JPS6313339B2 - - Google Patents
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- Publication number
- JPS6313339B2 JPS6313339B2 JP55104526A JP10452680A JPS6313339B2 JP S6313339 B2 JPS6313339 B2 JP S6313339B2 JP 55104526 A JP55104526 A JP 55104526A JP 10452680 A JP10452680 A JP 10452680A JP S6313339 B2 JPS6313339 B2 JP S6313339B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- semiconductor
- silicon nitride
- protective film
- nitride 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.)
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P14/00—Formation of materials, e.g. in the shape of layers or pillars
- H10P14/60—Formation of materials, e.g. in the shape of layers or pillars of insulating materials
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- Formation Of Insulating Films (AREA)
Description
【発明の詳細な説明】
本発明は半導体の表面保護膜の形成方法に関
し、更に詳しくは化学蒸着法および高周波スパツ
タリング法による半導体の表面保護膜の形成方法
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for forming a surface protective film on a semiconductor, and more particularly to a method for forming a surface protective film on a semiconductor using a chemical vapor deposition method and a high frequency sputtering method.
従来の化学蒸着法(Chemical Vapor
Deposition;以下CVD法と略記する)によれば、
反応ガスの熱分解反応を利用している。例えばシ
リコン酸化膜は、400℃〜600℃でSiH4(モノシラ
ン)ガスとO2(酸素)ガスの熱分解によつて形成
し、またシリコン酸化膜は600℃〜800℃でSiH4
ガスとNH3(アンモニア)ガスの熱分解によつて
形成している。このような高温で保護膜を形成す
る際、被蒸着体が熱に弱い物質、例えば−族
化合物半導体の場合、半導体表面の熱劣化すなわ
ち半導体表面層の熱分解損傷を避けることができ
ない。例えば、代表的な−族化合物半導体で
ある砒化ガリウムあるいは燐化インジウムは300
℃〜400℃から、構成元素である砒素あるいは燐
の蒸発が顕著となる。 Traditional chemical vapor deposition
According to deposition (hereinafter abbreviated as CVD method),
It utilizes the thermal decomposition reaction of a reactive gas. For example, silicon oxide film is formed by thermal decomposition of SiH 4 (monosilane) gas and O 2 (oxygen) gas at 400°C to 600°C, and silicon oxide film is formed by thermal decomposition of SiH 4 (monosilane) gas and O 2 (oxygen) gas at 600°C to 800°C.
It is formed by the thermal decomposition of gas and NH 3 (ammonia) gas. When forming a protective film at such a high temperature, if the material to be deposited is a heat-sensitive material, such as a - group compound semiconductor, thermal deterioration of the semiconductor surface, that is, thermal decomposition damage to the semiconductor surface layer cannot be avoided. For example, gallium arsenide or indium phosphide, which are representative - group compound semiconductors, have a
From ℃ to 400℃, the constituent elements arsenic or phosphorus evaporate significantly.
従つて、半導体表面の熱劣化が生じない低温で
保護膜を形成することが望ましく、この目的のた
めに通常高周波放電を利用したプラズマCVD法
あるいは高周波スパツタリング法による保護膜形
成が行なわれている。プラズマCVD法は、高周
波放電によつて反応ガスの分解反応を促進させ、
反応生成物を被蒸着体上に堆積させる方法であ
り、高周波スパツタリング法は、放電によつて生
じたイオンをターゲツトに衝突させ、はじき出さ
れたターゲツト粒子を被蒸着体上に堆積させる方
法である。 Therefore, it is desirable to form a protective film at a low temperature that does not cause thermal deterioration of the semiconductor surface, and for this purpose, protective film formation is usually performed by a plasma CVD method using high-frequency discharge or a high-frequency sputtering method. The plasma CVD method uses high-frequency discharge to accelerate the decomposition reaction of reactive gases.
The high-frequency sputtering method is a method of depositing a reaction product on an object to be evaporated, and the high-frequency sputtering method is a method in which ions generated by electric discharge collide with a target, and the ejected target particles are deposited on the object to be evaporated.
上記2通りの方法によれば、ともに低温で半導
体上に保護膜を形成することが可能であるが、真
空中の残留ガスあるいは反応ガスあるいはターゲ
ツト内に含まれている水素が、容易に保護膜中に
取り込まれてしまう。例えば、プラズマCVD法
で、シリコン窒化膜を形成する際、反応ガスであ
るSiH4とNH3の未分解によつてシリコン窒化膜
中に水素が混入する。また高周波スパツタリング
法で、シリコン酸化膜を形成する際、SiO2ター
ゲツト内に含まれるシラノール群(Si−OH基)
が多量に形成膜内に混入する。このため水素の混
入した膜は高温でのCVD法と比較して(1)吸湿性
を有する、(2)ち密な膜は得られ難い、(3)耐薬品性
が弱く、例えば、NH4:HF=6:1の溶液に対
して、プラズマCVD法で形成したシリコン窒化
膜は100〜1000倍エツチング速度が速い、等の欠
点を有する。従つて、従来の感光剤を用いた露光
技術によつて絶縁膜の一部を開孔してパターンを
描画する際、いわゆるサイドエツチングによつて
鮮明なパターンが形成されないという欠点を有す
る。 According to the above two methods, it is possible to form a protective film on the semiconductor at low temperature, but the residual gas in the vacuum, the reaction gas, or the hydrogen contained in the target can easily destroy the protective film. It gets taken inside. For example, when forming a silicon nitride film using plasma CVD, hydrogen is mixed into the silicon nitride film due to undecomposed reaction gases SiH 4 and NH 3 . In addition, when forming a silicon oxide film using the high frequency sputtering method, silanol groups (Si-OH groups) contained in the SiO 2 target are
is mixed into the formed film in large quantities. Therefore, compared to high-temperature CVD methods, films containing hydrogen (1) are hygroscopic, (2) are difficult to obtain dense films, and (3) have weak chemical resistance, such as NH 4 : A silicon nitride film formed by plasma CVD has a disadvantage that the etching rate is 100 to 1000 times faster than that of a solution of HF=6:1. Therefore, when a pattern is drawn by opening a part of the insulating film using the conventional exposure technique using a photosensitive agent, a clear pattern cannot be formed due to so-called side etching.
上記の欠点を除去するために、低温で保護膜を
形成した後に、Ar(アルゴン)、N2などの不活性
ガス雰囲気中で500℃〜900℃の高温で熱処理して
膜中の水素を離脱させることが従来から行なわれ
ている。しかしながら、高温熱処理によつて(1)保
護膜の形成されていない、すなわち半導体表面の
露出した部分の熱劣化を防ぐことができない。(2)
半導体も昇温するわけであるから、保護膜と半導
体の熱膨張係数の違いすなわち、一般に半導体の
方が熱膨張係数が大きいために、保護膜および半
導体が彎曲したり、亀裂が生じたり保護膜が剥れ
たりする、等の欠点を有する。 In order to eliminate the above drawbacks, after forming a protective film at a low temperature, heat treatment is performed at a high temperature of 500°C to 900°C in an inert gas atmosphere such as Ar (argon) or N2 to remove hydrogen from the film. This has traditionally been done. However, high-temperature heat treatment cannot (1) prevent thermal deterioration of the exposed portion of the semiconductor surface where the protective film is not formed; (2)
Since the temperature of the semiconductor also rises, the difference in the coefficient of thermal expansion between the protective film and the semiconductor, that is, the coefficient of thermal expansion of the semiconductor is generally larger, may cause the protective film and the semiconductor to bend or crack. It has disadvantages such as peeling.
本発明は、上記の欠点を除去することを目的と
した、半導体の表面保護膜の形成方法を提供する
ことにある。 An object of the present invention is to provide a method for forming a surface protective film for a semiconductor, which aims to eliminate the above-mentioned drawbacks.
本発明はプラズマCVD法あるいは高周波スパ
ツタリング法によつて低温で絶縁膜を半導体表面
上に形成した後、該絶縁膜表面の少なくとも一部
分に、荷電粒子あるいはレーザ光を照射して照射
部分を加熱する工程及びエツチングによつて照射
部以外を除去して、照射部のみにパターン化した
表面保護膜を形成する方法である。 The present invention is a process of forming an insulating film on a semiconductor surface at a low temperature by a plasma CVD method or a high-frequency sputtering method, and then irradiating at least a portion of the surface of the insulating film with charged particles or laser light to heat the irradiated portion. This is a method in which the area other than the irradiated area is removed by etching to form a patterned surface protective film only on the irradiated area.
本発明によれば、荷電粒子あるいはレーザ光を
半導体表面上に形成した絶縁膜表面に選択的に照
射するため、荷電粒子照射あるいはレーザ光照射
によつて発生する熱は主に絶縁膜の部分で吸収さ
れる。従つて、主に絶縁膜部分が加熱されるた
め、(1)半導体表面の露出した部分の熱劣化を防ぐ
ことができる、(2)電子ビーム照射加熱による半導
体の昇温の影響は、従来の不活性ガス雰囲気中熱
処理の場合に比べて小さく、したがつて熱膨張係
数の違いによる形成膜および半導体の彎曲、ある
いは亀裂、形成膜の剥れは発生しない、(3)絶縁膜
中に取り込まれている水素を昇温離脱させること
ができ、吸湿性のない、ち密な保護膜を形成する
ことができる、(4)選択的に緻密化することによ
り、従来の感光剤を用いた露光技術を用いずに、
直接的にパターン化された絶縁体被膜が形成でき
るという利点を有する。 According to the present invention, the surface of the insulating film formed on the semiconductor surface is selectively irradiated with charged particles or laser light, so that the heat generated by charged particle irradiation or laser light irradiation is mainly absorbed in the insulating film. Absorbed. Therefore, since mainly the insulating film portion is heated, (1) thermal deterioration of the exposed portion of the semiconductor surface can be prevented, and (2) the effect of temperature increase on the semiconductor due to electron beam irradiation heating is lower than that of conventional methods. The heat treatment is smaller than that in the case of heat treatment in an inert gas atmosphere, so there is no curvature or cracking of the formed film and semiconductor due to differences in thermal expansion coefficients, or peeling of the formed film. (3) Incorporation into the insulating film (4) Through selective densification, exposure technology using conventional photosensitizers can be eliminated by increasing temperature and forming a dense protective film that does not absorb moisture. without using
It has the advantage that a patterned insulator film can be formed directly.
以下、図を参照しながら、本発明の前提となる
実験結果、本発明の実施例を順に示すがこれらが
本発明をそれに限るものでないことは容易に理解
される。 EXAMPLES Hereinafter, with reference to the drawings, experimental results that are the premise of the present invention and examples of the present invention will be shown in order, but it will be easily understood that the present invention is not limited to these.
本発明の前提となる第1の実験として、シリコ
ン窒化膜を砒化ガリウム化合物半導体表面上に形
成した。シリコン窒化膜は、プラズマCVD法に
よつて形成したもので、反応ガスとして毎分5c.c.
流量のSiH4と毎分10c.c.流量のNH3と毎分70c.c.の
N2を流し、基板温度を300℃、圧力を1.0Torr、
放電電力を100Wにした。形成されたシリコン窒
化膜は、厚さが1470Åで屈折率は1.83であつた。
第1図aは上記の条件でシリコン窒化膜11を砒
化ガリウム半導体12の上に形成した状態の断面
図を示すもので、シリコン窒化膜11の熱膨張係
数は、砒化ガリウム半導体12のそれよりも小さ
いため、300℃の膜形成温度から室温に戻したと
き、シリコン窒化膜11は圧縮応力を受けて、図
の如くわずかに彎曲する。第1図aに示す試料を
従来の方法に従つてN2雰囲気中で600℃の温度で
30分間熱処理したところ、シリコン窒化膜11に
含まれている水素の離脱によつて該シリコン窒化
膜11は、ち密になる傾向のため縮み、砒化ガリ
ウム半導体12は熱膨張するため、該試料は、亀
裂やシリコン窒化膜11の剥れが生じてしまつ
た。本発明に従つて、第1図aの試料を2×
10-9Torrの真空内で5KVに加速された放射電流
3×10-7アンペアの電子ビームを該シリコン窒化
膜11の全表面に3分間照射したところ、第1図
bに示す如く、亀裂やシリコン窒化膜11の剥れ
は生じないばかりでなく電子ビーム照射前で約3
×1010ダイン/cm2の圧縮応力が約0.6×109ダイ
ン/cm2に低減され彎曲は顕著でなくなつた。これ
は、電子ビーム照射によつて主にシリコン窒化膜
11が加熱され、該シリコン窒化膜11に含まれ
ていた水素が離脱して該シリコン窒化膜11のち
密化のために該シリコン窒化膜11が縮んで応力
が緩和された結果である。電子ビーム照射によつ
てシリコン窒化膜11に含まれていた水素が離脱
したことは、赤外吸収分光で、Si−H基が約1/20
に減少したことで確めた。また、電子ビーム照射
後のシリコン窒化膜は、厚さが1430Åに減少し、
屈折率が1.98に増加し、NH4F:HF=6:1の
溶液に対するエツチング速度も、電子ビーム照射
前で毎分約3500Åであつたのが、毎分約150Åに
なり、該シリコン窒化膜11がち密になつたこと
を示した。 As a first experiment which is a premise of the present invention, a silicon nitride film was formed on the surface of a gallium arsenide compound semiconductor. The silicon nitride film was formed by the plasma CVD method, and the rate of reaction gas was 5 c.c./min.
Flow rate of SiH 4 and 10 c.c. per minute. Flow rate of NH 3 and 70 c.c. per minute.
Flow N 2 , set the substrate temperature to 300℃, and set the pressure to 1.0Torr.
The discharge power was set to 100W. The silicon nitride film formed had a thickness of 1470 Å and a refractive index of 1.83.
FIG. 1a shows a cross-sectional view of a silicon nitride film 11 formed on a gallium arsenide semiconductor 12 under the above conditions, and the coefficient of thermal expansion of the silicon nitride film 11 is higher than that of the gallium arsenide semiconductor 12. Because of its small size, when the silicon nitride film 11 is returned to room temperature from the film forming temperature of 300° C., it receives compressive stress and bends slightly as shown in the figure. The sample shown in Figure 1a was prepared at a temperature of 600°C in an N2 atmosphere according to the conventional method.
When heat treated for 30 minutes, the silicon nitride film 11 tends to become denser due to the release of hydrogen contained in the silicon nitride film 11 and shrinks, and the gallium arsenide semiconductor 12 thermally expands. Cracks and peeling of the silicon nitride film 11 occurred. According to the invention, the sample of FIG.
When the entire surface of the silicon nitride film 11 was irradiated with an electron beam with a radiation current of 3×10 -7 amperes accelerated to 5KV in a vacuum of 10 -9 Torr for 3 minutes, cracks and cracks were observed as shown in Figure 1b. Not only does the silicon nitride film 11 not peel off, but the peeling of the silicon nitride film 11 is approximately 3.
The compressive stress of ×10 10 dynes/cm 2 was reduced to approximately 0.6 × 10 9 dynes/cm 2 and the curvature became less noticeable. This is because the silicon nitride film 11 is mainly heated by the electron beam irradiation, hydrogen contained in the silicon nitride film 11 is released, and the silicon nitride film 11 is later densified. This is the result of contraction and stress relaxation. Infrared absorption spectroscopy shows that the hydrogen contained in the silicon nitride film 11 was released by the electron beam irradiation, and the Si-H group was approximately 1/20
This was confirmed by a decrease in In addition, the thickness of the silicon nitride film after electron beam irradiation decreased to 1430 Å,
The refractive index increased to 1.98, and the etching rate for a solution of NH 4 F:HF = 6:1, which was about 3500 Å per minute before electron beam irradiation, increased to about 150 Å per minute, and the etching rate for the silicon nitride film increased from about 3500 Å per minute before electron beam irradiation. 11 has become more dense.
本発明の前提となる第2の実験として、シリコ
ン酸化膜を高周波スパツタリング法で燐化インジ
ウム半導体表面上に形成した。シリコン酸化膜の
形成は0.1TorrのAr雰囲気中で、基板温度250℃、
放電電力200Wで行なつた。形成されたシリコン
酸化膜は、厚さが1260Åで屈折率が1.46であつ
た。シリコン酸化膜を燐化インジウム上に形成し
た状態は、第1図aの場合と全く同様で図中の1
1をシリコン酸化膜、12を燐化インジウムに置
き換えて考えればよい。本発明に従つて、第1の
実施例の場合と同一条件でシリコン酸化膜の全表
面を電子ビーム照射したところ、第1の実施例の
場合と同様、第1図bに示す如く、試料の彎曲は
低減された。赤外吸収分光で調べたところ該シリ
コン酸化膜に含まれていたシラノール群(Si−
OH基)が、電子ビーム照射で約1/10に低減して
いた。また、NH4F:HF=6:1の溶液に対す
るエツチング速度も、電子ビーム照射前で毎分約
3000Åであつたのに対し、電子ビーム照射後は毎
分約900Åに減少し、該シリコン酸化膜11がち
密化したことを示した。 As a second experiment which is the premise of the present invention, a silicon oxide film was formed on the surface of an indium phosphide semiconductor by high frequency sputtering. The silicon oxide film was formed in an Ar atmosphere of 0.1 Torr, at a substrate temperature of 250°C.
The discharge power was 200W. The silicon oxide film formed had a thickness of 1260 Å and a refractive index of 1.46. The state in which the silicon oxide film is formed on the indium phosphide is exactly the same as in the case of Fig. 1a, and is indicated by 1 in the figure.
Consider replacing 1 with a silicon oxide film and 12 with indium phosphide. According to the present invention, when the entire surface of the silicon oxide film was irradiated with an electron beam under the same conditions as in the first embodiment, similar to the first embodiment, as shown in FIG. Curvature has been reduced. Infrared absorption spectroscopy revealed that the silanol group (Si-
(OH group) was reduced to approximately 1/10 by electron beam irradiation. In addition, the etching rate for a solution of NH 4 F:HF = 6:1 is approximately
While it was 3000 Å, it decreased to about 900 Å per minute after electron beam irradiation, indicating that the silicon oxide film 11 had become dense.
本発明の実施例として、本発明による保護膜形
成法を、拡散マスクに適用した例を示す。第2図
は、従来から行なわれている拡散マスクの製造工
程を示している。まず半導体21の表面全面にシ
リコン窒化膜、シリコン酸化膜等の保護膜22を
従来の方法で形成(第2図a)した後、保護膜2
2の上に感光剤23を塗布する(第2図b)。そ
して紫外線露光技術により拡散するところの保護
膜を除去して、保護膜による拡散マスクが形成さ
れる(第2図c)。第3図は本発明による保護膜
形成法を用いて拡散マスクを製造した一例を示し
ている。まず、半導体31の上に、プラズマ
CVD法によつてシリコン窒化膜32を形成した
(第3図a)後、拡散する部分以外のシリコン窒
化膜32′を電子ビーム照射した(第3図b)。第
1の実施例で記述したように、電子ビーム照射部
のシリコン窒化膜32′は、電子ビーム照射をし
ていないシリコン窒化膜32″に比べてち密にな
つている。電子ビーム照射の後、NH4F:HF=
6:1の溶液でシリコン窒化膜のエツチングを行
なつたところ、電子ビーム照射されていないシリ
コン窒化膜32″は、電子ビーム照射部のシリコ
ン窒化膜32′よりも10倍以上速く選択的にエツ
チングされ、第3図cに示す如く拡散マスクが形
成された。また、CF4(フレオン)ガスの放電を
利用した乾式エツチングやArイオン等を用いた
イオンエツチングによつても同様に、電子ビーム
照射部以外のシリコン窒化膜32″が優先的に除
去される。これは、従来の紫外線露光技術を導入
することなく、直接、保護膜を電子ビームで描画
することによつて拡散マスクを形成することがで
きるという利点を有している。 As an example of the present invention, an example will be shown in which the protective film forming method according to the present invention is applied to a diffusion mask. FIG. 2 shows a conventional process for manufacturing a diffusion mask. First, a protective film 22 such as a silicon nitride film or a silicon oxide film is formed on the entire surface of the semiconductor 21 using a conventional method (FIG. 2a).
A photosensitive agent 23 is applied on top of the photosensitive material 2 (FIG. 2b). Then, the protective film where the light is diffused is removed by ultraviolet exposure technology, and a diffusion mask made of the protective film is formed (FIG. 2c). FIG. 3 shows an example of a diffusion mask manufactured using the protective film forming method according to the present invention. First, plasma is placed on the semiconductor 31.
After forming the silicon nitride film 32 by the CVD method (FIG. 3a), the silicon nitride film 32' other than the portion to be diffused was irradiated with an electron beam (FIG. 3b). As described in the first embodiment, the silicon nitride film 32' in the electron beam irradiation area is denser than the silicon nitride film 32'' that has not been irradiated with the electron beam.After electron beam irradiation, NH4F :HF=
When the silicon nitride film was etched with a 6:1 solution, the silicon nitride film 32'' that had not been irradiated with the electron beam was selectively etched more than 10 times faster than the silicon nitride film 32' in the electron beam irradiated area. A diffusion mask was formed as shown in FIG . The silicon nitride film 32'' other than the above portion is preferentially removed. This has the advantage that the diffusion mask can be formed by directly writing the protective film with an electron beam without introducing conventional ultraviolet exposure technology.
以上のように、本発明による半導体の保護膜形
成法は、プラズマCVD法あるいは高周波スパツ
タリング法を用いて低温のもとで保護膜を形成し
た際、保護膜中に含まれている水素を荷電粒子あ
るいはレーザ光照射によつて離脱させることがで
き、且つ、保護膜および半導体の彎曲や亀裂、保
護膜の剥れ等の問題を除去することができ、且つ
保護膜をち密化できるため、例えば電子ビーム照
射部と、照射されていない部分とで、エツチング
速度に選択性を持たせることができるという種々
の利点を有する。 As described above, in the method for forming a protective film for a semiconductor according to the present invention, when a protective film is formed at a low temperature using plasma CVD or high frequency sputtering, hydrogen contained in the protective film is transferred to charged particles. Alternatively, it can be separated by laser beam irradiation, and problems such as bending and cracking of the protective film and semiconductor, peeling of the protective film, etc. can be removed, and the protective film can be made denser. This method has various advantages in that the etching rate can be selectively determined between the beam irradiated portion and the non-irradiated portion.
第1図は、保護膜を半導体上に形成したときの
断面を示すものであつて、(a)は電子ビーム照射
前、(b)は電子ビーム照射後を示している。第1図
において11は保護膜、12は半導体である。第
2図は、従来の方法を用いた拡散マスクの製造方
法を示すもので、21は半導体、22は保護膜、
23は感光剤である。第3図は、本発明による拡
散マスクの製造方法を示すもので、31は半導
体、32は保護膜で、32′は電子ビーム照射部、
32″は電子ビーム照射をしていない部分の保護
膜である。
FIG. 1 shows a cross section of a protective film formed on a semiconductor, with (a) showing the state before electron beam irradiation, and (b) showing the state after electron beam irradiation. In FIG. 1, 11 is a protective film and 12 is a semiconductor. FIG. 2 shows a method of manufacturing a diffusion mask using a conventional method, in which 21 is a semiconductor, 22 is a protective film,
23 is a photosensitizer. FIG. 3 shows a method of manufacturing a diffusion mask according to the present invention, in which 31 is a semiconductor, 32 is a protective film, 32' is an electron beam irradiation part,
32'' is a protective film on a portion not irradiated with an electron beam.
Claims (1)
ング法によつて絶縁膜を半導体表面上に形成した
後、該絶縁膜表面の少なくとも一部分に、集束さ
れた荷電粒子ビームあるいはレーザ光ビームを選
択的に照射して、照射部分を加熱する工程、及
び、エツチングにより前記照射部分以外の絶縁膜
を優先的に除去することにより、照射部分のみを
絶縁膜を選択的に該半導体表面上に形成すること
を特徴とする半導体表面保護膜の形成方法。1 After forming an insulating film on a semiconductor surface by a plasma CVD method or a high-frequency sputtering method, at least a portion of the surface of the insulating film is selectively irradiated with a focused charged particle beam or a laser beam. A semiconductor surface characterized in that an insulating film is selectively formed on the semiconductor surface only in the irradiated part by heating the part and preferentially removing the insulating film other than the irradiated part by etching. How to form a protective film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10452680A JPS5730337A (en) | 1980-07-30 | 1980-07-30 | Formation of surface protecting film for semiconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10452680A JPS5730337A (en) | 1980-07-30 | 1980-07-30 | Formation of surface protecting film for semiconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5730337A JPS5730337A (en) | 1982-02-18 |
| JPS6313339B2 true JPS6313339B2 (en) | 1988-03-25 |
Family
ID=14382928
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10452680A Granted JPS5730337A (en) | 1980-07-30 | 1980-07-30 | Formation of surface protecting film for semiconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5730337A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6461026A (en) * | 1987-09-01 | 1989-03-08 | Nec Corp | Manufacture of semiconductor device |
| JPH088265B2 (en) * | 1988-09-13 | 1996-01-29 | 株式会社東芝 | Compound semiconductor device and manufacturing method thereof |
| US7585704B2 (en) * | 2005-04-01 | 2009-09-08 | International Business Machines Corporation | Method of producing highly strained PECVD silicon nitride thin films at low temperature |
| TWI338335B (en) * | 2005-11-07 | 2011-03-01 | Samsung Electronics Co Ltd | Semiconductor devices and methods of manufacturing the same |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| ATE441T1 (en) * | 1978-06-26 | 1981-12-15 | Contraves Ag | PROCEDURE FOR DIGITAL INTERPOLATION OF A PERIOD OF A THREE-PHASE ANALOG SIGNAL. |
-
1980
- 1980-07-30 JP JP10452680A patent/JPS5730337A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5730337A (en) | 1982-02-18 |
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