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JPH0447454B2 - - Google Patents
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JPH0447454B2 - - Google Patents

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Publication number
JPH0447454B2
JPH0447454B2 JP58161456A JP16145683A JPH0447454B2 JP H0447454 B2 JPH0447454 B2 JP H0447454B2 JP 58161456 A JP58161456 A JP 58161456A JP 16145683 A JP16145683 A JP 16145683A JP H0447454 B2 JPH0447454 B2 JP H0447454B2
Authority
JP
Japan
Prior art keywords
sample
light
light source
container
thin film
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
Application number
JP58161456A
Other languages
Japanese (ja)
Other versions
JPS6053016A (en
Inventor
Masahiko Hirose
Takaaki Kamimura
Masahiko Akyama
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP58161456A priority Critical patent/JPS6053016A/en
Publication of JPS6053016A publication Critical patent/JPS6053016A/en
Publication of JPH0447454B2 publication Critical patent/JPH0447454B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/29Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by the substrates
    • H10P14/2901Materials
    • H10P14/2922Materials being non-crystalline insulating materials, e.g. glass or polymers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/24Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials using chemical vapour deposition [CVD]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/20Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
    • H10P14/34Deposited materials, e.g. layers
    • H10P14/3402Deposited materials, e.g. layers characterised by the chemical composition
    • H10P14/3404Deposited materials, e.g. layers characterised by the chemical composition being Group IVA materials
    • H10P14/3411Silicon, silicon germanium or germanium

Landscapes

  • Drying Of Semiconductors (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、光化学反応を利用して試料上に薄膜
を形成し若しは試料上の薄膜をエツチングする試
料処理装置に係わり、特に光源の改良をはかつた
試料処理装置に関する。
Detailed Description of the Invention [Technical Field of the Invention] The present invention relates to a sample processing device that forms a thin film on a sample or etches a thin film on a sample using a photochemical reaction, and particularly relates to an improvement in a light source. The present invention relates to a sample processing device with the following functions.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

近時、光エネルギによる化学反応を利用し、化
合物ガスを分解して半導体ウエハ等の試料上に薄
膜を形成する方法が開発されている。この方法は
光CVDと称され、通常の薄膜形成法に比較し低
温で膜形成ができることや荷電粒子によるダメー
ジがない等の特徴を有しており、今後の薄膜形成
技術において重要な位置を占めるものとして注目
されている。
Recently, a method has been developed in which a chemical reaction using light energy is used to decompose a compound gas and form a thin film on a sample such as a semiconductor wafer. This method is called photo-CVD, and has features such as being able to form films at lower temperatures and not being damaged by charged particles compared to normal thin film forming methods, and will play an important role in future thin film forming technology. It is attracting attention as a thing.

ところで、この種の方法で用いられる光エネル
ギを放射するための光源としては、放電により光
を発生する放電管が一般的である。放電管の形状
は通常直線状若しくはU字状であり、一定の面積
を照射するためにはこれらを複数個並べる方式が
採られている。この場合、放電管を複数個並べる
ため、放電管相互間を一定距離に保つ必要があ
り、発行しない空間が生じ照射光強度が低下し不
均一となる。さらに、個々の放電管の発行強度の
バラツキによつても、照射光強度が不均一になる
等の問題がある。そして、この問題が光CVD法
による均一な薄膜形成を妨げる要因となつてい
る。
By the way, as a light source for emitting light energy used in this type of method, a discharge tube that generates light by discharge is generally used. The shape of the discharge tube is usually linear or U-shaped, and in order to irradiate a certain area, a method is adopted in which a plurality of discharge tubes are lined up. In this case, since a plurality of discharge tubes are arranged side by side, it is necessary to maintain a constant distance between the discharge tubes, which creates a space where no light is emitted, resulting in a decrease in the intensity of the irradiated light and non-uniformity. Further, there is a problem that the intensity of the irradiated light becomes non-uniform due to variations in the emission intensity of individual discharge tubes. This problem is a factor that hinders the formation of a uniform thin film using the optical CVD method.

なお、上述した照射光強度の不均一性の問題
は、光CVD法に限らず光化学反応を利用して試
料上の薄膜をエツチングする光エツチング法でも
大きな欠点となつている。すなわち、光エツチン
グ法では照射光強度の不均一性に起因してエツチ
ング速度が不均一になると云う欠点があつた。
The problem of non-uniformity of the irradiation light intensity mentioned above is a major drawback not only in the photo-CVD method but also in the photo-etching method that etches a thin film on a sample using a photochemical reaction. That is, the photo-etching method has a drawback in that the etching rate becomes non-uniform due to non-uniformity in the intensity of irradiated light.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、所定面積に均一に光を照射す
ることができ、光CVD法による形成薄膜の膜厚
均一化及び光エツチングによるエツチング均一性
向上等をはかり得る試料処理装置を提供すること
にある。
An object of the present invention is to provide a sample processing device that can uniformly irradiate a predetermined area with light, make the thickness of a thin film formed by optical CVD method uniform, and improve etching uniformity by optical etching. be.

〔発明の概要〕[Summary of the invention]

本発明の骨子は、光エネルギを放射する光源と
して、所定平面内で均一に発光する単一の光源を
用いることにある。
The gist of the present invention is to use a single light source that emits light uniformly within a predetermined plane as a light source that emits light energy.

すなわち本発明は、試料が収容された試料室内
に化合物ガスを導入すると共に、光源からの光を
試料室内に入射して上記ガスを励起分解し、試料
上に薄膜を形成または試料上の薄膜をエツチング
する試料処理装置において、前記光源は単一の放
電灯であり、この放電灯は前記試料表面と平行な
面を有する気密容器と、この気密容器内に設けら
れ上記平面と直交する面で容器内を仕切つて容器
内全てを通る1本の帯状放電灯を形成し、光源か
らの光を透過する部材により構成された仕切り板
と、該帯状放電灯の両端部にそれぞれ設けられた
電極とからなるものであることを特徴とする試料
処理装置である。
That is, in the present invention, a compound gas is introduced into a sample chamber containing a sample, and light from a light source is incident into the sample chamber to excite and decompose the gas, thereby forming a thin film on the sample or decomposing the thin film on the sample. In the sample processing apparatus for etching, the light source is a single discharge lamp, and the discharge lamp includes an airtight container having a surface parallel to the sample surface, and a container provided within the airtight container with a surface perpendicular to the plane. A strip-shaped discharge lamp that partitions the inside of the container and passes through the entire interior of the container is formed by a partition plate made of a member that transmits light from a light source, and electrodes provided at each end of the strip-shaped discharge lamp. This is a sample processing device characterized by:

より具体的には光源を、試料表面と平行な面を
有する気密容器と、この気密容器内に設けられ上
記平面と直交する複数の面で容器内を仕切つて容
器内全てを通る1本の帯状放電炉を形成する仕切
り板と、該帯状放電炉の両端部にそれぞれ設けら
れた電極とからなる単一の放電灯で構成するよう
にしたものである。
More specifically, the light source is comprised of an airtight container having a surface parallel to the sample surface, and a strip-shaped strip provided inside the airtight container that partitions the inside of the container with a plurality of surfaces perpendicular to the above-mentioned plane and passes through the entire inside of the container. A single discharge lamp is constructed of a partition plate forming a discharge furnace and electrodes provided at both ends of the strip-shaped discharge furnace.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、所定の平面で均一発光する単
一の光源を用いているので、複数の光源を用いた
場合のように光源間の発光しない空間が生じるこ
とはなく、しかも個々の光源の発光強度バラツキ
等の問題は生じない。このため、所望する領域に
光源からの光を均一に照射することができる。し
たがつて、光CVD法に適用した場合には、均一
な膜厚で薄膜を形成することができる。また、光
エツチング法に適用した場合には、均一なエツチ
ングを行うことが可能となり、半導体製造技術分
野における有用性は絶大である。
According to the present invention, since a single light source that emits light uniformly on a predetermined plane is used, there is no space between the light sources where no light is emitted, unlike when multiple light sources are used, and moreover, the individual light sources Problems such as variations in luminous intensity do not occur. Therefore, a desired area can be uniformly irradiated with light from the light source. Therefore, when applied to the optical CVD method, a thin film with a uniform thickness can be formed. Furthermore, when applied to a photoetching method, it becomes possible to perform uniform etching, and its usefulness in the field of semiconductor manufacturing technology is enormous.

〔発明の実施例〕[Embodiments of the invention]

第1図は本発明の一実施例に係わる光CVD装
置を示す概略構成図である。図中1は薄膜形成容
器(試料室)で、この容器1内には例えばガラス
基板からなる試料2を載置する試料台3が収容さ
れている。試料台3の内部には、上記試料2を加
熱するヒータ4が設けられている。また、容器1
内にはガス供給部5から化合物ガスを含む原料ガ
スが導入され、容器1内のガスは排気ポンプ6に
より排気されるものとなつている。
FIG. 1 is a schematic configuration diagram showing an optical CVD apparatus according to an embodiment of the present invention. In the figure, reference numeral 1 denotes a thin film forming container (sample chamber), and within this container 1 is accommodated a sample stage 3 on which a sample 2 made of, for example, a glass substrate is placed. A heater 4 for heating the sample 2 is provided inside the sample stage 3 . Also, container 1
A raw material gas containing a compound gas is introduced into the container 1 from a gas supply section 5, and the gas in the container 1 is exhausted by an exhaust pump 6.

一方、薄膜形成容器1の上部には、光源7を収
納した光源収納容器8が設けられている。光源7
は第2図に示す如くその発光領域(放電領域)を
渦巻状に形成された1個の放電灯からなるもの
で、この放電灯から放射された光エネルギは光通
過窓9を通過して前記容器1内に入射するものと
なつている。なお、光源7についての詳細は後述
する。また、容器8内には不活性ガスライン1
0,11を介して不活性ガス(例えば窒素、アル
ゴンなど)が通流され、これにより光源7が冷却
されるとともに、空気中の酸素によるオゾンの発
生を防いでいる。
On the other hand, a light source storage container 8 containing a light source 7 is provided above the thin film forming container 1 . light source 7
As shown in FIG. 2, the lamp consists of a single discharge lamp whose light emitting area (discharge area) is formed in a spiral shape. The light is incident into the container 1. Note that details regarding the light source 7 will be described later. In addition, an inert gas line 1 is provided in the container 8.
An inert gas (for example, nitrogen, argon, etc.) is passed through the tubes 0 and 11, thereby cooling the light source 7 and preventing the generation of ozone due to oxygen in the air.

ところで、前記光源7は第3図a〜gに示す工
程により作製されている。すなわち、まず第3図
aに示す如き合成石英製の円筒体31の下面に同
図bに示す如き合成石英製の円板32を溶着し、
同図cに示す如く円筒体31の下面開口を円板3
2で閉塞する。次いで、第3図dに示す如き合成
石英製の板を渦巻状に湾曲してなる支切板33
を、同図eに示す如く円筒体31内に配置して円
板32に溶着する。これにより、前記第2図にも
示した如き渦巻状の1本の帯状放電路34が形成
される。次いで、第3図fに示す如く前記円板3
2と同様な円板35に2個の開孔を設け、これら
の開孔を閉塞するよう円板35の上面に、電極3
6,37が収納されたガラス製の電極収納管3
8,39をそれぞれ溶着する。次いで、第3図g
に示す如く円筒体31の上面に円板35の下面を
溶着する。その後、上記円筒体31及び円板3
2,35等からなる容器内を真空排気すると共
に、該容器内に水銀を含むガス(例えばAr−Hg
混合ガス)を封入することによつて、前記光源7
としての放電灯(低圧水銀ランプ)が完成され
る。かくして作製された光源7は円板32側を下
にして前記容器1内の試料2と対向配置されるも
のとなつている。
By the way, the light source 7 is manufactured by the steps shown in FIGS. 3a to 3g. That is, first, a disk 32 made of synthetic quartz as shown in FIG. 3b is welded to the lower surface of a cylindrical body 31 made of synthetic quartz as shown in FIG.
As shown in figure c, the lower opening of the cylindrical body 31 is
Blocked at 2. Next, a dividing plate 33 made of a synthetic quartz plate curved in a spiral shape as shown in FIG.
are placed inside the cylindrical body 31 and welded to the disk 32 as shown in FIG. As a result, one spiral strip-shaped discharge path 34 as shown in FIG. 2 is formed. Next, as shown in FIG. 3f, the disk 3
Two holes are provided in a disk 35 similar to 2, and electrodes 3 are placed on the top surface of the disk 35 to close these holes.
Glass electrode storage tube 3 containing electrodes 6 and 37
8 and 39 are respectively welded. Next, Figure 3g
The lower surface of the disk 35 is welded to the upper surface of the cylindrical body 31 as shown in FIG. After that, the cylindrical body 31 and the disc 3
The inside of the container consisting of 2, 35, etc. is evacuated, and a gas containing mercury (for example, Ar-Hg) is evacuated into the container.
By enclosing a mixed gas), the light source 7
A discharge lamp (low-pressure mercury lamp) was completed. The light source 7 thus produced is arranged to face the sample 2 in the container 1 with the disk 32 side facing down.

このように構成された本装置では、光源7の発
光領域が1本の帯状放電路の渦巻により、前記円
筒体31が形成する円と平面内全域に広がつてい
るので、該平面内で均一な光エネルギ放射を行わ
せることができる。本発明者等の実験によつて
も、上記光源7を点灯させたところ均一な発光面
が得られるのが確認された。このため、容器1内
への光照射を均一に行うことができ、光CVD法
による均一膜厚の薄膜形成を実現することができ
る。
In this device configured in this manner, the light emitting area of the light source 7 is spread over the circle formed by the cylinder 31 and the entire plane within the plane due to the spiral of one strip-shaped discharge path, so that it is uniform within the plane. It is possible to emit light energy. In experiments conducted by the present inventors, it was confirmed that a uniform light emitting surface was obtained when the light source 7 was turned on. Therefore, light can be uniformly irradiated into the container 1, and a thin film with a uniform thickness can be formed by the optical CVD method.

ここで、光源7が合成石英製であることから、
光源7からの光は185〔nm〕、254〔nm〕の紫外
光が主である。そこで、上記波長の紫外光を用
い、前記原料ガスとしてH2希釈したSiH4(10%)
と水銀蒸気との混合ガス、原料ガス流量を50
〔sccμ〕、ガス圧力1、試料温度200〔℃〕、処理時
間1〔h〕の条件で薄膜形成を行つた。その結果、
試料2としてのガラス基板上に3600〔Å〕のアモ
ルフアス・シリコン膜が得られた。そして、この
膜の均一性は極めて良好で±5〔%〕以下であつ
た。また、光源7として従来のU字形ランプを用
いた場合、上記と同一条件下で膜厚は2800〔Å〕、
均一性は±10〔%〕程度であつた。
Here, since the light source 7 is made of synthetic quartz,
The light from the light source 7 is mainly ultraviolet light of 185 [nm] and 254 [nm]. Therefore, using ultraviolet light of the above wavelength, SiH 4 (10%) diluted with H 2 was used as the source gas.
Mixed gas with mercury vapor, raw material gas flow rate 50
The thin film was formed under the following conditions: [sccμ], gas pressure 1, sample temperature 200 [°C], and processing time 1 [h]. the result,
An amorphous silicon film with a thickness of 3600 Å was obtained on a glass substrate as Sample 2. The uniformity of this film was extremely good and was within ±5%. In addition, when a conventional U-shaped lamp is used as the light source 7, the film thickness is 2800 [Å] under the same conditions as above.
The uniformity was about ±10%.

このように本装置によれば、光CVD法によつ
て試料2上に均一に、かつ比較的速い速度で薄膜
(アモルフイス・シリコン)を形成することがで
きる。また、光源7が1個であることから複数の
光源を用いた場合のような個々の発光強度のバラ
ツキに起因する光照射の不均一性を招くことはな
い。さらに、経時的に発光強度が低下した場合で
あつても、光源7が1個であるため全体としての
発光強度は均一であり、したがつて経時的に光照
射量が不均一化する等の不都合はない。そして、
この発光強度の低下を他の条件により補正するこ
とも極めて容易である。例えば試料台3近傍に光
強度測定センサーを配置して照射強度を測定し、
あらかじめとつておいた光強度と膜形成速度との
関係を決めたデータを用いれば所定の膜厚を得る
ために必要な時間を決定することができる。この
場合、光源7が一本化されるので複数の光源を用
いた従来の方法の様に、経時的なばらつきがな
く、測定が容易である。しかも最小のセンサー、
例えば1つのセンサーによつても照射強度の測定
が可能である。また、光源7の電極36,37を
円筒体31の内部に収納するのではなく、円板3
5から突出した収納管38,39内に収納してい
るので、電極36,37近傍の暗部が光源7の下
面側に生じることはなく、これにより照射光強度
のより一層の均一化をはかり得る等の利点があ
る。
As described above, according to the present apparatus, a thin film (amorphous silicon) can be formed uniformly on the sample 2 at a relatively high speed by the optical CVD method. Furthermore, since there is only one light source 7, non-uniformity in light irradiation due to variations in the intensity of light emitted from each light source, unlike when a plurality of light sources are used, does not occur. Furthermore, even if the luminescence intensity decreases over time, the overall luminescence intensity is uniform because there is only one light source 7, and therefore the amount of light irradiation becomes uneven over time. There is no inconvenience. and,
It is also extremely easy to correct this decrease in emission intensity using other conditions. For example, a light intensity measurement sensor is placed near the sample stage 3 to measure the irradiation intensity,
The time required to obtain a predetermined film thickness can be determined by using data that has been prepared in advance and determines the relationship between light intensity and film formation rate. In this case, since the light source 7 is unified, there is no variation over time unlike in the conventional method using a plurality of light sources, and measurement is easy. Moreover, the smallest sensor
For example, it is possible to measure the irradiation intensity even with one sensor. Moreover, instead of storing the electrodes 36 and 37 of the light source 7 inside the cylindrical body 31, the electrodes 36 and 37 of the light source 7 are
Since the electrodes 36 and 37 are housed in storage tubes 38 and 39 protruding from the electrodes 5, dark areas near the electrodes 36 and 37 do not occur on the lower surface side of the light source 7, thereby making it possible to further equalize the intensity of the irradiated light. There are advantages such as

なお、本発明は上述した実施例に限定されるも
のではなく、その要旨を逸脱しない範囲で、種種
変形して実施することができる。例えば、前記光
源の発光部形状は円形に限るものではなく、第4
図に示す如く矩形であつても何ら差し支えない。
要は、発光領域が所定平面状に配置した帯状発光
路で形成され、かつ該発光路が上記平面上で重な
ることなく該平面の全面を覆うものであればよ
い。また、光源の製造方法は何ら実施例に限定さ
れるものではなく、適宜変更可能である。さら
に、光源は低圧水銀ランプに限るものではなく、
所定エネルギの光を所定平面内で均一に発光する
ものであればよい。
Note that the present invention is not limited to the embodiments described above, and can be implemented with various modifications without departing from the gist thereof. For example, the shape of the light emitting part of the light source is not limited to a circular shape, but
There is no problem even if it is rectangular as shown in the figure.
In short, it is sufficient that the light-emitting region is formed of band-shaped light-emitting paths arranged in a predetermined plane, and that the light-emitting paths cover the entire surface of the plane without overlapping. Furthermore, the method of manufacturing the light source is not limited to the embodiments, and can be modified as appropriate. Furthermore, the light source is not limited to low-pressure mercury lamps;
Any device that emits light with a predetermined energy uniformly within a predetermined plane may be used.

また、実施例では光CVD装置について説明し
たが、本発明は光エツチングに適用することも可
能である。現在、VLSIの微細加工技術の主流は、
種々の反応性ガスから生じるイオンを試料表面に
垂直に入射させて、これをエツチングするもの
で、反応性イオンエツチング(Reactive Ion
Etching;RIE)と呼ばれている。しかし、該方
法では電子、イオンなどの荷電粒子を用いるた
め、基板損傷、静電破壊などの照射損傷を生じ、
これらの除去に苦慮しているのが現状である。
Further, although the embodiments have been described with reference to an optical CVD apparatus, the present invention can also be applied to optical etching. Currently, the mainstream of VLSI microfabrication technology is
Reactive ion etching is a process in which ions generated from various reactive gases are incident perpendicularly onto the sample surface to etch the sample.
Etching (RIE). However, since this method uses charged particles such as electrons and ions, it causes irradiation damage such as substrate damage and electrostatic breakdown.
At present, we are struggling to remove these.

これに対して、最近、荷電粒子を用いない無照
射損傷のドライエツチング技術として、紫外線な
どの光励起プロセスの研究が盛んに行われてい
る。これら光プロセスを実用化するためには、前
記薄膜堆積同様、大口径、均一光源が不可欠であ
る。すなわち、近年、ウエハの大口径化の傾向は
著しく、6〜8インチウエハも使用されるに至つ
ており、エツチングの均一性のみならず、スルー
プツトの点も考慮して一括処理方式を可能にする
大口径光源への要求が高まつている。
On the other hand, recently, research has been actively conducted on photoexcitation processes such as ultraviolet rays as dry etching techniques that do not use charged particles and cause damage without irradiation. In order to put these optical processes into practical use, a large diameter, uniform light source is essential, as in the case of thin film deposition. In other words, in recent years, there has been a remarkable trend toward larger diameter wafers, and 6- to 8-inch wafers are now being used, making it possible to use a batch processing method that takes into consideration not only etching uniformity but also throughput. Demand for large diameter light sources is increasing.

本発明は、これら諸々の問題を一掃するもの
で、例えば、6インチのSiウエハ上の熱酸化
SiO2上に成長させたリン添加Poly−Siに、Cl2
で第2図に示したランプを照射した結果、エツチ
ングの均一性は±5%以下という値が得られ、極
めて有用であることが実証された。
The present invention eliminates these problems, for example, by thermal oxidation on a 6-inch Si wafer.
When phosphorus-doped Poly-Si grown on SiO 2 was irradiated with the lamp shown in Figure 2 in Cl 2 , an etching uniformity of less than ±5% was obtained, which is extremely useful. has been proven.

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

第1図は本発明の一実施例に係わる光CVD装
置を示す概略構成図、第2図は上記装置に使用し
た光源の発光部構造を示す平面図、第3図a〜g
は上記光源の製造工程を示す斜視図、第4図は変
形例を説明するための平面図である。 1……薄膜形成容器(試料室)、2……試料、
3……試料台、4……ヒータ、5……ガス供給
部、6……排気ポンプ、7……光源、8……光源
収納容器、9……光透過窓、31……円筒体、3
2,35……円板、33……支切板、34……放
電路(発光路)、36,37……電極。
Fig. 1 is a schematic configuration diagram showing an optical CVD device according to an embodiment of the present invention, Fig. 2 is a plan view showing the structure of a light emitting part of a light source used in the above device, and Figs. 3 a to g.
4 is a perspective view showing the manufacturing process of the light source, and FIG. 4 is a plan view for explaining a modification. 1... Thin film formation container (sample chamber), 2... Sample,
3...Sample stand, 4...Heater, 5...Gas supply section, 6...Exhaust pump, 7...Light source, 8...Light source storage container, 9...Light transmission window, 31...Cylindrical body, 3
2, 35... Disk, 33... Split plate, 34... Discharge path (light emitting path), 36, 37... Electrode.

Claims (1)

【特許請求の範囲】 1 試料が収容された試料室内に化合物ガスを導
入すると共に、光源からの光を試料室内に入射し
て上記ガスを励起分解し、上記試料上に薄膜を形
成または試料上の薄膜をエツチングする試料処理
装置において、前記光源は単一の放電灯であり、
この放電灯は前記試料表面と平行な面を有する気
密容器と、この気密容器内に設けられ上記平面と
直交する面で容器内を仕切つて容器内全てを通る
1本の帯状放電灯を形成し、光源からの光を透過
する部材により構成された仕切り板と、該帯状放
電灯の両端部にそれぞれ設けられた電極とからな
るものであることを特徴とする試料処理装置。 2 前記電極は、前記気密容器内から前記基板側
と反対側に突出した収納管内に収容されることを
特徴とする特許請求の範囲第1項記載の試料処理
装置。
[Claims] 1. A compound gas is introduced into a sample chamber in which a sample is housed, and light from a light source is incident into the sample chamber to excite and decompose the gas to form a thin film on the sample or to form a thin film on the sample. In a sample processing apparatus for etching a thin film, the light source is a single discharge lamp;
This discharge lamp includes an airtight container having a plane parallel to the sample surface, and a strip-shaped discharge lamp that is installed inside the airtight container and partitions the inside of the container with a plane perpendicular to the above-mentioned plane, passing through the entire inside of the container. A sample processing device comprising: a partition plate made of a member that transmits light from a light source; and electrodes provided at both ends of the strip-shaped discharge lamp. 2. The sample processing apparatus according to claim 1, wherein the electrode is housed in a storage tube that protrudes from inside the airtight container to a side opposite to the substrate side.
JP58161456A 1983-09-02 1983-09-02 Sample processing equipment Granted JPS6053016A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58161456A JPS6053016A (en) 1983-09-02 1983-09-02 Sample processing equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58161456A JPS6053016A (en) 1983-09-02 1983-09-02 Sample processing equipment

Publications (2)

Publication Number Publication Date
JPS6053016A JPS6053016A (en) 1985-03-26
JPH0447454B2 true JPH0447454B2 (en) 1992-08-04

Family

ID=15735447

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58161456A Granted JPS6053016A (en) 1983-09-02 1983-09-02 Sample processing equipment

Country Status (1)

Country Link
JP (1) JPS6053016A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2588511B2 (en) * 1986-09-24 1997-03-05 株式会社日立製作所 Processing equipment
JPS6355428U (en) * 1986-09-26 1988-04-13
JPS63222430A (en) * 1987-03-11 1988-09-16 Nikon Corp Light radiation apparatus
US5178682A (en) * 1988-06-21 1993-01-12 Mitsubishi Denki Kabushiki Kaisha Method for forming a thin layer on a semiconductor substrate and apparatus therefor

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS505721U (en) * 1973-05-17 1975-01-21

Also Published As

Publication number Publication date
JPS6053016A (en) 1985-03-26

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