JPH0520504B2 - - Google Patents
Info
- Publication number
- JPH0520504B2 JPH0520504B2 JP15596285A JP15596285A JPH0520504B2 JP H0520504 B2 JPH0520504 B2 JP H0520504B2 JP 15596285 A JP15596285 A JP 15596285A JP 15596285 A JP15596285 A JP 15596285A JP H0520504 B2 JPH0520504 B2 JP H0520504B2
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- light
- temperature
- film
- cvd
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 239000000758 substrate Substances 0.000 claims description 49
- 230000003287 optical effect Effects 0.000 claims description 30
- 239000010409 thin film Substances 0.000 claims description 17
- 238000006243 chemical reaction Methods 0.000 claims description 9
- 230000003252 repetitive effect Effects 0.000 claims description 7
- 238000006552 photochemical reaction Methods 0.000 claims description 4
- 239000010408 film Substances 0.000 description 43
- 230000008021 deposition Effects 0.000 description 13
- 239000007789 gas Substances 0.000 description 13
- 239000011651 chromium Substances 0.000 description 11
- 230000000694 effects Effects 0.000 description 9
- 238000010521 absorption reaction Methods 0.000 description 6
- 238000002834 transmittance Methods 0.000 description 5
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 4
- 229910052804 chromium Inorganic materials 0.000 description 4
- 238000010438 heat treatment Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 239000010453 quartz Substances 0.000 description 3
- 239000004065 semiconductor Substances 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 3
- 238000004140 cleaning Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000005068 transpiration Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 239000012159 carrier gas Substances 0.000 description 1
- 230000003749 cleanliness Effects 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000000354 decomposition reaction Methods 0.000 description 1
- 238000003795 desorption Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 239000002932 luster Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 230000001443 photoexcitation Effects 0.000 description 1
- 238000004088 simulation Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 230000003746 surface roughness Effects 0.000 description 1
- 239000012808 vapor phase Substances 0.000 description 1
Classifications
-
- 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
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/44—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
- C23C16/48—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation
- C23C16/483—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation using coherent light, UV to IR, e.g. lasers
Landscapes
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Optics & Photonics (AREA)
- General Chemical & Material Sciences (AREA)
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Mechanical Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Physical Or Chemical Processes And Apparatus (AREA)
- Chemical Vapour Deposition (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、光励起することにより薄膜を形成す
る装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an apparatus for forming a thin film by photoexcitation.
近年、半導体デバイス製造プロセスにおいて
は、光CVDなどのプロセス技術が、プロセスの
低温化、工程短縮などをもたらすものとして盛ん
に研究開発されている。光CVDの光誘起反応を
生じさせる光源としては、多くは物質に電子励起
を起こし得る紫外光源が用いられてきた。その中
でもパルス紫外光源は、照射する光の特性を適切
に選ぶことにより、照射部からの熱の広がりを抑
えながら光照射部の加熱を行うことができるため
に、微細パターンを直接基板上に形成できる利点
を有する。この種の光源としては、エキシマレー
ザやNd:YAGレーザの第4高調波システムが知
られている。基板を石英、CVDガスとしてCr
(CO)6、レーザ光源としてKrFエキシマレーザを
用いた実験で、高CVD反応過程における光加熱
効果が膜質改善に大きな効果を持つことが、1984
年のコンフアレンス・オン・レーザ・アンド・エ
レクトロ・オプテイクス〔CLEO(Conference
on Lasers and Electro Optics)〕のテクニカル
ダイジエスト FD−6 222ページ記載の論文
で、横山等により明らかにされている。また、光
源としてNd:YAGレーザの第4高調波を用いた
同様な実験と、熱広がりのシミユレーシヨン計算
とから、パルスレーザ光を用いれば、堆積膜の光
照射部からの広がりを1μm以下と微小にできるこ
とが、第27回半導体集積回路シンポジウム(1984
年12月4日)講演論文集ページ6に、森重等によ
り示されている。これらの結果は、繰り返しパル
ス紫外光源が光CVD光源として有用であること
を明らかにしている。
In recent years, in the semiconductor device manufacturing process, process technologies such as optical CVD have been actively researched and developed to lower process temperatures and shorten process steps. Ultraviolet light sources, which can cause electronic excitation in substances, have often been used as light sources to cause photoinduced reactions in photoCVD. Among these, pulsed ultraviolet light sources can heat the light irradiated area while suppressing the spread of heat from the irradiated area by appropriately selecting the characteristics of the irradiated light, so they can form fine patterns directly on the substrate. It has the advantage of being able to As this type of light source, excimer lasers and fourth harmonic systems of Nd:YAG lasers are known. Quartz substrate, Cr CVD gas
In 1984, experiments using a KrF excimer laser as a (CO) 6 laser light source showed that the optical heating effect during the high CVD reaction process had a significant effect on improving film quality.
2019 Conference on Laser and Electro Optics [CLEO (Conference
This was clarified by Yokoyama et al. in a paper published on page 222 of Technical Digest FD-6 (on Lasers and Electro Optics). In addition, similar experiments using the fourth harmonic of an Nd:YAG laser as a light source and simulation calculations of thermal spread revealed that if pulsed laser light is used, the spread of the deposited film from the light irradiated area can be reduced to less than 1 μm. The 27th Semiconductor Integrated Circuit Symposium (1984)
(December 4, 2013), as shown by Morishige et al. on page 6 of the collection of lecture papers. These results demonstrate that repeatedly pulsed UV light sources are useful as optical CVD light sources.
しかしながらこれらの例を含む従来のレーザを
用いたCVD装置では、照射するレーザ光の光強
度はCVD時間中一定に保たれ、その一定値の大
きさを選ぶことだけで最適照射条件を求めていた
ので、この従来の光CVD装置には以下のような
重大な欠点があつた。 However, in conventional laser-based CVD equipment, including these examples, the light intensity of the irradiated laser light is kept constant during the CVD time, and the optimal irradiation conditions are found simply by selecting the magnitude of that constant value. Therefore, this conventional optical CVD apparatus had the following serious drawbacks.
以下に、紫外パルス光源による石英基板上への
Cr(CO)6からのクロム膜形成を例にとつて、従来
装置の欠点とその原因について説明する。石英基
板は、紫外光に対し透明であり、基板の吸収によ
る加熱効果は無視できる。この場合の、CVD膜
の温度上昇について考案する。照射するレーザ光
の強度はCVD時間中一定とする。CVD開始直後
にはレーザ光の吸収は、基板表面に吸着した
CVDガスと気相のCVDガスとにより起こる。こ
の段階では、基板表面の温度上昇は僅かであり、
主に光化学反応による分解物が、基板上に堆積す
る。時間の経過と共に、基板表面の堆積層の厚み
が増加すると、堆積層に吸収されるレーザ光の割
合が増える結果、CVD膜のピーク表面温度は上
昇してゆく。膜温度の上昇は膜の質を向上させる
が、過大な温度上昇は膜の蒸散を起こすため、上
昇させ得る温度には上限がある。膜温度の上昇
は、CVD膜厚が照射レーザ光の吸収長程度の厚
みのとき最大となり、それ以上の厚みになると、
CVD膜の熱容量の増加が原因となつて、膜の温
度上昇は抑えられる。このため、CVD膜厚が照
射レーザ光の吸収長以上の領域では再び膜質が劣
化する。この結果CVD膜の深さ方向に大きな組
成不均一性を生ずる。また堆積開始直後の膜質は
悪く基板への付着力が低い欠点もあつた。また
1μm以上の比較的厚い膜を成長させる場合など
に、表面温度の低下が原因と思われる顕著な表面
荒れが発生し、滑らかな表面を持つ膜の形成が困
難である欠点があつた。 In the following, we will explain how to apply an ultraviolet pulsed light source onto a quartz substrate.
Using chromium film formation from Cr(CO) 6 as an example, we will explain the shortcomings of conventional equipment and their causes. The quartz substrate is transparent to ultraviolet light, and the heating effect due to absorption by the substrate can be ignored. Let us consider the temperature rise of the CVD film in this case. The intensity of the irradiated laser light is constant during the CVD time. Immediately after the start of CVD, the absorption of laser light was absorbed by the substrate surface.
This occurs due to CVD gas and vapor phase CVD gas. At this stage, the temperature rise on the substrate surface is slight;
Decomposition products mainly due to photochemical reactions are deposited on the substrate. As time passes, as the thickness of the deposited layer on the substrate surface increases, the proportion of laser light absorbed by the deposited layer increases, and as a result, the peak surface temperature of the CVD film increases. Increasing the film temperature improves the quality of the film, but an excessive rise in temperature causes evaporation of the film, so there is an upper limit to the temperature that can be raised. The increase in film temperature is maximum when the CVD film thickness is about the absorption length of the irradiated laser beam, and when the thickness increases beyond that,
The increase in heat capacity of the CVD film suppresses the temperature rise of the film. Therefore, in a region where the CVD film thickness is equal to or greater than the absorption length of the irradiated laser beam, the film quality deteriorates again. As a result, large compositional non-uniformity occurs in the depth direction of the CVD film. Another drawback was that the film quality was poor immediately after the start of deposition, and the adhesion to the substrate was low. Also
When growing a relatively thick film of 1 μm or more, significant surface roughness occurs, which is thought to be caused by a drop in surface temperature, making it difficult to form a film with a smooth surface.
本発明の目的は、CVD時間中照射光強度を一
定に保ちながら薄膜形成を行う従来装置の欠点を
除去し、高い付着力を持ち、深さ方向の均一性が
優れるCVD膜の形成を可能とする薄膜形成装置
を提供することにある。
The purpose of the present invention is to eliminate the drawbacks of conventional equipment that forms thin films while keeping the irradiation light intensity constant during CVD time, and to make it possible to form CVD films with high adhesion and excellent uniformity in the depth direction. An object of the present invention is to provide a thin film forming apparatus for forming a thin film.
本発明は、繰り返しパルス光源と、この繰り返
しパルス光源の出射光を基板に導く光学系と、前
記出射光の照射により光化学反応を生ずる気体を
基板上に導くガス供給系と、基板を前記気体の雰
囲気中に保持する機構と前記出射光を導入する窓
とを備えている反応セルとを具備する薄膜形成装
置において、前記光学系には光変調器を設け、か
つ基板上の光照射部の温度を検知する温度モニタ
ユニツトを設け、さらにこの温度モニタユニツト
の出力のピーク信号を求める回路と、前記ピーク
信号と所定の参照信号との差信号を求める回路と
からなる制御ユニツトを設け、前記制御ユニツト
の前記差信号を求める回路の出力信号で前記光変
調器を駆動することを特徴としている。
The present invention provides a repetitive pulse light source, an optical system that guides the emitted light of the repetitive pulse light source to a substrate, a gas supply system that guides a gas that causes a photochemical reaction onto the substrate by irradiation with the emitted light, and a gas supply system that guides the substrate to the substrate. In a thin film forming apparatus comprising a reaction cell having a mechanism for holding in an atmosphere and a window for introducing the emitted light, the optical system is provided with an optical modulator, and the temperature of the light irradiation part on the substrate is adjusted. A temperature monitor unit is provided to detect the temperature, and a control unit is provided which includes a circuit for obtaining a peak signal of the output of the temperature monitor unit and a circuit for obtaining a difference signal between the peak signal and a predetermined reference signal. The optical modulator is driven by an output signal of a circuit for obtaining the difference signal.
従来技術とその問題点の項での記述で明らかと
したCVD膜の付着力や厚み方向の不均一性など
の問題を解決するには、光パルス照射時の膜のピ
ーク温度をCVD時間中に良好な膜質が得られる
温度にほぼ一定に保つことが有効である。そのた
めに、CVD膜の温度を堆積開始直後の時間領域
と、膜厚が光の吸収長よりも厚くなつた時間領域
で、照射強度を高め、堆積時間中のCVD膜のピ
ーク表面温度を膜の蒸散温度のやや下の温度に保
つ。なお堆積開始の際には照射光の吸収がほとん
どないため、十分な堆積物の加熱を起こすに要す
る所要照射強度が著しく高くなり、基板のダメー
ジの発生などが起こる場合もあるので、堆積開始
の際の照射強度は基板ダメージの闘値以下に保つ
ておく。また、堆積前の基板表面の清浄度が、付
着力に大きく関係していることが知られているの
で、堆積開始直後に十分な膜の加熱を行うために
強い光照射を行うことは、光脱離による表面清浄
化も同時に行うことになり、基板との付着力を改
善できる。これらのことから、本発明の装置を用
いて薄膜形成を行えば、膜の厚み方向の不均一性
を解消でき、その結果として、1μm以上の厚い膜
の堆積をも可能にできる。また、基板と薄膜の間
に高い付着力が得られる。
In order to solve the problems such as adhesion of CVD films and non-uniformity in the thickness direction, which were clarified in the description in the section of the prior art and its problems, it is necessary to adjust the peak temperature of the film during light pulse irradiation during CVD time. It is effective to maintain the temperature at a substantially constant level at which good film quality can be obtained. To this end, the temperature of the CVD film is increased in the time region immediately after the start of deposition and in the time region when the film thickness becomes thicker than the light absorption length, and the peak surface temperature of the CVD film during the deposition time is reduced. Keep the temperature slightly below the transpiration temperature. Furthermore, since there is almost no absorption of irradiation light at the start of deposition, the required irradiation intensity required to sufficiently heat the deposit becomes extremely high, which may cause damage to the substrate. Keep the irradiation intensity below the threshold for board damage. In addition, it is known that the cleanliness of the substrate surface before deposition is greatly related to adhesion strength, so it is important to apply strong light irradiation to sufficiently heat the film immediately after the start of deposition. Surface cleaning by desorption is also performed at the same time, and the adhesion to the substrate can be improved. For these reasons, if thin films are formed using the apparatus of the present invention, non-uniformity in the film thickness direction can be eliminated, and as a result, it is possible to deposit films as thick as 1 μm or more. Moreover, high adhesion force can be obtained between the substrate and the thin film.
以下図面を用いて、本発明の実施例を詳細に説
明する。第1図は、本発明の具体的一実施例の構
成図である。この薄膜形成装置は、Qスイツチ
Nd:YAGレーザの第4高調波システムからなる
繰り返しパルス光源1と、出射レーザ光の強度を
減衰させる光減衰器2と、光強度変調を行う光変
調器3と、ミラー4と、スリツト5と、ビームス
プリツタ6と、レンズ7とより成り、繰り返しパ
ルス光源1からの出射レーザ光を基板に導く光学
系を備えている。なお、光減衰器2は本発明の作
用原理の項で述べた堆積開始の際の基板ダメージ
の発生を避けるために用いるものであり、光変調
器3の透過率が最大のときの基板への照射光強度
が基板にダメージを生じない範囲で最大になるよ
う設定する。スリツト5とレンズ7の間に置かれ
たビームスプリツタ6は繰り返しパルス光源1か
らの光は透過し、基板からの赤外光は反射するコ
ーテイングが施されている。
Embodiments of the present invention will be described in detail below with reference to the drawings. FIG. 1 is a block diagram of a specific embodiment of the present invention. This thin film forming device uses a Q switch.
A repetitive pulse light source 1 consisting of a fourth harmonic system of an Nd:YAG laser, an optical attenuator 2 that attenuates the intensity of the emitted laser beam, an optical modulator 3 that modulates the optical intensity, a mirror 4, and a slit 5. , a beam splitter 6, and a lens 7, and includes an optical system that guides the laser beam emitted from the repetitive pulse light source 1 to the substrate. The optical attenuator 2 is used to avoid damage to the substrate at the start of deposition as described in the section on the principle of operation of the present invention, and the optical attenuator 2 is used to prevent damage to the substrate when the transmittance of the optical modulator 3 is at its maximum. The irradiation light intensity is set to be maximum within a range that does not cause damage to the substrate. A beam splitter 6 placed between the slit 5 and the lens 7 is coated with a coating that transmits the light from the pulsed light source 1 and reflects the infrared light from the substrate.
薄膜形成装置は、さらに、ステージ10上に設
置された反応セル11と、この反応セル内に出射
光の照射により光化学反応を生ずる気体を供給す
るガス供給系12とを備えており、反応セル11
は、基板9を前記気体の雰囲気中に保持する機構
と、出射光を導入する窓8とを有している。な
お、ステージ10は、基板9の所要位置に光を照
射させるために用いる。 The thin film forming apparatus further includes a reaction cell 11 installed on the stage 10 and a gas supply system 12 that supplies a gas that causes a photochemical reaction by irradiating the reaction cell with emitted light.
has a mechanism for holding the substrate 9 in the gas atmosphere and a window 8 for introducing the emitted light. Note that the stage 10 is used to irradiate light onto a desired position on the substrate 9.
薄膜形成装置は、後述するようにビームスプリ
ツタ6から反射される赤外光から温度を検出する
赤外線検知方式の温度検出器を持つ温度モニタユ
ニツト14と、このユニツトからの信号に基づい
て、光変調器3を駆動する制御ユニツト13とを
さらに備えている。制御ユニツト13は、温度モ
ニタユニツト14の出力からの光照射時のピーク
温度を求めるピークホールド回路16と、参照温
度に対応する信号を発生する参照信号発生器17
と、参照信号発生器17の出力とピークホールド
回路16との差信号を増幅する差動増幅器15と
から成り、差動増幅器15の出力は光変調器3の
変調端子に入力する構成と成つている。温度モニ
タユニツト14、制御ユニツト13および光変調
器3は基板上に堆積する薄膜の表面温度が薄膜の
最適成長温度範囲内の値になるよう照射光強度の
フイードバツク制御を行う。つまり、温度モニタ
ユニツト14で測定されたピーク温度が参照温度
よりも高ければ光変調器3の透過率を下げること
により照射光強度を下げ、また逆にピーク温度が
低ければ照射光強度を上げるよう制御を行う。以
上のように構成された薄膜形成装置において、基
板9上へCr(CO)6からクロム膜を形成する場合の
動作を以下に説明する。 The thin film forming apparatus includes a temperature monitor unit 14 having an infrared detection type temperature detector that detects temperature from infrared light reflected from the beam splitter 6, as described later, and a temperature monitor unit 14 that detects the temperature based on the signal from this unit. It further includes a control unit 13 for driving the modulator 3. The control unit 13 includes a peak hold circuit 16 that determines the peak temperature during light irradiation from the output of the temperature monitor unit 14, and a reference signal generator 17 that generates a signal corresponding to the reference temperature.
and a differential amplifier 15 that amplifies the difference signal between the output of the reference signal generator 17 and the peak hold circuit 16, and the output of the differential amplifier 15 is input to the modulation terminal of the optical modulator 3. There is. The temperature monitor unit 14, the control unit 13, and the optical modulator 3 perform feedback control of the irradiation light intensity so that the surface temperature of the thin film deposited on the substrate is within the optimum growth temperature range of the thin film. In other words, if the peak temperature measured by the temperature monitor unit 14 is higher than the reference temperature, the transmittance of the optical modulator 3 is lowered to lower the intensity of the irradiated light, and conversely, if the peak temperature is lower, the intensity of the irradiated light is increased. Take control. In the thin film forming apparatus configured as described above, the operation of forming a chromium film from Cr(CO) 6 on the substrate 9 will be described below.
まず、ガスの供給ユニツト12はArガスをキ
ヤリアガスとしてCr(CO)6蒸気を反応セル11に
供給する。次に、ステージ10を用いて基板9を
所要位置まで移動させる。繰り返しパルス光源1
が駆動されると、繰り返しパルス光が出射され、
光減衰器2、光変調器3、ミラー4、スリツト
5、レンズ7を経て、反応セル11内の基板上9
に照射され、基板9上にクロム膜の堆積が開始す
る。堆積開始時には、フイードバツクループによ
り光変調器3は透過率が最大になるように設定さ
れており、光源1からのパルス光は光減衰器2に
より、基板9への照射光強度が基板9にダメージ
を生じない範囲で最大になるよう設定される。こ
のため堆積開始直後の照射光強度は高く、光脱離
による表面清浄化が行われる。クロム膜が堆積し
始めると、照射光の吸収が大きくなり、基板上の
光照射部の温度が上昇する。基板からの赤外光は
レンズ7を経て、ビームスプリツタ6により反射
され温度モニタユニツト14の温度検出器に入射
される。温度検出器は入射する赤外光に基づいて
基板上の光照射部の温度を検知する。検知された
温度は、制御ユニツト13のピークホールド回路
16に入力される。ピークホールド回路は入力さ
れる温度のピーク値をホールドすると、差動増幅
器15の一方の入力端子に入力する。一方、参照
信号発生器17は参照温度に対応する信号を発生
し、差動増幅器15の他方の入力端子に入力す
る。差動増幅器15は参照信号発生器17の出力
とピークホールド回路16の出力との差信号を増
幅し、増幅された差信号を光変調器3の変調端子
に入力する。光変調器3は、差動増幅器15の出
力に基づいてその透過率を変える。以上のような
フイードバツクループにより、基板19の光照射
部のピーク温度は、常に最適温度範囲になるよう
に制御される。 First, the gas supply unit 12 supplies Cr(CO) 6 vapor to the reaction cell 11 using Ar gas as a carrier gas. Next, the stage 10 is used to move the substrate 9 to a desired position. Repeated pulse light source 1
When driven, pulsed light is emitted repeatedly,
After passing through the optical attenuator 2, the optical modulator 3, the mirror 4, the slit 5, and the lens 7, the light is transmitted to the substrate 9 in the reaction cell 11.
The chromium film starts to be deposited on the substrate 9. At the start of deposition, the optical modulator 3 is set to maximize transmittance by the feedback loop, and the pulsed light from the light source 1 is controlled by the optical attenuator 2 to reduce the intensity of the light irradiated onto the substrate 9. It is set to the maximum value within a range that does not cause damage. Therefore, the intensity of the irradiated light is high immediately after the start of deposition, and surface cleaning is performed by photodesorption. When the chromium film begins to accumulate, the absorption of the irradiated light increases and the temperature of the light irradiated area on the substrate rises. The infrared light from the substrate passes through the lens 7, is reflected by the beam splitter 6, and enters the temperature detector of the temperature monitor unit 14. The temperature detector detects the temperature of the light irradiation part on the substrate based on the incident infrared light. The detected temperature is input to the peak hold circuit 16 of the control unit 13. When the peak hold circuit holds the peak value of the input temperature, it inputs it to one input terminal of the differential amplifier 15. On the other hand, the reference signal generator 17 generates a signal corresponding to the reference temperature and inputs it to the other input terminal of the differential amplifier 15. The differential amplifier 15 amplifies the difference signal between the output of the reference signal generator 17 and the output of the peak hold circuit 16, and inputs the amplified difference signal to the modulation terminal of the optical modulator 3. The optical modulator 3 changes its transmittance based on the output of the differential amplifier 15. By the feedback loop as described above, the peak temperature of the light irradiation portion of the substrate 19 is controlled so as to always be within the optimum temperature range.
照射光の吸収が少ない基板の場合、堆積開始の
際には変調器3の透過率がフイードバツクループ
の動作により最大となつても、基板表面温度は
CVD膜の最適温度範囲の温度にまで届かないこ
とが起こり得るが、その場合にも基板上にごくわ
ずかにCVD膜が堆積した後には、基板上の光照
射部のピーク温度はフイードバツクループにより
常に最適温度範囲になるよう制御される。最適温
度範囲はCr(CO)6の場合およそ800℃から1200℃
の範囲であり、このとき金属光沢があり表面の滑
らかな良好な膜が堆積し、温度が800℃より低い
と透明で表面荒れが激しい膜が堆積し、逆に1200
℃よりも高い場合、膜の一部に蒸散による穴の発
生が見られた。光照射強度は、堆積開始時に
10MW/cm2、開始後5秒後に2MW/cm2、開始後
10秒後に2.5MW/cm2とした場合に厚み0.3μmで、
堆積開始直後の悪い膜質の堆積層がなく、また、
膜の厚み方向の均一性も大きく改善された良好な
Cr膜の堆積が得られた。またこのときの基板と
薄膜の付着力は、基板9に洗浄を施さない場合で
もピンセツトによる引つかき試験ではがれないほ
ど強いことがわかつた。 In the case of a substrate that absorbs little irradiated light, even if the transmittance of the modulator 3 reaches its maximum due to the operation of the feedback loop at the start of deposition, the substrate surface temperature will remain low.
It may happen that the temperature does not reach the optimum temperature range of the CVD film, but even in that case, after a very small amount of the CVD film has been deposited on the substrate, the peak temperature of the light irradiated area on the substrate will become a feedback loop. The temperature is always controlled to be within the optimum temperature range. The optimum temperature range is approximately 800°C to 1200°C for Cr(CO) 6
At this time, a good film with a metallic luster and a smooth surface is deposited, and when the temperature is lower than 800°C, a transparent film with a severely rough surface is deposited;
When the temperature was higher than ℃, holes were observed in some parts of the film due to transpiration. The light irradiation intensity is set at the start of deposition.
10MW/cm 2 , 5 seconds after starting 2MW/cm 2 , after starting
At 2.5MW/ cm2 after 10 seconds, the thickness is 0.3μm,
There is no deposited layer with poor quality immediately after the start of deposition, and
The uniformity of the film in the thickness direction has also been greatly improved.
A deposit of Cr film was obtained. It was also found that the adhesion force between the substrate and the thin film at this time was so strong that it did not come off in a pull test using tweezers even when the substrate 9 was not cleaned.
上記の実施例の説明では、CVDガスをCr(CO)
6とした場合について述べたが、他の金属や半導
体もしくは絶縁体用のCVD材料でも良好なCVD
膜を得る上で光加熱効果が重要な働きを持つ材料
であれば本発明が有効になることは自明である。
また光加熱効果を必要としないCVDでも付着力
の改善に光洗浄効果が有効な基板であれば、本発
明により付着力を大きく改善できる。また、上記
実施例では繰り返しパルス光源としてNd:YAG
レーザの第4高調波を用いた場合について説明し
たが、パルス光による加熱効果が影響する点では
他の可視光パルスレーザ光源や、連続発振光源を
チヨツパで分割してパルス化した光源でも本発明
の効果を期待できることから、これらの光源を用
いて本発明による装置を実現できることは言うま
でもない。 In the above example description, the CVD gas is Cr(CO)
6 , but good CVD can be achieved with other metals, semiconductors, or insulators.
It is obvious that the present invention is effective for materials in which the optical heating effect plays an important role in obtaining a film.
Furthermore, even in CVD that does not require a photoheating effect, the present invention can greatly improve adhesion as long as the substrate has a photocleaning effect that is effective in improving adhesion. In addition, in the above embodiment, Nd:YAG was used as the repetitive pulse light source.
Although the case where the fourth harmonic of a laser is used has been described, the present invention can also be applied to other visible light pulsed laser light sources or a light source made by dividing a continuous wave light source into pulses with a chopper, in that the heating effect of the pulsed light is affected. Since these effects can be expected, it goes without saying that the apparatus according to the present invention can be realized using these light sources.
以上述べたように、従来装置による薄膜形成で
は、基板との密着性や膜の厚み方向の均一性のよ
い膜を堆積させることが難しかつた材料や基板に
対しても、本発明の堆積時間中のCVD膜のピー
ク温度が常に最適範囲になるよう照射光強度を時
間的に制御する装置によれば、付着力が高くかつ
膜の均一性の優れた良好なCVD膜を得ることが
可能となる。
As described above, the deposition time of the present invention can be applied to materials and substrates for which it is difficult to deposit a film with good adhesion to the substrate and uniformity in the thickness direction when forming thin films using conventional equipment. Using a device that temporally controls the intensity of the irradiated light so that the peak temperature of the CVD film inside is always within the optimum range, it is possible to obtain a good CVD film with high adhesion and excellent film uniformity. Become.
第1図は、本発明の一実施例の概略的構成図で
ある。
1……繰り返しパルス光源、2……光減衰器、
3……光変調器、4……ミラー、5……スリツ
ト、6……ビームスプリツタ、7……レンズ、8
……窓、9……基板、10……ステージ、11…
…反応セル、12……ガスの供給ユニツト、13
……制御ユニツト、14……温度モニタユニツ
ト、15………差動増幅器、16……ピークホー
ルド回路、17……参照信号発生器。
FIG. 1 is a schematic diagram of an embodiment of the present invention. 1... Repeated pulse light source, 2... Optical attenuator,
3... Optical modulator, 4... Mirror, 5... Slit, 6... Beam splitter, 7... Lens, 8
... window, 9 ... board, 10 ... stage, 11 ...
...Reaction cell, 12... Gas supply unit, 13
... Control unit, 14 ... Temperature monitor unit, 15 ... Differential amplifier, 16 ... Peak hold circuit, 17 ... Reference signal generator.
Claims (1)
光源の出射光を基板に導く光学系と、前記出射光
の照射により光化学反応を生ずる気体を基板上に
導くガス供給系と、基板を前記気体の雰囲気中に
保持する機構と前記出射光を導入する窓とを備え
ている反応セルとを具備する薄膜形成装置におい
て、前記光学系には光変調器を設け、かつ基板上
の光照射部の温度を検知する温度モニタユニツト
を設け、さらにこの温度モニタユニツトの出力の
ピーク信号を求める回路と、前記ピーク信号と所
定の参照信号との差信号を求める回路とからなる
制御ユニツトを設け、前記制御ユニツトの前記差
信号を求める回路の出力信号で前記光変調器を駆
動することを特徴とする薄膜形成装置。1 A repetitive pulse light source, an optical system that guides the emitted light of the repetitive pulse light source to the substrate, a gas supply system that guides a gas that causes a photochemical reaction onto the substrate by irradiation with the emitted light, and a substrate that is placed in an atmosphere of the gas. In a thin film forming apparatus comprising a holding mechanism and a reaction cell having a window for introducing the emitted light, the optical system is provided with a light modulator and detects the temperature of the light irradiation part on the substrate. A temperature monitor unit is provided, and a control unit is provided which includes a circuit for obtaining a peak signal of the output of the temperature monitor unit and a circuit for obtaining a difference signal between the peak signal and a predetermined reference signal, A thin film forming apparatus characterized in that the optical modulator is driven by an output signal of a circuit for obtaining the signal.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15596285A JPS6217178A (en) | 1985-07-17 | 1985-07-17 | Thin film forming device |
| EP86109787A EP0209131B1 (en) | 1985-07-17 | 1986-07-16 | Optical cvd method with a strong optical intensity used during an initial period and device therefor |
| DE8686109787T DE3682716D1 (en) | 1985-07-17 | 1986-07-16 | OPTICAL METHOD FOR PRODUCING LAYERS FROM THE GAS PHASE WITH A STRONG OPTICAL INTENSITY DURING THE BEGINNING PHASE, AND DEVICE THEREFOR. |
| US06/886,125 US4711790A (en) | 1985-07-17 | 1986-07-16 | Optical CVD method with a strong optical intensity used during an initial period and device therefor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15596285A JPS6217178A (en) | 1985-07-17 | 1985-07-17 | Thin film forming device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6217178A JPS6217178A (en) | 1987-01-26 |
| JPH0520504B2 true JPH0520504B2 (en) | 1993-03-19 |
Family
ID=15617338
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15596285A Granted JPS6217178A (en) | 1985-07-17 | 1985-07-17 | Thin film forming device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6217178A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4959244A (en) * | 1989-03-27 | 1990-09-25 | General Electric Company | Temperature measurement and control for photohermal processes |
-
1985
- 1985-07-17 JP JP15596285A patent/JPS6217178A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6217178A (en) | 1987-01-26 |
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