JPH01147828A - Manufacture of multilayer semiconductor substrate - Google Patents
Manufacture of multilayer semiconductor substrateInfo
- Publication number
- JPH01147828A JPH01147828A JP62305892A JP30589287A JPH01147828A JP H01147828 A JPH01147828 A JP H01147828A JP 62305892 A JP62305892 A JP 62305892A JP 30589287 A JP30589287 A JP 30589287A JP H01147828 A JPH01147828 A JP H01147828A
- Authority
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- Japan
- Prior art keywords
- opening
- insulating film
- semiconductor substrate
- film
- forming
- 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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Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は半導体基板の製造方法に関し、特に絶縁体上
に形成された単結晶半導体基板上にトランジスタ等の回
路素子を形成する半導体基板の製造方法に関するもので
ある。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a method for manufacturing a semiconductor substrate, and particularly to a method for manufacturing a semiconductor substrate in which circuit elements such as transistors are formed on a single crystal semiconductor substrate formed on an insulator. It is about the method.
[従来の技術]
半導体装置の高性能化のため回路素子を誘電体で分離し
て浮遊容量の少ない半導体集積回路を製造する試み、ま
たは回路素子を立体的に積層するいわゆる3次元回路素
子を製造する試みがなされており、その一方法として絶
縁層上に非単結晶の半導体層を形成し、これをレーザ光
などのエネルギ線を照射することによって表面層のみを
加熱し、単結晶の半導体層を形成する方法がある。この
際絶縁体に部分的に半導体ill結晶基板に達する開口
部を設けておき、非単結晶の半導体層の溶融を開口部の
単結晶半導体基板の表面にまで及ばせることにより、非
単結晶の半導体層を基板単結晶と同一の結晶軸をもった
単結晶にすることが試みられている。[Prior art] In order to improve the performance of semiconductor devices, attempts have been made to separate circuit elements with dielectrics to manufacture semiconductor integrated circuits with low stray capacitance, or to manufacture so-called three-dimensional circuit elements in which circuit elements are stacked three-dimensionally. One method is to form a non-single-crystal semiconductor layer on an insulating layer, heat only the surface layer by irradiating it with energy beams such as laser light, and form a single-crystal semiconductor layer. There is a way to form. At this time, an opening that partially reaches the semiconductor ill crystal substrate is provided in the insulator, and by causing the melting of the non-single crystal semiconductor layer to reach the surface of the single crystal semiconductor substrate in the opening, the non-single crystal semiconductor layer is melted. Attempts have been made to make the semiconductor layer a single crystal having the same crystal axis as the single crystal substrate.
第4図は従来のエネルギ線を照射する直前の結晶基板の
平面図であり、第5図は第4図の■−■断面図である。FIG. 4 is a plan view of a crystal substrate immediately before being irradiated with a conventional energy beam, and FIG. 5 is a cross-sectional view taken along the line -■ in FIG.
以下、両図を参照してその構成について説明する。The configuration will be described below with reference to both figures.
まず、111結晶よりなるシリコン基板1上に二酸化シ
リコンよりなる酸化膜2が厚さ1μmで形成され、所定
位置にシリコン基板1に達する開口3が設けられる。開
口3内部を含み、酸化膜2上に化学的気相成長法(CV
D法)で0.5μmの厚さに多結晶シリコン5を堆積さ
せ、その上にやはりCVD法で10OAの厚さに酸化膜
6を堆積させる。さらに酸化膜6上には開口部3上方位
置にCVD法で50OAの厚さにストライプ状の窒化膜
7が堆積される。また窒化膜7に挾まれた酸化膜6上に
は、同じ< CVD法で500Aの厚さの窒化膜12が
幅5μm1間隔10μmで形成される。ここで、開口3
は通常スクライブ線と呼ばれ幅100ないし200μm
、長さ10〜20mmで半導体集積回路のチップを分断
するための領域として設けられている。First, an oxide film 2 made of silicon dioxide is formed to a thickness of 1 μm on a silicon substrate 1 made of 111 crystal, and an opening 3 reaching the silicon substrate 1 is provided at a predetermined position. Chemical vapor deposition (CV) is performed on the oxide film 2, including the inside of the opening 3.
Polycrystalline silicon 5 is deposited to a thickness of 0.5 μm using the method D), and an oxide film 6 is deposited thereon to a thickness of 10 OA using the CVD method. Further, on the oxide film 6, a striped nitride film 7 is deposited to a thickness of 50 OA above the opening 3 by the CVD method. Further, on the oxide film 6 sandwiched between the nitride films 7, a nitride film 12 having a thickness of 500 Å is formed with a width of 5 μm and an interval of 10 μm using the same CVD method. Here, opening 3
is usually called a scribe line and has a width of 100 to 200 μm.
, is provided as a region for dividing a semiconductor integrated circuit chip with a length of 10 to 20 mm.
第6図はエネルギ線の照射時における半導体基板の断面
図である。FIG. 6 is a cross-sectional view of the semiconductor substrate during irradiation with energy beams.
以下、図を参照して照射状態について説明する。The irradiation state will be described below with reference to the drawings.
第5図のような構造の基板に連続発振のアルゴンレーザ
光9を100μmに絞って走査速度25cm/sで走査
しながら照射し、多結晶シリコン5を溶融させる。溶融
された溶融シリコン10の固化再結晶化は開口3の単結
晶のシリコン基板1から酸化膜2上の多結晶シリコン5
に向かって起こり、酸化膜2上の多結晶シリコン5はレ
ーザ光の照射が終了すると基板単結晶シリコンと同一の
結晶軸を持った単結晶化シリコン11になる。この際、
開口3上の窒化膜7はレーザ光照射時にレーザ光の反射
防止膜として働き、酸化膜2より熱拡散が大きい開口3
中の多結晶シリコンの温度下降を防ぐために設けられて
いる。さらに、酸化膜21−の多結晶シリコン5−Lに
設けられたストライプ状の窒化膜12は、レーザ光照射
時の多結晶シリコン5の横方向温度分布を制御し、単結
晶成長がチップ全体に続くように設けられており、その
再結晶化の機構については特願昭61−048468に
詳細に述べられている。また、酸化膜6はレーザ光照射
時に溶融した溶融シリフン10中へ窒化膜7,12中の
窒素が混入しないための混入阻止膜として設けられてい
る。レーザ光照射が終了し、チップ内の多結晶シリコン
5が単結晶化した後、窒化膜7.12および酸化膜6は
除去された後は通常の集積回路製造プロセスによって酸
化膜2上の単結晶化シリコン11に回路素子が形成され
る。全プロセス終了後に半導体基板は開口3に沿って分
断(スクライブ)され、10〜20m・m角の半導体集
積回路のチップが完成する。したがって、開口3は酸化
膜2」二に単結晶シリコン基板1と同じ結晶軸を持った
ilj結晶化シリコン11を製造する役割と、全プロセ
ス終了後集積回路チップを分断するためのスクライブ線
としての役割を持っている。A substrate having a structure as shown in FIG. 5 is irradiated with continuous wave argon laser light 9 focused to 100 μm while scanning at a scanning speed of 25 cm/s to melt polycrystalline silicon 5. The melted silicon 10 is solidified and recrystallized from the single crystal silicon substrate 1 in the opening 3 to the polycrystalline silicon 5 on the oxide film 2.
When the laser beam irradiation is completed, the polycrystalline silicon 5 on the oxide film 2 becomes a single crystal silicon 11 having the same crystal axis as the single crystal silicon substrate. On this occasion,
The nitride film 7 on the aperture 3 acts as an anti-reflection film for laser light during laser light irradiation, and the aperture 3 has greater thermal diffusion than the oxide film 2.
This is provided to prevent the temperature of the polycrystalline silicon inside from dropping. Furthermore, the striped nitride film 12 provided on the polycrystalline silicon 5-L of the oxide film 21- controls the lateral temperature distribution of the polycrystalline silicon 5 during laser beam irradiation, and allows single crystal growth to occur over the entire chip. The recrystallization mechanism is described in detail in Japanese Patent Application No. 61-048468. Further, the oxide film 6 is provided as a contamination prevention film to prevent nitrogen in the nitride films 7 and 12 from being mixed into the molten silicon 10 melted during laser beam irradiation. After the laser beam irradiation is finished and the polycrystalline silicon 5 in the chip has become a single crystal, the nitride film 7.12 and the oxide film 6 are removed, and then the single crystal on the oxide film 2 is formed by a normal integrated circuit manufacturing process. Circuit elements are formed on the silicon oxide 11. After all processes are completed, the semiconductor substrate is scribed along the openings 3 to complete semiconductor integrated circuit chips of 10 to 20 m square. Therefore, the opening 3 serves to manufacture the ilj crystallized silicon 11 having the same crystal axis as the single crystal silicon substrate 1 on the oxide film 2, and also as a scribe line for dividing the integrated circuit chip after the completion of all processes. have a role.
[発明が解決しようとする問題点]
上記のような従来の製造方法においては、開口3が直線
上に大きな領域にわたって形成されていた。したがって
開口3中の多結晶シリコン5と酸化膜2上の多結晶シリ
コン5の溶融時の温度分布が違う(酸化膜2上の多結晶
シリコン5の温度が高い)ため、溶融シリコン10の粘
度は酸化膜2上の方が小さくなる。そのため酸化膜2.
6との界面Cと働く表面張力により、開口3端に接する
酸化膜2上の多結晶シリコン5は再結晶化時(単結晶化
時)にその膜厚が薄くなってしまう。[Problems to be Solved by the Invention] In the conventional manufacturing method as described above, the opening 3 is formed in a straight line over a large area. Therefore, since the temperature distribution during melting of the polycrystalline silicon 5 in the opening 3 and the polycrystalline silicon 5 on the oxide film 2 is different (the temperature of the polycrystalline silicon 5 on the oxide film 2 is higher), the viscosity of the molten silicon 10 is The portion on the oxide film 2 is smaller. Therefore, the oxide film 2.
Due to the surface tension acting on the interface C with 6, the thickness of the polycrystalline silicon 5 on the oxide film 2 in contact with the end of the opening 3 becomes thin during recrystallization (single crystallization).
第7図はこの状態を示した半導体基板の断面図である。FIG. 7 is a sectional view of the semiconductor substrate showing this state.
図に示すように開口3端部の酸化膜2上の多結晶シリコ
ン5は凹んで四部15となり、その凹んだ部分は走査下
流側の開口3端部の酸化膜21−の11t結晶化シリコ
ン11を膨れさせて凸部16を生じさせる。場合によっ
てはこの凹みがさらに進み開口3端での単結晶化シリコ
ン11が、溶融時の溶融シリコン10の移動により消滅
(膜厚が0になる)してしまうという問題点があった。As shown in the figure, the polycrystalline silicon 5 on the oxide film 2 at the end of the opening 3 is recessed to form a fourth part 15, and the recessed part is the 11t crystallized silicon 11 of the oxide film 21- at the end of the opening 3 on the downstream scanning side. The convex portion 16 is generated by swelling the convex portion 16. In some cases, this depression may progress further and the monocrystalline silicon 11 at the end of the opening 3 may disappear (the film thickness becomes 0) due to the movement of the molten silicon 10 during melting.
この問題は開口3と酸化膜2上での多結晶シリコン5の
溶融時の温度を均一にすれば解決されることは明白であ
るが、事実工種々の構造において温度を均一にすること
はコストの問題上困難であった。このようにスクライブ
線としての1辺5μm以上の長方形(直線状)の開口3
の周辺の単結晶化シリコン11は再結晶化後必ず膜厚が
減少し、他方端でその凸部を生じてしまうのである。It is clear that this problem can be solved by making the temperature uniform during melting of the polycrystalline silicon 5 on the opening 3 and the oxide film 2, but in fact it is costly to make the temperature uniform in various structures. It was difficult due to the problem of In this way, a rectangular (linear) opening 3 with each side of 5 μm or more is used as a scribe line.
After recrystallization, the single crystal silicon 11 around the single crystallized silicon 11 always decreases in film thickness, and a convex portion is formed at the other end.
この発明は上記のような問題点を解決するためになされ
たもので、単結晶半導体基板上に絶縁膜を介してlit
結晶の半導体層を膜厚の減少なしに得ることを目的とす
る。This invention was made to solve the above-mentioned problems.
The purpose is to obtain a crystalline semiconductor layer without reducing the film thickness.
[問題点を解決するための手段]
この発明に係る多層半導体基板の製造方法は、熱エネル
ギを走査して与えて非単結晶の半導体層を溶融させる際
、絶縁膜に形成された開口の熱エネルギの走査下流側で
あって所定範囲の絶縁膜上の半導体層だけを溶融させな
いものである。[Means for Solving the Problems] In the method for manufacturing a multilayer semiconductor substrate according to the present invention, when thermal energy is scanned and applied to melt a non-single-crystal semiconductor layer, the heat of the opening formed in the insulating film is This method does not melt only the semiconductor layer on the insulating film in a predetermined range on the downstream side of the energy scan.
[作用〕
この発明においては開口の熱エネルギの走査下流側の半
導体層を溶融させないので、この部分を凹ませるとなく
再結晶化後の単結晶化した半導体層の膜厚変化を抑える
。[Function] In the present invention, since the semiconductor layer on the downstream side of the scan of the thermal energy of the opening is not melted, this portion is not depressed, and the change in film thickness of the single crystal semiconductor layer after recrystallization is suppressed.
[実施例]
第1A図〜第1F図はこの発明の一実施例における製造
方法を示す概略工程断面図であり、第2図はエネルギ線
照射時の第1D図に対応する半導体基板の・[也面図で
ある。[Example] FIGS. 1A to 1F are schematic process cross-sectional views showing a manufacturing method in an embodiment of the present invention, and FIG. 2 is a cross-sectional view of a semiconductor substrate corresponding to FIG. It is also a side view.
以下、これらの図を参照してこの製造方法について説明
する。This manufacturing method will be explained below with reference to these figures.
まず、単結晶よりなるシリコン基板1にに厚さ1μmの
二酸化シリコンよりなる酸化膜2を形成しく第1A図参
照)、これをパターニングすることによってシリコン基
板1に達する開口3.4を形成する。ここで開口3はス
クライブ線(幅100〜200μm、長さ10〜20m
m)として用いるものであり、開口4は後工程での多結
晶半導体層の単結晶化時の種付用として用いられるもの
である。したがって、非単結晶の半導体層を単結晶シリ
コン基板と同一の結晶軸を持った単結晶とするまでもな
い場合は開口4を形成しなくてもよい(第1B図参照)
。First, an oxide film 2 made of silicon dioxide having a thickness of 1 μm is formed on a silicon substrate 1 made of a single crystal (see FIG. 1A), and an opening 3.4 reaching the silicon substrate 1 is formed by patterning this. Here, the opening 3 is a scribe line (width 100 to 200 μm, length 10 to 20 m)
m), and the opening 4 is used for seeding during single crystallization of a polycrystalline semiconductor layer in a later step. Therefore, if the non-single crystal semiconductor layer does not need to be a single crystal with the same crystal axis as the single crystal silicon substrate, it is not necessary to form the opening 4 (see Figure 1B).
.
開口3,4内部を含み、酸化膜2上にCVD法で多結晶
シリコンを厚さ0,5μmに堆積させ、さらにその」二
に同じ<CVD法で酸化膜6を厚さ100Aに堆積させ
る(第1C図参照)。Polycrystalline silicon is deposited to a thickness of 0.5 μm on the oxide film 2, including inside the openings 3 and 4, using the CVD method, and then an oxide film 6 is deposited to a thickness of 100 A using the same CVD method ( (See Figure 1C).
続いて、酸化膜6上にCVD法で窒化膜を堆積し、これ
をパターニングすることによって開口3゜4のそれぞれ
上方に対応する位置に厚さ500Aのストライプ状およ
び矩形状の窒化膜7,8を形成する(第1D図参照)。Next, a nitride film is deposited on the oxide film 6 by the CVD method, and this is patterned to form striped and rectangular nitride films 7 and 8 with a thickness of 500A at positions corresponding to the respective upper portions of the openings 3 and 4. (see Figure 1D).
第1D図の状態の平面図を示したのが第2図である(第
1D図は第2図のx−x’断面図である)が、第2図に
示すように窒化膜7で囲まれた酸化膜6上の領域には、
さらにストライブ状の窒化膜12が所定間隔で設けられ
ている。この窒化膜12はレーザ光照射時の多結晶シリ
コン5の横方向(レーザ走査方向)の温度分布を制御し
て、単結晶成長がチップ全体に続くように機能するのは
従来例と同じであるが、この発明では図面において左側
の窒化膜7の右側で20μmの範囲で窒化膜12が設け
られていない。FIG. 2 shows a plan view of the state shown in FIG. 1D (FIG. 1D is a sectional view taken along line xx' in FIG. 2). In the area on the oxidized film 6,
Furthermore, striped nitride films 12 are provided at predetermined intervals. As in the conventional example, this nitride film 12 functions to control the temperature distribution in the lateral direction (laser scanning direction) of the polycrystalline silicon 5 during laser beam irradiation so that single crystal growth continues throughout the chip. However, in this invention, the nitride film 12 is not provided in a range of 20 μm on the right side of the nitride film 7 on the left side in the drawing.
このような構成の半導体基板の、上方からビーム径10
0μmのアルゴンレーザ光9を第2図のX−X′の方向
に走査しながら照射する。するとまず最初にX側の開口
3の多結晶シリコン5が溶融して溶融シリコン10とな
る。しかしその右側の酸化膜2の上の窒化膜12が形成
されていない多結晶シリコン5はレーザ光が照射されて
いてもその反射率が高いため(波長4880Aのレーザ
光に対して酸化膜100Aのみの場合の反射率は約38
%、窒化膜50OA/酸化膜100Aの場合の反射率は
0. 2%)溶融しない。したがって、表面張力等の力
が働かないため開口3の右端での多結晶シリコン5の膜
厚の減少は起こらない。次にレーザ光は開口4の上を照
射することになるが、開口4は1辺5μmの正方形でか
つ離散的に設けられているので、多結晶シリコン5の溶
融時の温度の不均一性は小さい開口4周辺に限定される
。Beam diameter 10 from above of a semiconductor substrate with such a configuration
A 0 μm argon laser beam 9 is irradiated while scanning in the direction of X-X' in FIG. Then, first, the polycrystalline silicon 5 in the opening 3 on the X side melts and becomes molten silicon 10. However, the polycrystalline silicon 5 on the right side on which the nitride film 12 is not formed on the oxide film 2 has a high reflectance even when irradiated with laser light (only the oxide film 100A is exposed to the laser light with a wavelength of 4880A). The reflectance in case of is about 38
%, and the reflectance in the case of nitride film 50OA/oxide film 100A is 0. 2%) does not melt. Therefore, since forces such as surface tension do not work, the film thickness of polycrystalline silicon 5 does not decrease at the right end of opening 3. Next, the laser beam will irradiate the top of the aperture 4, but since the aperture 4 is a square with a side of 5 μm and is provided discretely, the non-uniformity of the temperature when the polycrystalline silicon 5 is melted is reduced. It is limited to the area around the small opening 4.
このため、開口4の周辺での再結晶化後の単結晶化シリ
コン11の膜厚の減少は低減されてかつ再結晶化後の単
結晶化シリコン11の結晶軸を単結晶シリコン基板1と
同一にすることができる(第1E図参照)。Therefore, the decrease in the film thickness of the single crystal silicon 11 after recrystallization around the opening 4 is reduced, and the crystal axis of the single crystal silicon 11 after recrystallization is the same as that of the single crystal silicon substrate 1. (see Figure 1E).
レーザ光照射が終了した後には窒化膜7,8゜12およ
び酸化膜6を除去し、単結晶化シリコン11−1xに通
常の集積回路の製造プロセスによって回路素子を形成す
ることができる(第1F図参照)なお、1−記実施例で
は、スクライブ線に相当する開口3端部の多結晶シリコ
ンを溶融させないようにしたが、直線状の開口部であっ
てエネルギ線の走査進行方向の端の辺の長さが(走査方
向に対して直角)j向)5μm以上ある開口部であれば
その目的(スクライブ線またはアライメントマークなど
)を問わず同様に適用することができる。After the laser beam irradiation is completed, the nitride films 7, 8° 12 and the oxide film 6 are removed, and circuit elements can be formed on the single crystal silicon 11-1x by a normal integrated circuit manufacturing process (1st F). Note that in Example 1-1, the polycrystalline silicon at the end of the opening 3, which corresponds to the scribe line, was not melted; Any opening having a side length of 5 μm or more (in the j direction (perpendicular to the scanning direction)) can be similarly applied regardless of its purpose (such as a scribe line or an alignment mark).
また、上記実施例では、開口3の端部の多結晶シリコン
を溶融させないためにその上方に窒化膜12を形成しな
いようにしたが、レーザ光の照射強度を変化させること
によってその部分のみ溶融させないとすることでも同様
の効果を奏する。In the above embodiment, the nitride film 12 was not formed above the polycrystalline silicon at the end of the opening 3 in order to prevent it from melting, but by changing the irradiation intensity of the laser beam, only that part is prevented from melting. A similar effect can also be achieved by doing so.
また、」二記実施例では、開口3上に窒化膜7を設けて
多結晶シリコン5を溶融するようにしたが、その必要が
なければ直線状の開口3゛の多結晶シリコンを溶融させ
なくてもよい。In addition, in the second embodiment, the nitride film 7 is provided over the opening 3 to melt the polycrystalline silicon 5, but if it is not necessary, the polycrystalline silicon in the linear opening 3 may not be melted. You can.
さらに、1−記実施例では、酸化膜2の下にデバイスが
形成されていない例を示したが、デバイスが形成されて
いても同様の効果を奏する。Further, in the embodiment 1-, an example was shown in which no device was formed under the oxide film 2, but the same effect can be obtained even if a device is formed.
第3図は他の実施例としてこのような構成を示す概略断
面図である。FIG. 3 is a schematic sectional view showing such a configuration as another embodiment.
図において、シリコン基板1上にゲート電極13や配線
14等により構成されたデバイスが酸化膜2に覆われて
おり、その上に多結晶シリコン5、さらに酸化膜6が形
成されている。レーザ光の照射要領等は上記実施例と同
様である。In the figure, a device made up of a gate electrode 13, wiring 14, etc. on a silicon substrate 1 is covered with an oxide film 2, on which a polycrystalline silicon 5 and an oxide film 6 are formed. The laser beam irradiation procedure and the like are the same as in the above embodiment.
[発明の効果コ
以上のようにこの発明によれば、開口の熱エネルギの走
査下流側の所定範囲の非単結晶の甲導体層を溶融しない
ようにしたので、熱エネルギ走査後の単結晶化した半導
体層が膜厚の凹凸なしに絶縁体1−に得られる効果があ
る。[Effects of the Invention] As described above, according to the present invention, the non-single crystal A conductor layer in a predetermined range downstream of the thermal energy scanning of the aperture is prevented from melting, so that the single crystallization after the thermal energy scanning is prevented. There is an effect that a semiconductor layer having a uniform thickness can be obtained in the insulator 1- without unevenness in film thickness.
第1A図〜第1F図はこの発明の一実施例における製造
方法を示す概略工程断面図、第2図は第1D図に対応す
る平面図(第1D図は第2図のX−X′断面図)、第3
図はこの発明の他の実施例におけるエネルギ線照射時の
概略断面図である。
第4図〜第7図はすべて従来例を示すものであり、第4
図はエネルギ線照射前の半導体基板の平面図、第5図は
第4図のV−■断面図、第6図はエネルギ線照射時の半
導体基板の断面図、第7図はエネルギ線照射後の半導体
層の状態を示した半導体基板の断面図である。
図において、1はシリコン基板、2は酸化膜、3.4は
開口、5は多結晶シリコン、6は酸化膜、7は窒化膜、
9はレーザ光、10は溶融シリコン、11は単結晶化シ
リコン、12は窒化膜である。
なお、各図中、同一符号は同一または相当部分を示す。
特許出願人 工業技術院長 飯 塚 幸 三第1A図
第3圀
第4図
85図
第6図
萬ワ唄1A to 1F are schematic process sectional views showing a manufacturing method in an embodiment of the present invention, and FIG. 2 is a plan view corresponding to FIG. Figure), 3rd
The figure is a schematic cross-sectional view during energy beam irradiation in another embodiment of the present invention. Figures 4 to 7 all show conventional examples;
The figure is a plan view of the semiconductor substrate before energy beam irradiation, Figure 5 is a cross-sectional view taken along the line V-■ in Figure 4, Figure 6 is a cross-sectional view of the semiconductor substrate during energy beam irradiation, and Figure 7 is after energy beam irradiation. FIG. 2 is a cross-sectional view of a semiconductor substrate showing the state of a semiconductor layer. In the figure, 1 is a silicon substrate, 2 is an oxide film, 3.4 is an opening, 5 is polycrystalline silicon, 6 is an oxide film, 7 is a nitride film,
9 is a laser beam, 10 is molten silicon, 11 is single crystal silicon, and 12 is a nitride film. In each figure, the same reference numerals indicate the same or corresponding parts. Patent applicant: Director of the Agency of Industrial Science and Technology Sachi Iizuka Figure 1A Figure 3 Figure 4 Figure 85 Figure 6 Manwa Uta
Claims (7)
る工程と、前記半導体基板の前記主面上に第1の絶縁膜
を形成する工程と、前記第1の絶縁膜の所定の位置に前
記半導体基板に達する所定の大きさの第1の開口を形成
する工程と、前記第1の開口内部を含み、前記第1の絶
縁膜上に非単結晶からなる半導体層を形成する工程と、
前記半導体層上に第2の絶縁膜を形成する工程と、前記
第1の開口を横断する方向に走査して、走査下流側の前
記第1の開口に接した所定範囲の前記第1の絶縁膜上の
領域の前記半導体層を除く前記半導体層を溶融するよう
に熱エネルギを与え、溶融した前記半導体層を単結晶化
する工程と、前記第2の絶縁膜を除去する工程とを備え
た、多層半導体基板の製造方法。(1) A step of preparing a semiconductor substrate made of a single crystal having a main surface, a step of forming a first insulating film on the main surface of the semiconductor substrate, and a step of forming a first insulating film at a predetermined position of the first insulating film. forming a first opening of a predetermined size that reaches the semiconductor substrate; forming a non-single-crystal semiconductor layer on the first insulating film, including the inside of the first opening;
forming a second insulating film on the semiconductor layer; and scanning in a direction across the first opening to form a second insulating film in a predetermined range in contact with the first opening on the downstream side of the scanning. The method includes the steps of: applying thermal energy to melt the semiconductor layer except for the semiconductor layer in a region on the film, converting the melted semiconductor layer into a single crystal; and removing the second insulating film. , a method for manufacturing a multilayer semiconductor substrate.
ギの走査下流側の前記所定範囲を除いた前記第1の絶縁
膜に前記半導体基板に達する第2の開口を形成する工程
を含み、前記半導体層が前記第2の開口内部にも形成さ
れる、特許請求の範囲第1項記載の多層半導体基板の製
造方法。(2) The step of forming the first opening includes the step of forming a second opening reaching the semiconductor substrate in the first insulating film excluding the predetermined range on the downstream side of scanning of the thermal energy. 2. The method of manufacturing a multilayer semiconductor substrate according to claim 1, wherein the semiconductor layer is also formed inside the second opening.
第1の開口の大きさに対応した第1の窒化膜を形成する
工程と、 前記第1の絶縁膜上方の前記第2の絶縁膜上に、前記熱
エネルギの走査方向に沿ったストライプ状の第2の窒化
膜を形成する工程とをさらに備え、前記第2の窒化膜は
、前記所定範囲の前記第1の絶縁膜の一部上の前記半導
体上方には形成されない、特許請求の範囲第1項または
第2項記載の多層半導体基板の製造方法。(3) forming a first nitride film corresponding to the size of the first opening on the second insulating film above the first opening; and forming a striped second nitride film along the scanning direction of the thermal energy on the second insulating film, wherein the second nitride film covers the first insulating film in the predetermined range. 3. The method of manufacturing a multilayer semiconductor substrate according to claim 1, wherein the semiconductor is not formed above the semiconductor on a part of the film.
体層は多結晶シリコンであり、前記第1および第2の絶
縁膜は二酸化シリコンである、特許請求の範囲第1項、
第2項または第3項記載の多層半導体基板の製造方法。(4) The semiconductor substrate is a silicon substrate, the semiconductor layer is polycrystalline silicon, and the first and second insulating films are silicon dioxide,
The method for manufacturing a multilayer semiconductor substrate according to item 2 or 3.
生する、特許請求の範囲第1項ないし第4項のいずれか
に記載の多層半導体基板の製造方法。(5) The method for manufacturing a multilayer semiconductor substrate according to any one of claims 1 to 4, wherein the thermal energy is generated by irradiation with energy beams.
である、特許請求の範囲第5項記載の多層半導体基板の
製造方法。(6) The method for manufacturing a multilayer semiconductor substrate according to claim 5, wherein the energy beam is continuous wave argon laser light.
角方向に5μm以上の長さを有する、特許請求の範囲第
1項ないし第6項のいずれかに記載の多層半導体基板の
製造方法。(7) The method for manufacturing a multilayer semiconductor substrate according to any one of claims 1 to 6, wherein the first opening has a length of 5 μm or more in a direction perpendicular to the energy scanning direction. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62305892A JPH0693429B2 (en) | 1987-12-04 | 1987-12-04 | Method for manufacturing multilayer semiconductor substrate |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62305892A JPH0693429B2 (en) | 1987-12-04 | 1987-12-04 | Method for manufacturing multilayer semiconductor substrate |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01147828A true JPH01147828A (en) | 1989-06-09 |
| JPH0693429B2 JPH0693429B2 (en) | 1994-11-16 |
Family
ID=17950565
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62305892A Expired - Lifetime JPH0693429B2 (en) | 1987-12-04 | 1987-12-04 | Method for manufacturing multilayer semiconductor substrate |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0693429B2 (en) |
-
1987
- 1987-12-04 JP JP62305892A patent/JPH0693429B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0693429B2 (en) | 1994-11-16 |
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