JPS60216561A - Heat-treating method - Google Patents
Heat-treating methodInfo
- Publication number
- JPS60216561A JPS60216561A JP59073285A JP7328584A JPS60216561A JP S60216561 A JPS60216561 A JP S60216561A JP 59073285 A JP59073285 A JP 59073285A JP 7328584 A JP7328584 A JP 7328584A JP S60216561 A JPS60216561 A JP S60216561A
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- heated
- light
- heating
- depth
- 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.)
- Pending
Links
- 238000000034 method Methods 0.000 title claims abstract description 8
- 238000010438 heat treatment Methods 0.000 claims abstract description 29
- 239000000758 substrate Substances 0.000 abstract description 15
- 239000012535 impurity Substances 0.000 abstract description 12
- 238000006243 chemical reaction Methods 0.000 abstract description 5
- 238000009792 diffusion process Methods 0.000 abstract description 4
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 7
- 229910052710 silicon Inorganic materials 0.000 description 7
- 239000010703 silicon Substances 0.000 description 7
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 4
- 230000010355 oscillation Effects 0.000 description 4
- 230000035515 penetration Effects 0.000 description 4
- 239000004065 semiconductor Substances 0.000 description 4
- 239000007789 gas Substances 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 2
- 238000000137 annealing Methods 0.000 description 2
- 230000001276 controlling effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 229910052757 nitrogen Inorganic materials 0.000 description 2
- 230000005855 radiation Effects 0.000 description 2
- 230000002411 adverse Effects 0.000 description 1
- BJQHLKABXJIVAM-UHFFFAOYSA-N bis(2-ethylhexyl) phthalate Chemical compound CCCCC(CC)COC(=O)C1=CC=CC=C1C(=O)OCC(CC)CCCC BJQHLKABXJIVAM-UHFFFAOYSA-N 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000005674 electromagnetic induction Effects 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 239000000615 nonconductor Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 238000001556 precipitation Methods 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 239000010979 ruby Substances 0.000 description 1
- 229910001750 ruby Inorganic materials 0.000 description 1
- 230000005469 synchrotron radiation Effects 0.000 description 1
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
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/30—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
- H01L21/324—Thermal treatment for modifying the properties of semiconductor bodies, e.g. annealing, sintering
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Manufacturing & Machinery (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
本発明は、物体の一部分を所望の温度まで加熱する熱処
理方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of the Invention] The present invention relates to a heat treatment method for heating a portion of an object to a desired temperature.
物体を所望の温度まで加熱するには通常高温空−間を有
する炉内に物体を挿入するか、あるいは高温液体中に物
体を浸漬する方法がとられる。従って加熱温度はその空
間あるいは液体の温度によって規制され、加熱温度を変
更するにはその都度温度調整を行わねばならず、熱容量
に応じたかなり長い時間を必要とする。一方直接加熱方
法とじて電磁誘導により導電性物体を加熱する誘導加熱
、誘電体損によって誘電体を加熱する防電加熱、マイク
ロ波によりて非電導体を加熱するマイクロ波加熱などが
ある。しかしこれらは装置の費用がかさむこと、温度の
調節は加熱入力の調整によって行われることが多く、微
妙な温度調整は困難である。また赤外線放射によって熱
エネルギーを伝える赤外線加熱も広く行われているが、
物体表面全体が加熱され、加熱温度の微妙なaXも困難
である。一方半導体技術の発展に伴ない、半導体基板の
一部、すなわち平面的な所定の領域、あるいは表面から
の所定の厚さを不純物拡散あるいは表面歪解消のために
加熱する必要が生じている。この場合所定の区域に対し
て所定の加熱温度が満足されないと、加熱効果が達せら
れないばかりでなく半導体装置の特性をかえって害する
ことがある。To heat an object to a desired temperature, the object is usually inserted into a furnace having a high-temperature space, or immersed in a high-temperature liquid. Therefore, the heating temperature is regulated by the temperature of the space or liquid, and in order to change the heating temperature, the temperature must be adjusted each time, which requires a considerably long time depending on the heat capacity. On the other hand, direct heating methods include induction heating in which a conductive object is heated by electromagnetic induction, electrostatic heating in which a dielectric is heated by dielectric loss, and microwave heating in which a non-conductor is heated by microwaves. However, these devices are expensive, and the temperature is often adjusted by adjusting the heating input, making delicate temperature adjustment difficult. Infrared heating, which transmits heat energy through infrared radiation, is also widely used.
The entire surface of the object is heated, and it is difficult to maintain the delicate heating temperature aX. On the other hand, with the development of semiconductor technology, it has become necessary to heat a part of a semiconductor substrate, that is, a predetermined planar region or a predetermined thickness from the surface, in order to diffuse impurities or eliminate surface strain. In this case, if a predetermined heating temperature is not satisfied for a predetermined area, not only will the heating effect not be achieved, but the characteristics of the semiconductor device may be adversely affected.
局部的に加熱する方法として電子ビーム加熱が知られて
いるが、この場合も加熱温度、加熱深さの調整も限度が
あり、また装置の高価な欠点がある。□〔発明の目的〕
本発明は、上述の欠点を除去し、物体の所定の面領域お
よび所定の深さを所定の温度に加熱することが容易にで
きる熱処理方法を提供することを目的とする。Electron beam heating is known as a method of locally heating, but in this case as well, there are limits to the adjustment of heating temperature and heating depth, and the device is expensive. □ [Object of the Invention] An object of the present invention is to eliminate the above-mentioned drawbacks and provide a heat treatment method that can easily heat a predetermined surface area and a predetermined depth of an object to a predetermined temperature. .
本発明によれば、所望の加熱温度、加熱深さに応じて選
ばれた波長、光量の光のビームによって加熱すべき面領
域を走査することにより上記の目的が達成される。According to the present invention, the above object is achieved by scanning the surface area to be heated with a beam of light having a wavelength and light intensity selected according to the desired heating temperature and heating depth.
以下図を引用して本発明の実施例について説明する。第
1図において、気相からの析出などにより表面に拡散不
純物源膜11を有するシリコン基板lを反応室2の底部
に置き、反応室2内を真空ポンプ3によって排気したの
ち、窒素ボンベ4よりN2ガスを導入し、NdYAGレ
ーザの波長1.064mの近赤外線発振光5を鏡6、レ
ンズ7を介して基板1の上に入射させ、基板1の不純物
を導入すべき領域上を走査する。レーザ光の基板上にお
けるエネルギー密度を1.751/cIaにした場合、
基板1の表面は1400〜1500℃に加熱される。こ
れによって不純物膜11から不純物が光の照射領域にお
いてのみ基板内に拡散する。不純物拡散のための加熱に
は波長10.6μmの中間赤外線の光を発振するCOz
ガスレーザも適している。周波数が小さくなると直接格
子振動を励起して熱エネルギーへの変換効率が向上する
。Embodiments of the present invention will be described below with reference to the drawings. In FIG. 1, a silicon substrate l having a diffused impurity source film 11 on its surface due to precipitation from the gas phase is placed at the bottom of a reaction chamber 2, and after the inside of the reaction chamber 2 is evacuated by a vacuum pump 3, a nitrogen cylinder 4 is evacuated. N2 gas is introduced, and near-infrared oscillation light 5 of a wavelength of 1.064 m from a NdYAG laser is made incident on the substrate 1 via a mirror 6 and a lens 7 to scan the region of the substrate 1 into which impurities are to be introduced. When the energy density of the laser beam on the substrate is set to 1.751/cIa,
The surface of the substrate 1 is heated to 1400-1500°C. As a result, impurities from the impurity film 11 are diffused into the substrate only in the light irradiation region. COz, which oscillates mid-infrared light with a wavelength of 10.6 μm, is used for heating for impurity diffusion.
Gas lasers are also suitable. As the frequency decreases, it directly excites lattice vibrations and improves the efficiency of conversion into thermal energy.
MO8構造においてゲート酸化膜とシリコン基板との界
面のダングリングボンドの解消のだめの熱処理、すなわ
ちアニーリングには、例えば2490Aの波長のKvF
エキシマレーザ発振光、あるいは6940 kの波長の
ルビーレーザ発振光を用いるのがよい。In the MO8 structure, heat treatment to eliminate dangling bonds at the interface between the gate oxide film and the silicon substrate, that is, annealing, is performed using KvF with a wavelength of 2490A, for example.
It is preferable to use excimer laser oscillation light or ruby laser oscillation light with a wavelength of 6940 k.
さらに一つの光源を用いて波長の制御により適応した波
長の光を照射することもできる。これには例えば発振光
の波長の範囲か広く、回折格子、プリズム、エタロンあ
るいはフィルタなどの光学素子を共振器として用い℃狭
帯域化される色素レーザ、あるいはシンクロトロン放射
(80R光)と回折格子などの組合せを用いることが有
効である。Furthermore, it is also possible to irradiate light with an appropriate wavelength by controlling the wavelength using one light source. Examples of this include a dye laser whose oscillation light has a wide wavelength range and whose band is narrowed by using an optical element such as a diffraction grating, prism, etalon, or filter as a resonator, or a dye laser that uses synchrotron radiation (80R light) and a diffraction grating. It is effective to use combinations such as
加熱される層の深さは、照射された光の物体への侵入距
離に依存する。侵入距離はその光に対する物体の吸収係
数に反比例する。第2図は、25℃におけるシリコン中
の光の侵入距離とシリコンの光の吸収係数の波長依存性
を示す。従って波長の長い光を用いることによって厚い
層を加熱することが可能になる。これにより、例えば不
純物の拡散深さの精密な調整ができる。The depth of the heated layer depends on the penetration distance of the irradiated light into the object. The penetration distance is inversely proportional to the object's absorption coefficient for the light. FIG. 2 shows the wavelength dependence of the light absorption coefficient of silicon and the penetration distance of light in silicon at 25°C. It is therefore possible to heat thick layers by using light with a long wavelength. Thereby, for example, the diffusion depth of impurities can be precisely adjusted.
本発明は、光を用いた熱放射により物体を加熱する場合
に光の照射をビームによって行い、光の波長、光量を変
更、制御することにより所定の領域のみを所定の厚さま
で所定の温度に加熱するもので、特に微妙な制御を必要
とする半導体基板の不純物拡散あるいは表面歪解消のた
めのアニーリングに極めて有効に適用することができる
。When heating an object by thermal radiation using light, the present invention irradiates the object with a beam, and by changing and controlling the wavelength and intensity of the light, only a predetermined area is heated to a predetermined temperature to a predetermined thickness. It heats and can be extremely effectively applied to impurity diffusion in semiconductor substrates or annealing to eliminate surface strain, which requires particularly delicate control.
181図は本発明の一実施例のための装置の断面図、第
2図はシリコン中の光の侵入距離およびシリコンの光の
吸収係数と波長との関係線図である。
1・・・シリコン基板、11・・・不純物源膜、2・・
・反応室、4・・・窒素ボンベ、5・・・YAGレーザ
光。
7長 (pれ)FIG. 181 is a sectional view of a device according to an embodiment of the present invention, and FIG. 2 is a diagram showing the relationship between the penetration distance of light into silicon and the absorption coefficient of light in silicon and wavelength. 1... Silicon substrate, 11... Impurity source film, 2...
-Reaction chamber, 4...Nitrogen cylinder, 5...YAG laser light. 7 length (pre)
Claims (1)
加熱する方法であって、加熱温度、加熱深さに応じて選
ばれた波長、光量の光のビームによって加熱すべき面領
域を走査することを特徴とする熱処理方法。1) A method of heating a predetermined surface area of an object to a predetermined temperature to a predetermined depth, in which the surface area to be heated is heated by a beam of light with a wavelength and light intensity selected according to the heating temperature and heating depth. A heat treatment method characterized by scanning.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59073285A JPS60216561A (en) | 1984-04-12 | 1984-04-12 | Heat-treating method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59073285A JPS60216561A (en) | 1984-04-12 | 1984-04-12 | Heat-treating method |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60216561A true JPS60216561A (en) | 1985-10-30 |
Family
ID=13513718
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59073285A Pending JPS60216561A (en) | 1984-04-12 | 1984-04-12 | Heat-treating method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60216561A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63148685A (en) * | 1986-12-11 | 1988-06-21 | Sharp Corp | Manufacture of solar cell element |
JPS63169024A (en) * | 1987-01-05 | 1988-07-13 | Nec Corp | Impurity doping method |
JP2008211177A (en) * | 2007-02-27 | 2008-09-11 | Wafermasters Inc | Optical processing at selective depth |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4926456A (en) * | 1972-07-11 | 1974-03-08 | ||
JPS5758363A (en) * | 1980-09-26 | 1982-04-08 | Oki Electric Ind Co Ltd | Manufacture of mos type semiconductor device |
-
1984
- 1984-04-12 JP JP59073285A patent/JPS60216561A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4926456A (en) * | 1972-07-11 | 1974-03-08 | ||
JPS5758363A (en) * | 1980-09-26 | 1982-04-08 | Oki Electric Ind Co Ltd | Manufacture of mos type semiconductor device |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63148685A (en) * | 1986-12-11 | 1988-06-21 | Sharp Corp | Manufacture of solar cell element |
JPH0565066B2 (en) * | 1986-12-11 | 1993-09-16 | Sharp Kk | |
JPS63169024A (en) * | 1987-01-05 | 1988-07-13 | Nec Corp | Impurity doping method |
JP2008211177A (en) * | 2007-02-27 | 2008-09-11 | Wafermasters Inc | Optical processing at selective depth |
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