JPS6070721A - Laterally epitaxial growth - Google Patents
Laterally epitaxial growthInfo
- Publication number
- JPS6070721A JPS6070721A JP58176902A JP17690283A JPS6070721A JP S6070721 A JPS6070721 A JP S6070721A JP 58176902 A JP58176902 A JP 58176902A JP 17690283 A JP17690283 A JP 17690283A JP S6070721 A JPS6070721 A JP S6070721A
- Authority
- JP
- Japan
- Prior art keywords
- sio2
- regions
- single crystal
- region
- silicon layer
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H01L21/02675—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth using laser beams
- H01L21/02683—Continuous wave laser beam
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02367—Substrates
- H01L21/0237—Materials
- H01L21/02373—Group 14 semiconducting materials
- H01L21/02381—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02439—Materials
- H01L21/02488—Insulating materials
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02494—Structure
- H01L21/02496—Layer structure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02521—Materials
- H01L21/02524—Group 14 semiconducting materials
- H01L21/02532—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02587—Structure
- H01L21/0259—Microstructure
- H01L21/02598—Microstructure monocrystalline
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02656—Special treatments
- H01L21/02664—Aftertreatments
- H01L21/02667—Crystallisation or recrystallisation of non-monocrystalline semiconductor materials, e.g. regrowth
- H01L21/02691—Scanning of a beam
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Microelectronics & Electronic Packaging (AREA)
- General Physics & Mathematics (AREA)
- Manufacturing & Machinery (AREA)
- Computer Hardware Design (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Power Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Optics & Photonics (AREA)
- Materials Engineering (AREA)
- Recrystallisation Techniques (AREA)
Abstract
Description
【発明の詳細な説明】
発明の技術分野
本発明はラテラルエピタキシャル成長方法に係り、特に
ビームアニールによるラテラルエピタキシャル成長方法
に関するものである。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to a lateral epitaxial growth method, and more particularly to a lateral epitaxial growth method using beam annealing.
技術の背景
単結晶基板上に堆積させた非単結晶層1例えば多結晶シ
リコン層にレーザービーム、電子ビーム。Background of the Technology A non-single-crystalline layer 1, for example a polycrystalline silicon layer, deposited on a single-crystalline substrate is treated with a laser beam or an electron beam.
イオンビーム等のエネルギビームQl照射することによ
って横方向にエピタキシャル成長(ラテラルエピタキシ
ャル成長、以下単にLEGと記す)全行ない該多結晶シ
リコン全基板単結晶と同一結晶方位のシリコンに単結晶
化せしめる方法が知られている。特に数ミリ角以上の大
面積のシリコン層を完全に単結晶化することは結晶粒界
や結晶転移の発生のために容易ではない。There is a known method of performing lateral epitaxial growth (hereinafter simply referred to as LEG) by irradiating the polycrystalline silicon with an energy beam Ql such as an ion beam to form a single crystal of silicon having the same crystal orientation as the single crystal of the entire polycrystalline silicon substrate. ing. In particular, it is not easy to completely monocrystallize a silicon layer with a large area of several millimeters square or more because of the occurrence of crystal grain boundaries and crystal dislocations.
従来技術と問題点
上記のように大きな面積部分のシリコン層全単結晶化す
ることが出来ないため、従来Device領域等の孤立
した各々数十ミクロン角〜数百ミクロン角程度の小面積
のみQ Sol領域(5iliconOn In5ul
ator )として、その周囲の単結晶シリコン層を単
結晶化の種結晶にすることが行なわれている。第1図に
は単結晶シリコン層1上にデバイス領域となる3つの5
i02領域2が示されている。第2図には第1図のA−
A断面図が示されている。Prior Art and Problems As mentioned above, it is not possible to completely single-crystallize a silicon layer in a large area, so conventionally Q Sol is applied only to isolated small areas such as device regions, each several tens of microns square to several hundred microns square. Area (5iliconOn In5ul
Ator), the surrounding single crystal silicon layer is used as a seed crystal for single crystallization. Figure 1 shows three 5
i02 area 2 is shown. Figure 2 shows A- in Figure 1.
A sectional view is shown.
嬉1.第2図に示されているような配置においてレーザ
ーアニール(スキャニング方向をBとする)によって5
i02領域2上に形成した多結晶シリコン層3を単結晶
化する場合(第2図中1°aは多結晶シリコン層3を単
結晶化するための種結晶部)、該レーザーアニールによ
り充分に単結晶シリコン基板1が加熱溶融されると第3
図に示すように溶融シリコンの融液の中で5in2領域
2が元の位置2aから多くの場合スキャニング方向のあ
る位置2bに漂流し、予定した位置にSol領域全形成
することが出来ないことがしばしば発生した。Happy 1. 5 by laser annealing (scanning direction B) in the arrangement shown in Figure 2.
When the polycrystalline silicon layer 3 formed on the i02 region 2 is to be made into a single crystal (1°a in FIG. 2 is a seed crystal portion for making the polycrystalline silicon layer 3 into a single crystal), the laser annealing is sufficient. When the single crystal silicon substrate 1 is heated and melted, the third
As shown in the figure, in many cases, the 5in2 region 2 drifts from the original position 2a to a certain position 2b in the scanning direction in the molten silicon, making it impossible to form the entire Sol region at the planned position. occurred often.
発明の目的
上記欠点を鑑み本発明は予定された位置にSol領域を
形成することが可能なラテラルエピタキシャル成長方法
全提供することである。OBJECTS OF THE INVENTION In view of the above-mentioned drawbacks, the present invention provides a complete lateral epitaxial growth method capable of forming Sol regions at predetermined locations.
発明の構成
本発明は半導体基板上に複数の絶縁領域全形成し5該絶
縁層上を含む部分に非単結晶層を形成し。Structure of the Invention In the present invention, a plurality of insulating regions are all formed on a semiconductor substrate, and a non-single crystal layer is formed in a portion including the top of the insulating layer.
次に該非単結晶層にエネルギーブームを照射して該非単
結晶層全単結晶化せしめるラテラルエビタ −キシャル
成長方法において前記複数の絶縁領域の各々が他の絶縁
領域に対して相互に連結手段を有するように前記複数の
絶縁領域を形成することを特徴とするラテラルエピタキ
シャル成長方法によって達成される、
本発明において上記の連結手段は少なくとも半導体基板
の融点において、溶融せず且つ変形しない物質例えばS
i02 、 S i 3N4等から作られるのが好ま
しい。Next, in the lateral epitaxy growth method in which the non-single crystal layer is irradiated with an energy boom to make all of the non-single crystal layer single crystal, each of the plurality of insulating regions has means for interconnecting with other insulating regions. In the present invention, the connecting means is made of a material that does not melt or deform at least at the melting point of the semiconductor substrate, such as S.
Preferably, it is made from i02, S i 3N4, etc.
発明の実施例 以下本発明の実施例全図面に基づいて説明する。Examples of the invention Embodiments of the present invention will be described below based on all the drawings.
第4図は本発明の1実施例會示す概略平面図である。FIG. 4 is a schematic plan view showing one embodiment of the present invention.
第4図に示すように例えば単結晶シリコン基板11上に
3つの矩形状のSi0g領域(島)12及びその3つの
8i02領域12t一連結する例えば8 i 02から
なる連結橋14がバターニングによって同時に形成され
ている。この3つ連結橋14の幅は5i02領域12の
各辺の長さの約4゜の長さであるのが好ましい。という
のは5i02領域周辺の該基板11が単結晶化の種とな
るために、該連結橋がシリコンの融点温度で変形しない
程度に出来るぞけ、連結橋の幅全細くすべきだからであ
る。As shown in FIG. 4, for example, three rectangular Si0g regions (islands) 12 and their three 8i02 regions 12t are connected together on a connecting bridge 14 consisting of, for example, 8i02, on a single crystal silicon substrate 11, simultaneously by patterning. It is formed. Preferably, the width of the three-piece connecting bridge 14 is approximately 4° the length of each side of the 5i02 region 12. This is because the substrate 11 around the 5i02 region serves as a seed for single crystallization, so the width of the connecting bridge should be made narrow in its entirety so that it can be formed to such an extent that it does not deform at the melting point temperature of silicon.
このようにして5i02からなる連結橋14を有した5
in2領域12上方にOVD法によって多結晶シリコン
層(図示せず)を形成し、5in2領域周辺から従来通
り連続発振アルゴンレーザ全円いてアニールを行ない多
結晶シリコン層をラテラルエピタキシャル成長させ単結
晶化せしめた。該レーザアニールによって単結晶シリコ
ン基板11が溶融して被アニール多結晶シリコン層下の
5iOz領域12が浮遊状態になったとしても照射され
ていない他の2つのSi0g領域に連結された連結橋に
よって動き全抑制さn S i 02領域の漂流全防止
□することが可能となる。この実施例ではS i 0
2領域は同形の矩形で短辺8oμm、長辺1’00μm
の長さを有するように形成したので連結橋の幅を2μ
m〜5μInの長さに形成した。In this way, the 5
A polycrystalline silicon layer (not shown) was formed above the 5in2 region 12 by the OVD method, and annealing was performed using a continuous wave argon laser in the entire circle from around the 5in2 region in the conventional manner to cause lateral epitaxial growth of the polycrystalline silicon layer to form a single crystal. . Even if the single crystal silicon substrate 11 is melted by the laser annealing and the 5iOz region 12 under the annealed polycrystalline silicon layer becomes a floating state, it will move due to the connecting bridge connected to the other two Si0g regions that are not irradiated. It becomes possible to completely prevent drifting in the n S i 02 area. In this example, S i 0
The two areas are identical rectangles with short sides of 8oμm and long sides of 1'00μm.
Since it was formed to have a length of , the width of the connecting bridge was 2μ
It was formed to have a length of m to 5 μIn.
本発明の実施例においてアルゴンレーザビームを用いて
アニールを行なったが電子ビーム、イオンビーム、ラン
プ(放電、タングステンランプ)等の種々のエネルギー
ビームを用いても同様に行なうことが出来る。Although an argon laser beam was used for annealing in the embodiments of the present invention, the annealing can be similarly performed using various energy beams such as an electron beam, ion beam, lamp (discharge, tungsten lamp), etc.
発明の詳細
な説明したように本発明によれば予定された位置に80
I領域を形成することが出来る。According to the present invention, as described in detail, 80
An I region can be formed.
第1図から第3図迄は従来技術を説明するための図であ
り、第4図は本発明の1実施例を説明するための概略平
面図である。
1.11・・・単結晶シリコン基板。
2.12・・・8i02領域(島)。
3・・・多結晶シリコン層。
14・・・連結橋(”5i02)。
第1図
第2図
第3図
第4図1 to 3 are diagrams for explaining the prior art, and FIG. 4 is a schematic plan view for explaining one embodiment of the present invention. 1.11...Single crystal silicon substrate. 2.12...8i02 area (island). 3... Polycrystalline silicon layer. 14... Connecting bridge ("5i02). Figure 1 Figure 2 Figure 3 Figure 4
Claims (1)
単結晶層にエネルギービームを照射して該非単結晶化せ
しめるラテラルエピタキシャル成長方法において。 前記複数の絶縁領域の各々が他の絶縁領域に対して相互
に連結手段全有するように前記複数の絶縁領域を形成す
ることを特徴とするラテラルエピタキシャル成長方法。 2、前記連結手段に少なくとも前記半導体基板の融点に
おいて溶融せず且つ変形しない物質からなることを特徴
とする特許請求の範囲第1項記載のラテラルエピタキシ
ャル成長方法。[Claims] 1. A plurality of insulating regions are formed on a semiconductor substrate. In a lateral epitaxial growth method, a non-single crystal layer is formed in a portion including the top of the insulating layer, and the non-single crystal layer is first irradiated with an energy beam to make the non-single crystal layer. A method of lateral epitaxial growth, characterized in that the plurality of insulating regions are formed such that each of the plurality of insulating regions has interconnection means to other insulating regions. 2. The lateral epitaxial growth method according to claim 1, wherein the connecting means is made of a material that does not melt or deform at least at the melting point of the semiconductor substrate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58176902A JPS6070721A (en) | 1983-09-27 | 1983-09-27 | Laterally epitaxial growth |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58176902A JPS6070721A (en) | 1983-09-27 | 1983-09-27 | Laterally epitaxial growth |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6070721A true JPS6070721A (en) | 1985-04-22 |
JPH0377654B2 JPH0377654B2 (en) | 1991-12-11 |
Family
ID=16021749
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58176902A Granted JPS6070721A (en) | 1983-09-27 | 1983-09-27 | Laterally epitaxial growth |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6070721A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0303320A2 (en) * | 1987-08-11 | 1989-02-15 | Koninklijke Philips Electronics N.V. | A method of forming thin, defect-free, monocrystalline layers of semiconductor materials on insulators |
-
1983
- 1983-09-27 JP JP58176902A patent/JPS6070721A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0303320A2 (en) * | 1987-08-11 | 1989-02-15 | Koninklijke Philips Electronics N.V. | A method of forming thin, defect-free, monocrystalline layers of semiconductor materials on insulators |
Also Published As
Publication number | Publication date |
---|---|
JPH0377654B2 (en) | 1991-12-11 |
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