JPH02260637A - Photochemical reaction and device therefor - Google Patents

Photochemical reaction and device therefor

Info

Publication number
JPH02260637A
JPH02260637A JP8257289A JP8257289A JPH02260637A JP H02260637 A JPH02260637 A JP H02260637A JP 8257289 A JP8257289 A JP 8257289A JP 8257289 A JP8257289 A JP 8257289A JP H02260637 A JPH02260637 A JP H02260637A
Authority
JP
Japan
Prior art keywords
gas
reaction
photochemical
substrate
photochemical reaction
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.)
Pending
Application number
JP8257289A
Other languages
Japanese (ja)
Inventor
Kenji Shibata
芝田 健二
Hiroshi Yuasa
博司 湯浅
Saburo Adaka
阿高 三郎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Power Ltd
Original Assignee
Babcock Hitachi KK
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Babcock Hitachi KK filed Critical Babcock Hitachi KK
Priority to JP8257289A priority Critical patent/JPH02260637A/en
Publication of JPH02260637A publication Critical patent/JPH02260637A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To prevent the cloud of a window and to perform a uniform film formation by a method wherein two kinds or more of gases for producing active species are separately supplied in a reaction space through the blow-off nozzles of porous plates made of a sintered body consisting of heat-resistant particles, the gas, with which a solid matter is not generated, is supplied to the side of the light-transmitting window and the gas, with which a solid matter is generated, is supplied to the side of a substrate. CONSTITUTION:Porous plates 5a and 5b obtainable by sintering a metal consisting of fine particles of a particle diameter of 0.2 to 500mum are made on the side surface of a reaction chamber. Each reaction gas obtainable by diluting respectively O2 and monosilane with N2 or the like is supplied in a reaction space keeping their respective linear speeds V in a range of 0.01<=V<=8 (N.cm/s). In the reaction space, the ratio Rv of the linear speed of the O2- containing gas to the linear speed or the monosilane-containing gas is selected in 0.7<=Rv<=1.2, the total pressure Pt is selected in 0.3Torr or higher, the molar fraction of the monosilane- containing gas is selected in 0.001 or higher and tn 0.2 or lower and the molar fraction of the O2-containing gas is selected in the quantum theory ratio or higher of the monosilane- containing gas. The number Rv of rotations of a substrate is selected in 0.01<=Rv<=20 and active species are produced by the light of light sources 4 through a window 22. According to this constitution, the cloud of the window is prevented and a uniform thin film can be formed on the substrate.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光化学反応方法及び装置に係り、特に光透過窓
の曇り防止と共に均一成膜を達成するのに好適な光化学
反応方法及び装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a photochemical reaction method and apparatus, and more particularly to a photochemical reaction method and apparatus suitable for preventing fogging of a light-transmitting window and achieving uniform film formation.

〔従来の技術〕[Conventional technology]

光化学反応は反応性ガスにそのガスの吸収波長に応じた
波長を有する光を照射することにより化学反応を促進す
るものである。照射する光と反応ガスとの組合せにより
反応を選択的に進行させることが可能である。さらに光
化学反応は熱化学反応のような高温が要求されないので
プロセスの低温化に有効であり、プラズマ反応のような
荷電粒子の影響がないため、堆積した膜やエツチングし
た下地の膜の損傷がないことから、シリコン酸化膜の形
成に有効であると考えられている。
A photochemical reaction promotes a chemical reaction by irradiating a reactive gas with light having a wavelength corresponding to the absorption wavelength of the gas. It is possible to selectively advance the reaction by combining the irradiated light and the reaction gas. Furthermore, photochemical reactions do not require high temperatures like thermochemical reactions, so they are effective in lowering the process temperature, and unlike plasma reactions, they are not affected by charged particles, so there is no damage to deposited films or etched underlying films. Therefore, it is considered to be effective in forming a silicon oxide film.

しかしながら、光化学反応を用いた薄膜製造装置では、
反応容器内に反応ガスを供給し、基板上に薄膜を堆積さ
せるものであるため、光透過窓の表面に反応生成物が付
着し、反応容器内の光の強度を低下させる他、析出物の
落下によるパーティクル生成の問題がある。
However, in thin film manufacturing equipment using photochemical reactions,
Since a reaction gas is supplied into the reaction vessel and a thin film is deposited on the substrate, reaction products adhere to the surface of the light-transmitting window, reducing the intensity of light inside the reaction vessel. There is a problem with particle generation due to falling.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

光化学反応装置では、反応室内の基板上に、例えばSi
nオが析出すると同時に光透過窓面にもS i Otが
析出する。光透過窓面の温度は、基板面の温度よりも低
く、光透過窓面に析出するStO!は、緻密性が低く、
紫外光を吸収・散乱するため、光透過窓における透過光
強度を低下させる要因となっている。
In a photochemical reaction device, for example, Si is deposited on a substrate in a reaction chamber.
At the same time that nO is precipitated, S i Ot is also precipitated on the light transmitting window surface. The temperature of the light transmitting window surface is lower than the temperature of the substrate surface, and StO! precipitates on the light transmitting window surface. is less dense,
Since it absorbs and scatters ultraviolet light, it is a factor that reduces the intensity of transmitted light in the light transmission window.

一般的に光化学反応方法では、基板温度・反応ガス組成
比・圧力を一定に保った条件下では、基板上に堆積する
薄膜の成膜速度は、光の照射強度に比例して速くなるこ
とが知られている。したがって、光透過窓面にSin、
が析出することは、薄膜の成膜速度を径時的に低下させ
るばかりでなく、均一に成膜させることを困難なものと
している。
In general, in the photochemical reaction method, under conditions where the substrate temperature, reaction gas composition ratio, and pressure are kept constant, the deposition rate of the thin film on the substrate increases in proportion to the light irradiation intensity. Are known. Therefore, Sin,
The precipitation not only reduces the deposition rate of the thin film over time, but also makes it difficult to uniformly deposit the film.

本発明の目的は、上記した従来技術の課題を解決し、光
透過窓に対する析出物による窓曇りを防止し、かつ均一
な成膜を可能とした光化学反応方法及び装置を提供する
ことにある。
An object of the present invention is to provide a photochemical reaction method and apparatus that solves the problems of the prior art described above, prevents fogging of the light-transmitting window due to precipitates, and enables uniform film formation.

〔課題を解決するための手段〕[Means to solve the problem]

上記した目的を達成するために、本発明の方法は耐熱性
粒子を焼結した微細連通孔を多数有する焼結体からなる
多孔板で形成されたガス吹き出し口から光励起によって
活性種を生成する2種以上のガスを各々別個に反応空間
に供給するようにし、光透過窓側は固形物を生成しない
反応ガス、基板側はこの反応ガスと反応して固形物を生
成するガスとしたものである。
In order to achieve the above-mentioned object, the method of the present invention generates active species by photoexcitation from a gas outlet formed of a porous plate made of a sintered body having a large number of fine communication holes made by sintering heat-resistant particles. More than one type of gas is separately supplied to the reaction space, with the light-transmitting window side being a reactive gas that does not produce solid matter, and the substrate side being a gas that reacts with this reactive gas to produce solid matter.

また、本発明の装置は、耐熱性粒子を焼結した微細連通
孔を多数有する焼結体からなる多孔板で形成したガス吹
き出し口を備えたガス供給部を反応室側面に設け、この
ガス吹き出し口における反応空間と反対面の反応室側面
にガス排気口を備えたガス排気部を設けると共にガス吹
き出し口を上下に2段以上に区画し、ガス排気部奥行を
ガス吹き出し口と、はぼ同等の大きさに形成したもので
ある。・本発明の光化学反応方法において、反応空間に
反応ガスを供給するガス吹き出し口は、耐熱性粒子を焼
結した微細連通孔を多数有する焼結体からなる多孔板で
形成される。耐熱性粒子としては、特にOo−1p〜1
m、好ましくは0.2μm 〜500μmの平均粒子か
らなる金属粒子又はセラミックス粒子の焼結体が望まし
い。
Further, the apparatus of the present invention is provided with a gas supply section on the side surface of the reaction chamber, which is equipped with a gas outlet formed of a perforated plate made of a sintered body having a large number of fine communication holes made by sintering heat-resistant particles. A gas exhaust section with a gas exhaust port is provided on the side of the reaction chamber opposite to the reaction space at the mouth, and the gas outlet is divided into two or more stages vertically, so that the depth of the gas exhaust section is approximately the same as that of the gas outlet. It was formed to the size of . - In the photochemical reaction method of the present invention, the gas outlet for supplying the reaction gas to the reaction space is formed of a porous plate made of a sintered body having a large number of fine communication holes formed by sintering heat-resistant particles. As the heat-resistant particles, especially Oo-1p~1
A sintered body of metal particles or ceramic particles having an average particle size of 0.2 μm to 500 μm is desirable.

上記のようなガス吹き出し口から光励起によって活性種
を生成する2種以上のガスが一各々別個に反応空間に供
給される。ここで光励起によって活性種を生成するガス
は、基板に堆積させるための薄膜の成分によって任意に
選定される。
Two or more types of gases that generate active species by photoexcitation are each separately supplied to the reaction space from the gas outlet as described above. Here, the gas that generates active species upon photoexcitation is arbitrarily selected depending on the components of the thin film to be deposited on the substrate.

例えば、基板側の反応空間には周期表111B族元素若
しくはIVB族元素を含むガス、Taを含むガス又は周
期表VIA族元素とIVB族元素とを含むガスを用いる
ことができる。したがって、上記の各元素はそれら元素
に応じて塩化物、水素化物等のガス化可能な化合物の形
態とされて使用される。
For example, a gas containing an element of group 111B or group IVB of the periodic table, a gas containing Ta, or a gas containing an element of group VIA and group IVB of the periodic table can be used in the reaction space on the substrate side. Therefore, each of the above elements is used in the form of a gasifiable compound such as a chloride or a hydride depending on the element.

光透過窓側の反応空間には基板に堆積させるべき上記元
素の酸化物又は、窒化物に応じてOl又はN H’sを
含むガスが使用される。基板側に供給されるガス及び光
透過窓側に供給されるガスは必要に応じて各々不活性ガ
スにより希釈されるが、希釈ガスとしては第0族の稀ガ
ス、特にN8ガスが好適である。
A gas containing Ol or NH's is used in the reaction space on the light transmission window side, depending on the oxide or nitride of the above element to be deposited on the substrate. The gas supplied to the substrate side and the gas supplied to the light transmission window side are each diluted with an inert gas as necessary, and the dilution gas is preferably a Group 0 rare gas, particularly N8 gas.

基板上にSin、を堆積する場合、基板側の反応空間部
にはモノシラン(S i H4) 、ジシラン(Siz
H−)、)ジシラン(SisHs)等の高次シラン、ジ
メチルシラン [S i Ht(CHs)オl。
When depositing Sin on a substrate, monosilane (S i H4) and disilane (Siz
Higher order silanes such as H-), )disilane (SisHs), dimethylsilane [S i Ht(CHs)ol.

テトラエトキシシラン [S (OCg Hs ) 4
]等の有機シラン系ガスが好適に使用され、光透過窓例
の反応空間には(18又はN2で希釈されたOtが供給
される。また、基板上にシリコン窒化膜を堆積させる場
合には、基板側の反応空間に上記のシラン系化合物から
なるガスが供給され、光透過窓側の反応空間にNH,を
含むガスが供給される。
Tetraethoxysilane [S (OCg Hs) 4
] is preferably used, and Ot diluted with (18 or N2) is supplied to the reaction space of the light transmission window example.Also, when depositing a silicon nitride film on the substrate, A gas made of the above silane compound is supplied to the reaction space on the substrate side, and a gas containing NH is supplied to the reaction space on the light transmission window side.

特にシリコン酸化膜を形成する場合には、光透過窓側の
反応空間に(18をN2で希釈した第1の反応ガスを供
給し、基板側の反応空間にS i H4を’Nxで希釈
した第2の反応ガスをそれぞれ多孔板からなるガス吹き
出し口から噴流を生じないように供給することが望まし
い。
In particular, when forming a silicon oxide film, a first reaction gas (18 diluted with N2) is supplied to the reaction space on the light transmission window side, and a first reaction gas (18 diluted with Nx) is supplied to the reaction space on the substrate side. It is desirable that the two reaction gases be supplied from gas outlets each made of a perforated plate so as not to generate jets.

本発明において、光源としては低圧水銀ランプの他に重
水素ランプ、エキシマレーザ等を使用することもできる
In the present invention, as a light source, a deuterium lamp, excimer laser, etc. can also be used in addition to a low-pressure mercury lamp.

上記した反応ガスを反応空間に供給させる際は、操作条
件によって反応空間に整流状態で導入されるガスの特性
を維持し、均一成膜を達成することができる。これらの
操作条件としては、反応ガスの線速度、光透過窓例の反
応ガスと基板側の反応ガスの線速度比、反応空間の全圧
、反応ガスのモル分率、反応空間における基板の回転数
等が挙げられる0例えば反応ガスの線速度は0.01≦
V≦8(N−cm/s)、光透過窓側の反応ガスの線速
度/基板側の反応ガスの線速度の比は、0.7≦Rv≦
1.2、反応空間の全圧はPt≧0.3Torr、基板
側の反応空間に導入される有機シラン化合物を含むガス
(例えば5iHa)の5i)(。
When the above-mentioned reaction gas is supplied to the reaction space, the characteristics of the gas introduced into the reaction space in a rectified state can be maintained depending on the operating conditions, and uniform film formation can be achieved. These operating conditions include the linear velocity of the reaction gas, the linear velocity ratio of the reaction gas in the light transmission window example and the reaction gas on the substrate side, the total pressure in the reaction space, the molar fraction of the reaction gas, and the rotation of the substrate in the reaction space. For example, the linear velocity of the reaction gas is 0.01≦
V≦8 (N-cm/s), the ratio of the linear velocity of the reaction gas on the light transmission window side/the linear velocity of the reaction gas on the substrate side is 0.7≦Rv≦
1.2. The total pressure of the reaction space is Pt≧0.3 Torr, and the gas (for example, 5iHa) containing an organic silane compound is introduced into the reaction space on the substrate side.

モル分率は0.001≦m5iH,≦0.2、光透過窓
側の反応空間に導入される0□モル分率は5tH4の量
論比以上、反応空間に配置される基板の回転数は0.0
1≦Rr≦20(rpm)とすることが望ましい。
The mole fraction is 0.001≦m5iH,≦0.2, the 0□ mole fraction introduced into the reaction space on the light transmission window side is more than the stoichiometric ratio of 5tH4, and the rotation speed of the substrate placed in the reaction space is 0. .0
It is desirable that 1≦Rr≦20 (rpm).

上記のように操作条件によって、光透過窓の光透過率を
大概95%以上に保持でき、膜厚を均一なものとするこ
とができる。
As described above, depending on the operating conditions, the light transmittance of the light transmitting window can be maintained at approximately 95% or more, and the film thickness can be made uniform.

〔作用〕[Effect]

微細連通孔を有する焼結体からなる多孔板から、反応空
間に導入される反応ガスは、光源から光透過窓を透過し
た光エネルギーによって励起・分解し、所定の反応生成
物が基板に堆積する。このとき、反応ガスは多孔板から
なるガス吹き出し口が少な(とも2段に区画されており
、光透過窓側と基板側に分離されて整流状態で反応空間
を流れる。
The reaction gas introduced into the reaction space through a porous plate made of a sintered body with fine communication holes is excited and decomposed by the light energy transmitted from the light source through the light transmission window, and predetermined reaction products are deposited on the substrate. . At this time, the reaction gas flows through the reaction space in a rectified state, separated into a light-transmitting window side and a substrate side, with a small number of gas blow-off ports made of a porous plate (both partitioned into two stages).

そして、上記した各操作条件に設定すると、光透過窓側
とガス流れと基板側のガス流の混合1巻き込みが防止さ
れて、光透過窓の光透過率を高度に維持し、均一な膜厚
が保障される。
When the above operating conditions are set, mixing and entrainment of the gas flow on the light transmission window side, the gas flow on the substrate side, and the gas flow on the substrate side are prevented, the light transmittance of the light transmission window is maintained at a high level, and a uniform film thickness is achieved. Guaranteed.

〔実施例〕〔Example〕

以下、本発明の実施例を図面に基づいて説明する。 Embodiments of the present invention will be described below based on the drawings.

第1図は本発明の光化学反応装置の一実施例を示す縦断
面図、第2図は第1図におけるガス供給部及びガス排気
部の詳細図である。
FIG. 1 is a longitudinal sectional view showing one embodiment of the photochemical reaction device of the present invention, and FIG. 2 is a detailed view of the gas supply section and gas exhaust section in FIG. 1.

この光化学反応装置は、第1図に示すように反応室1と
予備室2とから主として構成され、反応室lと予備室2
との間はゲート機構3を介して開閉自在に連通されてい
る。反応室1は、室内上部に複数本の低圧水銀ランプ4
が並設され、室内中段部にガス供給部5及びガス排気部
6が配設されている0反応室1の底部には複数本のヒー
タ7が並設され、反応室底部中心部にはその上端面にサ
セプタ8を有する基板回転昇降機構9が設けられている
As shown in FIG. 1, this photochemical reaction device mainly consists of a reaction chamber 1 and a preliminary chamber 2.
The gate mechanism 3 is connected to the gate mechanism 3 so as to be freely openable and closable. The reaction chamber 1 has multiple low-pressure mercury lamps 4 installed in the upper part of the chamber.
A plurality of heaters 7 are arranged in parallel at the bottom of the reaction chamber 1, in which a gas supply section 5 and a gas exhaust section 6 are arranged in the middle part of the chamber. A substrate rotating/elevating mechanism 9 having a susceptor 8 on the upper end surface is provided.

予備室2には、搬送アーム10及び搬送アーム11を備
えた基板搬送機構12が設けられ、基板搬送機構12に
隣接して設けられた基板仮置台13はエアシリンダ14
の作動によって昇降自在となっており、ベロー15によ
るシール構造となっている。また、予備室2内の排気を
行うための排気口16と搬送アーム11による基板搬送
口の開閉を行うためのゲート機構17が設けられている
The preliminary chamber 2 is provided with a substrate transfer mechanism 12 including a transfer arm 10 and a transfer arm 11, and a substrate temporary storage table 13 provided adjacent to the substrate transfer mechanism 12 is equipped with an air cylinder 14.
It can be raised and lowered by the operation of the bellows 15, and has a sealing structure with bellows 15. Further, an exhaust port 16 for evacuating the interior of the preliminary chamber 2 and a gate mechanism 17 for opening and closing the substrate transfer port by the transfer arm 11 are provided.

反応室1に設けられるガス供給部5は第2図に示すよう
にガス吹き出し面が多孔板5aで形成された箱型ガス供
給部5cと、ガス吹き出し面が多孔板5bで形成された
箱型ガス供給部5dとを積み重ねた構造となっている。
As shown in FIG. 2, the gas supply section 5 provided in the reaction chamber 1 includes a box-shaped gas supply section 5c whose gas blowing surface is formed of a perforated plate 5a, and a box-shaped gas supply section whose gas blowing surface is formed of a perforated plate 5b. It has a structure in which gas supply sections 5d are stacked.

ガス排気部6の奥行は多孔板5a及び5bからなるガス
吹き出し面とほぼ同一面積となっており、下方に延設さ
れた排気口を備えている。
The depth of the gas exhaust section 6 is approximately the same area as the gas blowing surface made up of the perforated plates 5a and 5b, and is provided with an exhaust port extending downward.

多孔板5a、5bは、微細な連通孔を有する多孔質物質
で構成されており、多孔質物質には、例えば平均粒径が
0.1um〜1■、好ましくは0.2μm〜500μm
の金属粒子若しくはセラミックスの焼結体又はテフロン
等の耐熱性樹脂等で形成可能であるが、特に金属粒子の
焼結体が望ましい。
The porous plates 5a and 5b are made of a porous material having fine communicating holes, and the porous material has an average particle size of, for example, 0.1 um to 1 μm, preferably 0.2 μm to 500 μm.
Although it can be formed from a sintered body of metal particles or ceramics, or a heat-resistant resin such as Teflon, a sintered body of metal particles is particularly desirable.

低圧水銀ランプ4とガス供給部5及びガス排気部6との
間の領域には、第1図及び第2図に示すようにそれぞれ
の反応室壁面に対し直交する4本のロッド18が各々シ
ール部19を介して接続されたアクチュエータ20によ
って各ロッド18の軸を中心に90°Cの角度で回動可
能となっている。
In the area between the low-pressure mercury lamp 4, the gas supply section 5, and the gas exhaust section 6, four rods 18 perpendicular to the wall surface of each reaction chamber are provided with seals, as shown in FIGS. 1 and 2. An actuator 20 connected through a portion 19 allows each rod 18 to rotate about its axis at an angle of 90°.

そして各ロッド1日に固定された支持板21はロッド1
8の回動に伴い、ロッド18を支点として第2図に示す
水平面から垂直面に揺動可能となっている。
And the support plate 21 fixed on each rod 1 is
8, it can swing from a horizontal plane to a vertical plane as shown in FIG. 2 using the rod 18 as a fulcrum.

また、支持板21が水平面に配置されたときに、反応空
間の中心部に円形状の空間部が形成されるようになって
いる。なお、24はプレートを示している。
Furthermore, when the support plate 21 is placed on a horizontal plane, a circular space is formed at the center of the reaction space. Note that 24 indicates a plate.

この光化学反応装置では搬送アーム10を水平面で回動
させると、搬送アームlOに対する搬送アームの軸交叉
角度が変化して搬送アーム11はゲート機構17上方の
予備室外部、予備室21反応室1内を移動することによ
って光透過窓22゜基板23を搬送する。
In this photochemical reaction device, when the transfer arm 10 is rotated in a horizontal plane, the axis intersection angle of the transfer arm with respect to the transfer arm IO changes, and the transfer arm 11 is moved between the outside of the preliminary chamber above the gate mechanism 17 and the inside of the preliminary chamber 21 and the reaction chamber 1. The substrate 23 is transported through the light transmitting window 22 by moving the light transmitting window 22 .

そして、昇降回転機構9を介して光透過窓22を支持板
21で支持し、一方、昇降回転機構9上端に設置された
サセプタ8を第2図に示す位置に配置する。
Then, the light transmitting window 22 is supported by the support plate 21 via the elevating and rotating mechanism 9, while the susceptor 8 installed at the upper end of the elevating and rotating mechanism 9 is placed at the position shown in FIG.

そして10−’Torrオーダまで排気され、反応室1
内のヒータ7によってサセプタ8上の基板23は所定の
温度まで加熱される。
Then, the reaction chamber 1 is evacuated to the order of 10-' Torr.
The substrate 23 on the susceptor 8 is heated to a predetermined temperature by the heater 7 inside.

次に、例えば0.又はN、で希釈されたO!が焼結多孔
板5aを経て整流となって反応空間に導入され、一方、
SiH,又はN!で希釈された5iHaが焼結多孔体5
bを経て整流となって反応空間に導入される。
Next, for example 0. or O! diluted with N! is introduced into the reaction space through the sintered porous plate 5a as a rectified flow, and on the other hand,
SiH, or N! 5iHa diluted with sintered porous body 5
It is rectified through b and introduced into the reaction space.

この場合、一般にノズルからのガスや流体の流量はノズ
ル前後での圧力差の2分の1乗に比例する。したがって
、吹き出し口を形成する焼結多孔体5a、5bの前後の
圧損が大きい、このため、ノズル内のガス圧力はほぼ一
定値となり、焼結多孔体5a、5bで形成されたガス吹
き出し口から吹き出すガスの流速は多孔板面で一樺とな
り、偏流は起こらない、さらに多孔板表面には多数の孔
を有するのでそれらの孔から吹き出すガスの流速は極め
て小さい、しかも各孔が極めて近接しているので各孔間
に存在するデッドスペースが相対的に小さくなり、ガス
の乱れが生じにくい、その結果、焼結多孔体5a、5b
より吹き出すガスは乱れや偏りがなく、整流されたもの
となる。
In this case, the flow rate of gas or fluid from the nozzle is generally proportional to the 1/2 power of the pressure difference before and after the nozzle. Therefore, the pressure loss before and after the sintered porous bodies 5a and 5b that form the blowout ports is large. Therefore, the gas pressure inside the nozzle remains at a nearly constant value, and the gas blowout ports formed by the sintered porous bodies 5a and 5b The flow rate of the gas blown out is constant on the perforated plate surface, and no drift occurs.Furthermore, since the perforated plate surface has many holes, the flow rate of the gas blown out from those holes is extremely small, and each hole is very close to each other. As a result, the dead space existing between each hole is relatively small, and gas turbulence is less likely to occur.As a result, the sintered porous bodies 5a, 5b
The gas blown out is not turbulent or biased, and is rectified.

したがって、多孔板5aからのガスは整流された上段の
ガス流、多孔板5bからのガスは整流された下段のガス
流をそれぞれ形成する。
Therefore, the gas from the perforated plate 5a forms a rectified upper gas flow, and the gas from the perforated plate 5b forms a rectified lower gas flow.

また、下段側のガス流れは濃度拡散現象によりガス排気
部6側になるにつれて次第に光透過窓22側に上昇する
。このため、多孔板5a側の上下方向距離を多孔板5b
の上下方向距離より太き(することが望ましい0例えば
、上段側ガスに02を含むガス、下段側ガスに5iHa
を含むガスを使用する場合、多孔板5aの上下方向距離
/多孔板5bの上下方向距離の比としては、大略3程度
が望ましい。
Moreover, the gas flow on the lower stage side gradually rises toward the light transmission window 22 side as it approaches the gas exhaust section 6 due to the concentration diffusion phenomenon. For this reason, the vertical distance on the perforated plate 5a side is set to the perforated plate 5b.
(preferably 0) For example, the upper gas contains 02, and the lower gas contains 5iHa.
When using a gas containing gas, it is desirable that the ratio of the vertical distance of the perforated plate 5a/the vertical distance of the perforated plate 5b be about 3.

また、反応空間のガス流路はチャンバの側壁とプレート
24.サセプタ13及び光透過窓22により形成され、
その流路断面はガス供給部25のガス吹き出し口及びガ
ス排気部の奥行と同一面積とされ、反応空間のガス流路
に凹凸形状がないためにガスの整流化を維持することが
容易となる。
Further, the gas flow path of the reaction space is connected to the side wall of the chamber and the plate 24. Formed by a susceptor 13 and a light transmission window 22,
The cross section of the flow path has the same area as the depth of the gas outlet and gas exhaust section of the gas supply section 25, and since there is no uneven shape in the gas flow path of the reaction space, it is easy to maintain gas rectification. .

また、第2図に示すガス排気部6において、ガス排気部
6の内部高さをH;排気口の巾をWとしたとき 0.1 ≦  W/H≦  1 の関係が成立する構造がガスの整流化の面から望ましく
、特にW/H−115が最も望ましい。
In addition, in the gas exhaust section 6 shown in FIG. 2, a structure in which the relationship of 0.1 ≦ W/H ≦ 1 holds, where the internal height of the gas exhaust section 6 is H and the width of the exhaust port is W, is the gas exhaust section 6. W/H-115 is particularly desirable from the viewpoint of rectification.

さらに第3図は光透過窓22をガス供給部5及びガス排
気部6の上端面に載置した実施例を示し、この場合ガス
排気部6の構造は前述同様であり、ガス供給部5におい
ては Δt ≦ 0.015 L 、”/L 。
Furthermore, FIG. 3 shows an embodiment in which a light transmission window 22 is placed on the upper end surface of the gas supply section 5 and the gas exhaust section 6. In this case, the structure of the gas exhaust section 6 is the same as described above, and the gas supply section 5 is is Δt≦0.015L,”/L.

とすることがガスを整流化させ、光透過窓22の曇りを
防止する面から望ましい。
This is desirable from the viewpoint of rectifying the gas and preventing fogging of the light transmission window 22.

次に光化学反応方法における種々の操作条件と、光透過
窓の紫外光透過率、基板に対する膜厚均一性及び成膜速
度等との関係を説明する。
Next, the relationship between various operating conditions in the photochemical reaction method, ultraviolet light transmittance of the light transmitting window, film thickness uniformity with respect to the substrate, film formation rate, etc. will be explained.

第4図は反応空間に導入されるガスの線速度と窓透過率
との関係図、第5図は反応空間に導入されるガスの線速
度と基板に対する膜厚均一性との“関係図である。第4
図はガスの線速度が0.01≦V≦8(N−Cal/S
)の範囲内では窓透過率がほぼ95%以上と高い値を示
し、第5図は線速度が8を超えると粉体が生じ、また線
速度が0.01よりも小さいと膜均一性が急激に低下し
ていることを示している。
Figure 4 is a relationship diagram between the linear velocity of gas introduced into the reaction space and window transmittance, and Figure 5 is a relationship diagram between the linear velocity of gas introduced into the reaction space and film thickness uniformity with respect to the substrate. Yes. 4th
The figure shows that the gas linear velocity is 0.01≦V≦8 (N-Cal/S
), the window transmittance shows a high value of approximately 95% or more, and Figure 5 shows that when the linear velocity exceeds 8, powder is generated, and when the linear velocity is less than 0.01, the film uniformity decreases. It shows that it is rapidly decreasing.

この理由は、V<0.01 (N−cm/s)では反応
ガスの濃度拡散によって光透過窓に5iHaが到達し、
窓透過率が低下し、また反応ガスの濃度拡散によってガ
ス吹き出し口付近で光化学反応が進行し、膜厚均一性が
低下する。ただし、基板が小さい場合、この程度の膜厚
分布は無視することができる。
The reason for this is that when V<0.01 (N-cm/s), 5iHa reaches the light transmission window due to the concentration diffusion of the reactant gas.
The window transmittance decreases, and photochemical reactions proceed near the gas outlet due to the concentration diffusion of the reactant gas, resulting in a decrease in film thickness uniformity. However, if the substrate is small, this level of film thickness distribution can be ignored.

また、V>8 (N−cm/s)では、反応空間内の僅
かな凹凸がガス乱れの原因となり、上段側のガス流れと
下段側のガス流れとの混合作用が加速されるために窓透
過率が低下すると共に膜が生成することなく粉体が生じ
る。
In addition, at V > 8 (N-cm/s), slight irregularities in the reaction space cause gas turbulence, and the mixing action between the gas flow on the upper stage and the gas flow on the lower stage is accelerated, so the window is closed. As the transmittance decreases, powder is generated without forming a film.

第6図は上段(光透過窓)側のガスの線速度/下段(基
板)側のガスの線速度の比(以下、単に線速度比という
)と窓透過率との関係図、第7図は線速度比と膜厚均一
性との関係図である。
Figure 6 is a relationship diagram between the ratio of the linear velocity of the gas on the upper stage (light transmission window) side/the linear velocity of the gas on the lower stage (substrate) side (hereinafter simply referred to as linear velocity ratio) and the window transmittance. is a relationship diagram between linear velocity ratio and film thickness uniformity.

第6図は線速度が0.7≦Rv≦1.2の範囲で窓透過
率が95%以上を示し、第7図は0.7≦Rv≦1.2
の範囲で膜厚均一性が5±%以下を示している。この理
由は、線速度が大きい領域は負圧となり、線速度が小さ
い領域側のガスを巻き込むことになるが、特にRv <
 0.7の場合、光透過窓側ガス(OS又はN*+o*
)が基板側ガス(SiH4又はN、+5iH4)に巻き
込まれ、その反動によって光透過窓の下流側に曇りが生
じる。
Figure 6 shows that the window transmittance is 95% or more in the linear velocity range of 0.7≦Rv≦1.2, and Figure 7 shows that the window transmittance is 95% or more in the range of linear velocity of 0.7≦Rv≦1.2.
The film thickness uniformity is 5±% or less within the range of . The reason for this is that the region where the linear velocity is high becomes negative pressure, which entrains the gas in the region where the linear velocity is low, especially when Rv <
In the case of 0.7, the light-transmitting window side gas (OS or N*+o*
) is drawn into the substrate side gas (SiH4 or N, +5iH4), and the reaction causes fogging on the downstream side of the light transmission window.

方Rv > 1.2では基板側ガスが光透過窓側ガスに
巻き込まれるためにS i H,の濃度拡散が加速され
、光透過窓透過率が低下する。そして、ガスの巻き込み
が生じると、ガス流れの混合が加速されて粉体を生成す
ることになる。
When Rv > 1.2, the substrate-side gas is involved in the light-transmitting window-side gas, so that the concentration diffusion of S i H is accelerated, and the light-transmitting window transmittance decreases. When gas entrainment occurs, the mixing of the gas flows is accelerated to produce powder.

第8図は全圧ptと窓透過率との関係図、第9図は全圧
Ptと成膜速度との関係図、第1O図は全圧Ptと膜厚
均一性との関係図を各々示している。第8図は全圧0.
3Torr付近以上で窓透過率が95%以上を示し、第
9図は全圧0.3Torr付近以上で成膜速度が向上し
始め、特に全圧3 Torr以上で成膜速度が大きくな
っていることを示している。
Figure 8 shows the relationship between total pressure Pt and window transmittance, Figure 9 shows the relationship between total pressure Pt and film formation rate, and Figure 1O shows the relationship between total pressure Pt and film thickness uniformity. It shows. Figure 8 shows the total pressure 0.
The window transmittance shows 95% or more at around 3 Torr or higher, and Figure 9 shows that the film formation rate begins to improve at a total pressure of around 0.3 Torr or higher, and especially increases at a total pressure of 3 Torr or higher. It shows.

また、第10図は全圧0.3Torr以上で膜厚均一が
比較的高く、特に全圧I Torr〜6 Torrの範
囲では膜厚均一性が5十%以下を示している。この理由
は、全圧P t < 0.3Torrでは、ガスの流れ
が分子流領域に近づき、5iHnの拡散量が増大するた
め窓透過率が低下し、また高圧側においてガス吹き出し
口近傍での反応が速く、膜厚分布は低下するが窓の曇り
による窓透過率の低下は問題なく、成膜速度は飽和する
Further, FIG. 10 shows that the film thickness uniformity is relatively high at a total pressure of 0.3 Torr or more, and in particular, the film thickness uniformity is 50% or less in the range of a total pressure of I Torr to 6 Torr. The reason for this is that when the total pressure P t < 0.3 Torr, the gas flow approaches the molecular flow region and the amount of 5iHn diffusion increases, resulting in a decrease in window transmittance. Although the film thickness distribution decreases, there is no problem with the decrease in window transmittance due to fogging of the window, and the film formation rate is saturated.

第11図、第12図及び第13図はそれぞれSiH,モ
ル分率と窓透過率、成膜速度、膜厚均一性との関係図で
ある。SiH,モル分率が0.001よりも小さいと成
膜せず、また、S i H4モル分率が0.2よりも大
きいと、S i H4の燃焼反応が起こり、かつ粉体が
生成する。したがって、窓透過率、成膜速度、膜厚均−
性を考慮すると、SiH4モル分率はo、oot〜0.
2の範囲内に調整することが望ましい。
FIG. 11, FIG. 12, and FIG. 13 are relationship diagrams of SiH, mole fraction, window transmittance, film formation rate, and film thickness uniformity, respectively. If the SiH mole fraction is less than 0.001, no film will be formed, and if the SiH4 mole fraction is greater than 0.2, a combustion reaction of SiH4 will occur and powder will be produced. . Therefore, window transmittance, film formation rate, film thickness uniformity -
Considering the properties, the SiH4 mole fraction is o,oot~0.
It is desirable to adjust within the range of 2.

第14図、第15図及び第16図は、それぞれ0□モル
分率と、窓透過率、成膜速度、膜厚均一性との関係図を
示している。(18モル分率が0.0(15(量論比以
下)の場合、SiH4の光透過窓側への拡散量が増加し
、窓透過率が添加する。(18モル分率がo、oos以
上では、窓透過率、成膜速度、膜厚均−性に対して悪影
響がないことを示している。ただし、SiH,モル分率
の最小値は0.001であるから、O寡モル分率の許容
範囲は0.001以上が望ましい。
FIG. 14, FIG. 15, and FIG. 16 each show a relationship between the 0□ mole fraction, window transmittance, film formation rate, and film thickness uniformity. (When the 18 mole fraction is 0.0 (15 (stoichiometric ratio or less), the amount of diffusion of SiH4 to the light transmission window side increases and the window transmittance increases. (18 mole fraction is o, oos or more) This shows that there is no adverse effect on the window transmittance, film formation rate, and film thickness uniformity.However, since the minimum value of the SiH mole fraction is 0.001, the O-poor mole fraction It is desirable that the allowable range is 0.001 or more.

第17図及び第18図は、それぞれサセプタ上に載置さ
れる基板の回転数と、窓透過率、膜厚均一性の関係図を
示している。第17図は回転数Rrが2Orpmよりも
大きいと、窓透過率が約90%以下となり、第18図は
回転数Rrが0.01よりも小さいと、膜厚分布が著し
く低下し、かつ回転数Rrが20よりも大きいと、粉体
が生成することを示している。この理由は、回転数Rr
が0、Olよりも小さいと、基板に対する紫外光の照射
強度が不均一となり、また回転数Rrが20よりも大き
いと、基板及びサセプタの回転によって基板側ガスの流
れが乱れ、基板側のガスと光透過窓側のガスの混合が促
進されて粉体が生じ、窓透過率が低下するためである。
FIGS. 17 and 18 respectively show relationships between the rotational speed of a substrate placed on a susceptor, window transmittance, and film thickness uniformity. Figure 17 shows that when the rotational speed Rr is larger than 2 Orpm, the window transmittance is about 90% or less, and Fig. 18 shows that when the rotational speed Rr is smaller than 0.01, the film thickness distribution decreases significantly, and A number Rr greater than 20 indicates that powder is generated. The reason for this is that the rotation speed Rr
If Rr is smaller than 0 or Ol, the irradiation intensity of ultraviolet light on the substrate becomes non-uniform, and if the rotation speed Rr is larger than 20, the flow of gas on the substrate side is disturbed by the rotation of the substrate and susceptor, and the gas on the substrate side becomes uneven. This is because the mixing of the gas on the light-transmitting window side is promoted and powder is generated, reducing the window transmittance.

また、上記した実施例では、光CVD方による薄膜形成
について説明したが、本発明は光励起エツチングに適用
できることはいうまでもない0例えば、Si基板上に形
成した熱酸化Sin、膜の上に、更にリン添加ポリSi
膜をCI!、、Fを含むガス(例えばC2,ガス)中で
低圧水銀ランプからの紫外光を照射して、エツチングを
行うことができる。
Further, in the above-mentioned embodiments, thin film formation by photo-CVD method was explained, but it goes without saying that the present invention can be applied to photo-excited etching. Furthermore, phosphorus-added poly-Si
CI membrane! Etching can be performed by irradiating ultraviolet light from a low-pressure mercury lamp in a gas containing F (for example, C2 gas).

操作例 上段側ガスにN!で希釈された0□を用い、下段側ガス
にN、で希釈されたS i Haを用いて、下記の条件
下で光化学反応方法を実施した。
Operation example: N to the upper gas! A photochemical reaction method was carried out under the following conditions using 0□ diluted with N and S i Ha diluted with N as the lower stage gas.

全圧 P t = 3 Torr 線速度  V  = 0.2N −cm/s (ato
 ’C,1atm)線速度比 Rv = 1.0 全供給ガス中のS I Haのモル分率mS i H,
=0.0(15 全供給ガス中のOlのモル分率 mO□千〇 、(15 基板回転数   Rr=1 rpm この結果、光透過窓の曇りが防止され、高速成凝膜厚均
−性が達成された。
Total pressure P t = 3 Torr Linear velocity V = 0.2N -cm/s (ato
'C, 1 atm) linear velocity ratio Rv = 1.0 molar fraction of S I Ha in the total feed gas mS i H,
= 0.0 (15 molar fraction of Ol in the total supply gas mO□1,000, (15 Substrate rotation speed Rr = 1 rpm) As a result, clouding of the light transmission window is prevented and the uniformity of the thickness of the rapidly deposited film is improved. was achieved.

〔発明の効果〕〔Effect of the invention〕

以上のように本発明によれば、反応空間に供給されるガ
スを光透過窓側と基板側にそれぞれ層流状態で流すこと
ができ、反応ガスの濃度拡散を抑制し、光透過窓側ガス
と基板側ガスの混合、巻き込みを防止することによって
光透過窓の曇りを防止し、基板に対し均一な膜厚の薄膜
を製造することができる。
As described above, according to the present invention, the gas supplied to the reaction space can be flowed in a laminar flow state to the light-transmitting window side and the substrate side, respectively, suppressing the concentration diffusion of the reaction gas, and causing the gas on the light-transmitting window side and the substrate side to flow in a laminar flow state. By preventing the mixing and entrainment of side gases, clouding of the light transmission window can be prevented, and a thin film with a uniform thickness can be produced on the substrate.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の光化学反応装置の一実施例を示す縦断
面図、第2図は第1図の装置におけるガス供給部とガス
排気部の拡大詳細図、第3図は第2図の変形例を示す拡
大詳細図、第4図は反応空間に導入される反応ガスの線
速度と窓透過率との関係図、第5図は反応空間に導入さ
れる反応ガスの線速度と基板に対する膜厚均一性との関
係図、第6図は線速度比と窓透過率との関係図、第7図
は線速度比と膜厚均一性との関係図、第8図は全圧と窓
透過率との関係図、第9図は全圧と成膜速度との関係図
、第10図は全圧と膜厚均一性との関係図、第11図は
5iHnモル分率と窓透過率との関係図、第12図は3
iH4モル分率と成膜速度との関係図、第13図はSi
H4モル分率と膜厚均一性との関係図、第14図は0□
モル分率と窓透過率との関係図、第15図は0□モル分
率と成膜速度との関係図、第16図は0□モル分率と膜
厚均一性との関係図、第17図は反応空間における基板
の回転数と窓透過率との関係図、第18回は反応空間に
おける基板の回転数と膜厚均一性との関係図である。 1・・・・・・反応室、2・・・・・・予備室、3・・
・・・・ゲート機構、4・・・・・・低圧水銀ランプ、
5・・・・・・ガス供給部、6・・・・・・ガス排気部
、7・・・・・・ヒータ、8・・・・・・サセプタ、9
・・・・・・基板回転昇降機構、10.11・・・・・
・搬送アーム、12・・・・・・基板搬送機構、13・
・・・・・基板仮置台、14・・・・・・エアシリンダ
、15・・・・・・ベロー16・・・・・・排気口、1
7・・・・・・ゲート機構、18・・・・・・ロッド、
19・・・・・・シール部、20・・・・・・アクチュ
エータ、21・・・・・・支持板、22・・・・・・光
透過窓、23・・・・・・基板、24・・・・・・プレ
ート。 代理人  弁理士  西 元 勝 第2 図 第3図 ○○ゝO○○ ○○ 第4 図 第5図 線速Iし くN−cm/s)
FIG. 1 is a vertical cross-sectional view showing one embodiment of the photochemical reaction device of the present invention, FIG. 2 is an enlarged detailed view of the gas supply section and gas exhaust section in the device of FIG. 1, and FIG. 3 is the same as that of FIG. An enlarged detailed view showing a modified example, Figure 4 is a diagram showing the relationship between the linear velocity of the reaction gas introduced into the reaction space and the window transmittance, and Figure 5 is a diagram showing the relationship between the linear velocity of the reaction gas introduced into the reaction space and the substrate. Figure 6 is a diagram of the relationship between linear velocity ratio and window transmittance, Figure 7 is a diagram of the relationship between linear velocity ratio and film thickness uniformity, and Figure 8 is a diagram of the relationship between linear velocity ratio and window transmittance. Figure 9 is a diagram of the relationship between total pressure and film formation rate, Figure 10 is a diagram of the relationship between total pressure and film thickness uniformity, and Figure 11 is a diagram of the relationship between 5iHn mole fraction and window transmittance. The relationship diagram, Figure 12, is 3
Figure 13 shows the relationship between iH4 mole fraction and film formation rate.
Relationship diagram between H4 mole fraction and film thickness uniformity, Figure 14 is 0□
Figure 15 is a diagram showing the relationship between mole fraction and window transmittance. Figure 15 is a diagram showing the relationship between 0□ mole fraction and film formation rate. Figure 16 is a diagram showing the relationship between 0□ mole fraction and film thickness uniformity. Figure 17 is a diagram showing the relationship between the rotation speed of the substrate in the reaction space and window transmittance, and Figure 18 is a diagram showing the relationship between the rotation speed of the substrate in the reaction space and film thickness uniformity. 1...Reaction chamber, 2...Preliminary room, 3...
...Gate mechanism, 4...Low pressure mercury lamp,
5... Gas supply section, 6... Gas exhaust section, 7... Heater, 8... Susceptor, 9
・・・・・・Substrate rotation lifting mechanism, 10.11・・・・・・
・Transport arm, 12...Substrate transfer mechanism, 13.
...Temporary board storage stand, 14...Air cylinder, 15...Bello 16...Exhaust port, 1
7...Gate mechanism, 18...Rod,
19... Seal part, 20... Actuator, 21... Support plate, 22... Light transmission window, 23... Substrate, 24 ······plate. Agent Patent Attorney Masaru Nishimoto (2) Figure 3 ○○ゝO○○ ○○ 4 Figure 5 Linear speed (N-cm/s)

Claims (1)

【特許請求の範囲】 (1)耐熱性粒子を焼結した微細連通孔を有する焼結体
からなる多孔板で形成されたガス吹き出し口からガスを
各々別個に反応空間に供給すると共に前記ガスが光透過
窓側の反応空間に供給される第1の反応ガスと基板側の
反応空間に供給される第2の反応ガスとからなり、第1
の反応ガスは光で励起されることにより活性種を生成す
るが固形物を生成しないガス、第2の反応ガスは前記第
1の反応ガスとの反応により固形物を生成するガスであ
ることを特徴とする光化学反応方法。 (2)前記焼結体が、0.2μm〜500μmの微粒子
からなる金属又はセラミックスの焼結体であることを特
徴とする請求項(1)記載の光化学反応方法。 (3)前記第1の反応ガス及び第2の反応ガスがそれぞ
れ、不活性ガスにより希釈されることを特徴とする請求
項(1)記載の光化学反応方法。 (4)前記不活性ガスがN_2又はHe若しくはAr等
の第O族の稀ガスであることを特徴とする請求項(3)
記載の光化学反応方法。 (5)前記第1の反応ガスがO_2又はNH_3である
ことを特徴とする請求項(1)記載の光化学反応方法。 (6)前記第2の反応ガスが、有機系シラン化合物を含
むガスであることを特徴とする請求項(1)記載の光化
学反応方法。 (7)前記有機系シラン化合物が、モノシラン、ジシラ
ン、トリシラン、ジメチルシラン、テトラエトキシシラ
ンの群から選ばれることを特徴とする請求項(6)記載
の光化学反応方法。 (8)前記第1の反応ガス及び第2の反応ガスを、それ
ぞれの線速度Vを0.01≦V≦8(N・cm/s)の
範囲で反応空間に供給することを特徴とする請求項(1
)記載の光化学反応方法。 (9)前記第1の反応ガスの反応空間におけるガス速度
/第2の反応ガスの反応空間におけるガス速度の比(線
速度比)Rvを0.7≦Rv≦1.2の範囲とすること
を特徴とする請求項(1)記載の光化学反応力法。 (10)前記反応空間の全圧Ptを0.3Torr以上
とすることを特徴とする請求項(1)記載の光化学反応
方法。 (11)前記反応空間に供給される全ガス中の前記シラ
ン化合物を含む第2の反応ガスのモル分率を0.001
以上、0.2以下とすることを特徴とする請求項(1)
記載の光化学反応方法。 (12)前記シラン化合物がモノシランであることを特
徴とする請求項(11)記載の光化学反応方法(13)
前記反応空間に供給される全ガス中の前記O_2又はN
H_3を含む第1の反応ガスのモル分率を前記第2の反
応ガスの量論比以上とすることを特徴とする請求項(1
)記載の光化学反応方法。 (14)前記反応空間に配置される前記基板の回転数R
rを0.01≦Rr≦20(rpm)とすることを特徴
とする請求項(1)記載の光化学反応方法。 (15)耐熱性粒子を焼結した微細連通孔を有する焼結
体からなる多孔板で形成したガス吹き出し口を備えたガ
ス供給部を反応室側面側に設け、前記ガス吹き出し口に
おける反応空間と反対面の反応室側面側にガス排気口を
備えたガス排気部を設けると共にガス吹き出し口を上下
に少なくとも2段以上に区画し、前記ガス排気口を前記
ガス吹き出し口の同等以下の大きさとしたことを特徴と
する光化学反応装置。 (16)前記焼結体が、0.2μm〜500μmの微粒
子からなる金属又はセラミックスの焼結体であることを
特徴とする請求項(15)記載の光化学反応装置。 (17)前記ガス吹き出し口及び前記ガス排気部奥行を
、前記反応空間の流路断面とほぼ同一の面積としたこと
を特徴とする請求項(15)記載の光化学反応装置。 (18)前記ガス吹き出し口が2段に区画され、光透過
窓側のガス吹き出し口の上下方向距離が基板側のガス吹
き出し口の上下方向距離よりも大きいことを特徴とする
請求項(15)記載の光化学反応装置。 (19)前記反応室内に基板を載置するサセプタを昇降
及び回転させるための昇降回転機構を有することを特徴
とする請求項(15)記載の光化学反応装置。 (20)前記昇降回転機構によりサセプタを上昇させた
ときにこのサセプタによって反応空間の底面を構成する
ようにしたことを特徴とする請求項(15)記載の光化
学反応装置。
[Scope of Claims] (1) Gases are separately supplied to the reaction space from gas outlets formed of a perforated plate made of a sintered body having fine communication holes made by sintering heat-resistant particles, and the gases are The first reaction gas consists of a first reaction gas supplied to the reaction space on the light transmission window side and a second reaction gas supplied to the reaction space on the substrate side.
The reactive gas is a gas that generates active species but does not generate solid substances when excited by light, and the second reactive gas is a gas that generates solid substances by reaction with the first reactive gas. Characteristic photochemical reaction method. (2) The photochemical reaction method according to claim 1, wherein the sintered body is a metal or ceramic sintered body made of fine particles of 0.2 μm to 500 μm. (3) The photochemical reaction method according to claim (1), wherein the first reaction gas and the second reaction gas are each diluted with an inert gas. (4) Claim (3) characterized in that the inert gas is N_2 or a group O rare gas such as He or Ar.
Photochemical reaction method described. (5) The photochemical reaction method according to claim (1), wherein the first reaction gas is O_2 or NH_3. (6) The photochemical reaction method according to claim (1), wherein the second reaction gas is a gas containing an organic silane compound. (7) The photochemical reaction method according to claim (6), wherein the organic silane compound is selected from the group consisting of monosilane, disilane, trisilane, dimethylsilane, and tetraethoxysilane. (8) The first reaction gas and the second reaction gas are supplied to the reaction space at respective linear velocities V in the range of 0.01≦V≦8 (N cm/s). Claim (1
) Photochemical reaction method described. (9) The ratio (linear velocity ratio) of the gas velocity of the first reaction gas in the reaction space/the gas velocity of the second reaction gas in the reaction space is in the range of 0.7≦Rv≦1.2. The photochemical reaction force method according to claim (1), characterized in that: (10) The photochemical reaction method according to claim (1), characterized in that the total pressure Pt in the reaction space is 0.3 Torr or more. (11) The mole fraction of the second reaction gas containing the silane compound in the total gas supplied to the reaction space is 0.001.
Claim (1) characterized in that it is 0.2 or less.
Photochemical reaction method described. (12) The photochemical reaction method (13) according to claim (11), wherein the silane compound is monosilane.
The O_2 or N in the total gas supplied to the reaction space
Claim (1) characterized in that the mole fraction of the first reaction gas containing H_3 is greater than or equal to the stoichiometric ratio of the second reaction gas.
) Photochemical reaction method described. (14) Rotation speed R of the substrate placed in the reaction space
The photochemical reaction method according to claim 1, characterized in that r is 0.01≦Rr≦20 (rpm). (15) A gas supply section equipped with a gas outlet formed of a porous plate made of a sintered body having fine communication holes formed by sintering heat-resistant particles is provided on the side of the reaction chamber, and the reaction space at the gas outlet is A gas exhaust section with a gas exhaust port is provided on the opposite side of the reaction chamber, and the gas outlet is divided into at least two stages above and below, and the gas exhaust port has a size equal to or smaller than that of the gas outlet. A photochemical reaction device characterized by: (16) The photochemical reaction device according to claim 15, wherein the sintered body is a sintered body of metal or ceramics made of fine particles of 0.2 μm to 500 μm. (17) The photochemical reaction device according to claim (15), wherein the depth of the gas outlet and the gas exhaust section are approximately the same area as the cross section of the flow path of the reaction space. (18) The gas outlet is divided into two stages, and the distance in the vertical direction of the gas outlet on the light transmission window side is larger than the distance in the vertical direction of the gas outlet on the substrate side. photochemical reaction device. (19) The photochemical reaction apparatus according to claim (15), further comprising an elevating and rotating mechanism for elevating, lowering and rotating a susceptor on which a substrate is placed within the reaction chamber. (20) The photochemical reaction device according to claim (15), characterized in that when the susceptor is raised by the lifting/lowering rotation mechanism, the susceptor constitutes a bottom surface of the reaction space.
JP8257289A 1989-03-31 1989-03-31 Photochemical reaction and device therefor Pending JPH02260637A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8257289A JPH02260637A (en) 1989-03-31 1989-03-31 Photochemical reaction and device therefor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8257289A JPH02260637A (en) 1989-03-31 1989-03-31 Photochemical reaction and device therefor

Publications (1)

Publication Number Publication Date
JPH02260637A true JPH02260637A (en) 1990-10-23

Family

ID=13778200

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8257289A Pending JPH02260637A (en) 1989-03-31 1989-03-31 Photochemical reaction and device therefor

Country Status (1)

Country Link
JP (1) JPH02260637A (en)

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