (ad) represents an adsorption state.

前述した新方式のCVD装置においては、MClとCl*との割合を適正に保つことで、成膜反応が適切に行われる。即ち、成膜条件として、Cl2ガスの流量、圧力、パワー、基板及び被エッチング部材の温度、基板と被エッチング部材との距離等を適正に設定することで、MClとCl*との割合をほぼ等しく制御することができ、成膜速度を低下させることなく、しかも、基板に対してCl*によるエッチング過多が生じることなくMが析出される。 In the above-described new type CVD apparatus, the film forming reaction is appropriately performed by keeping the ratio of MCl and Cl * appropriately. That is, as the film formation conditions, the ratio of MCl and Cl * is set by appropriately setting the flow rate of Cl 2 gas, pressure, power, the temperature of the substrate and the member to be etched, the distance between the substrate and the member to be etched, and the like. It can be controlled almost equally, and M is deposited without reducing the deposition rate and without causing excessive etching by Cl * on the substrate.

上述した新方式のCVD装置では、膜厚の均一性(例えば、平均膜厚に対し±3%以下)に優れた成膜を行うために、機器や環境に合わせた成膜条件(プロセス条件)や装置条件の設定が行われている。この場合、周囲の温度や成膜履歴などの影響を受けて条件が変化するため、成膜結果に応じて、プロセス条件や装置条件を補正することで周囲の温度や成膜履歴などの影響を最小限に抑制し、膜厚の均一性を保っている。   In the above-described new type CVD apparatus, in order to perform film formation with excellent film thickness uniformity (for example, ± 3% or less of the average film thickness), film formation conditions (process conditions) suited to the equipment and environment. And device conditions are set. In this case, the conditions change due to the influence of the ambient temperature and film formation history, etc., so that the influence of the ambient temperature and film formation history is affected by correcting the process conditions and equipment conditions according to the film formation result. Minimized to keep the film thickness uniform.

しかしながら、成膜結果に応じて周囲の環境に合わせたプロセス条件の調整が必要になるため、周辺環境の変化に対する追従が遅くなり、また、調整にかかわる時間が増大してしまう。このため、作業時間の短縮や歩留まりの向上には限界があるのが実情であった。   However, since it is necessary to adjust the process conditions according to the surrounding environment according to the film formation result, the follow-up to the change in the surrounding environment is delayed, and the time required for the adjustment increases. For this reason, the actual situation is that there is a limit to shortening the working time and improving the yield.

特開2003−147534号公報JP 2003-147534 A

本発明は上記状況に鑑みてなされたもので、周囲の環境や成膜履歴に拘わらず処理時間を長くすることなく均一な薄膜が作製できるようにした薄膜作製装置及び薄膜作製方法を提供することを目的とする。   The present invention has been made in view of the above situation, and provides a thin film production apparatus and a thin film production method capable of producing a uniform thin film without increasing the processing time regardless of the surrounding environment and film formation history. With the goal.

上記目的を達成するための請求項1に係る本発明の薄膜作製装置は、基板が収容されるチャンバと、基板が対向する位置におけるチャンバに設けられる金属製の被エッチング部材と、チャンバの内部にハロゲンを含有する作用ガスを供給する作用ガス供給手段と、チャンバの内部をプラズマ化し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成するプラズマ発生手段とを備え、基板側の温度を被エッチング部材の温度よりも低くして前記前駆体中の金属を基板に成膜させる成膜装置において、チャンバ内に帯状のレーザー光を照射してチャンバ内の前記前駆体を発光させるレーザー照射手段と、レーザー光による前記前駆体の発光分布をモニタして画像処理する画像処理手段と、膜の作製条件に応じた前記前駆体の発光分布が予め記憶されており、該記憶された発光分布に基づいて、前記画像処理手段で画像処理した発光分布が均一になるように薄膜の作製条件を変更する制御手段とを備えたことを特徴とする。また、請求項2に係る本発明の薄膜作製装置は、基板が収容されるチャンバと、基板が対向する位置におけるチャンバに設けられる金属製の被エッチング部材と、チャンバの内部にハロゲンを含有する作用ガスを供給する作用ガス供給手段と、チャンバの内部をプラズマ化し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成するプラズマ発生手段とを備え、基板側の温度を被エッチング部材の温度よりも低くして前記前駆体中の金属を基板に成膜させる成膜装置において、チャンバ内に帯状のレーザー光を照射して、前記前駆体が前記ハロゲンラジカルで還元されることでチャンバ内に生成するガス状態の前記金属の原子を発光させるレーザー照射手段と、レーザー光による前記金属の原子の発光分布をモニタして画像処理する画像処理手段と、薄膜の作製条件に応じた前記金属の原子の発光分布が予め記憶されており、該記憶された発光分布に基づいて、前記画像処理手段で画像処理した発光分布が均一になるように薄膜の作製条件を変更する制御手段とを備えたことを特徴とする。 In order to achieve the above object, a thin film manufacturing apparatus according to a first aspect of the present invention includes a chamber in which a substrate is accommodated, a metal member to be etched provided in a chamber at a position where the substrate faces, and an interior of the chamber. Working gas supply means for supplying a working gas containing halogen and plasma inside the chamber, generating working gas plasma to generate halogen radicals, and etching the member to be etched with the halogen radicals. metal in the precursor is a plasma generating means for generating a precursor which is a metal halide gas state consisting of metals and halogens, the temperature of the substrate side to be lower than the temperature of the etched member included in the deposition apparatus for depositing on the substrate, said precursor in the chamber by irradiating a belt-like laser beam into the chamber A laser irradiation means to emit light, and an image processing means for image processing by monitoring the light emission distribution of the precursor by a laser beam, and light emission distribution of the precursor in accordance with the production conditions of the thin film is stored in advance, based on the emission distribution which is the storage, characterized in that a control means for changing the image processing light emission distribution uniform fabrication conditions of I ing urchin film by the image processing means. According to a second aspect of the present invention, there is provided a thin film manufacturing apparatus of the present invention, a chamber in which a substrate is accommodated, a metal member to be etched provided in a chamber facing the substrate, and an action containing halogen inside the chamber. Working gas supply means for supplying a gas, and plasma inside the chamber, generating a working gas plasma to generate halogen radicals, and etching the member to be etched with the halogen radicals, and the metal and halogen contained in the member to be etched And a plasma generating means for generating a precursor which is a metal halide in a gas state, and the temperature of the substrate is made lower than the temperature of the member to be etched to form the metal in the precursor on the substrate. In the film forming apparatus, the precursor is reduced by the halogen radicals by irradiating a chamber with a laser beam. The laser irradiation means for emitting the metal atoms in the gas state generated in the chamber, the image processing means for monitoring the light emission distribution of the metal atoms by the laser light and image processing, and the thin film production conditions The light emission distribution of the corresponding metal atoms is stored in advance, and control for changing the thin film production conditions based on the stored light emission distribution so that the light emission distribution image-processed by the image processing means is uniform. Means.

請求項1及び2に係る本発明では、前駆体又は金属の原子(解離物)の発光分布状況に基づいて薄膜の作製条件を適宜変更し、基板の上部の解離物が均一になる発光状況にすることで、基板毎に解離物の密度が均一になり、周囲の温度や成膜履歴などの影響を最小限に抑制して膜厚の均一性を保つことができる。 In the present invention according to claims 1 and 2 , the thin film preparation conditions are appropriately changed based on the light emission distribution status of the precursor or metal atoms (dissociated products) , so that the dissociated material on the upper part of the substrate becomes uniform. By doing so, the density of the dissociated material becomes uniform for each substrate, and the influence of the ambient temperature, film formation history, etc. can be suppressed to the minimum, and the film thickness uniformity can be maintained.

そして、請求項に係る本発明の薄膜作製装置は、請求項1又は2に記載の薄膜作製装置において、前記レーザー照射手段で照射される帯状のレーザー光は、基板の中心を通り基板を横断する帯状であることを特徴とする。 The thin film production apparatus of the present invention according to claim 3 is the thin film production apparatus according to claim 1 or 2 , wherein the laser beam irradiated by the laser irradiation means crosses the substrate through the center of the substrate . It is characterized by having a strip shape.

請求項に係る本発明では、基板の中心上の解離物の分布に基づいて薄膜の作製条件を変更することができる。 According to the third aspect of the present invention, the thin film production conditions can be changed based on the distribution of dissociated substances on the center of the substrate.

また、請求項に係る本発明の薄膜作製装置は、請求項1〜3のいずれか一項に記載の薄膜作製装置において、前記画像処理手段は、レーザー光の面を撮影するカメラと、カメラの画像を発光強度の分布を表す二次元画像に処理する処理手段とを備えたことを特徴とする。 Moreover, the thin film manufacturing apparatus of this invention which concerns on Claim 4 is a thin film manufacturing apparatus as described in any one of Claims 1-3. The said image processing means is a camera which image | photographs the surface of a laser beam, and a camera. And a processing means for processing the image into a two-dimensional image representing the distribution of light emission intensity.

請求項に係る本発明では、発光強度の分布を二次元画像に表して薄膜の作製条件を変更することができる。 In the present invention according to claim 4 , it is possible to change the production conditions of the thin film by representing the distribution of the emission intensity in a two-dimensional image.

また、請求項に係る本発明の薄膜作製装置は、請求項1〜4のいずれか一項に記載の薄膜作製装置において、前記作用ガス供給手段には流量を制御する流量調整手段が備えられると共に、チャンバを所定の真空圧力にする真空手段が備えられ、プラズマ発生手段はRF電源により電力が供給されてチャンバの内部をプラズマ化するものであり、前記薄膜の作製条件は、真空手段の調整によるチャンバ内の圧力、流量調整手段の調整による作用ガスの流量、RF電源のRFパワーのうち少なくとも一つを含むことを特徴とする。 Moreover, the thin film manufacturing apparatus of this invention which concerns on Claim 5 is a thin film manufacturing apparatus as described in any one of Claims 1-4. WHEREIN: The flow volume adjustment means which controls flow volume is provided in the said working gas supply means. together, provided with vacuum means for the chamber at a predetermined vacuum pressure, a plasma generating means serves to plasma inside the chamber is supplied with electric power by the RF power source, production conditions of the thin film, the adjustment of the vacuum means At least one of the pressure in the chamber according to the above, the flow rate of the working gas by adjusting the flow rate adjusting means, and the RF power of the RF power source.

請求項に係る本発明では、チャンバ内の圧力、作用ガスの流量、RFパワーのうち少なくとも一つを変更して解離物の密度を均一にすることができる。 In the present invention according to claim 5 , the density of the dissociated material can be made uniform by changing at least one of the pressure in the chamber, the flow rate of the working gas, and the RF power.

また、請求項に係る本発明の薄膜作製装置は、請求項1〜5のいずれか一項に記載の薄膜作製装置において、前記ハロゲンを含有する作用ガスはハロゲンとして塩素を含有する作用ガスであることを特徴とする。 Moreover, the thin film production apparatus of the present invention according to claim 6 is the thin film production apparatus according to any one of claims 1 to 5 , wherein the working gas containing halogen is a working gas containing chlorine as a halogen. It is characterized by being.

請求項に係る本発明では、安価な塩素を含有する作用ガスを用いて薄膜を作製することができる。 In the present invention according to claim 6 , it is possible to produce a thin film using an inexpensive working gas containing chlorine.

上記目的を達成するための請求項に係る本発明の薄膜作製方法は、金属製の被エッチング部材が備えられたチャンバ内にハロゲンを含有する作用ガスを供給し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成し、基板側の温度を被エッチング部材の温度よりも低くすることにより前記前駆体の金属を基板に成膜させる薄膜作製方法においてチャンバ内に帯状のレーザー光を照射してチャンバ内の前記前駆体を発光させて、前記前駆体の発光分布を検出し、薄膜の作製条件に応じた前記前駆体の既知の発光分布に基づいて、前記検出した発光分布が均一になるように薄膜の作製条件を変更して成膜を行うことを特徴とする。また、請求項8に係る本発明の薄膜作製方法は、金属製の被エッチング部材が備えられたチャンバ内にハロゲンを含有する作用ガスを供給し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成し、基板側の温度を被エッチング部材の温度よりも低くすることにより前記前駆体中の金属を基板に成膜させる薄膜作製方法において、チャンバ内に帯状のレーザー光を照射して、前記前駆体が前記ハロゲンラジカルで還元されることでチャンバ内に生成するガス状態の前記金属の原子を発光させて、前記金属の原子の発光分布を検出し、薄膜の作製条件に応じた前記金属の原子の既知の発光分布に基づいて、前記検出した発光分布が均一になるように薄膜の作製条件を変更して成膜を行うことを特徴とする。 In order to achieve the above object, the thin film manufacturing method of the present invention according to claim 7 is to supply a working gas containing halogen into a chamber provided with a metal member to be etched to generate a working gas plasma. generates a halogen radical, to form a precursor which is a metal halide gas state consisting of metals and halogens contained in the etched member by etching the etched member with a halogen radical, the temperature of the substrate side in thin-film producing method for forming a metallic in the precursor to the substrate by lower than the temperature of the etched member, and by irradiating a belt-like laser beam is emitted to the precursors in the chamber into the chamber, wherein the detection of luminescence distribution of the precursor, based on the known emission distribution of the precursor in accordance with the production conditions of the film, is uniformly the detected emission distribution And performing film deposition by changing the manufacturing conditions of the thin film so that. In the thin film manufacturing method of the present invention according to claim 8, a halogen-containing working gas is supplied into a chamber provided with a metal member to be etched, and a working gas plasma is generated to generate a halogen radical. Etching the member to be etched with halogen radicals generates a precursor that is a metal halide in a gas state composed of a metal and halogen contained in the member to be etched, and the temperature on the substrate side is made higher than the temperature of the member to be etched. In the thin film manufacturing method in which the metal in the precursor is deposited on the substrate by lowering the thickness, the precursor is reduced by the halogen radicals by irradiating the chamber with a belt-shaped laser beam and generated in the chamber The metal atoms in a gas state to emit light, detect the light emission distribution of the metal atoms, and the gold according to the thin film production conditions Based of the known emission distribution of atoms, and performing film deposition by changing the manufacturing conditions of the thin film so that the detected light emission distribution becomes uniform.

請求項7及び8に係る本発明では、解離物の分布に応じたレーザー誘起蛍光の発光分布状況に基づいて薄膜の作製条件を適宜変更し、基板の上部の解離物が均一になるレーザー誘起蛍光の発光状況にすることで、基板毎に解離物の密度が均一になり、周囲の温度や成膜履歴などの影響を最小限に抑制して膜厚の均一性を保つことができる。 In the present invention according to claims 7 and 8 , the laser-induced fluorescence in which the dissociation material on the upper portion of the substrate becomes uniform by appropriately changing the thin film preparation conditions based on the emission distribution of the laser-induced fluorescence according to the dissociation material distribution. In this light emission state, the density of dissociated substances becomes uniform for each substrate, and the influence of the ambient temperature, film formation history, etc. can be minimized and the film thickness uniformity can be maintained.

そして、請求項に係る本発明の薄膜作製方法は、請求項7又は8に記載の薄膜作製方法において、前記帯状のレーザー光は、基板の中心を通り基板を横断する帯状であることを特徴とする。 The thin film production method of the present invention according to claim 9 is the thin film production method according to claim 7 or 8 , wherein the belt-like laser light is in a belt shape passing through the center of the substrate and crossing the substrate. And

請求項に係る本発明では、基板の中心上の解離物の分布に基づいて薄膜の作製条件を変更することができる。 In the present invention according to claim 9 , the conditions for forming the thin film can be changed based on the distribution of dissociated substances on the center of the substrate.

また、請求項10に係る本発明の薄膜作製方法は、請求項7〜9のいずれか一項に記載の薄膜作製方法において、前記発光分布の検出を、レーザー光の面を撮影した画像を発光強度の分布を表す二次元画像に処理することで行うことを特徴とする。 The thin film production method of the present invention according to claim 10 is the thin film production method according to any one of claims 7 to 9 , wherein the emission distribution is detected by emitting an image obtained by photographing a surface of a laser beam. It is characterized by processing by processing into a two-dimensional image representing the intensity distribution .

請求項10に係る本発明では、レーザー誘起蛍光の強度分布を二次元画像に表して薄膜の作製条件を変更することができる。 In the present invention according to claim 10 , the intensity distribution of the laser-induced fluorescence can be represented in a two-dimensional image to change the thin film production conditions.

また、請求項11に係る本発明の薄膜作製方法は、請求項8〜10のいずれか一項に記載の薄膜作製方法において、前記薄膜の作製条件は、チャンバ内の圧力、作用ガスの流量、プラズマを発生させるためのRFパワーのうち少なくとも一つを含むことを特徴とする。 The thin film production method of the present invention according to claim 11 is the thin film production method according to any one of claims 8 to 10 , wherein the thin film production conditions include pressure in a chamber, flow rate of working gas, It includes at least one of RF power for generating plasma.

請求項11に係る本発明では、チャンバ内の圧力、作用ガスの流量、RFパワーのうち少なくとも一つを変更して解離物の密度を均一にすることができる。 In the present invention according to claim 11 , the density of the dissociated material can be made uniform by changing at least one of the pressure in the chamber, the flow rate of the working gas, and the RF power.

また、請求項12に係る本発明の薄膜作製方法は、請求項7〜11のいずれか一項に記載の薄膜作製方法において、前記ハロゲンを含有する作用ガスはハロゲンとして塩素を含有する作用ガスであることを特徴とする。 The thin film production method of the present invention according to claim 12 is the thin film production method according to any one of claims 7 to 11 , wherein the working gas containing halogen is a working gas containing chlorine as a halogen. It is characterized by being.

請求項12に係る本発明では、安価な塩素を含有する作用ガスを用いて薄膜を作製することができる。 In the present invention according to claim 12 , it is possible to produce a thin film using an inexpensive working gas containing chlorine.

本発明の薄膜作製装置及び薄膜作製方法は、周囲の環境や成膜履歴に拘わらず処理時間を長くすることなく均一な薄膜を作製することができる。   The thin film production apparatus and thin film production method of the present invention can produce a uniform thin film without lengthening the processing time regardless of the surrounding environment and film formation history.

図1には本発明の一実施形態例に係る薄膜作製装置の概略側面、図2には本発明の一実施形態例に係る薄膜作製装置の概略平面を示してある。また、図3から図5には薄膜の作製条件に応じたCu原子の分布状況、図6から図9には薄膜の作製条件に応じたCuCl分子の分布状況を示してある。   FIG. 1 shows a schematic side view of a thin film production apparatus according to an embodiment of the present invention, and FIG. 2 shows a schematic plane of the thin film production apparatus according to an embodiment of the present invention. FIGS. 3 to 5 show the distribution state of Cu atoms in accordance with the thin film production conditions, and FIGS. 6 to 9 show the distribution state of CuCl molecules in accordance with the thin film production conditions.

図1、図2に基づいて本発明の薄膜作製方法を実施するための薄膜作製装置の構成を説明する。本実施形態例では、Clラジカルにより金属であるCu製の被エッチング部材をエッチングし、主に、前駆体を基板に吸着させると共にCl還元により基板上の前駆体をCu成分とする薄膜の作製を例に挙げて説明してある。   The configuration of a thin film production apparatus for carrying out the thin film production method of the present invention will be described with reference to FIGS. In this embodiment, a member to be etched made of Cu, which is a metal, is etched by Cl radicals, and a precursor is mainly adsorbed on the substrate and a thin film having the precursor on the substrate as a Cu component is formed by Cl reduction. It is explained with an example.

図に示すように、円筒状に形成された、例えば、セラミックス製(絶縁材製)のチャンバ1の底部近傍にはサセプタとしての支持台2が設けられ、支持台2には基板3が載置される。支持台2にはヒータ4及び冷媒流通手段5を備えた温度制御手段6が設けられ、支持台2は温度制御手段6により所定温度(例えば、基板3が100℃から300℃に維持される温度)に制御される。   As shown in the figure, a support base 2 as a susceptor is provided in the vicinity of the bottom of a chamber 1 made of, for example, ceramics (made of an insulating material), and a substrate 3 is placed on the support base 2. Is done. The support base 2 is provided with a temperature control means 6 including a heater 4 and a refrigerant flow means 5, and the support base 2 is set to a predetermined temperature (for example, a temperature at which the substrate 3 is maintained at 100 ° C. to 300 ° C.) by the temperature control means 6. ) Is controlled.

尚、チャンバの形状は円筒状に限らず、例えば、矩形状のチャンバを適用することも可能である。   The shape of the chamber is not limited to a cylindrical shape, and for example, a rectangular chamber can be applied.

チャンバ1の上面は開口部とされ、開口部は絶縁材料製(例えば、セラミックス製)の板状の天井板7によって塞がれている。天井板7の上方にはチャンバ1の内部をプラズマ化するためのプラズマアンテナ8が設けられ、プラズマアンテナ8は天井板7の面と平行な平面リング状に形成されている。プラズマアンテナ8には整合器9及び電源10が接続されて高周波が供給される。プラズマアンテナ8、整合器9及び電源10(RF電源)により誘導プラズマを発生させるプラズマ発生手段が構成されている。   The upper surface of the chamber 1 is an opening, and the opening is closed by a plate-like ceiling plate 7 made of an insulating material (for example, made of ceramics). A plasma antenna 8 for converting the inside of the chamber 1 into plasma is provided above the ceiling plate 7, and the plasma antenna 8 is formed in a planar ring shape parallel to the surface of the ceiling plate 7. A matching unit 9 and a power source 10 are connected to the plasma antenna 8 to supply a high frequency. Plasma generating means for generating induction plasma is constituted by the plasma antenna 8, the matching unit 9, and the power source 10 (RF power source).

チャンバ1には、例えば、銅製(Cu製)の被エッチング部材11が保持され、被エッチング部材11はプラズマアンテナ8の電気の流れに対して基板3と天井板7の間に不連続状態で配置されている。例えば、被エッチング部材11は、格子状に形成されてプラズマアンテナ8の電気の流れ方向である周方向に対して構造的に不連続な状態とされている。   The chamber 1 holds a member to be etched 11 made of, for example, copper (made of Cu), and the member to be etched 11 is disposed in a discontinuous state between the substrate 3 and the ceiling plate 7 with respect to the electric flow of the plasma antenna 8. Has been. For example, the member 11 to be etched is formed in a lattice shape and is structurally discontinuous with respect to the circumferential direction, which is the direction of electricity flow of the plasma antenna 8.

尚、プラズマアンテナ8の電気の流れに対して不連続状態にする構成としては、被エッチング部材11を網目状に構成したり、リングの内周側に複数の長尺突起を形成する等の構成とすることも可能である。また、被エッチング部材11をチャンバ1の外部に退避自在な構成にすることも可能である。   In addition, as a structure which makes a discontinuous state with respect to the electric flow of the plasma antenna 8, the structure to be etched 11 is formed in a mesh shape, or a plurality of long protrusions are formed on the inner peripheral side of the ring. It is also possible. In addition, the member to be etched 11 can be configured to be retractable outside the chamber 1.

被エッチング部材11の上方におけるチャンバ1の筒部にはチャンバ1の内部にハロゲンとしての塩素を含有する作用ガス(Heにより所定の濃度に希釈されたガス:Cl2ガス)17を供給するガスノズル14が1本設けられている。ガスノズル14はチャンバ1の中心部まで延び、先端が上方に向けられてガス噴出口15とされている。HeとCl2ガスは流量制御器16で流量及び圧力が制御され、Heで希釈されたCl2ガス17がガスノズル14に送られる(作用ガス供給手段)。 A gas nozzle 14 for supplying a working gas 17 containing chlorine as a halogen (a gas diluted to a predetermined concentration with He: Cl 2 gas) 17 into the cylindrical portion of the chamber 1 above the member 11 to be etched. Is provided. The gas nozzle 14 extends to the center of the chamber 1, and the tip is directed upward to form a gas jet 15. The flow rate and pressure of He and Cl 2 gas are controlled by the flow rate controller 16, and the Cl 2 gas 17 diluted with He is sent to the gas nozzle 14 (working gas supply means).

ガスノズル14をチャンバ1の筒部の周囲に等間隔で複数接続し、チャンバ1の筒部の周囲からCl2ガス17をチャンバ1内に供給することも可能である。また、作用ガスに含有されるハロゲンとしては、フッ素、臭素及びヨウ素等を適用することが可能である。ハロゲンとして塩素を用いたことにより、安価な塩素ガスを用いて薄膜を作製することができる。 It is also possible to connect a plurality of gas nozzles 14 around the cylindrical portion of the chamber 1 at equal intervals and supply the Cl 2 gas 17 into the chamber 1 from the peripheral portion of the cylindrical portion of the chamber 1. In addition, as halogen contained in the working gas, fluorine, bromine, iodine, or the like can be applied. By using chlorine as the halogen, a thin film can be manufactured using inexpensive chlorine gas.

成膜に関与しないガス等は排気口18から排気される。天井板7によって塞がれたチャンバ1の内部は真空装置19によって所定の圧力に維持される。   Gases that are not involved in film formation are exhausted from the exhaust port 18. The interior of the chamber 1 closed by the ceiling plate 7 is maintained at a predetermined pressure by the vacuum device 19.

支持台2の上側におけるチャンバ1の筒部にはレーザー照射手段が設けられている。レーザー照射手段は、例えば、半導体レーザーダイオードからなるレーザー発光手段22とレーザー光を受ける受光手段23とを備えている。レーザー発光手段22からチャンバ1内に照射されるレーザー光24は帯状のレーザー光であり、レーザー光24の面は、基板3の中心を通り基板3に対して直交する面とされている。そして、レーザー光24の面を撮影するカメラ25が備えられている。   Laser irradiation means is provided on the cylindrical portion of the chamber 1 above the support base 2. The laser irradiation means includes, for example, a laser light emitting means 22 made of a semiconductor laser diode and a light receiving means 23 for receiving the laser light. The laser light 24 irradiated into the chamber 1 from the laser light emitting means 22 is a belt-shaped laser light, and the surface of the laser light 24 passes through the center of the substrate 3 and is orthogonal to the substrate 3. And the camera 25 which image | photographs the surface of the laser beam 24 is provided.

レーザー光24がチャンバ1内の物質(後述するCu原子、CuCl分子:解離物)に照射されると、レーザー誘起蛍光が発生する。レーザー誘起蛍光は指向性と単色性のよい入射光と異なる方向で異なる波長で検出され、レーザー誘起蛍光の状況がカメラ25で撮影される。カメラ25の画像は画像処理装置26(図2参照)により発光強度の分布を表す二次元画像に処理され、制御手段20に送られる。二次元画像に処理されたレーザー誘起蛍光の強度分布は、解離物の分布に応じた状態で表われるようになっている。   When the laser beam 24 is irradiated to a substance (a Cu atom, CuCl molecule: dissociated material described later) in the chamber 1, laser-induced fluorescence is generated. Laser-induced fluorescence is detected at different wavelengths in different directions from incident light having good directivity and monochromaticity, and the state of laser-induced fluorescence is photographed by the camera 25. The image of the camera 25 is processed into a two-dimensional image representing the distribution of light emission intensity by an image processing device 26 (see FIG. 2) and sent to the control means 20. The intensity distribution of the laser-induced fluorescence processed into the two-dimensional image appears in a state corresponding to the distribution of dissociation products.

制御手段20には、薄膜の作製条件(チャンバ1内の圧力、Cl2ガス17の流量、RFパワー等:具体的には後述する)に応じた解離物の強度分布(発光分布)が予め種々記憶されている。そして、制御手段20からは、二次元画像で表された解離物の発光分布及び記憶された情報に基づいて、解離物が均一になる発光状況となるように、薄膜の作製条件を適宜変更するように制御信号が出力される。 The control means 20 has various dissociation intensity distributions (light emission distributions) in advance according to thin film production conditions (pressure in the chamber 1, flow rate of Cl 2 gas 17, RF power, etc., specifically described later). It is remembered. And from the control means 20, based on the light emission distribution of the dissociated product represented by the two-dimensional image and the stored information, the thin film production conditions are appropriately changed so that the dissociated product becomes a uniform light emission state. Thus, a control signal is output.

つまり、図2に示すように、画像処理された二次元画像31(大きな分布が生じている状態)の発光強度状況に基づいて、目標となる分布画像32(分布が抑制された状態)の発光強度状況となるように、薄膜の作製条件を変更する信号が出力される。   That is, as shown in FIG. 2, the light emission of the target distribution image 32 (in which the distribution is suppressed) based on the light emission intensity state of the image-processed two-dimensional image 31 (in the state where a large distribution is generated). A signal for changing the manufacturing conditions of the thin film is output so as to obtain the strength state.

上述した薄膜作製装置では、チャンバ1の内部にガスノズル14のガス噴出口15からCl2ガス17を供給する。プラズマアンテナ8から電磁波をチャンバ1の内部に入射することで、Cl2ガス17をイオン化してCl2ガスプラズマを発生させ、Clラジカルを生成する。プラズマは、ガスプラズマ12で図示する領域に発生する。この時の反応は、次式で表すことができる。
Cl2→2Cl* ・・・・(1)
ここで、Cl*は塩素ラジカルを表す。
In the thin film manufacturing apparatus described above, the Cl 2 gas 17 is supplied into the chamber 1 from the gas outlet 15 of the gas nozzle 14. When electromagnetic waves are incident on the inside of the chamber 1 from the plasma antenna 8, the Cl 2 gas 17 is ionized to generate Cl 2 gas plasma to generate Cl radicals. The plasma is generated in the region shown by the gas plasma 12. The reaction at this time can be expressed by the following formula.
Cl 2 → 2Cl * (1)
Here, Cl * represents a chlorine radical.

ガスプラズマ12がCu製の被エッチング部材11に作用することにより、被エッチング部材11が加熱されると共に、Cuにエッチング反応が生じる。この時の反応は、例えば、次式で表される。
Cu(s)+Cl*→CuCl(g) ・・・・(2)
ここで、sは固体状態、gはガス状態を表す。式(2)は、Cuがガスプラズマ12(塩素ラジカルCl*)によりエッチングされ、前駆体13とされた状態である。
When the gas plasma 12 acts on the member to be etched 11 made of Cu, the member to be etched 11 is heated and an etching reaction occurs in Cu. The reaction at this time is represented by the following formula, for example.
Cu (s) + Cl * → CuCl (g) (2)
Here, s represents a solid state and g represents a gas state. Formula (2) is a state in which Cu is etched by gas plasma 12 (chlorine radical Cl * ) to be a precursor 13.

ガスプラズマ12を発生させることにより被エッチング部材11を加熱し(例えば、300℃〜700℃)、更に、温度制御手段6により基板3の温度を被エッチング部材11の温度よりも低い温度(例えば、100℃〜300℃)に設定する。この結果、前駆体13は基板3に吸着(堆積)される。この時の反応は、例えば、次式で表される。
CuCl(g)→CuCl(ad) ・・・・(3)
The member to be etched 11 is heated by generating the gas plasma 12 (for example, 300 ° C. to 700 ° C.), and the temperature of the substrate 3 is lower than the temperature of the member to be etched 11 by the temperature control means 6 (for example, 100 ° C. to 300 ° C.). As a result, the precursor 13 is adsorbed (deposited) on the substrate 3. The reaction at this time is represented by the following formula, for example.
CuCl (g) → CuCl (ad) (3)

基板3に吸着したCuは、塩素ラジカルCl*により還元されてCu成分となる。
この時の反応は、例えば、次式で表される。
CuCl(ad)+Cl*→Cu(s)+Cl2↑・・・・(4)
Cu adsorbed on the substrate 3 is reduced by the chlorine radical Cl * to become a Cu component.
The reaction at this time is represented by the following formula, for example.
CuCl (ad) + Cl * → Cu (s) + Cl 2 ↑ (4)

更に、上式(2)において発生したガス化したCuCl(g)の一部は、基板3に吸着する(上式(3)参照)前に、塩素ラジカルCl*により還元されてガス状態のCuとなる場合もある。この時の反応は、例えば、次式で表される。
CuCl(g)+Cl*→Cu(g)+Cl2↑ ・・・・(5)
この後、ガス状態のCu成分は、基板3に吸着される。
これにより、基板3にCuの薄膜が作製される。
Further, a part of the gasified CuCl (g) generated in the above formula (2) is reduced by the chlorine radical Cl * before being adsorbed on the substrate 3 (see the above formula (3)), and is in a gaseous state. It may become. The reaction at this time is represented by the following formula, for example.
CuCl (g) + Cl * → Cu (g) + Cl 2 ↑ (5)
Thereafter, the gaseous Cu component is adsorbed on the substrate 3.
As a result, a Cu thin film is formed on the substrate 3.

上述したCuの薄膜の作製に際し、レーザー発光手段22から帯状のレーザー光24がチャンバ1内に照射される。レーザー光24がチャンバ1内の解離物(例えば、Cu原子、CuCl分子)に照射されると、Cu原子、CuCl分子の密度分布に応じた発光強度分布のレーザー誘起蛍光が発生する。レーザー誘起蛍光の状況(解離物の密度分布に応じた発光強度分布)がカメラ25で撮影され、二次元画像に処理されたレーザー誘起蛍光の強度分布の情報が制御手段20に送られる。基板3の上部の解離物の密度分布に応じたレーザー誘起蛍光の強度分布に基づいて(入力された二次元画像の情報に基づいて)、レーザー誘起蛍光の強度分布が均一になるように薄膜の作製条件が変更される。   When the above-described Cu thin film is produced, a belt-like laser beam 24 is irradiated from the laser emission means 22 into the chamber 1. When the laser beam 24 irradiates dissociated substances (for example, Cu atoms and CuCl molecules) in the chamber 1, laser-induced fluorescence having an emission intensity distribution corresponding to the density distribution of Cu atoms and CuCl molecules is generated. The state of laser-induced fluorescence (the emission intensity distribution corresponding to the density distribution of the dissociated product) is photographed by the camera 25, and information on the intensity distribution of the laser-induced fluorescence processed into a two-dimensional image is sent to the control means 20. Based on the intensity distribution of the laser-induced fluorescence corresponding to the density distribution of the dissociation material on the upper part of the substrate 3 (based on the information of the input two-dimensional image), the intensity of the laser-induced fluorescence is made uniform so as to be uniform. The production conditions are changed.

制御手段20には、薄膜の作製条件である、チャンバ1内の圧力、Cl2ガス17の流量、RFパワー等に応じた解離物の強度分布(発光分布)が予め種々記憶されている。制御手段20では、記憶された強度分布を適宜組み合わせ、入力された二次元画像の強度分布を打ち消す状態の強度分布となるようにチャンバ1内の圧力、Cl2ガス17の流量、RFパワー等のプロセス条件を変更し、基板3上の解離物が均一になる発光状況とする。つまり、基板3毎に、Cu原子やCuCl分子の密度が均一になるようなプロセス条件に変更され、薄膜の作製の均一性が高められる。 The control means 20 stores in advance various dissociation intensity distributions (light emission distributions) according to the pressure in the chamber 1, the flow rate of the Cl 2 gas 17, the RF power, and the like, which are the thin film production conditions. In the control means 20, the stored intensity distributions are appropriately combined, and the pressure in the chamber 1, the flow rate of the Cl 2 gas 17, the RF power, etc. are adjusted so as to cancel the intensity distribution of the input two-dimensional image. The process conditions are changed so that the dissociated material on the substrate 3 becomes uniform. That is, the process conditions are changed so that the density of Cu atoms and CuCl molecules is uniform for each substrate 3, and the uniformity of thin film production is improved.

これにより、周囲の温度環境や成膜履歴により最適な薄膜の作製条件(プロセス条件)が初期の条件から変化しても、基板3毎に最適なプロセス条件を得ることができ、周囲環境に素早く追随して均一な膜厚で薄膜を作製することが可能になる。   As a result, even if the optimum thin film production conditions (process conditions) change from the initial conditions due to the ambient temperature environment and film formation history, the optimum process conditions can be obtained for each substrate 3, and the ambient conditions can be quickly adjusted. Following this, it becomes possible to produce a thin film with a uniform film thickness.

図3から図5に基づいて、制御手段20に予め記憶されているプロセス条件とCu原子の分布状況の一例を説明する。   Based on FIG. 3 to FIG. 5, an example of process conditions and Cu atom distribution state stored in advance in the control means 20 will be described.

図3は圧力とCu原子の分布状況との関係を示してある。図3(a)は110mTorr、図3(b)は150mTorr、図3(c)は200mTorrの時の二次元画像の状況と光の強度の分布である。110mTorr、150mTorr、200mTorrへと圧力が変化するにともない、レーザー誘起蛍光の強度が強い部位(白抜き、斜線、網目の順で強度が強いことを示してある)が徐々に多くなり、Cu原子の密度に対応した光強度の分布が強弱の大きな山形となる。   FIG. 3 shows the relationship between pressure and Cu atom distribution. 3A is 110 mTorr, FIG. 3B is 150 mTorr, and FIG. 3C is a two-dimensional image situation and light intensity distribution at 200 mTorr. As the pressure changes to 110 mTorr, 150 mTorr, and 200 mTorr, the portion where the intensity of the laser-induced fluorescence is strong (indicating that the intensity is strong in the order of white lines, diagonal lines, and meshes) gradually increases. The distribution of light intensity corresponding to the density is a large mountain shape with strength.

図4はRFパワーとCu原子の分布状況との関係を示してある。図4(a)は500W、図4(b)は700W、図4(c)は1000Wの時の二次元画像の状況と光の強度の分布である。圧力の関係と同様に、500W、700W、1000WへとRFパワーの変化にともない、レーザー誘起蛍光の強度が強い部位(白抜き、網目の順で強度が強いことを示してある)が多くなり、1000Wで急激に増加し、Cu原子の密度に対応した光強度の分布が強弱の大きな山形となる。   FIG. 4 shows the relationship between RF power and Cu atom distribution. 4A shows the state of the two-dimensional image and the light intensity distribution at 500 W, FIG. 4B at 700 W, and FIG. 4C at 1000 W. As with the relationship of pressure, as the RF power changes to 500 W, 700 W, and 1000 W, there are many sites where the intensity of laser-induced fluorescence is strong (indicating that the intensity is strong in the order of white and mesh), It rapidly increases at 1000 W, and the light intensity distribution corresponding to the density of Cu atoms becomes a large and small mountain shape.

図5はCl2ガス17の流量とCu原子の分布状況との関係を示してある。図5(a)は30sccm、図5(b)は50sccm、図5(c)は70sccmの時の二次元画像の状況と光の強度の分布である。30sccm、50sccmへとCl2ガス17の流量の変更にともない、レーザー誘起蛍光の強度が強い部位(白抜き、斜線、網目の順で強度が強いことを示してある)が多くなり、50sccm、70sccmへとCl2ガス17の流量の変更にともない、レーザー誘起蛍光の強度が強い部位(白抜き、斜線、網目の順で強度が強いことを示してある)が少なくなり、Cu原子の密度に対応した光強度の分布が強くなった後に弱くなる状態の山形となる。 FIG. 5 shows the relationship between the flow rate of the Cl 2 gas 17 and the distribution of Cu atoms. FIG. 5A shows the state of the two-dimensional image and the light intensity distribution at 30 sccm, FIG. 5B at 50 sccm, and FIG. 5C at 70 sccm. As the flow rate of the Cl 2 gas 17 is changed to 30 sccm and 50 sccm, the portion where the intensity of the laser-induced fluorescence is strong (indicating that the intensity is strong in the order of white lines, diagonal lines, and meshes) increases, and 50 sccm and 70 sccm. As the flow rate of Cl 2 gas 17 changes, the number of sites where the intensity of laser-induced fluorescence is strong (indicating that the intensity is strong in the order of white lines, diagonal lines, and meshes) decreases and corresponds to the density of Cu atoms. The resulting light intensity distribution becomes a mountain shape that becomes weaker after becoming stronger.

基板3の上におけるCu原子の密度を均一にする場合、予め記憶された、例えば、図3から図5の状況に基づいてプロセス条件を変更し、基板3上のCu原子が均一になる発光状況を創りだす。これにより、基板3上のCu原子の密度が均一な状態にされ、均一性の高いCu薄膜が作製される。   When the density of Cu atoms on the substrate 3 is made uniform, the process conditions are changed based on, for example, the conditions of FIGS. 3 to 5 stored in advance, so that the Cu atoms on the substrate 3 become uniform. Create. Thereby, the density of Cu atoms on the substrate 3 is made uniform, and a highly uniform Cu thin film is produced.

図6から図9に基づいて、制御手段20に予め記憶されているプロセス条件とCuCl分子の分布状況の一例を説明する。   Based on FIGS. 6 to 9, an example of the process conditions stored in advance in the control means 20 and the distribution state of CuCl molecules will be described.

図6は圧力とCuCl分子の分布状況との関係を示してある。図6(a)は110mTorr、図6(b)は150mTorr、図6(c)は200mTorrの時の二次元画像の状況と光の強度の分布である。110mTorr、150mTorr、200mTorrへと圧力が変化するにともない、レーザー誘起蛍光の強度が強い部位(白抜き、斜線、網目の順で強度が強いことを示してある)が徐々に多くなり、CuCl分子の密度に応じた光強度の分布が強弱の大きな山形となる。   FIG. 6 shows the relationship between the pressure and the distribution of CuCl molecules. 6A shows 110 mTorr, FIG. 6B shows 150 mTorr, and FIG. 6C shows the state of a two-dimensional image and light intensity distribution at 200 mTorr. As the pressure changes to 110 mTorr, 150 mTorr, and 200 mTorr, the portion of the laser-induced fluorescence intensity (indicating that the intensity is higher in the order of white, diagonal lines, and mesh) gradually increases, and the CuCl molecule The light intensity distribution according to the density is a large mountain shape.

図7はRFパワーとCuCl分子の分布状況との関係を示してある。図7(a)は500W、図7(b)は700Wの時の二次元画像の状況と光の強度の分布である。500W、700WへとRFパワーが変化しても、レーザー誘起蛍光の強度が強い部位(斜線、網目の部位)は増加せず、CuCl分子の密度に対応した光強度の分布が小さな山形となる。   FIG. 7 shows the relationship between RF power and CuCl molecule distribution. FIG. 7A shows the state of the two-dimensional image and the distribution of light intensity at 500 W and FIG. 7B at 700 W. Even if the RF power is changed to 500 W or 700 W, the portion where the intensity of laser-induced fluorescence is strong (diagonal line, mesh portion) does not increase, and the light intensity distribution corresponding to the density of CuCl molecules becomes a small mountain shape.

図8はCl2ガス17の流量とCuCl分子の分布状況との関係を示してある。図8(a)は30sccm、図8(b)は50sccm、図8(c)は70sccmの時の二次元画像の状況と光の強度の分布である。30sccm、50sccm、70sccmへとCl2ガス17の流量の変更にともない、レーザー誘起蛍光の強度が強い部位(白抜き、斜線の順で強度が強いことを示してある)が徐々に多くなり、CuCl分子の密度に対応した光強度の分布が徐々に大きくなる状態の山形となる。 FIG. 8 shows the relationship between the flow rate of the Cl 2 gas 17 and the distribution state of CuCl molecules. FIG. 8A shows the situation of the two-dimensional image and the light intensity distribution at 30 sccm, FIG. 8B at 50 sccm, and FIG. 8C at 70 sccm. As the flow rate of the Cl 2 gas 17 is changed to 30 sccm, 50 sccm, and 70 sccm, the site where the intensity of laser-induced fluorescence is strong (indicating that the intensity is strong in the order of white and diagonal lines) gradually increases, and CuCl It becomes a mountain shape in which the light intensity distribution corresponding to the density of the molecules gradually increases.

図9はArの添加量とCuCl分子の分布状況との関係を示してある。図9(a)は添加がない場合(Cl2/He:30sccm)、図9(b)はArの添加がある場合(Cl2/He:10sccm、Ar20sccm)の時の二次元画像の状況と光の強度の分布である。Arを添加することにより、レーザー誘起蛍光の強度が強い部位(白抜き、斜線の順で強度が強いことを示してある)が若干多くなり、CuCl分子の密度に対応した光強度の分布が若干大きくなる状態の山形となる。 FIG. 9 shows the relationship between the amount of Ar added and the distribution of CuCl molecules. FIG. 9A shows the situation of a two-dimensional image when there is no addition (Cl 2 / He: 30 sccm), and FIG. 9B shows the situation of a two-dimensional image when Ar is added (Cl 2 / He: 10 sccm, Ar 20 sccm). It is a distribution of light intensity. By adding Ar, there are slightly more sites where the intensity of laser-induced fluorescence is strong (indicated by white and diagonal lines), and there is a slight distribution of light intensity corresponding to the density of CuCl molecules. It becomes Yamagata in the state of growing.

基板3の上におけるCuCl分子の密度を均一にする場合、予め記憶された、例えば、図6から図9の状況に基づいてプロセス条件を変更し、基板3上のCuCl分子が均一になる発光状況を創りだす。これにより、基板3上のCuCl分子の密度が均一な状態にされ、均一性の高いCu薄膜が作製される。   In the case where the density of CuCl molecules on the substrate 3 is made uniform, the process conditions are changed based on, for example, the conditions of FIGS. 6 to 9 stored in advance so that the CuCl molecules on the substrate 3 become uniform. Create. Thereby, the density of CuCl molecules on the substrate 3 is made uniform, and a highly uniform Cu thin film is produced.

上述した実施形態例では、金属薄膜としてCu薄膜の作製を例に挙げて説明したが、Ti、Ta、Ni、Al等他の金属の被エッチング部材を用いて各種金属や合金の薄膜の作製に適用することが可能である。また、解離物としてCu原子やCuCl分子の密度分布を撮影する例を挙げて説明したが、撮影する波長を選択することで、Cl原子の密度分布を撮影することも可能である。   In the above-described embodiment, the Cu thin film has been described as an example of the metal thin film. However, various metal and alloy thin films can be formed using other metal members to be etched such as Ti, Ta, Ni, and Al. It is possible to apply. Further, although an example of photographing the density distribution of Cu atoms and CuCl molecules as dissociated materials has been described, the density distribution of Cl atoms can be photographed by selecting the wavelength to be photographed.

また、薄膜の作製条件としては、チャンバ1内の圧力、Cl2ガス17の流量、RFパワー、Arの添加を例に挙げて説明したが、温度、ガスノズル14の位置、複数のガスノズル14を用いた供給停止の個別調整、支持台2の昇降等、種々のプロセス条件を適用し、各条件に応じた解離物の強度分布の状況を記憶させて上記制御を実施することが可能である。 Further, as the thin film production conditions, the pressure in the chamber 1, the flow rate of the Cl 2 gas 17, the RF power, and the addition of Ar have been described as examples. However, the temperature, the position of the gas nozzle 14 and a plurality of gas nozzles 14 are used. The above control can be performed by applying various process conditions such as individual adjustment of supply stop and raising / lowering of the support base 2 and storing the intensity distribution state of the dissociated material according to each condition.

また、レーザー光24を、基板3の中心を通り基板3に対して直交する帯状のものとしたが、基板3に対する角度は任意であり、例えば、基板3に対して平行な帯状のレーザー光を用いて上側から発光状況を撮影するようにすることも可能である。また、基板3の中心を通り基板3に対して直交する帯状のレーザー光を基板3に対して平行な方向に移動させながら発光状況を撮影することも可能である。   Further, although the laser beam 24 is in the form of a band passing through the center of the substrate 3 and orthogonal to the substrate 3, the angle with respect to the substrate 3 is arbitrary, for example, a band-shaped laser beam parallel to the substrate 3 is used. It is also possible to photograph the light emission state from above. It is also possible to take a picture of the light emission state while moving a belt-like laser beam passing through the center of the substrate 3 and orthogonal to the substrate 3 in a direction parallel to the substrate 3.

上述した薄膜作製装置及び薄膜作製方法では、周囲の環境や成膜履歴が変化してもプロセス条件の調整を行う必要がなく、外的要因に拘わらず処理時間を長くすることなく均一な薄膜を作製することができる。このため、周囲の環境や成膜履歴が変化してもプロセス条件の調整に係る時間が不要となり、薄膜作製の効率が向上すると共に歩留まりの低下を抑制することができる。   In the thin film manufacturing apparatus and the thin film manufacturing method described above, it is not necessary to adjust the process conditions even if the surrounding environment or the film forming history changes, and a uniform thin film can be formed without increasing the processing time regardless of external factors. Can be produced. For this reason, even if the surrounding environment and the film formation history change, the time for adjusting the process conditions is not required, and the efficiency of thin film production can be improved and the decrease in yield can be suppressed.

本発明は、環境や成膜履歴に拘わらず処理時間を長くすることなく均一な薄膜が作製できる薄膜作製装置及び薄膜作製方法の産業分野で利用することができる。   INDUSTRIAL APPLICABILITY The present invention can be used in the industrial field of a thin film manufacturing apparatus and a thin film manufacturing method capable of manufacturing a uniform thin film without increasing the processing time regardless of the environment and the film forming history.

本発明の一実施形態例に係る薄膜作製装置の概略側面図である。1 is a schematic side view of a thin film manufacturing apparatus according to an embodiment of the present invention. 本発明の一実施形態例に係る薄膜作製装置の概略平面図である。1 is a schematic plan view of a thin film manufacturing apparatus according to an embodiment of the present invention. 薄膜の作製条件に応じたCu原子の分布状況説明図である。It is explanatory drawing of the distribution condition of Cu atom according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCu原子の分布状況説明図である。It is explanatory drawing of the distribution condition of Cu atom according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCu原子の分布状況説明図である。It is explanatory drawing of the distribution condition of Cu atom according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCuCl分子の分布状況説明図である。It is explanatory drawing of the distribution condition of CuCl molecule | numerator according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCuCl分子の分布状況説明図である。It is explanatory drawing of the distribution condition of CuCl molecule | numerator according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCuCl分子の分布状況説明図である。It is explanatory drawing of the distribution condition of CuCl molecule | numerator according to the preparation conditions of a thin film. 薄膜の作製条件に応じたCuCl分子の分布状況説明図である。It is explanatory drawing of the distribution condition of CuCl molecule | numerator according to the preparation conditions of a thin film.

1 チャンバ
2 支持台
3 基板
4 ヒータ
5 冷媒流通手段
6 温度制御手段
7 天井板
8 プラズマアンテナ
9 整合器
10 電源
11 被エッチング部材
12 ガスプラズマ
13 前駆体
14 ガスノズル
15 ガス噴出口
16 流量制御器
17 作用ガス(Cl2ガス)
18 排気口
19 真空装置
20 制御手段
22 レーザー発光手段
23 受光手段
25 カメラ
26 画像処理装置
31 二次元画像
32 分布画像
DESCRIPTION OF SYMBOLS 1 Chamber 2 Support stand 3 Substrate 4 Heater 5 Refrigerant distribution means 6 Temperature control means 7 Ceiling board 8 Plasma antenna 9 Matching device 10 Power supply 11 Member to be etched 12 Gas plasma 13 Precursor 14 Gas nozzle 15 Gas jet 16 Flow controller 17 Action Gas (Cl 2 gas)
DESCRIPTION OF SYMBOLS 18 Exhaust port 19 Vacuum apparatus 20 Control means 22 Laser light emission means 23 Light reception means 25 Camera 26 Image processing apparatus 31 Two-dimensional image 32 Distribution image

Claims (12)

基板が収容されるチャンバと、
基板が対向する位置におけるチャンバに設けられる金属製の被エッチング部材と、チャンバの内部にハロゲンを含有する作用ガスを供給する作用ガス供給手段と、チャンバの内部をプラズマ化し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成するプラズマ発生手段とを備え、基板側の温度を被エッチング部材の温度よりも低くして前記前駆体中の金属を基板に成膜させる成膜装置において、
チャンバ内に帯状のレーザー光を照射してチャンバ内の前記前駆体を発光させるレーザー照射手段と、
レーザー光による前記前駆体の発光分布をモニタして画像処理する画像処理手段と、
膜の作製条件に応じた前記前駆体の発光分布が予め記憶されており、該記憶された発光分布に基づいて、前記画像処理手段で画像処理した発光分布が均一になるように薄膜の作製条件を変更する制御手段と
を備えたことを特徴とする薄膜作製装置。
A chamber containing a substrate;
A metal member to be etched provided in the chamber at a position where the substrate faces, a working gas supply means for supplying a working gas containing halogen to the inside of the chamber, and plasmaizing the inside of the chamber to generate working gas plasma. Te generates a halogen radical, and a plasma generating means for generating a precursor which is a metal halide gas state consisting of metals and halogens contained in the etched member by etching the etched member with a halogen radical In the film forming apparatus for forming the metal in the precursor on the substrate by lowering the temperature on the substrate side lower than the temperature of the member to be etched,
Laser irradiation means for irradiating the chamber with a laser beam to emit the precursor in the chamber ; and
Image processing means for image processing by monitoring the light emission distribution of the precursor by a laser beam,
Emission distribution of the precursor in accordance with the production conditions of the thin film is stored in advance, based on the light emission distribution that is the storage, image processing and emission distribution uniform by ing urchin film by the image processing unit And a control means for changing the manufacturing conditions of the thin film manufacturing apparatus.
基板が収容されるチャンバと、A chamber containing a substrate;
基板が対向する位置におけるチャンバに設けられる金属製の被エッチング部材と、チャンバの内部にハロゲンを含有する作用ガスを供給する作用ガス供給手段と、チャンバの内部をプラズマ化し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成するプラズマ発生手段とを備え、基板側の温度を被エッチング部材の温度よりも低くして前記前駆体中の金属を基板に成膜させる成膜装置において、A metal member to be etched provided in the chamber at a position where the substrate faces, a working gas supply means for supplying a working gas containing halogen to the inside of the chamber, and plasmaizing the inside of the chamber to generate working gas plasma. Generating a halogen radical, and etching a member to be etched with the halogen radical, thereby generating a precursor that is a metal halide in a gas state composed of a metal contained in the member to be etched and halogen, and a plasma generating means, In the film forming apparatus for forming the metal in the precursor on the substrate by lowering the temperature on the substrate side lower than the temperature of the member to be etched,
チャンバ内に帯状のレーザー光を照射して、前記前駆体が前記ハロゲンラジカルで還元されることでチャンバ内に生成するガス状態の前記金属の原子を発光させるレーザー照射手段と、A laser irradiation means for irradiating a belt-shaped laser beam in the chamber, and emitting the metal atoms in a gas state generated in the chamber by reducing the precursor with the halogen radical;
レーザー光による前記金属の原子の発光分布をモニタして画像処理する画像処理手段と、Image processing means for performing image processing by monitoring the light emission distribution of the metal atoms by laser light;
薄膜の作製条件に応じた前記金属の原子の発光分布が予め記憶されており、該記憶された発光分布に基づいて、前記画像処理手段で画像処理した発光分布が均一になるように薄膜の作製条件を変更する制御手段とThe light emission distribution of the metal atoms corresponding to the thin film production conditions is stored in advance, and the thin film production is performed so that the light emission distribution image-processed by the image processing means is uniform based on the stored light emission distribution. Control means to change the condition and
を備えたことを特徴とする薄膜作製装置。A thin film manufacturing apparatus comprising:
前記レーザー照射手段で照射される帯状のレーザー光は、基板の中心を通り基板を横断する帯状であることを特徴とする請求項1又は2に記載の薄膜作製装置。 3. The thin film manufacturing apparatus according to claim 1, wherein the belt-shaped laser light irradiated by the laser irradiation unit has a belt shape passing through the center of the substrate and crossing the substrate. 前記画像処理手段は、レーザー光の面を撮影するカメラと、カメラの画像を発光強度の分布を表す二次元画像に処理する処理手段とを備えたことを特徴とする請求項1〜3のいずれか一項に記載の薄膜作製装置。 The said image processing means is provided with the camera which image | photographs the surface of a laser beam, and the processing means which processes the image of a camera into the two-dimensional image showing distribution of emitted light intensity, The any one of Claims 1-3 characterized by the above-mentioned. thin-film producing apparatus according to an item or. 前記作用ガス供給手段には流量を制御する流量調整手段が備えられると共に、チャンバを所定の真空圧力にする真空手段が備えられ、プラズマ発生手段はRF電源により電力が供給されてチャンバの内部をプラズマ化するものであり、
前記薄膜の作製条件は、真空手段の調整によるチャンバ内の圧力、流量調整手段の調整による作用ガスの流量、RF電源のRFパワーのうち少なくとも一つを含むことを特徴とする請求項1〜4のいずれか一項に記載の薄膜作製装置。
The working gas supply means is provided with a flow rate adjusting means for controlling the flow rate and a vacuum means for setting the chamber to a predetermined vacuum pressure. The plasma generating means is supplied with electric power from an RF power source, and plasma is generated inside the chamber. Is,
Conditions for producing the thin film according to claim 1 to 4, characterized in that it comprises pressure in the chamber by adjusting the vacuum means, the flow rate of the working gas by adjusting the flow rate adjusting means, at least one of RF power of the RF power source The thin film production apparatus according to any one of the above .
前記ハロゲンを含有する作用ガスはハロゲンとして塩素を含有する作用ガスであることを特徴とする請求項1〜5のいずれか一項に記載の薄膜作製装置。 The thin-film manufacturing apparatus according to claim 1, wherein the working gas containing halogen is a working gas containing chlorine as a halogen . 金属製の被エッチング部材が備えられたチャンバ内にハロゲンを含有する作用ガスを供給し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成し、基板側の温度を被エッチング部材の温度よりも低くすることにより前記前駆体の金属を基板に成膜させる薄膜作製方法において
チャンバ内に帯状のレーザー光を照射してチャンバ内の前記前駆体を発光させて、前記前駆体の発光分布を検出し、薄膜の作製条件に応じた前記前駆体の既知の発光分布に基づいて、前記検出した発光分布が均一になるように薄膜の作製条件を変更して成膜を行うことを特徴とする薄膜作製方法。
A member to be etched is supplied by supplying a working gas containing halogen into a chamber equipped with a metal member to be etched, generating a working gas plasma to generate halogen radicals, and etching the member to be etched with halogen radicals. include generating a metallic and a metal halide is precursor gas state consisting of halogens, a substrate metals in the precursor by the temperature of the substrate side to be lower than the temperature of the etched member to In a thin film manufacturing method for forming a film ,
By irradiating the chamber with a band-shaped laser beam, the precursor in the chamber emits light, detects the light emission distribution of the precursor, and based on the known light emission distribution of the precursor according to the thin film production conditions A thin film manufacturing method characterized in that the thin film manufacturing conditions are changed so that the detected light emission distribution becomes uniform.
金属製の被エッチング部材が備えられたチャンバ内にハロゲンを含有する作用ガスを供給し、作用ガスプラズマを発生させてハロゲンラジカルを生成し、ハロゲンラジカルで被エッチング部材をエッチングすることにより被エッチング部材に含まれる金属とハロゲンとからなるガス状態のハロゲン化金属である前駆体を生成し、基板側の温度を被エッチング部材の温度よりも低くすることにより前記前駆体中の金属を基板に成膜させる薄膜作製方法において、A member to be etched is supplied by supplying a working gas containing halogen into a chamber equipped with a metal member to be etched, generating a working gas plasma to generate halogen radicals, and etching the member to be etched with halogen radicals. A precursor, which is a metal halide in a gas state composed of a metal and a halogen contained in the substrate, is generated, and the metal in the precursor is formed on the substrate by setting the temperature on the substrate side lower than the temperature of the member to be etched. In the thin film manufacturing method to
チャンバ内に帯状のレーザー光を照射して、前記前駆体が前記ハロゲンラジカルで還元されることでチャンバ内に生成するガス状態の前記金属の原子を発光させて、前記金属の原子の発光分布を検出し、薄膜の作製条件に応じた前記金属の原子の既知の発光分布に基づいて、前記検出した発光分布が均一になるように薄膜の作製条件を変更して成膜を行うことを特徴とする薄膜作製方法。By irradiating a strip-shaped laser beam into the chamber, the precursor is reduced by the halogen radicals so that the metal atoms generated in the chamber emit light, and the emission distribution of the metal atoms is obtained. Based on the known light emission distribution of the metal atoms according to the detection conditions of the thin film, the film formation is performed by changing the thin film preparation conditions so that the detected light emission distribution is uniform. Thin film manufacturing method.
前記帯状のレーザー光は、基板の中心を通り基板を横断する帯状であることを特徴とする請求項7又は8に記載の薄膜作製方法。 The thin film manufacturing method according to claim 7 or 8, wherein the belt-like laser light has a belt-like shape passing through the center of the substrate and crossing the substrate . 前記発光分布の検出を、レーザー光の面を撮影した画像を発光強度の分布を表す二次元画像に処理することで行うことを特徴とする請求項7〜9のいずれか一項に記載の薄膜作製方法。 The thin film according to any one of claims 7 to 9, wherein the emission distribution is detected by processing an image obtained by photographing a surface of a laser beam into a two-dimensional image representing the distribution of emission intensity. Manufacturing method. 前記薄膜の作製条件は、チャンバ内の圧力、作用ガスの流量、プラズマを発生させるためのRFパワーのうち少なくとも一つを含むことを特徴とする請求項8〜10のいずれか一項に記載の薄膜作製方法。 Conditions for producing the thin film, the pressure in the chamber, the working gas flow rate, according to any one of claims 8-10, characterized in that it comprises at least one of RF power for generating a plasma Thin film manufacturing method. 前記ハロゲンを含有する作用ガスはハロゲンとして塩素を含有する作用ガスであることを特徴とする請求項7〜11のいずれか一項に記載の薄膜作製方法。 The method for producing a thin film according to claim 7, wherein the working gas containing halogen is a working gas containing chlorine as a halogen .
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