JPH0666278B2 - Film forming equipment - Google Patents
Film forming equipmentInfo
- Publication number
- JPH0666278B2 JPH0666278B2 JP62334624A JP33462487A JPH0666278B2 JP H0666278 B2 JPH0666278 B2 JP H0666278B2 JP 62334624 A JP62334624 A JP 62334624A JP 33462487 A JP33462487 A JP 33462487A JP H0666278 B2 JPH0666278 B2 JP H0666278B2
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- JP
- Japan
- Prior art keywords
- film
- substrate
- microwave
- reaction chamber
- film forming
- Prior art date
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Description
【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、次世代の超LSI製造工程で要求される低温の
条件で良質な膜を成膜する装置を提供するものである。DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention provides an apparatus for forming a good quality film under the low temperature condition required in the next-generation VLSI manufacturing process.
〈従来の技術〉 今後の超LSIの開発にあたっては、現在の超LSIの高集積
化を実現している素子回路寸法の縮小という技術の延長
からだけでは採算や素子の信頼性を考えると限界を迎え
る事態が予測される。そのような将来の超LSIの高集積
化は、三次元LSIで提案されているように絶縁膜を介し
て回路を多層化するSOI技術や、従来の半導体装置のよ
うに回路平面上に水平に形成していたトランジスタを垂
直方向に形成する等をして実現されると予測される。ま
たLSIの高機能化を実現するために1つの基板上にMOS−
FETとバイポーラトランジスタを混在させるBi−CMOS技
術も普及すると期待される。<Prior art> In the future development of VLSI, there is a limit when considering the profitability and the reliability of the device only by extending the technology of reducing the device circuit size, which realizes the high integration of the present VLSI. The situation is expected to be reached. Such high integration of VLSIs in the future can be achieved by SOI technology that multi-layers circuits with insulating films as proposed in 3D LSIs, or by horizontally leveling on the circuit plane like conventional semiconductor devices. It is expected to be realized by forming the formed transistor in the vertical direction. Moreover, in order to realize the high functionality of LSI, MOS-on one substrate
Bi-CMOS technology that mixes FETs and bipolar transistors is also expected to spread.
〈発明が解決しようとする問題点〉 このような素子構造の変化に対応するためには既存の技
術では対応できない。例えば三次元LSIのようにLSI上に
多層構造で回路を集積しようとすると、上層部の素子形
成時に不純物拡散や絶縁膜形成として1000度程度の熱処
理を必要とし、これに対応するために配線材料に高抵抗
の高融点金属を使わざるを得ない。しかし回路の集積度
をあげるためには、配線材料としてはより低抵抗である
アルミ合金の方が有利である。またBi−CMOS技術におい
ては、バイポーラを形成するために単結晶成長をしなけ
ればならないため同様に1000度近傍の高温熱処理を要す
る。また高温の熱処理サイクルを経るに従って基板の反
りや配線材料の断線等が生じ製造中に不良品が発生しや
すく、製造条件も厳しくなる等の問題がある。<Problems to be Solved by the Invention> In order to cope with such a change in the element structure, the existing technology cannot cope. For example, when trying to integrate a circuit in a multi-layered structure on an LSI such as a three-dimensional LSI, it is necessary to perform a heat treatment at about 1000 degrees for impurity diffusion or insulating film formation when forming an upper layer element. Inevitably, a refractory metal with high resistance is used. However, in order to increase the degree of circuit integration, an aluminum alloy having a lower resistance is more advantageous as a wiring material. Further, in the Bi-CMOS technology, a single crystal growth must be performed to form a bipolar, so a high temperature heat treatment in the vicinity of 1000 degrees is also required. Further, there is a problem that a warp of a substrate, a disconnection of a wiring material, and the like occur due to a heat treatment cycle at high temperature, a defective product is likely to occur during manufacturing, and manufacturing conditions are severe.
処で超LSIの各種材料の成膜は現在500度以上の高温を必
要とするものが多い。その理由は、膜の原料ガスを分解
する方法として基板温度を上昇させて熱分解する方法を
用いる熱CVDが良質な膜を成膜できることにある。例え
ば従来から開発されている低温の成膜技術であるプラズ
マCVDを用いると、シリコン等の半導体材料の成膜は可
能であるが、超LSI等に使用される微細なトランジスタ
を形成するのに欠陥密度が多いため実用化できていな
い。また低温成膜であっても欠陥を誘起しにくい光CVD
法を用いると、低温で成膜することは可能であるが、膜
質としては400度程度の温度では結晶の粒径も小さく成
長速度も小さいという問題点がある。それに加えて水銀
増感法を用いないと紫外域のレーザやランプで分解可能
な原料ガスは限られており、設備に高価なものを使用し
なければならない。また光を入射する窓への膜堆積が生
じることによって膜堆積速度が変化したり発塵したりす
るため装置上の問題点もある。At present, film formation of various materials for VLSI often requires a high temperature of 500 ° C. or higher. The reason is that thermal CVD, which uses a method of thermally decomposing the substrate temperature as a method of decomposing the raw material gas of the film, can form a high-quality film. For example, using plasma CVD, which is a low-temperature film-forming technology that has been developed in the past, it is possible to form semiconductor materials such as silicon, but it is a defect in forming minute transistors used in VLSIs. It has not been put to practical use due to its high density. Also, optical CVD that does not easily induce defects even at low temperature film formation
When the method is used, it is possible to form a film at a low temperature, but the film quality has a problem that the crystal grain size is small and the growth rate is small at a temperature of about 400 degrees. In addition, the source gas that can be decomposed by a laser or lamp in the ultraviolet region is limited unless the mercury sensitization method is used, and expensive equipment must be used. There is also a problem in the apparatus because the film deposition rate changes or dust is generated due to film deposition on the window into which light is incident.
そのために近年においては、400℃程度の低温で超LSIに
必要な各種材料を形成する技術が各方面で精力的に研究
されている。Therefore, in recent years, various techniques have been vigorously studied in various fields for forming various materials required for VLSI at a low temperature of about 400 ° C.
本発明は上記従来の成膜装置の問題点に鑑みてなされた
もので、超LSIの製造に必要な半導体、絶縁体、金属等
の材料を低温の条件で成膜する装置を提供することにあ
る。The present invention has been made in view of the problems of the conventional film forming apparatus described above, and provides an apparatus for forming a film of a material such as a semiconductor, an insulator, or a metal necessary for manufacturing a VLSI under a low temperature condition. is there.
〈問題点を解決するための手段〉 本発明は、原料ガスのマイクロ波放電による分解と同時
に基板表面に紫外レーザ光照射を行って原料ガスに含ま
れた成分の薄膜を成膜する成膜装置において、上記マイ
クロ波が放電される領域を囲む内壁面が絶縁体で被覆さ
れており、且つ、側面に上記紫外レーザ光が上記基板表
面に照射されるように設けられた透光性窓を有する反応
室と、上記基板に対し、平行に且つ上方から上記マイク
ロ波を上記反応室に導入するマイクロ波導入管と、上記
紫外レーザ光を上記透光性窓を通して上記基板表面に対
して斜めに照射する位置に配置される光学系とを有する
ことを特徴とする成膜装置を提供する。<Means for Solving Problems> The present invention is directed to a film forming apparatus for forming a thin film of a component contained in a raw material gas by simultaneously irradiating a substrate surface with an ultraviolet laser beam while decomposing the raw material gas by microwave discharge. In, the inner wall surface surrounding the region where the microwave is discharged is covered with an insulator, and has a translucent window provided on a side surface so that the ultraviolet laser light is irradiated to the substrate surface. A microwave introduction tube for introducing the microwave into the reaction chamber from above and in parallel to the reaction chamber and the substrate, and the ultraviolet laser light is obliquely applied to the surface of the substrate through the transparent window. And an optical system arranged at a position to provide a film forming apparatus.
〈作用〉 本発明によれば、成膜を要する基板表面において、基板
表面に照射するレーザ光は予め強度が調整されているた
め成膜領域全体に亘って均一な膜成長を低温で行うこと
ができ、欠陥の少ない安定した膜を形成することができ
る。<Operation> According to the present invention, on the substrate surface requiring film formation, the intensity of the laser beam irradiated on the substrate surface is adjusted in advance, so that uniform film growth can be performed at low temperature over the entire film formation region. It is possible to form a stable film with few defects.
〈実施例〉 本発明は400℃以下で超LSIの各種材料膜を成膜する際、
原料ガスの放電による分解と同時にレーザ光照を行って
成膜する装置であり、このようにプラズマCVDと光CVDの
両者の利点を組み合わせることにより低温で良質な膜の
堆積が可能である。また本発明は、大口径の基板に均一
に成膜する方式であり、しかも荷電粒子による照射損傷
を低減する方式を併せ持つ成膜装置である。<Example> The present invention, when forming various material films of VLSI at 400 ° C or lower,
This is an apparatus for performing film formation by performing laser irradiation at the same time as decomposition of the raw material gas by discharge, and by combining the advantages of both plasma CVD and optical CVD in this way, it is possible to deposit a high-quality film at low temperatures. Further, the present invention is a film forming apparatus having a method of uniformly forming a film on a large-diameter substrate and also a method of reducing irradiation damage due to charged particles.
第1図において、反応室1には成膜のための基板2を支
持する傾斜自在の保持台3が設けられている。反応室1
の壁面には導波管4が結合され、上記基板2の表面に対
して平行に2.45GHzのマイクロ波が導入され、該導入さ
れたマイクロ波に対して進行方向と垂直方向に磁石10に
よって磁界がかけられる。また反応室1には透光性の窓
5が設けられ、エキシマレーザ光6を所望の角度で上記
基板2上に照射する。上記エキシマレーザ光6はレーザ
発生装置7で投射された後、光強度の調整を行なうため
の減衰器(反射板)やレンズからなる光強度調整部8を
通過し、更にレーザビーム走査機構9を通過する際にビ
ーム方向が制御され、基板2への入射角度のみならず照
射領域を調整して基板2面を2次元に走査する。11及び
12は上記反応室1に原料ガス或いは希釈ガスを供給し、
排気するための系路である。上記反応室1のマイクロ導
波管4が結合された放電領域13は少なくとも内壁面が石
英等の絶縁体で被覆されている。In FIG. 1, the reaction chamber 1 is provided with a tiltable holding table 3 for supporting a substrate 2 for film formation. Reaction chamber 1
A waveguide 4 is coupled to the wall surface of the substrate 2, a microwave of 2.45 GHz is introduced parallel to the surface of the substrate 2, and a magnetic field is generated by a magnet 10 in a direction perpendicular to the introduced microwave. Can be applied. Further, a translucent window 5 is provided in the reaction chamber 1, and the substrate 2 is irradiated with the excimer laser light 6 at a desired angle. After the excimer laser light 6 is projected by the laser generator 7, the excimer laser light 6 passes through a light intensity adjusting unit 8 including an attenuator (reflecting plate) and a lens for adjusting the light intensity, and a laser beam scanning mechanism 9 is further applied. When passing, the beam direction is controlled, and not only the incident angle to the substrate 2 but also the irradiation area is adjusted to scan the surface of the substrate 2 two-dimensionally. 11 and
12 supplies a raw material gas or a dilution gas to the reaction chamber 1,
It is a system for exhausting air. At least the inner wall surface of the discharge region 13 of the reaction chamber 1 to which the micro-waveguide 4 is coupled is covered with an insulator such as quartz.
まずプラズマCVDと光CVDを併用する成膜装置の特性につ
いて説明する。First, the characteristics of a film forming apparatus that uses both plasma CVD and optical CVD will be described.
上記成膜装置はマイクロ波放電部において原料ガスの分
解を行なうため、光CVDで問題になるような原料ガスに
対する制約はない。しかし、マイクロ波放電によるガス
分解を用いた場合放電領域で発生している荷電粒子、と
くに電子の基板への拡散をおさえることが必要である。
なぜならばマイクロ波をプラズマの励起源として用いる
と汚染源である無電極放電は容易に実現できるが、電磁
波で発生する電場強度の振動に対して追従性のよい電子
がイオンにくらべて高いエネルギーの状態になるために
様々な問題が生じる。即ち基板への電子拡散を抑える手
段を併用しない場合、基板にたいする電子の照射損傷が
生じたりまた電子とイオンの移動度に大きな差があるた
めにプラズマの電位が上昇し、イオンの堆積膜への打ち
込みが欠陥を誘起したりする。そこで電子の拡散を抑え
るために反応室1内に磁石10を設置して磁場を印加す
る。このように電子が加速される電場の方向に対して垂
直に磁場をかけることにより、電子の運動を螺旋状にし
て実効的な電子の拡散速度を低下させることができる。
また反応室1のマイクロ波放電領域を絶縁膜で被覆する
ことによって電子のプラズマからの拡散を一層抑え得
る。Since the film forming apparatus decomposes the raw material gas in the microwave discharge part, there is no restriction on the raw material gas which causes a problem in photo CVD. However, when gas decomposition by microwave discharge is used, it is necessary to suppress the diffusion of charged particles, especially electrons, generated in the discharge region to the substrate.
This is because the electrodeless discharge that is a pollution source can be easily realized by using the microwave as the excitation source of the plasma, but the electron, which has good followability to the vibration of the electric field strength generated by the electromagnetic wave, has a higher energy state than the ion. Therefore, various problems occur. That is, when the means for suppressing the electron diffusion to the substrate is not used together, electron damage to the substrate occurs and the mobility of electrons and ions has a large difference, so that the potential of the plasma rises and the ion deposition on the deposited film is increased. Implantation may induce defects. Therefore, in order to suppress the diffusion of electrons, a magnet 10 is installed in the reaction chamber 1 and a magnetic field is applied. By thus applying a magnetic field perpendicular to the direction of the electric field in which the electrons are accelerated, it is possible to make the motion of the electrons spiral and reduce the effective diffusion rate of the electrons.
Further, by covering the microwave discharge region of the reaction chamber 1 with an insulating film, diffusion of electrons from plasma can be further suppressed.
さらに基板2にレーザ照射を行なっているのは、レーザ
光6を堆積膜の表面に照射することにより堆積膜の最表
面のみが温度上昇し拡散して荷電粒子による欠陥を除去
し、さらに熱アニールの効果により膜質を熱CVDで得ら
れるものと同等なレベルまで改善することができる。こ
の場合紫外領域の光を用いると、一般的に固体における
紫外域の光吸収係数が大きいため表面のみが光吸収し、
基板全体の温度上昇は100度以内程度に抑えることが可
能である。Further, the substrate 2 is laser-irradiated by irradiating the surface of the deposited film with the laser beam 6 so that only the outermost surface of the deposited film rises in temperature and diffuses to remove defects due to charged particles. By the effect of, the film quality can be improved to a level equivalent to that obtained by thermal CVD. In this case, when light in the ultraviolet region is used, generally only the surface absorbs light because the light absorption coefficient in the ultraviolet region of a solid is large,
The temperature rise of the entire substrate can be suppressed to within 100 degrees.
また放電領域からの反応種の拡散により成膜しているの
で基板表面は基板に相対する放電領域の端からの距離を
一定にしないと基板全体で均一な膜成長は不可能であ
る。そのためレーザ光6は基板2の表面に対して斜めに
入射する必要がある。本実施例では保持台3が19.5度の
角度で傾斜し、従ってレーザ光6は基板2に70.5度の角
度で照射される。Further, since the film is formed by diffusing the reactive species from the discharge region, uniform film growth cannot be performed on the entire substrate unless the distance from the end of the discharge region facing the substrate is constant. Therefore, the laser light 6 needs to be obliquely incident on the surface of the substrate 2. In this embodiment, the holding table 3 is tilted at an angle of 19.5 degrees, so that the laser beam 6 is irradiated onto the substrate 2 at an angle of 70.5 degrees.
また現状ではレーザの出力で制限されるためレーザ光を
固定すると処理面積は数センチ角であり将来の超LSIの
製造に使用される半径10cm程度の基板の処理は不可能で
ある。そこで本実施例では走査機構9を設けてレーザ光
6を基板表面2に対して2次元的に走査することにより
大面積の処理に対応している。また成膜は基板全体で進
行している一方、レーザによるアニール効果は膜が厚く
なると効果が薄くなると考えられるので成膜中レーザは
全面の走査を1サイクルとしそのサイクルを繰り返し行
ない基板の全面に対して逐次レーザ照射して成膜する。In addition, since the output of the laser is limited at present, the processing area is a few centimeters square when the laser light is fixed, and it is impossible to process a substrate with a radius of about 10 cm which will be used in the manufacture of future VLSI. Therefore, in the present embodiment, a scanning mechanism 9 is provided to two-dimensionally scan the laser beam 6 on the substrate surface 2 to cope with a large area process. Also, while film formation is progressing over the entire substrate, it is considered that the annealing effect by the laser becomes less effective as the film becomes thicker. Therefore, during film formation, the laser scans the entire surface as one cycle and repeats that cycle to cover the entire surface of the substrate. On the other hand, laser irradiation is sequentially performed to form a film.
上記装置において、レーザとしてKrF(248nm)エキシマ
レーザ、マイクロ波(2.45GHz)としては100Hzのパルス
発振の発振器を用い、原料ガスとしてSiH4ガスとArガ
スを混合させて基板温度400℃でガラス基板2上に成膜
させたところ、結晶成長が確認された。第2図は上記成
膜装置を用いて成長させたシリコン結晶薄膜のX線回折
の結果を示し、半値幅の小さい回折パターンピークが得
られており、比較的大粒径の結晶が成長したことが判
る。尚従来の650℃で堆積させる熱CVDシリコン膜の成長
速度は10−20nm/min、結晶は(110)配向でX線回折ピ
ークの半値幅から求めた粒径は約20nmであったが、上記
成膜装置では、成膜速度が20−30nm/minで(111)配向
の結晶粒径は約40nmであり、本実施例の方が成膜速度は
速くしかも結晶粒径の大きい膜を成長させることができ
る。In the above equipment, a KrF (248 nm) excimer laser is used as a laser, a pulse oscillation oscillator of 100 Hz is used as a microwave (2.45 GHz), and SiH 4 gas and Ar gas are mixed as a raw material gas to obtain a glass substrate at a substrate temperature of 400 ° C. When a film was formed on No. 2, crystal growth was confirmed. FIG. 2 shows the result of X-ray diffraction of a silicon crystal thin film grown using the above film-forming apparatus. A diffraction pattern peak with a narrow half width was obtained, indicating that a crystal with a relatively large grain size grew. I understand. The growth rate of the conventional thermal CVD silicon film deposited at 650 ° C. was 10-20 nm / min, and the crystal grain size was about 20 nm in the (110) orientation and the half-value width of the X-ray diffraction peak. In the film-forming apparatus, the film-forming speed is 20-30 nm / min and the (111) -oriented crystal grain size is about 40 nm. In this example, the film-formation rate is faster and a film having a larger crystal grain size is grown. be able to.
第3図は希釈ガスと原料ガスSiH4との流量比に対する
膜堆積速度の関係を示す。FIG. 3 shows the relationship between the film deposition rate and the flow rate ratio of the diluent gas and the source gas SiH 4 .
口径の大きい基板上への成膜に対応するため、レーザビ
ームを走査機構9で2次元的に走査し、基板全域に均一
にレーザ光を照射して成膜させることにより、基板面積
に拘らず均質な薄膜を成長させることができる。In order to cope with film formation on a substrate with a large aperture, the scanning mechanism 9 scans the laser beam two-dimensionally and irradiates the laser light uniformly over the entire substrate to form a film, regardless of the substrate area. A homogeneous thin film can be grown.
上記実施例はシリコン膜を成膜する場合を挙げて説明し
たが、他の金属膜や絶縁膜を同様に成膜することもでき
る。Although the above embodiment has been described with reference to the case where a silicon film is formed, other metal films or insulating films can be similarly formed.
〈効果〉 以上本発明によれば、マイクロ波放電によるガス分解を
用いた場合に放電領域で発生している電子の拡散を抑え
ることができるので、基板に対する電子の照射損傷の発
生やイオンの堆積膜への打ち込みによる欠陥の誘発を生
じさせることなく、低温で薄膜を成膜することができ、
高温処理に伴うウェハーの反りや配線切れ等の問題点を
解決することができ、また高温処理による不純物拡散が
なくなり、超LSI設計に際してアルミ合金の使用も可能
になって自由度が著しく増し、高集積化された半導体装
置の製造を容易にすることができる。<Effect> As described above, according to the present invention, since it is possible to suppress the diffusion of electrons generated in the discharge region when gas decomposition by microwave discharge is used, it is possible to cause the electron irradiation damage to the substrate and the deposition of ions. A thin film can be formed at a low temperature without causing defects due to implantation into the film,
Problems such as wafer warpage and wiring breakage due to high temperature processing can be solved, impurity diffusion due to high temperature processing is eliminated, and aluminum alloy can be used in VLSI design, significantly increasing the degree of freedom, It is possible to easily manufacture the integrated semiconductor device.
第1図は本発明の一実施例を示す概略構成図、第2図は
本発明を適用した薄膜のX線回折図、第3図は本発明に
よる原料ガスと堆積膜速度との関係を示す図である。 1:反応室、2:基板、3:保持台、4:導波管、6:レーザービ
ーム、7:光源、8:強度調整部、9:走査機構、10:磁石。FIG. 1 is a schematic configuration diagram showing an embodiment of the present invention, FIG. 2 is an X-ray diffraction diagram of a thin film to which the present invention is applied, and FIG. 3 shows a relationship between a source gas and a deposition film velocity according to the present invention. It is a figure. 1: reaction chamber, 2: substrate, 3: holding table, 4: waveguide, 6: laser beam, 7: light source, 8: intensity adjusting unit, 9: scanning mechanism, 10: magnet.
Claims (1)
時に基板表面に紫外レーザ光照射を行って原料ガスに含
まれた成分の薄膜を成膜する成膜装置において、 上記マイクロ波が放電される領域を囲む内壁面が絶縁体
で被覆されており、且つ、側面に上記紫外レーザ光が上
記基板表面に照射されるように設けられた透光性窓を有
する反応室と、 上記基板に対し、平行に且つ上方から上記マイクロ波を
上記反応室に導入するマイクロ波導入管と、 上記紫外レーザ光を上記透光性窓を通して上記基板表面
に対して斜めに照射する位置に配置される光学系とを有
することを特徴とする成膜装置。1. A microwave is discharged in a film forming apparatus for forming a thin film of a component contained in a raw material gas by irradiating a substrate surface with an ultraviolet laser beam simultaneously with decomposition of the raw material gas by microwave discharge. An inner wall surface surrounding the region is covered with an insulator, and a reaction chamber having a translucent window provided on the side surface so that the ultraviolet laser light is irradiated to the substrate surface, and the substrate, A microwave introduction tube for introducing the microwave into the reaction chamber in parallel and from above, and an optical system arranged at a position for obliquely irradiating the substrate surface with the ultraviolet laser light through the transparent window. A film forming apparatus comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62334624A JPH0666278B2 (en) | 1987-12-26 | 1987-12-26 | Film forming equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62334624A JPH0666278B2 (en) | 1987-12-26 | 1987-12-26 | Film forming equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01173616A JPH01173616A (en) | 1989-07-10 |
| JPH0666278B2 true JPH0666278B2 (en) | 1994-08-24 |
Family
ID=18279461
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62334624A Expired - Fee Related JPH0666278B2 (en) | 1987-12-26 | 1987-12-26 | Film forming equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0666278B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0865964A (en) * | 1994-07-20 | 1996-03-08 | Ogawa Seisakusho:Kk | Rotation control motor |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61230318A (en) * | 1985-04-05 | 1986-10-14 | Hitachi Ltd | Method for scanning laser |
| JPH0692280B2 (en) * | 1986-01-24 | 1994-11-16 | 株式会社日立製作所 | Crystal thin film manufacturing method |
-
1987
- 1987-12-26 JP JP62334624A patent/JPH0666278B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0865964A (en) * | 1994-07-20 | 1996-03-08 | Ogawa Seisakusho:Kk | Rotation control motor |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01173616A (en) | 1989-07-10 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |