JPH057824B2 - - Google Patents
Info
- Publication number
- JPH057824B2 JPH057824B2 JP56215709A JP21570981A JPH057824B2 JP H057824 B2 JPH057824 B2 JP H057824B2 JP 56215709 A JP56215709 A JP 56215709A JP 21570981 A JP21570981 A JP 21570981A JP H057824 B2 JPH057824 B2 JP H057824B2
- Authority
- JP
- Japan
- Prior art keywords
- electron beam
- laser
- irradiated
- irradiated object
- irradiation
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/30—Electron-beam or ion-beam tubes for localised treatment of objects
- H01J37/317—Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation
Landscapes
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Recrystallisation Techniques (AREA)
Description
【発明の詳細な説明】
(a) 発明の技術分野
本発明は複合ビーム照射装置にかゝり、複数の
異なるビームを同時に同一点を照射させることが
できるビーム照射装置の基本構造に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field of the Invention The present invention relates to a composite beam irradiation device, and more particularly, to the basic structure of a beam irradiation device that can simultaneously irradiate the same point with a plurality of different beams.
(b) 技術の背景
半導体装置を製造する際に、不純物イオンを注
入した後、注入イオンを活性化するための加熱処
理(アニール)がなされるが、加熱処理炉を用い
て、半導体基板全体を加熱することは、所望のイ
オン注入領域のみならず他部分をも加熱して、か
えつて半導体特性を劣化する悪影響があるため、
最近は所望領域のみを局部的に加熱する方法が研
究されており、それにはレーザ光を照射するいわ
ゆるレーザアニール法が注目されている。(b) Background of the technology When manufacturing semiconductor devices, after impurity ions are implanted, heat treatment (annealing) is performed to activate the implanted ions. Heating not only heats the desired ion-implanted region but also other parts, which has the adverse effect of deteriorating semiconductor characteristics.
Recently, methods of locally heating only desired regions have been studied, and a so-called laser annealing method in which laser light is irradiated has been attracting attention.
また、レーザアニールによつて多結晶を単結晶
化する結晶成長法も研究されており、その場合は
局部加熱によつて欠陥の少ない結晶成長が行なわ
れることに着目したものである。 A crystal growth method in which polycrystals are made into single crystals by laser annealing has also been studied, and in this case, attention has been paid to the fact that crystal growth with fewer defects can be achieved by localized heating.
しかしながら、このような局部的加熱法はでき
るだけエネルギーを大きくして、できるだけ短時
間に処理する方式が無欠陥結晶成長や素子特性向
上の点から好ましく、それは不要部分への熱伝達
が少なくなるためである。 However, in such localized heating methods, it is preferable to increase the energy as much as possible and process the process in as short a time as possible from the viewpoint of defect-free crystal growth and improvement of device characteristics, since heat transfer to unnecessary parts is reduced. be.
(c) 発明の目的
本発明は上記の趣旨から強いエネルギーを瞬時
に加えることのできる照射精度の高いビーム照射
装置を提案する。(c) Purpose of the Invention Based on the above-mentioned purpose, the present invention proposes a beam irradiation device with high irradiation accuracy that can instantaneously apply strong energy.
(d) 発明の構成
かような目的は、被照射体に電子ビームを照射
して該被照射体を予備加熱する電子銃、該電子ビ
ームを制御するための電子ビーム制御系、および
これらを納めたコラム外より集束されたレーザ光
を透過窓を通して該被照射体に該電子ビームと共
に照射するレーザ照射手段を有し、上記電子ビー
ムと該レーザ光を該被照射体の同一位置に同時に
照射することにより、該被照射体を熱処理する機
能をもたせた複合ビーム照射装置によつて達成さ
れる。(d) Structure of the invention The object is to provide an electron gun for preheating an irradiated object by irradiating the object with an electron beam, an electron beam control system for controlling the electron beam, and an electron beam control system containing these. a laser irradiation means for irradiating the irradiated object together with the electron beam through a transmission window with a laser beam focused from outside the column, and irradiates the same position of the irradiated object with the electron beam and the laser light at the same time. This can be achieved by using a composite beam irradiation device that has a function of heat-treating the object to be irradiated.
以下図面を参照して本発明を詳細に説明する。 The present invention will be described in detail below with reference to the drawings.
(e) 発明の実施例
第1図は本発明にかゝる複合ビーム照射装置の
一実施例の断面構造図である。図において、被照
射体の半導体ウエハー1はX方向とY方向とに可
動するステージ2上に載せて、ステージ2は駆動
系3により外部から動かされる。真空系4によつ
て吸引されてコラム5の内部は高真空になつてお
り、ステージ2の垂直上に電子銃6とそれより発
射された電子ビーム7を制御する電磁レンズ、ス
リツトなどからなる制御系8とがあり、これらは
公知の露光装置に類似している。(e) Embodiment of the Invention FIG. 1 is a cross-sectional structural diagram of an embodiment of a composite beam irradiation device according to the present invention. In the figure, a semiconductor wafer 1 as an object to be irradiated is placed on a stage 2 movable in the X direction and the Y direction, and the stage 2 is moved from the outside by a drive system 3. The interior of the column 5 is drawn into a high vacuum by the vacuum system 4, and a control device consisting of an electron gun 6 and an electromagnetic lens, slit, etc. that controls the electron beam 7 emitted from the electron gun 6 is placed vertically above the stage 2. system 8, which are similar to known exposure devices.
真空コラム5の側面部にレーザ光源9からのレ
ーザ光10を入射させるレーザ導入ポート11が
凹部状に設けられ、又他のコラム側部には光学顕
微鏡で照射位置を目視できる顕微鏡導入ポート1
2が同じく凹部状に設けられる。このようにレー
ザ光10を側面より傾斜させて照射するのは、電
子ビーム7を傾向させることが装置面で困難なた
めである。 A laser introduction port 11 is provided in a concave shape on the side of the vacuum column 5 to allow the laser beam 10 from the laser light source 9 to enter therein, and a microscope introduction port 1 is provided on the other side of the column so that the irradiation position can be visually observed with an optical microscope.
2 is similarly provided in the shape of a recess. The reason why the laser beam 10 is irradiated at an angle from the side surface is that it is difficult to direct the electron beam 7 in terms of equipment.
第2図は電子ビームとレーザ光との混合照射部
分を拡大した部分断面図で、レーザ導入ポート1
1をも併せて示す。レーザ導入ポートでは、レー
ザ光10は反射ミラー13で照射方向を変化させ
て、石英窓14を通つて対物レンズ15で集束
し、絞られたレーザ光が保護ガラス16を透過し
て、真空コラム5内に入り、電子ビーム7と同一
位置を同時に照射する。 Figure 2 is an enlarged partial cross-sectional view of the mixed irradiation area of the electron beam and laser light, showing the laser introduction port 1.
1 is also shown. At the laser introduction port, the laser beam 10 changes its irradiation direction with a reflection mirror 13, passes through a quartz window 14, and is focused by an objective lens 15. The narrowed laser beam passes through a protective glass 16 and enters a vacuum column 5. The electron beam enters the interior and irradiates the same position as the electron beam 7 at the same time.
このように反射ミラー13、対物レンズ15を
真空コラム5外におく目的は、これらは絶縁体で
あるから真空コラム内ではチヤージアツプして、
ビーム特に電子ビームに影響を与え、照射位置に
狂いが生ずるのを防止するためである。対物レン
ズ15の焦点距離fは50〜70mmが妥当であり、そ
れより短かいと半導体ウエハー1からの蒸発物の
付着が多くなつて、処理中に照度を一定に保て
ず、又それより長いとレーザ光の絞りが難かしく
なる。しかし、この蒸発物の付着は対物レンズ前
面の保護ガラス16であつて、そのため絶えず保
護ガラスは交換を必要とする。又、保護ガラスは
真空中にあるからチヤージアツプを防止するよう
に、表面にレーザ光を透過するメタル薄膜をスパ
ツタしておく方が望ましい。また石英窓14は対
物レンジ15の保護用で、充分に密封されてお
り、万一保護ガラス16の交換で、封止が不充分
でも石英窓がこれを補なう役目をする。一方、顕
微鏡導入ポート12の封止ガラス17は目視者の
眼をレーザ光から保護するため特殊ガラスにする
必要があり、この封止ガラス17は半導体ウエハ
ー1の照射位置より遠く差し支えないので、蒸発
物の付着は少なくなる。 The purpose of placing the reflecting mirror 13 and objective lens 15 outside the vacuum column 5 is that since they are insulators, they will charge up inside the vacuum column.
This is to prevent the beam, especially the electron beam, from being affected and the irradiation position to be distorted. The appropriate focal length f of the objective lens 15 is 50 to 70 mm; if it is shorter than that, a lot of evaporated matter from the semiconductor wafer 1 will adhere to it, making it impossible to keep the illuminance constant during processing, and if it is shorter than that, This makes it difficult to narrow down the laser beam. However, this evaporated material adheres to the protective glass 16 in front of the objective lens, and therefore the protective glass constantly needs to be replaced. Furthermore, since the protective glass is in a vacuum, it is preferable to sputter a thin metal film that transmits laser light onto the surface to prevent charge-up. Furthermore, the quartz window 14 is used to protect the objective range 15 and is sufficiently sealed, so that even if the protective glass 16 is replaced and the sealing is insufficient, the quartz window serves to compensate for this. On the other hand, the sealing glass 17 of the microscope introduction port 12 needs to be made of special glass to protect the viewer's eyes from the laser beam, and since this sealing glass 17 can be far away from the irradiation position of the semiconductor wafer 1, There will be less adhesion of objects.
特に本装置の重要なことは、電子ビームは垂直
に照射する構造としているが、レーザ光は傾斜し
て照射されることで、レーザ光も可能な限り垂直
に近くして照射する方が良い。例えば、電子ビー
ムを偏向させて照射するスキヤンニング機能をも
与えるとすると、レーザ光の対物レンズと半導体
ウエハー1の照射位置との距離を50〜70mmとし、
スキヤンニングが数cmの幅であれば、電子ビーム
とレーザ光との中心線角度θは出来るだけ垂直線
に近接して25〜30°となる。スキヤンニング機能
を与えなければその角度θは更に小さくなること
は言うまでもない。また、反射ミラー13での反
射角もできるだけ小さい方が良くて、これらの入
射方向の問題はすべて照射スポツトの強度分布を
不均一としないための配慮である。 What is particularly important about this device is that the electron beam is irradiated vertically, but the laser beam is irradiated obliquely, so it is better to irradiate the laser beam as close to vertical as possible. For example, if a scanning function is also provided in which the electron beam is deflected and irradiated, the distance between the objective lens of the laser beam and the irradiation position of the semiconductor wafer 1 is set to 50 to 70 mm.
If the scanning width is several centimeters, the centerline angle θ between the electron beam and the laser beam will be 25 to 30 degrees, as close as possible to the vertical line. Needless to say, the angle θ would be even smaller if no scanning function was provided. Further, it is preferable that the reflection angle at the reflection mirror 13 be as small as possible, and all of these problems regarding the direction of incidence are taken into consideration to prevent the intensity distribution of the irradiation spot from becoming non-uniform.
尚、上記説明でステージ2が可動するに拘わら
ず、電子ビームにスキヤンニング機能を与えるの
は高速処理を目指しており、その場合は電子ビー
ムのスキヤンニングに応じて、レーザ光の反射ミ
ラー13を同期させて動かす機構を附加し、絶え
ず両者が被照射体の同一位置を照射させることが
必要である。尚、ステージ移動が25cm/秒程度で
あるのに対し、スキヤンニングすると速度は
5m/秒と速くすることができる。 Incidentally, although the stage 2 is movable in the above explanation, the purpose of providing a scanning function to the electron beam is to achieve high-speed processing, and in that case, the reflection mirror 13 of the laser beam is It is necessary to add a mechanism to move them in synchronization so that both of them constantly irradiate the same position on the object to be irradiated. Furthermore, while stage movement is approximately 25 cm/sec, scanning speed is approximately 25 cm/sec.
It can be as fast as 5m/sec.
ここで電子ビームは、被熱処理領域を予備加熱
(プレアニール)しており、予備加熱された被熱
処理領域に対してレーザ光を照射することによ
り、本発明は被処理体に対して瞬時に強いエネル
ギーを加えて短時間で熱処理を行うことができ
る。 Here, the electron beam preheats (pre-anneals) the area to be heat treated, and by irradiating the preheated area to be heat treated with a laser beam, the present invention can instantaneously apply strong energy to the object to be processed. can be added to perform heat treatment in a short time.
また、電子ビームとレーザ光との照射位置は一
致しなければならないが、両方の照射スポツトの
大きさが同一である必要はなく、例えば電子ビー
ム照射スポツトを100μmφとし、レーザ光の照射
スポツトを20〜30μmφとして使用してもよい。 Furthermore, although the irradiation positions of the electron beam and the laser beam must match, it is not necessary that the sizes of both irradiation spots be the same; for example, the electron beam irradiation spot can be set to 100 μmφ, and the laser beam irradiation spot can be set to 20 μmφ. It may be used as a diameter of ~30 μm.
更に電子ビームはレーザ光と異なり、電子の加
速エネルギーを調整することで被処理体の表面あ
ら所望の深さの領域を加熱することも可能である
ため、レーザ光による加熱と同時に用いることに
より被熱処理領域を3次元的に選択することも可
能となる。 Furthermore, unlike laser light, electron beams can heat a region of the desired depth on the surface of the object by adjusting the acceleration energy of the electrons. It also becomes possible to select the heat treatment area three-dimensionally.
(f) 発明の効果
以上述べたように本発明によれば、電子ビーム
がレーザ光と異なり、電流を調整することで出力
をかなり上げることができるため、レーザ光に比
べてビーム径を大きくすることが可能であり、レ
ーザ光の照射領域全体を確実に予備加熱すること
ができる。(f) Effects of the Invention As described above, according to the present invention, unlike a laser beam, the output of an electron beam can be considerably increased by adjusting the current, so the beam diameter can be increased compared to a laser beam. This makes it possible to reliably preheat the entire laser beam irradiation area.
また、本発明にかかる複合ビーム照射装置は、
電子ビームにより予備加熱すると共にレーザ光を
被照射体に同時に照射するので、強いエネルギー
を被照射体に瞬時に加えることができ、不要部分
への熱伝達を極力少なくした局部加熱処理を高精
度に行うことができる。このため本発明は、単結
晶成長やイオン注入後のアニールに役立ち、高品
位の半導体装置、特に集積回路の製造に大きく寄
与するものである。 Further, the composite beam irradiation device according to the present invention includes:
Since the object to be irradiated is preheated by an electron beam and simultaneously irradiated with laser light, strong energy can be instantly applied to the object to be irradiated, allowing highly accurate local heating treatment that minimizes heat transfer to unnecessary parts. It can be carried out. Therefore, the present invention is useful for single crystal growth and annealing after ion implantation, and greatly contributes to the production of high-quality semiconductor devices, especially integrated circuits.
第1図は本発明にかゝる複合ビーム照射装置の
断面概要図、第2図はその部分拡大図である。
図中、1は被照射体、2は可動ステージ、5は
真空コラム、6は電子銃、7は電子ビーム、8は
電子ビーム制御系、9はレーザ光源、10はレー
ザ光、13は反射ミラー、15は対物レンズ、1
6は透過窓を示す。
FIG. 1 is a schematic cross-sectional view of a composite beam irradiation device according to the present invention, and FIG. 2 is a partially enlarged view thereof. In the figure, 1 is an irradiated object, 2 is a movable stage, 5 is a vacuum column, 6 is an electron gun, 7 is an electron beam, 8 is an electron beam control system, 9 is a laser light source, 10 is a laser beam, 13 is a reflecting mirror , 15 is an objective lens, 1
6 indicates a transmission window.
Claims (1)
を予備加熱する電子銃、該電子ビームを制御する
ための電子ビーム制御系、およびこれらを納めた
コラム外より集束されたレーザ光を透過窓を通し
て該被照射体に該電子ビームと共に照射するレー
ザ照射手段を有し、上記電子ビームと該レーザ光
を該被照射体の同一位置に同時に照射することに
より、該被照射体を熱処理する機能をもたせたこ
とを特徴とする複合ビーム照射装置。1 An electron gun that irradiates an irradiated object with an electron beam to preheat the irradiated object, an electron beam control system that controls the electron beam, and a column containing these that transmits focused laser light from outside. A function of heat-treating the irradiated object by having a laser irradiation means for irradiating the irradiated object together with the electron beam through a window, and simultaneously irradiating the same position of the irradiated object with the electron beam and the laser light. A composite beam irradiation device characterized by having.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56215709A JPS58115741A (en) | 1981-12-28 | 1981-12-28 | Composite beam irradiator unit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56215709A JPS58115741A (en) | 1981-12-28 | 1981-12-28 | Composite beam irradiator unit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58115741A JPS58115741A (en) | 1983-07-09 |
| JPH057824B2 true JPH057824B2 (en) | 1993-01-29 |
Family
ID=16676857
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56215709A Granted JPS58115741A (en) | 1981-12-28 | 1981-12-28 | Composite beam irradiator unit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58115741A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS625547A (en) * | 1985-07-01 | 1987-01-12 | Ulvac Corp | Apparatus for checking foreign matter on substrate surface |
| US20160052056A1 (en) * | 2014-08-22 | 2016-02-25 | Arcam Ab | Enhanced electron beam generation |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51113468A (en) * | 1975-03-29 | 1976-10-06 | Toshinobu Takagi | Solid surface processing system |
-
1981
- 1981-12-28 JP JP56215709A patent/JPS58115741A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58115741A (en) | 1983-07-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4439245A (en) | Electromagnetic radiation annealing of semiconductor material | |
| US9466402B2 (en) | Processes and systems for laser crystallization processing of film regions on a substrate utilizing a line-type beam, and structures of such film regions | |
| US4581520A (en) | Heat treatment machine for semiconductors | |
| US6852162B2 (en) | Laser annealing apparatus | |
| WO2005029548A2 (en) | System and process for providing multiple beam sequential lateral solidification | |
| JPH08195357A (en) | Laser irradiating device | |
| US4303694A (en) | Method and device of deposition through vacuum evaporation making use _of a modulated electron beam and a screen | |
| US5415901A (en) | Laser ablation device and thin film forming method | |
| JPH057824B2 (en) | ||
| US7335260B2 (en) | Laser annealing apparatus | |
| JPH01246828A (en) | Beam annealing device | |
| JPH06291035A (en) | Beam annealing apparatus | |
| JPS58110042A (en) | Beam irradiation apparatus | |
| JP2548961B2 (en) | Laser heat treatment equipment | |
| JPH01146319A (en) | Laser heat treatment device | |
| JPH0142618B2 (en) | ||
| JPH01120556A (en) | Device for correcting patterned film | |
| GB2133618A (en) | Fabricating semiconductor circuits | |
| JPS63259947A (en) | Linear electron beam device | |
| JPS62213055A (en) | Electron beam annealing device | |
| JPS635514A (en) | Beam annealing device | |
| JPH06192821A (en) | Laser PVD device | |
| JP2000144386A (en) | Method of forming thin film by laser vapor deposition method and laser vapor deposition apparatus used in the method of forming a thin film | |
| JPH0391925A (en) | Laser annealing device | |
| JPS5816747B2 (en) | ion implanter |