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JP2526494B2 - Insulation separation method - Google Patents
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JP2526494B2 - Insulation separation method - Google Patents

Insulation separation method

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Publication number
JP2526494B2
JP2526494B2 JP5174525A JP17452593A JP2526494B2 JP 2526494 B2 JP2526494 B2 JP 2526494B2 JP 5174525 A JP5174525 A JP 5174525A JP 17452593 A JP17452593 A JP 17452593A JP 2526494 B2 JP2526494 B2 JP 2526494B2
Authority
JP
Japan
Prior art keywords
substrate
ions
region
ion
insulating
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 - Lifetime
Application number
JP5174525A
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Japanese (ja)
Other versions
JPH0729973A (en
Inventor
寿夫 馬場
アンリ レゼク
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
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Filing date
Publication date
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Priority to JP5174525A priority Critical patent/JP2526494B2/en
Publication of JPH0729973A publication Critical patent/JPH0729973A/en
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Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は微細構造における絶縁分
離領域の作製に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the production of insulating isolation regions in fine structures.

【0002】[0002]

【従来の技術】半導体微細構造の絶縁分離技術は、高速
なトランジスタや量子効果を利用した新たなデバイスの
集積化を行う上で重要である。これまで一般的に用いら
れてきた微細構造の絶縁分離技術は、フォトレジストを
用いたパターン形成とエッチングによる伝導層の除去で
あった。この方法は多くの素子を一度に作る場合に適し
た方法であるが、多くの工程を経る必要があり、ナノメ
ートル程度の幅で絶縁分離をすることは容易ではない。
この方法に替わるものとして、集束した高エネルギーの
イオンを基板にぶつけて基板表面の原子を削るイオンミ
リングがある。この方法は転写工程が無く単純なため、
ナノメートル程度の幅で絶縁分離をすることが容易であ
る。この方法については例えば、メルンゲイリスにより
ジャーナル・オブ・バキューム・サイエンス・アンド・
テクノロジー(”Focusedion beam t
echnology and application
s”,John Melngailis,Journa
l of VacuumScience & Tech
nology B,Vol.5,No.2,pp.46
9−495,1987)に報告されている。
2. Description of the Related Art Insulation and isolation technology for semiconductor microstructures is important for the integration of high speed transistors and new devices utilizing the quantum effect. Conventionally used fine structure insulation isolation techniques have been patterning using photoresist and removal of the conductive layer by etching. This method is suitable for manufacturing many devices at one time, but it requires many steps, and it is not easy to perform insulation separation with a width of about nanometer.
As an alternative to this method, there is ion milling in which focused high-energy ions are bombarded on a substrate to scrape atoms on the substrate surface. Since this method has no transfer step and is simple,
It is easy to perform insulation separation with a width of about nanometer. This method is described, for example, by Melungeiris in the Journal of Vacuum Science and
Technology ("Focusedion beamt"
technology and application
s ", John Melngailis, Journa
l of VacuumScience & Tech
nology B, Vol. 5, No. 2, pp. 46
9-495, 1987).

【0003】図2は従来の集束イオンを用いたイオンミ
リングによる絶縁分離の工程図である。(A)はイオン
照射中、(B)はイオン照射後の基板を示しており、1
は絶縁性の結晶基板、2は伝導層、3は集束したイオ
ン、4はダメージ領域、5は絶縁分離領域である。
FIG. 2 is a process diagram of insulation separation by ion milling using conventional focused ions. (A) shows the substrate during ion irradiation and (B) shows the substrate after ion irradiation.
Is an insulating crystal substrate, 2 is a conductive layer, 3 is focused ions, 4 is a damaged region, and 5 is an insulating separation region.

【0004】この従来の微細構造の作製方法について、
基板1に半絶縁性のGaAs、伝導層にn−GaAs、
イオン3にAr+ を用いて説明する。高エネルギーのA
+基板に照射すると、Ar+ イオンはGaAs基板に
打ち込まれてダメージ領域4を形成するが、その衝撃に
よって基板表面のGaやAs原子が基板の外に飛び出
す。このため、イオン照射された基板表面には選択的に
溝が形成される。溝の深さが伝導層より深い場合には伝
導層が分断され、絶縁分離領域5となる。溝の領域はほ
ぼ照射するイオンの広がりで決められるため、微細な絶
縁分離領域の形成が容易である。
Regarding this conventional method for producing a fine structure,
Semi-insulating GaAs on the substrate 1, n-GaAs on the conductive layer,
An explanation will be given using Ar + for the ion 3. High energy A
When the r + substrate is irradiated, Ar + ions are implanted into the GaAs substrate to form the damaged region 4, but Ga and As atoms on the substrate surface jump out of the substrate due to the impact. Therefore, a groove is selectively formed on the surface of the substrate irradiated with ions. When the depth of the groove is deeper than the conductive layer, the conductive layer is divided to form the insulating isolation region 5. Since the region of the groove is almost determined by the spread of the ions to be irradiated, it is easy to form a fine insulating separation region.

【0005】[0005]

【発明が解決しようとする課題】この集束イオンを用い
たイオンミリングによる絶縁分離の方法では、微細な絶
縁分離領域の形成が容易に行えるが、形成した絶縁分離
領域(溝)の周辺にはダメージ領域4が残るため、そこ
に深い準位などが形成され伝導層の電気的不安定性を引
き起こす。絶縁分離領域を狭くし、微細な素子を高密度
に形成するためにはこのようなダメージ領域の除去が望
まれる。イオン照射後の熱処理により、ある程度のダメ
ージは回復するが、基板中に注入されるイオンの量が多
いために、ダメージの除去は容易ではない。
In this method of insulation isolation by ion milling using focused ions, fine insulation isolation regions can be easily formed, but the periphery of the formed insulation isolation regions (grooves) is damaged. Since the region 4 remains, a deep level or the like is formed there, causing electrical instability of the conductive layer. In order to narrow the insulating isolation region and form fine elements with high density, it is desired to remove such a damaged region. The heat treatment after the ion irradiation recovers some damage, but it is not easy to remove the damage because the amount of ions implanted into the substrate is large.

【0006】本発明の目的は、電気的な不安定性を引き
起こす基板ダメージが少なく、微細な絶縁分離領域の形
成を簡単に行なう方法を提供することにある。
An object of the present invention is to provide a method for easily forming a fine insulating isolation region with less substrate damage that causes electrical instability.

【0007】[0007]

【課題を解決するための手段】本発明の絶縁分離の方法
は、絶縁性の基板上の薄い半導体層の一部に、少なくと
も結晶構成原子間の結合を切断しかつスパッタリングを
生じない量の加速したイオンを選択的に打ち込み、その
後加熱処理を施してイオン打ち込み領域に選択的な溝の
形成を行い、半導体を層を分断することを特徴としてい
る。
SUMMARY OF THE INVENTION The method of dielectric isolation of the present invention is directed to a portion of a thin semiconductor layer on an insulative substrate that is capable of severing at least the bonds between crystalline constituent atoms and accelerating an amount that does not cause sputtering. It is characterized in that the ion is selectively implanted, and then heat treatment is performed to form a selective groove in the ion-implanted region to divide the semiconductor into layers.

【0008】この方法によれば、基板ダメージが少な
く、容易に微細な絶縁分離領域の形成ができる。
According to this method, the substrate is less damaged and the fine insulating isolation region can be easily formed.

【0009】[0009]

【実施例1】以下、本発明について実施例を示す図面を
参照して詳細に説明する。図1は本発明の実施例を示す
工程図である。図1において、図2と同じ記号は図2と
同等物で同一機能を果たすものである。また、(a)は
イオン注入中、(b)はイオン注入後、(c)は熱処理
後の工程である。
Embodiment 1 The present invention will be described in detail below with reference to the drawings showing an embodiment. FIG. 1 is a process drawing showing an embodiment of the present invention. 1, the same symbols as those in FIG. 2 are equivalent to those in FIG. 2 and have the same functions. Further, (a) is a step during ion implantation, (b) is a step after ion implantation, and (c) is a step after heat treatment.

【0010】この本発明の結晶基板の加工方法につい
て、基板1に半絶縁性のGaAs、伝導層2にn−Ga
As、イオン3にSi+ を例に説明する。まず、n−G
aAs伝導層2が形成されている半絶縁性GaAs基板
1に集束したSi+ イオン3を打ち込む。基板に打ち込
まれたイオンは基板内部で結晶原子との衝突によってエ
ネルギーを失い停止する。この過程で結晶を構成してい
た原子の結合が切れるため、イオンが打ち込まれたダメ
ージ領域4では基板は非晶質化する(図1(b))。非
晶質化した領域は原子同士の結合が切れているので、結
晶領域よりも体積が膨張する。このため、図1(b)の
ようにダメージ領域4の上には隆起した領域が形成され
る。もちろん一部の基板表面原子は外へ飛び出すが、本
発明の方法では注入するイオンの質量やエネルギーが大
きいため基板深く入り込むことと、注入するイオンの量
がイオンミリングに比べ非常に小さいため、外へ飛び出
す原子はほとんど無視できる。この工程では最適なイオ
ン注入量を設定する必要がある。打ち込むイオンの量が
通常の不純物ドーピングのように少ない場合には、充分
に結晶の結合を切断することができないため、非晶質化
させることができない。また、イオンミリングに使用す
る程度にイオンの量が多すぎる場合には、従来例の方法
となり表面はスパッタリングにより削り取られ、最終的
に多くのダメージ領域を残す。このように、本発明のイ
オン注入の工程では、注入イオンの量をこれらの中間に
なるように注意深く設定しておく必要がある。
Regarding the method of processing a crystal substrate of the present invention, the substrate 1 is semi-insulating GaAs, and the conductive layer 2 is n-Ga.
A description will be given by taking Si + as an As and ion 3. First, n-G
The focused Si + ions 3 are implanted into the semi-insulating GaAs substrate 1 on which the aAs conductive layer 2 is formed. The ions that have been implanted into the substrate lose their energy due to collision with crystal atoms inside the substrate and stop. In this process, the bonds of the atoms forming the crystal are broken, so that the substrate becomes amorphous in the damaged region 4 in which the ions are implanted (FIG. 1B). Since the atoms in the amorphized region are broken, the volume thereof expands more than that of the crystalline region. Therefore, as shown in FIG. 1B, a raised area is formed on the damaged area 4. Of course, some of the substrate surface atoms jump out, but in the method of the present invention, the mass and energy of the ions to be implanted are large enough to penetrate deeply into the substrate, and the amount of ions to be implanted is much smaller than that of ion milling. The atoms that jump out to can be almost ignored. In this step, it is necessary to set the optimum ion implantation amount. If the amount of ions to be implanted is small as in the case of usual impurity doping, the crystal bonds cannot be sufficiently broken, so that it cannot be made amorphous. Further, when the amount of ions is too large to be used for ion milling, the method of the conventional example is used, and the surface is scraped off by sputtering, and many damage areas are left in the end. As described above, in the ion implantation step of the present invention, it is necessary to carefully set the amount of implanted ions to be in the middle thereof.

【0011】つぎに、非晶質化したダメージ領域4の結
晶性が回復するような温度での熱処理を加えると、非晶
質化した部分は再び結晶化を始め、隆起した領域は減少
して行く。また、結合が切れた原子は動き易く反応性が
高いため、ダメージ領域の原子はその周辺に移動した
り、蒸発したり、熱処理雰囲気中に取り込まれたりす
る。
Next, when a heat treatment is performed at a temperature at which the crystallinity of the amorphized damaged region 4 is restored, the amorphized portion starts to crystallize again and the raised region decreases. go. Further, since the atom whose bond has been broken is easy to move and has high reactivity, the atom in the damaged region moves to its periphery, is evaporated, or is taken into the heat treatment atmosphere.

【0012】その結果、ダメージ領域の原子は減少し、
そこに絶縁性基板まで達する溝(絶縁領域5)が形成さ
れるようになる(図1(c))。この熱処理により非晶
質化した領域はほとんど消え、さらには結晶欠陥の入っ
たダメージ領域もアニールされて結晶性の改善がなされ
る。したがって、絶縁領域5の下や周辺にもダメージ領
域はなくなり、電気的不安定性を引き起こすことはな
い。
As a result, the number of atoms in the damaged area decreases,
A groove (insulating region 5) reaching the insulating substrate is formed therein (FIG. 1C). By this heat treatment, most of the amorphized region disappears, and the damaged region containing crystal defects is also annealed to improve the crystallinity. Therefore, there is no damaged region under or around the insulating region 5 and no electrical instability occurs.

【0013】厚さ20nmのn−GaAs層を形成した
半絶縁性GaAs基板に直径100nmのSi+ 集束イ
オンビームを加速電圧260keV、線密度101 0
-1 でライン状に注入したところ、注入した領域の表
面が20nm隆起した。引き続いて、この基板をアルシ
ンガスを流しながら650℃において15分間熱処理し
たところ、幅200nmで深さ25nmのくさび型の溝
が形成され、n−GaAs層の絶縁分離を行うことがで
きた。
[0013] The semi-insulating GaAs substrate to 100nm diameter forming the n-GaAs layer having a thickness of 20 nm Si + focused ion beam acceleration voltage 260 keV, linear density 10 1 0 c
When injected linearly at m −1 , the surface of the injected region was raised by 20 nm. Subsequently, when this substrate was heat-treated at 650 ° C. for 15 minutes while flowing arsine gas, a wedge-shaped groove having a width of 200 nm and a depth of 25 nm was formed, and the n-GaAs layer could be isolated.

【0014】またSi+ イオンの替わりにAu+ イオン
を用いた場合にも程度の差はあるが、同様のことが生じ
た。厚さ15nmのn−GaAs層を形成した半絶縁性
GaAs基板に直径100nmのAu+ 集束イオンビー
ムを加速電圧260keV、線密度3×101 9 xcm
- 1 でライン状に注入したところ、注入した領域の表面
が3nm隆起した。引き続いて、この基板をアルシンガ
スを流しながら650℃において15分間熱処理したと
ころ、幅200nmで深さ20nmのくさび型の溝が形
成れ、n−GaAs層の絶縁分離ができた。
Also, when Au + ions were used instead of Si + ions, the same thing occurred, although there were some differences. An Au + focused ion beam having a diameter of 100 nm was applied to a semi-insulating GaAs substrate having a 15 nm thick n-GaAs layer formed thereon at an acceleration voltage of 260 keV and a linear density of 3 × 10 19 xcm.
When the line was injected at -1 , the surface of the injected region was raised by 3 nm. Subsequently, when this substrate was heat-treated at 650 ° C. for 15 minutes while flowing arsine gas, a wedge-shaped groove having a width of 200 nm and a depth of 20 nm was formed, and the n-GaAs layer was isolated.

【0015】このような深さの溝を従来のイオンミリン
グの方法で作製するには、本発明で用いたイオンの注入
量よりも106 倍も多くのイオンが必要であり、長い注
入時間と基板表面に多くのダメージが残ることになる。
In order to form a groove having such a depth by the conventional ion milling method, 10 6 times as many ions as the ion implantation amount used in the present invention are required, which requires a long implantation time. A lot of damage will remain on the substrate surface.

【0016】以上の本発明の実施例では25nm程度の
深さの絶縁分離領域の形成しか示さなかったが、注入イ
オンの質量、加速エネルギー、分布を選ぶことにより、
溝の深さや形状を調節することができる。また、熱処理
温度や時間を調節することによっても溝の深さや形状を
調節ることができる。
In the above-mentioned embodiments of the present invention, only the formation of the insulating isolation region having a depth of about 25 nm has been shown. However, by selecting the mass, acceleration energy and distribution of implanted ions,
The depth and shape of the groove can be adjusted. The depth and shape of the groove can also be adjusted by adjusting the heat treatment temperature and time.

【0017】基板としては単結晶のGaAsしか示さな
かったが、Si,Ge,InP,GaSbなどその他の
半導体単結晶基板や多結晶基板にも本発明が適用できる
ことは明かである。また絶縁体の単結晶基板や多結晶基
板にも適用できることも明かである。またSOI(Se
miconductor on Insulator)
のように結晶性でない基板や膜の上に、単結晶あるいは
それに近い半導体膜を形成したときの絶縁分離にも本発
明は適用できる。なお、前述の実施例では半絶縁性Ga
As基板上にn−GaAs層を形成したあと、このn−
GaAs層を分断したが、n−GaAsでなくi−Ga
As層を形成し、これを分断したあとイオン注入等でn
型不純物をドープしてもよい。
Although only single crystal GaAs is shown as the substrate, it is obvious that the present invention can be applied to other semiconductor single crystal substrates such as Si, Ge, InP, GaSb and polycrystalline substrates. It is also clear that it can be applied to an insulating single crystal substrate or a polycrystalline substrate. In addition, SOI (Se
microphone on insulator)
The present invention can also be applied to insulation separation when a single crystal or a semiconductor film similar thereto is formed on a substrate or film which is not crystalline as described above. In the above-mentioned embodiment, the semi-insulating Ga is used.
After forming an n-GaAs layer on the As substrate, this n-
The GaAs layer was divided, but i-Ga instead of n-GaAs
After forming the As layer and dividing it, n is formed by ion implantation or the like.
A type impurity may be doped.

【0018】注入するイオンとしてはSi+ とAu+
か示さなかったが、Ga+ ,As+,Sb+ などその他
のイオンでもよいことも明かである。
Although only Si + and Au + are shown as the ions to be implanted, it is also clear that other ions such as Ga + , As + , Sb + may be used.

【0019】また、熱処理の雰囲気としてはアルシンガ
スしか示さなかったが、その他のガスでもよく、加圧や
減圧さらには真空中でもよいことも明かである。
Further, although only arsine gas was shown as the atmosphere for the heat treatment, it is also clear that other gas may be used, and pressurization, depressurization, and vacuum may be performed.

【0020】本発明では微細構造作製工程を容易にする
ために集束したイオンビームを用いることが望ましい
が、広い領域を一度に加工する場合には、広がったイオ
ンビームを用い、基板表面に配置したマスクを通して選
択的にイオンを注入してもよいことも明かである。
In the present invention, it is desirable to use a focused ion beam for facilitating the fine structure manufacturing process. However, when processing a large area at a time, a spread ion beam is used and placed on the substrate surface. It is also apparent that the ions may be selectively implanted through the mask.

【0021】[0021]

【発明の効果】本発明の絶縁分離の方法により微細な絶
縁分離領域の形成ができ、微細な半導体素子を高密度に
作り込むことが可能になる。
According to the method of insulation separation of the present invention, fine insulation separation regions can be formed, and fine semiconductor elements can be formed at high density.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例を示す工程図である。(a)は
イオン注入中、(b)はイオン注入後、(c)は熱処理
後を示している。
FIG. 1 is a process drawing showing an example of the present invention. (A) shows during ion implantation, (b) shows after ion implantation, and (c) shows after heat treatment.

【図2】従来のイオンミリングによる絶縁分離の工程図
である。(A)はイオン照射中、(B)はイオン照射後
を示している。
FIG. 2 is a process drawing of insulation separation by conventional ion milling. (A) shows during ion irradiation and (B) shows after ion irradiation.

【符号の説明】[Explanation of symbols]

1 絶縁性結晶基板 2 伝導層 3 イオン 4 基板ダメージ領域 5 絶縁分離領域 1 Insulating Crystal Substrate 2 Conductive Layer 3 Ion 4 Substrate Damage Area 5 Insulation Separation Area

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 H01L 21/265 Q ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification code Office reference number FI technical display location H01L 21/265 Q

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 絶縁性の基板上の薄い半導体層の一部
に、結晶構成原子間の結合を切断しかつスパッタリング
を生じない量の加速したイオンを選択的に打ち込み、そ
の後加熱処理を施してイオン打ち込み領域に選択的な溝
の形成を行い、前記半導体層を分断して絶縁分離を行う
方法。
1. A part of a thin semiconductor layer on an insulating substrate is selectively implanted with accelerated ions in an amount that does not cause a bond between crystal constituent atoms and does not cause sputtering, and is then subjected to heat treatment. A method in which a groove is selectively formed in an ion-implanted region and the semiconductor layer is divided to perform insulation separation.
JP5174525A 1993-07-14 1993-07-14 Insulation separation method Expired - Lifetime JP2526494B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5174525A JP2526494B2 (en) 1993-07-14 1993-07-14 Insulation separation method

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