JPS629212B2 - - Google Patents
Info
- Publication number
- JPS629212B2 JPS629212B2 JP55081600A JP8160080A JPS629212B2 JP S629212 B2 JPS629212 B2 JP S629212B2 JP 55081600 A JP55081600 A JP 55081600A JP 8160080 A JP8160080 A JP 8160080A JP S629212 B2 JPS629212 B2 JP S629212B2
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor layer
- groove
- single crystal
- layer
- grooves
- 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
Links
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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/29—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by the substrates
- H10P14/2901—Materials
- H10P14/2922—Materials being non-crystalline insulating materials, e.g. glass or polymers
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/38—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by treatments done after the formation of the materials
- H10P14/3802—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H10P14/3808—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth using laser beams
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/29—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by the substrates
- H10P14/2924—Structures
- H10P14/2925—Surface structures
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/34—Deposited materials, e.g. layers
- H10P14/3402—Deposited materials, e.g. layers characterised by the chemical composition
- H10P14/3404—Deposited materials, e.g. layers characterised by the chemical composition being Group IVA materials
- H10P14/3411—Silicon, silicon germanium or germanium
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/34—Deposited materials, e.g. layers
- H10P14/3451—Structure
- H10P14/3452—Microstructure
- H10P14/3458—Monocrystalline
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/38—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by treatments done after the formation of the materials
- H10P14/3802—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H10P14/3818—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth using particle beams
-
- 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
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/38—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by treatments done after the formation of the materials
- H10P14/3802—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H10P14/382—Scanning of a beam
Landscapes
- Recrystallisation Techniques (AREA)
Description
【発明の詳細な説明】
本発明は、誘電体基板上に半導体層を形成する
いわゆるSOI(Silicon on Insulator)構造の半導
体装置の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a semiconductor device having a so-called SOI (Silicon on Insulator) structure in which a semiconductor layer is formed on a dielectric substrate.
二酸化シリコン(SiO2)、石英ガラス等の誘電
体(絶縁)基板の表面に溝を設け、該基板表面に
多結晶シリコンまたは非晶質シリコン層を被着
し、該層をレーザアニールすると該溝を核として
SOS(Silicon on Sapphire)構造と同等もしく
はより良質の単結晶が成長することが知られてい
る。第1図aはその一例を示すもので、1は誘電
体基板、2はその表面に深さ1000〜2000Å程度に
形成された溝、3は厚さ5000Å程度のシリコン層
である。シリコン層3は例えば化学気相成長
(CVD)法で多結晶シリコンを成長させ、それを
レーザアニールしてメルトしたもので、凝固する
際に溝2が核となつて単結晶化したものである。
従つて、シリコン層3にはSOSと同様に例えば
MOSトランジスタ等の素子を形成できる。第1
図bはシリコン層3の平担部3aにソースSおよ
びドレインD拡散を行なつてMOSトランジスタ
を形成したもので、4はゲート酸化膜、5はゲー
ト電極である。 Grooves are formed on the surface of a dielectric (insulating) substrate such as silicon dioxide (SiO 2 ) or quartz glass, a polycrystalline silicon or amorphous silicon layer is deposited on the surface of the substrate, and the layer is laser annealed to form the grooves. as the core
It is known that a single crystal with a quality equal to or better than the SOS (Silicon on Sapphire) structure can be grown. FIG. 1A shows an example of this, in which 1 is a dielectric substrate, 2 is a groove formed on its surface to a depth of about 1000 to 2000 Å, and 3 is a silicon layer about 5000 Å thick. The silicon layer 3 is made by growing polycrystalline silicon by, for example, chemical vapor deposition (CVD) and melting it by laser annealing, and when it solidifies, the groove 2 becomes a nucleus and becomes a single crystal. .
Therefore, the silicon layer 3 has, for example, similar to SOS.
Elements such as MOS transistors can be formed. 1st
In FIG. b, a MOS transistor is formed by performing source S and drain D diffusion in the flat part 3a of the silicon layer 3, where 4 is a gate oxide film and 5 is a gate electrode.
ところで、素子の形成領域が第1図cのように
例えば溝2の上部であると、この部分のシリコン
層3は下部に溝2があり、表面が凹部になつてい
て、平担部3aとは結晶性又はシリコン膜厚など
が異なり、素子は図示の如くなつて同図bに示さ
れる素子と同等の特性にならない。例えばSOS構
造の利点の1つはソース、ドレインの下部が絶縁
体であつて接合容量が無視できる程小であるとい
う点であり、第1図bに示される構造ではこれが
期待できるが、同図cに示される構造ではソース
領域Sの接合容量が無視できなくなる。勿論、溝
2は単結晶化の際の核としてであるが、かかる溝
2の存在によつて1チツプ内の多数の素子の特性
が不揃いになることは好ましくない。 By the way, if the formation region of the element is, for example, the upper part of the groove 2 as shown in FIG. The elements differ in crystallinity, silicon film thickness, etc., and the element becomes as shown in the figure and does not have the same characteristics as the element shown in Figure b. For example, one of the advantages of the SOS structure is that the lower portions of the source and drain are insulators, so the junction capacitance is negligibly small, and this can be expected in the structure shown in Figure 1b. In the structure shown in c, the junction capacitance of the source region S cannot be ignored. Of course, the groove 2 is used as a nucleus during single crystallization, but it is not preferable that the presence of the groove 2 causes the characteristics of many elements within one chip to become uneven.
本発明は上記した点に鑑みてなされたもので誘
電体基板表面に予めスクライブラインに沿つて溝
を設け、次いで該基板表面に非単結晶半導体層を
形成し、さらに該半導体層をレーザ、光線または
電子線等のエネルギビームによりアニールして単
結晶化し、しかる後該単結晶化された半導体層の
前記溝の上層部分を除く部分に所要とする半導体
素子を形成することを特徴とするが、以下図示の
実施例を参照しながらこれを詳細に説明する。 The present invention has been made in view of the above points, and involves forming grooves in advance on the surface of a dielectric substrate along scribe lines, then forming a non-single-crystal semiconductor layer on the surface of the substrate, and further layering the semiconductor layer with laser or light beams. Alternatively, the method is characterized in that it is annealed with an energy beam such as an electron beam to form a single crystal, and then a desired semiconductor element is formed in a portion of the single crystallized semiconductor layer excluding the upper layer portion of the groove, This will be explained in detail below with reference to the illustrated embodiments.
第2図は本発明の一実施例を示す要部平面図
で、1はスクライブライン6に沿つて多数のツプ
(少くとも1個の能動素子及び/又は受動素子を
含む素子個片)に分割される大径の誘電体基板で
ある。本発明ではこのスクライブライン6に沿つ
て誘電体基板1表面に縦横に溝2を設ける。素子
の形成方法は第1図a,bに示される従来方法と
同様であり、先ず溝2を設けた基板1上に多結晶
シリコン等の非単結晶半導体(レーザ加熱性は非
晶質シリコンの方が良好)層3をCVD法で厚さ
5000Å程度に成長させる。第3図は該非単結晶半
導体層3を形成した後の断面(第2図A―A断
面)を示す。次いでレーザアニールして該溝2を
核にして非単結晶半導体層を単結晶層に変換す
る。第2図の溝2を例えばダイヤモンドブレード
で形成すればその幅は10〜100μm程度となり、
また溝2相互間の間隔はチツプサイズによるがmm
オーダとなる。深さは第1図と同様に1000〜2000
Å、或いはスクライブ時の切断作業を容易にする
ため、基板1の厚みの半分程度とする。 FIG. 2 is a plan view of a main part showing an embodiment of the present invention, in which 1 shows a large number of chips (element pieces including at least one active element and/or passive element) along a scribe line 6. This is a large diameter dielectric substrate that is divided into parts. In the present invention, grooves 2 are provided vertically and horizontally on the surface of the dielectric substrate 1 along the scribe line 6. The method for forming the device is the same as the conventional method shown in FIGS. (better) layer 3 by CVD method
Grow to about 5000 Å. FIG. 3 shows a cross section (cross section AA in FIG. 2) after the non-single crystal semiconductor layer 3 is formed. Next, laser annealing is performed to convert the non-single crystal semiconductor layer into a single crystal layer using the grooves 2 as nuclei. If the groove 2 in Fig. 2 is formed with a diamond blade, for example, its width will be about 10 to 100 μm,
Also, the distance between grooves 2 depends on the chip size, but
It becomes an order. The depth is 1000 to 2000 as in Figure 1.
Å, or approximately half the thickness of the substrate 1 in order to facilitate the cutting operation during scribing.
基板1上に形成された非単結晶シリコン層に対
するレーザ照射には、1溝2で囲まれるチツプ領
域7全体をビーム径の大なるレーザスポツトで覆
うようにする方法、2小径のレーザビームで該領
域7を走査する方法等がある。いずれの場合でも
図中実線矢印で示すように、溝2から中央部へ向
けて単結晶化が進行し、例えば結晶面100の単
結晶が成長する。この後MOSトランジスタ等を
第1図b等と同様に形成するが、その領域はチツ
プ領域7(第1図の平担部3aに相当する)内に
限定し、少なくとも溝2の上部は使用しない。そ
して、素子形成後にスクライブライン6に沿つて
切断し、チツプ領域7単位の半導体素子チツプを
得る。尚、非単結晶シリコン層のアニールはレー
ザ光に限らず、アーク光等の強い光線を集束した
ものまたは電子線等でもよい。 For laser irradiation of the non-single crystal silicon layer formed on the substrate 1, there are two methods: (1) covering the entire chip region 7 surrounded by the groove 2 with a laser spot with a large beam diameter, and (2) using a laser beam with a small diameter. There are methods such as scanning the area 7. In either case, as shown by the solid arrow in the figure, single crystallization progresses from the groove 2 toward the center, and for example, a single crystal of crystal plane 100 grows. Thereafter, MOS transistors and the like are formed in the same manner as in FIG. 1b, etc., but the area is limited to the chip region 7 (corresponding to the flat part 3a in FIG. 1), and at least the upper part of the groove 2 is not used. . After the device is formed, it is cut along the scribe line 6 to obtain a semiconductor device chip having seven chip regions. Note that the annealing of the non-single-crystal silicon layer is not limited to laser light, and may be performed using focused strong light such as arc light, electron beam, or the like.
以上述べた本発明の半導体装置の製造方法によ
れば、単結晶の核となる溝をスクライブラインに
一致させることにより、素子形成用のチツプ領域
は平担で均一になるため、チツプ内の多数の素子
相互間の特性が均一化され、SOI構造を一層実用
的なものとし得る利点がある。 According to the method for manufacturing a semiconductor device of the present invention described above, by aligning the grooves that serve as the core of the single crystal with the scribe lines, the chip area for forming elements becomes flat and uniform, so that many This has the advantage that the characteristics between the elements can be made uniform, making the SOI structure more practical.
第1図は誘電体基板に溝を設けた半導体装置を
示す断面図、第2図及び第3図は本発明の一実施
例を示す平面図である。
図中、1は誘電体基板、2は溝、3はシリコン
層、6はスクライブライン、7はチツプ領域であ
る。
FIG. 1 is a sectional view showing a semiconductor device in which a groove is provided in a dielectric substrate, and FIGS. 2 and 3 are plan views showing an embodiment of the present invention. In the figure, 1 is a dielectric substrate, 2 is a groove, 3 is a silicon layer, 6 is a scribe line, and 7 is a chip region.
Claims (1)
つて溝を設け、次いで該基板表面に非単結晶半導
体層を形成し、さらに該半導体層をレーザ、光線
または電子線等のエネルギビームによりアニール
して単結晶化し、しかる後該単結晶化された半導
体層の前記溝の上層部分を除く部分に所要とする
半導体素子を形成することを特徴とする半導体装
置の製造方法。1. Grooves are previously formed on the surface of a dielectric substrate along scribe lines, then a non-single crystal semiconductor layer is formed on the surface of the substrate, and the semiconductor layer is further annealed with an energy beam such as a laser, a light beam, or an electron beam to form a single crystal. A method for manufacturing a semiconductor device, comprising: crystallizing the single crystallized semiconductor layer, and then forming a desired semiconductor element in a portion of the single crystallized semiconductor layer excluding the upper layer portion of the groove.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8160080A JPS577117A (en) | 1980-06-17 | 1980-06-17 | Manufacture of semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8160080A JPS577117A (en) | 1980-06-17 | 1980-06-17 | Manufacture of semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS577117A JPS577117A (en) | 1982-01-14 |
| JPS629212B2 true JPS629212B2 (en) | 1987-02-27 |
Family
ID=13750804
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8160080A Granted JPS577117A (en) | 1980-06-17 | 1980-06-17 | Manufacture of semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS577117A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100234894B1 (en) * | 1997-05-12 | 1999-12-15 | 구본준 | Crystallization method of amorphous silicon layer and manufacturing method of thin film transistor using same |
-
1980
- 1980-06-17 JP JP8160080A patent/JPS577117A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS577117A (en) | 1982-01-14 |
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