TWI283445B - Method and apparatus for thermally treating substrates - Google Patents
Method and apparatus for thermally treating substrates Download PDFInfo
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- H—ELECTRICITY
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- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/67—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere
- H01L21/67005—Apparatus not specifically provided for elsewhere
- H01L21/67242—Apparatus for monitoring, sorting or marking
- H01L21/67248—Temperature monitoring
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- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
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- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/44—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
- C23C16/48—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation
- C23C16/481—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation by radiant heating of the substrate
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- C30B31/00—Diffusion or doping processes for single crystals or homogeneous polycrystalline material with defined structure; Apparatus therefor
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- C30B33/00—After-treatment of single crystals or homogeneous polycrystalline material with defined structure
- C30B33/02—Heat treatment
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- H01L21/67115—Apparatus for thermal treatment mainly by radiation
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- H05B3/00—Ohmic-resistance heating
- H05B3/0033—Heating devices using lamps
- H05B3/0038—Heating devices using lamps for industrial applications
- H05B3/0047—Heating devices using lamps for industrial applications for semiconductor manufacture
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- H—ELECTRICITY
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- H01L21/67—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere
- H01L21/67005—Apparatus not specifically provided for elsewhere
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Abstract
Description
B7 1283445 五、發明說明( 本發明係關於—軸處理基板之方法及裝置,尤其是半 導體晶圓。 電腦晶片及其他電子材料主要係由圓 形之半導體碟 片即所明之卵圓’所製造生產。相應於該有許多不同之必 要作業步驟及作業程序,例如結構化流程、平板印刷程序、 植離子作業、糊錢層。尤其是鐘層程序巾,為了有效建 互電鍵層’必須在預定大氣環境中進行晶圓之溫度變化控 ^。然而絲I情晶騎進行之純溫度测,也常在其先 則f理步驟後之後處理流程中進行,例如在有效植入離子後 進行’ 〃鱗子植人&序乃為了清除晶圓晶格在植人過程中 可能產生之損壞。 、由於晶®溫度_之需要,其所相應之快速加熱裝置, 亦稱之為RTP裝置(Rapld Thermai pr〇cessing)之重要性因而 與曰俱增。可在—預定之流程條件狀況下,進行-快速且準 =空制晶圓之熱處_序。RTp裝置可以只在幾秒鐘内便讓 待處理之晶《加熱至贈c或更高之溫度。純值 此,树其罐峨,軸裝置之關 輸入考I因素為其加熱速度,即在短時間内產生極高之熱量 為了能使-餘,例如由頻城之半導體 母秒加熱幾百度之加熱處理過程,晶圓可 ,衣置例如在專利案DE_A_胸5 524中已經提出十 知<快速加熱裝置包含-衫英玻麵製成之處理室,用/來 本紙張尺度It用_家標準(C—咖X 297公幻_ -4-B7 1283445 V. INSTRUCTION DESCRIPTION OF THE INVENTION (The present invention relates to a method and apparatus for processing a substrate, particularly a semiconductor wafer. Computer chips and other electronic materials are mainly produced by a circular semiconductor disc, that is, an oval of the invention] Corresponding to this there are many different necessary work steps and operating procedures, such as structured processes, lithographic procedures, implant ion operations, paste layer, especially the bell layer towel, in order to effectively build the mutual bond layer 'must be in the predetermined atmosphere In the environment, the temperature change of the wafer is controlled. However, the pure temperature measurement performed by the silk I is often carried out in the process after the first step, for example, after the effective implantation of ions. The sub-plant & order is to remove the damage that may occur in the wafer lattice during the implantation process. Because of the temperature of the crystal _, the corresponding rapid heating device, also known as the RTP device (Rapld Thermai pr The importance of 〇cessing) is thus increasing. It can be carried out under the condition of the predetermined process conditions - fast and accurate = the hot spot of the wafer. The RTp device can only be In a few seconds, the crystal to be processed is heated to a temperature of c or higher. The pure value is the value of the can, and the input of the shaft device is the heating factor of the heating factor, that is, the pole is generated in a short time. High heat in order to enable -, for example, the heat treatment process of several hundred degrees by the semiconductor mother of the frequency city, the wafer can be placed, for example, in the patent DE_A_ chest 5 524 has been proposed Contains the processing room made of -British glass surface, with / to the paper scale It uses _ home standard (C-Cai X 297 phantom _ -4-
-J.. !| 訂·! - - ---— (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 1283445 A7 f __ _ B7 五、發明說明(2·) 裝載基板。在該處理室之上方及下方則分別裝設加熱燈,藉 以產生電磁輻射線,以便進行基板之熱處理。該加熱燈及處 理室乃由另一室(反射室)所包圍,該反射室包含反射之内 壁,以用於反射加熱燈所產生之電磁輻射線。 該處理室中之石英玻璃對於加熱燈所產生之電磁輕射 線之光譜而言,基本上具有穿透性。此外,該處理室中裝設 有處理氣體之進氣及排放裝置,透過該裝置,可以在基板進 行熱處理時’在處理室中產生一適當之大氣環境。 為了達到測I晶圓溫度之目的’乃裝設一高溫計作為溫 度測1裝置。為了使由晶圓所放射或由晶圓所反射之輕射線 能與穿透過晶圓之輻射線區分開來,可對加熱燈之輻射線進 行調整。藉由該調整作業也可將由基板所放射之輻射線與由 基板所反射及穿透之輻射線區分開來。另外藉由區分作業, 可方便確認晶圓之放射率,這對靠晶圓放射之輻射線來進行 溫度控制是十分必要的。與該相關之調整及溫度控制之細 節,業已在習知之專利案DE-A-199 05 524或 US-A_5,154,512 中公開。 然而以高溫計測量溫度之方式容易產生下列問題,亦即 在處理室及反射室中會充斥有極強之輻射線,這會使得由晶 圓所放射之輻射線很難與其他輻射線區分開來。由晶圓所放 射之溫度輻射線與透過高溫計測得之溫度輻射線將會與其 餘之輻射線重疊。因而只能在(其餘輻射線之)背景環境中^ 得極不清楚之(由晶圓所放射之輻射線)訊號。該問題在晶圓 溫度低之狀況下特別明顯,因為由晶圓所放射之輻射線會^-J.. !| Book·! - - ---- (Please read the notes on the back and fill out this page) Printed by the Ministry of Economic Affairs, Intellectual Property Office, Staff and Consumers Co., Ltd. 1283445 A7 f __ _ B7 V. Invention Description (2·) Loading the substrate. Heat lamps are installed above and below the processing chamber to generate electromagnetic radiation for heat treatment of the substrate. The heat lamp and processing chamber are surrounded by another chamber (reflecting chamber) that includes a reflective inner wall for reflecting the electromagnetic radiation generated by the heat lamp. The quartz glass in the processing chamber is substantially penetrating for the spectrum of the electromagnetic light ray generated by the heating lamp. Further, the processing chamber is provided with an intake and discharge means for processing gas through which an appropriate atmosphere can be generated in the processing chamber when the substrate is subjected to heat treatment. In order to achieve the purpose of measuring the temperature of the I wafer, a pyrometer is installed as the temperature measuring device. In order to distinguish light rays reflected by or reflected by the wafer from radiation passing through the wafer, the radiation of the heating lamp can be adjusted. The radiation emitted by the substrate can also be distinguished from the radiation reflected and penetrated by the substrate by the adjustment operation. In addition, by distinguishing the operation, it is convenient to confirm the emissivity of the wafer, which is necessary for temperature control by the radiation radiated from the wafer. The details of the adjustments and the temperature control are disclosed in the prior art patents DE-A-199 05 524 or US-A-5,154,512. However, the method of measuring the temperature with a pyrometer is prone to the following problems, that is, the processing chamber and the reflecting chamber are filled with extremely strong radiation, which makes the radiation radiated by the wafer difficult to distinguish from other radiation. . The temperature radiation emitted by the wafer and the temperature radiation measured by the pyrometer will overlap with the remaining radiation. Therefore, it is only in the background environment (the rest of the radiation) that the signal (radiation radiated by the wafer) is extremely unclear. This problem is particularly noticeable at low wafer temperatures because the radiation emitted by the wafer will be ^
-----Ί I 1.—--i 1 I I I I I 1-----I (請先閱讀背面之注意事項再填寫本頁) 1283445 經濟部智慧財產局員工消費合作社印製 A7 五、發明說明(3· 著溫度卩祕祕快地_。因此補訊號_背景_練關係狀 況也因而會隨著晶圓溫度之降低而變得不_。在溫度低於 400°C時,晶圓只會放射極微之輻射線,因而晶圓在低於該 溫度之狀況下,對於加熱輻射線而言是有穿透性的,也因此 輕射訊號背景棚雜況會變財差。所以在溫度低於 400°C時,基本上傳統之處理方式是不可能藉由高溫計測量 來確認晶圓溫度。 為了改善RTP裝置能以向溫計測量溫度之方式確認輕 射訊號-背景-輻射關係狀況,在專利案DE-A-40 ί2 614中已 提出下列建議’亦即採用含有氳氧元素之石英材質來製造處 理室。該類石英材質之特性在於,可以吸收波長範圍介於 2·6μπι至2·8μιη之紅外線。藉此可使在處理室中之晶圓透過 輕射線加熱,使其輻射線之光譜在波長介於2 6μπι至2 8μιη 之間具有缺口。該石英室中裝設有一透視窗,其在上述之波 長範圍内設計成可透視,並且可以朝向裝設在晶圓上之高溫 計。該高溫計乃用於測量由晶圓所放射之波長為2·7μπι之紅 外線輻射線。因為由加熱燈所放射之波長範圍2·7μηι之輻射 線操法進入處理室’所以南溫計所測量之溫度為單單由晶圓 所放射之輻射線。 藉由該方法可以好好地測量晶圓之溫度輻射線。然而進 行晶圓之溫度剩整時’確定波長為2,7μιη時之反射率及穿透 率是十分重要的。 專利案DE-A-199 05 524中曾提出習知之確定穿透率及 放射率之方法,其利用一特別之調整器來測量晶圓所反射及 ‘紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 6 ---Γ----ΊΙΙΊΙ JAW ^ ill — — I — (請先閲讀背面之注意事項再填寫本頁) 1283445 A7 ________B7 _ 五、發明說明(4·) 穿透晶圓之輕射線;然而該方法並無法為本發明所利用,因 其加熱燈之波長為2·7μιη之輻射線會被處理室壁牆所吸收。 因此本發明之任務係在於,透過—解且低成本之方式 來裝設-湖高溫計之基板溫度測量裝置,目的在於即使在 低溫狀赵下仍可以準確地進行溫度測章。 經濟部智慧財產局員工消費合作社印製 本發明之任務係藉由一熱處理基板,尤其是半導體晶圓 之裝置來解決,其至少裝設有第一及第二輻射源,至少一介 於第一輻射源與基板之間之透明隔絕體,以利吸收一預定波 長之輻射線,至少一與第二輻射源同一側且朝向基板之輻射 測量器,以利測量預定波長之輻射線,一可調整由輕射源所 放射之輻射線之裝置,以及一可測量由第二輻射源所放射之 輕射線纟裝置。本發明乃裝設有一可將第一輕射源之預定波 長之輻射線濾除之裝置,該預定波長乃在朝向基板之輻射測 ΐ體之測I範圍内。藉此可明顯地改善基板輻射線與其餘輻 射線之間之輻射訊號-背景-輻射關係狀況。此外,至少對沒 有濾光且裝射在輻射測量體側邊上之燈進行調整,並藉此確 .認其所放射之輻射線,並且測得晶圓之反射率,藉此可進一 步反推得知晶®在高溫計之測量波長顧之放鱗。最後根 據该放射率及由晶圓所測量之輻射線可推振 根據本發明之一較佳之實施形式,輻射源乃分別裝I在 基板彼此相對之兩侧,以便可將經濾光之輻射線與未濾光之 輻射線分開。尤其是第二輻射源僅裝設在基板之一側/ 了且該 輕射測量器乃麵基板之—側,以便在高溫計上只會測量到 由晶圓所放射之輻射線及由其反射之輻射線。曰 本紙張尺度適用中國國家標準(CNS)A4規格⑽x 297公爱) 1283445 A7 B7 五、發明說明(S· 射源ΪΞΐ發明之Γ較佳之實施形式’錢設有調節第一輻 (請先閱讀背面之注意事項再填寫本頁) =由、.4光《#—輻射源來砸晶圓之溫度。藉此可 之測量波長細之贿射線之反射強度突 …、%增,進而方便決定其溫度。 該輕射源最好為加熱燈。根據本發明之實施形式,其具 2可吸收燈猶線之歉波長之透明贼體,碰透明隔絕 肢乃由加熱燈之燈泡所組成。藉此可以—簡單且低成本之方 式來達成所期望之滤光功能。尤其是針對一既已建立之系 統,可以單單藉由交換加熱燈便完成改裝作業。 „在本發明另-較佳之實施形式中,透鶴絕義為一介 於第ϋ射源與基板之間之處理室壁牆,該壁牆可吸收預定 波長。該可吸收輻射之處理室壁牆乃裝設在與高溫計相反之 基板侧邊上,以便可確保與輻射測量器同一側不會出現有該 預定波長之輻射照射。 經濟部智慧財產局員工消費合作社印製 叆透明隔絕體最好至少包含一濾光層,以利吸收預定波 長,根據另一實施形式,該濾光層與另一透明材質,例如由 石英玻璃製成之處理室壁橋隔開。該透明隔絕體最好採用含 有氫氧元素之石英玻璃來製造,該石英玻璃最好可以吸收介 於2·6μπι至2·8μιη之波長。為了避免該可吸收預定波長之 透明隔絕體有過熱狀況,因而裝設一用來冷卻透明隔絕體之 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱)-----Ί I 1.---i 1 IIIII 1-----I (Please read the note on the back and fill out this page) 1283445 Ministry of Economic Affairs Intellectual Property Bureau employee consumption cooperative printed A7 V. Invention Explanation (3. The temperature is secret and fast. _. Therefore, the signal of the ___ background_ ing relationship will not become _ as the temperature of the wafer decreases. At temperatures below 400 °C, the wafer only Will radiate very little radiation, so the wafer is penetrating for heating the radiation below this temperature, so the light background signal shed will become poor, so the temperature is low. At 400 ° C, basically the traditional way of processing is impossible to confirm the wafer temperature by pyrometer measurement. In order to improve the RTP device can confirm the light-light signal-background-radiation relationship by measuring the temperature to the thermometer, The following proposal has been made in the patent application DE-A-40 ί2 614, which uses a quartz material containing a bismuth oxide element to produce a processing chamber. The characteristics of this type of quartz material are that the absorption wavelength range is from 2·6 μm to 2 · 8μιη infrared, which can be used in the processing room The circle is heated by light rays such that the spectrum of the radiation has a gap between wavelengths of 2 6 μm to 28 μm. The quartz chamber is provided with a see-through window which is designed to be see-through in the above-mentioned wavelength range and can be The pyrometer is mounted on the wafer. The pyrometer is used to measure the infrared radiation emitted by the wafer at a wavelength of 2·7 μm. Because of the radiation range of the wavelength range of 2·7 μηι emitted by the heating lamp The method enters the processing chamber' so the temperature measured by the south thermometer is the radiation radiated by the wafer alone. By this method, the temperature radiation of the wafer can be well measured. However, when the temperature of the wafer is reconditioned, it is determined. The reflectance and the transmittance at a wavelength of 2,7 μm are important. A method for determining the transmittance and emissivity is proposed in the patent application DE-A-199 05 524, which utilizes a special regulator. Measuring wafer reflection and 'paper size applicable to China National Standard (CNS) A4 specification (210 X 297 mm) 6 ---Γ----ΊΙΙΊΙ JAW ^ ill — — I — (Please read the back note first) Fill in this Page) 1283445 A7 ________B7 _ V. Description of invention (4·) Light rays penetrating the wafer; however, this method cannot be utilized for the present invention because the radiation of the heater lamp having a wavelength of 2·7 μηη will be processed by the chamber. The wall wall is absorbed. Therefore, the task of the present invention is to install a substrate temperature measuring device of a lake pyrometer by means of a solution and a low cost, so that the temperature can be accurately measured even under a low temperature condition. The mission of the invention is printed by a device for heat-treating a substrate, in particular a semiconductor wafer, which is provided with at least one of the first and second radiation sources, at least one being first a transparent insulator between the radiation source and the substrate for absorbing radiation of a predetermined wavelength, at least one radiation measuring device on the same side of the second radiation source and facing the substrate, for measuring the radiation of the predetermined wavelength, and being adjustable A device for radiating radiation from a light source, and a light ray device capable of measuring radiation emitted by the second source. The present invention is provided with a means for filtering out radiation of a predetermined wavelength of the first light source, the predetermined wavelength being within the range I of the radiation measuring body facing the substrate. Thereby, the radiation signal-background-radiation relationship between the substrate radiation and the remaining radiation can be significantly improved. In addition, at least the lamp that is not filtered and mounted on the side of the radiation measuring body is adjusted, and thereby the radiation emitted by the radiation is confirmed, and the reflectance of the wafer is measured, thereby further pushing back It is known that Crystal® is scaled at the measurement wavelength of the pyrometer. Finally, according to the emissivity and the radiation measured by the wafer, according to a preferred embodiment of the present invention, the radiation source is separately mounted on opposite sides of the substrate so that the filtered radiation can be filtered. Separated from unfiltered radiation. In particular, the second radiation source is only disposed on one side of the substrate and the light-emitting measuring device is on the side of the surface substrate, so that only the radiation radiated by the wafer and the reflection thereof are measured on the pyrometer. Radiation.曰本纸标准Applicable to China National Standard (CNS) A4 Specification (10)x 297 公爱) 1283445 A7 B7 V. Invention Description (S· 射 ΪΞΐ ΪΞΐ ΪΞΐ ΪΞΐ Γ Γ Γ Γ 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱 钱Note on the back side of this page) = by, .4 light "# - radiation source to the temperature of the wafer. This can be used to measure the reflection intensity of the brittle ray of the wavelength, ... increase, and then it is convenient to decide Preferably, the light source is a heat lamp. According to an embodiment of the invention, the transparent thief body having a wavelength of apology for absorbing the light of the lamp is formed by a bulb of the heat lamp. The desired filtering function can be achieved in a simple and low-cost manner. Especially for an already established system, the conversion can be carried out simply by exchanging the heating lamp. „ In a further preferred embodiment of the invention The through-the-shoulder is a processing chamber wall between the first source and the substrate, and the wall can absorb a predetermined wavelength. The wall of the radiation-absorbing processing chamber is mounted on the opposite side of the substrate from the pyrometer. On the side so that Make sure that the radiation of the predetermined wavelength does not appear on the same side as the radiation measuring device. The Ministry of Economic Affairs, the Intellectual Property Office, the employee consumption cooperative, the printed transparent transparent body preferably contains at least one filter layer to absorb the predetermined wavelength, according to another In an embodiment, the filter layer is separated from another transparent material, such as a processing chamber wall bridge made of quartz glass. The transparent insulation body is preferably made of quartz glass containing hydrogen and oxygen elements, and the quartz glass is preferably Absorbs the wavelength between 2·6μπι and 2·8μηη. In order to avoid the overheating condition of the transparent insulator which can absorb the predetermined wavelength, the paper size for cooling the transparent insulator is applicable to the Chinese National Standard (CNS) A4. Specifications (210 X 297 public)
Q 1283445 A7 五、發明說明(6·) 裝置。該冷卻裝置最好具有冷卻氣體或冷卻流體。 根據本發明之-較佳之實施形式,輕細彳量器乃為一高 溫計。基板最好是經鍍層處理之半導體晶圓,尤其是有= 及/或Ti麟處理之料體。為了避免在蚊放射率時 還需另外制量穿透率,該細最好有—錄而幾乎可忽略 之穿透率。該基板之穿透率最好小於〇15。 在本發明另-實施形式中,其裝設—朝向基板之第二輕 射測量器,其裝置方式最好要使其能進行穿透率之測量,以 便精確地測得基板放射率之大小。在本發明之實施形式中, 孩第二輕射測量器乃可以測量超出預定波長之輕射線,如此 万可測量姉社未被錄且敏後之铺線。同時該第二 輻射測量器最好測量比預定波長稍低或稍高之輕射線,以便 可以透過植入法,尤其是線性植入法’料算會被吸收之波 長之基板穿透率。 、在本發明另-貫施形.式中’其乃特別適用於加熱燈之燈 泡有滤,功能之狀況,在該設計模式中,該第二轉射測量器 乃朝向第二讀源之方向但制隔姐板,讀用於測量在 2波仙之雜。藉此可以賴以帛二加紐職射並穿 透基板之輻射線來測得穿透率。 本發月之基本任務係藉由熱處理基板方法,尤其是半導 =圓以下列程序步驟來解決,即以至少第一及第二輕射 ,,基板,吸收介於第_輕射源與基板之間之第一輕射 ::疋波長’以—輕射測量器來測量由基板所放射之在預 足波長之勒博,妹_量器骑财鮮二觖源同一 — ^----^---^---^ -------I ------- (請先閲讀背面之注意事項再填寫本頁) -Q_ 1283445 A7 圖一 1^3 一 圖一 圖三 圖四 圖五 五、發明說明( 側之方向上’雜㈣二輕射_放射之帛二輻射線,並測 量該由第二__放射之第二輻射線。藉由上述方法再配 合上迷提及之裝置,將可達成所期望之優點,亦即藉由吸收 第一輕射線之預定波長來改善補減_背景_輕射關係狀 況’同時可透糊整第二輻射線來確認晶圓之放射率。 以下將藉由較佳之發明實施例,以圖示進一步說明本發 明。各圖示之内容如下: 根據本發明之第一實施例所示之快速加熱裝置之示 意剖面圖,· 根據本發明之第二實施例所示之快速加熱裝置之示 意剖面圖; 某特定晶圓之穿透率及反射率關係之圖示說明; 經姑鍍層處理之晶圓熱處理之溫度曲線圖; 根據本發明之實施例之調控測量範圍所進行之穿透 率測量之圖示說明。 以下將藉由較佳之發明實施例進一步說明本發明。 圖一顯示一快速加熱系統1之剖面圖,該系統乃根據本 發明之第一貫施形式來快速加熱半導體晶圓。内部安置有一 半導肖豆日Εί圓3之處理室2,其由一位於上方之透明板4及一 位於下方之透明板5所形成,其中透明板之材質最好以石英 板為佳。在處理室2中,晶圓3乃放置於一承載裝置6上。 其中圖中未圖示出之有處理氣體之進氣友排放裝置,藉此乃 產生處理程序中適當之大氣環境。 位於處理室2之上方及/或下方分別裝設有加熱裝置, 卜紙張尺度適用中國國家標準(CNS)A4規格(21〇 X 297公釐) -1Π . lfll — ΊΙΙΊ — t _ I ---1 (請先閱讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 1283445Q 1283445 A7 V. INSTRUCTIONS (6·) DEVICE. The cooling device preferably has a cooling gas or a cooling fluid. According to a preferred embodiment of the invention, the light gauge is a pyrometer. Preferably, the substrate is a plated semiconductor wafer, especially a material having a = and/or Ti Lin treatment. In order to avoid the need to additionally produce a penetration rate in the case of mosquito emissivity, it is preferable to have a recording rate which is almost negligible. The substrate preferably has a transmittance of less than 〇15. In a further embodiment of the invention, it is provided with a second light measuring device facing the substrate, preferably in such a way as to enable measurement of the transmittance in order to accurately measure the emissivity of the substrate. In the embodiment of the present invention, the second light-emitting measuring device can measure light rays exceeding a predetermined wavelength, so that the unlineed and sensitive lines can be measured. At the same time, the second radiation measuring device preferably measures light rays which are slightly lower or slightly higher than the predetermined wavelength so that the substrate penetration rate which is absorbed by the implantation method, especially the linear implantation method, can be calculated. In the present invention, it is particularly suitable for the bulb of the heating lamp to have a filtering function, in which the second transducer is oriented toward the second reading source. But the sewer board is read and used to measure the miscellaneous in 2 waves. This allows the penetration rate to be measured by the radiation of the substrate and the radiation through the substrate. The basic task of this month is solved by heat-treating the substrate method, especially the semi-conductor=circle in the following program steps, that is, at least the first and second light-emitting, the substrate, the absorption between the first light source and the substrate The first light shot between::疋 wavelength' is measured by the light-emitting measuring device. The Lebo, which is radiated by the substrate at the pre-wavelength, is the same as the source------ ^---^---^ -------I ------- (Please read the notes on the back and fill out this page) -Q_ 1283445 A7 Figure 1 1^3 Figure 1 Three figures, four figures, five five, invention description (the side of the direction of the 'hetero (four) two light-radiation 帛 two radiation, and the second __ radiation of the second radiation. Measured by the above method The device mentioned by the fan will achieve the desired advantages, that is, by absorbing the predetermined wavelength of the first light ray to improve the addition and subtraction _ background_light relationship relationship, and at the same time, the second radiation can be confirmed by the paste. The present invention will be further illustrated by the following description of preferred embodiments of the invention. The contents of the drawings are as follows: A schematic cross-sectional view of the rapid heating device shown in the example, a schematic cross-sectional view of the rapid heating device according to the second embodiment of the present invention; a graphical representation of the relationship between the transmittance and the reflectance of a particular wafer; Temperature profile of the wafer heat treatment of the plating process; illustration of the transmittance measurement by the control measurement range according to an embodiment of the present invention. The present invention will be further illustrated by the preferred embodiments of the invention. A cross-sectional view of a rapid heating system 1 is shown, which is based on the first embodiment of the present invention to rapidly heat a semiconductor wafer. A processing chamber 2 of a half-guided Bean Bean 3 is placed inside, which is located above The transparent plate 4 and a transparent plate 5 located below are formed, wherein the transparent plate is preferably made of a quartz plate. In the processing chamber 2, the wafer 3 is placed on a carrying device 6. Illustrated is a gas-filled friend discharge device for processing gas, thereby generating an appropriate atmosphere in the processing procedure. Heating devices are disposed above and/or below the processing chamber 2, respectively. The paper scale applies to the Chinese National Standard (CNS) A4 specification (21〇X 297 mm) -1Π. lfll — ΊΙΙΊ — t _ I ---1 (Please read the note on the back and fill out this page) Ministry of Economics Intellectual Property Bureau employee consumption cooperative printed 1283445
it-------:---裝 (請先閲讀背面之注意事項再填寫本頁) ’八尤、裝置乃以長條燈管7及8裝設。其中透明板4及5 =刀抓於卵UJ 3與長條燈管7及8之間,因為有透明隔絕 =效果’藉此可以建立—糊之處理室。整個裝置外面乃 由一爐室9所_,該爐室乃構成處理室2之側壁,並且其 土 I至V部份有反射功效。長條燈管7及8乃分別由許多彼 此平仃裝設之長條狀鎢-齒素们〇及η所組成。當然也可 使用其他燈,例如點紐。由燈耻射之電磁輻射線來對晶 圓3進行加熱。根據圖一之實施形式中,位於上方長條燈管 7《加熱燈1G,其贼將料成可吸收就波長之燈管輕射 線。在本發明較佳之實彡式中,燈泡乃由含氫氧元素之石 英玻璃所製成,並且可吸收介於2.6μπι至2·8μιη之波長。 藉此便可以讓上方長條燈管所放射之輻射線,在波長範圍介 於2.6μπι至2·8μπι產生光譜缺口。而對於位於下方長條燈 管8之加熱燈11燈泡而言,加熱燈電磁波之整個光譜範圍 基本上都疋可穿透的,因而整個光譜範圍之輻射線將會照射 在處理室2之晶圓3上。 經濟部智慧財產局員工消費合作社印製 该位於下方長條燈管之加熱燈Η,其輻射線乃透過圖 中未示出之一調整單元進行調整,而且該調整單元乃透過一 預定之參數來進行調整;該設計方式例如在上述專利案 DE-A_199 05 524中已為習知,本發明乃沿用該專利案之調 整技術’為了避免重覆,在此不再累述。 用於測量晶圓溫度之溫度測量裝置乃為一高溫計13, 其裝設在下方長條燈管之侧邊並朝向晶圓之下方長條燈管 8之侧邊裝設。該高溫計13之測量範圍乃包括有上方長條 本紙張尺度適用中國國家標準(CNS)A4規格(21〇 X 297公釐) -11 - 1283445 A7 五、發明說明(9·) ^管之補線之《光譜缺口鋼。例如高溫計i3可以測 t長為2·7μιη之輕射線。因此,高溫計13基本上只能測 2晶圓:所放射之輻射線,或由下核條燈管8之未經滤 μ理,第τ加熱燈11所放射而再由晶圓所反射回來之輻 、、’右對第一加熱燈11所放射之輻射線進行調整作業, 則可赠未經調整之晶圓所放射之輕射線與由晶圓所反射 讀管輻射線區分開來。下方長條燈管8之恤絲之加鼽 燈U之輕射線經調整後,可落在高溫計之測量範圍内,亦 即在晶圓輻射線之旁側,並與其區分開來,因此相對於一般 習知之系統,其上方長條燈管之輕射波長也落在高溫計之測 量波長範㈣,織計核可以纽餘之傭訊號_背景-輻射關係狀況。 、、在朝向晶I®方向設置之高溫計13之侧邊,裝設有一所 紅燈源高溫計,其裝設方向乃朝向下方長條燈管8之未經 滤光及調整之至少-加倾u,以便可確認雜線之強 度。由該直接測得之加熱燈U之輕射強度,及由該第二加 熱燈11所放射,再由晶圓3反射而經高溫計13所測得之輻 射強度,該輕射強度因經晶圓輕射調整之故,所以可以區別 而得知,藉此將彳進-步測得晶圓之反射率。藉此反射率可 以推斷晶圓之放射率,晶圓之放射率在決定晶圓溫度上十分 重要,因為僅由所測得之晶圓輕射線而無放射率之資料並無 法計算推斷晶圓之溫度。 、另-項決定放射率之因素為穿透率,亦即晶圓在所測得 之波長細$之穿透程度。-般半導體晶目之穿透率通常很 本紙張尺度適用中國國家標準(CNS)A4規格(½ X 297公爱)' -Γ . C請先聞讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 1283445It-------:---Installation (please read the notes on the back and fill out this page) ‘Beau, the installation is installed with long strips 7 and 8. Among them, the transparent plates 4 and 5 = the knife is caught between the egg UJ 3 and the long tubes 7 and 8, because of the transparent isolation = effect ' thereby establishing a paste processing chamber. The outside of the entire apparatus is made up of a furnace chamber 9 which constitutes the side wall of the processing chamber 2 and has a reflective effect on the soil I to V portions. The long strips 7 and 8 are respectively composed of a plurality of strip-shaped tungsten-teeth elements and η which are mounted on the flat side. Of course, other lights, such as dots, can also be used. The crystal 3 is heated by the electromagnetic radiation of the lamp. According to the embodiment of Fig. 1, in the upper strip lamp 7 "heating lamp 1G, the thief will be made into a light pipe that can absorb the wavelength of the lamp. In a preferred embodiment of the invention, the bulb is made of quartz glass containing hydrogen and oxygen and absorbs wavelengths between 2.6 μm and 2·8 μm. Thereby, the radiation emitted by the upper long tube can be made to generate a spectral gap in the wavelength range from 2.6 μm to 2·8 μm. For the heat lamp 11 bulb located in the lower strip lamp 8, the entire spectral range of the electromagnetic wave of the heater lamp is substantially permeable, so that the radiation of the entire spectral range will be irradiated to the wafer of the processing chamber 2. 3 on. The Ministry of Economic Affairs' Intellectual Property Office staff consumption cooperative prints the heating lamp 位于 located in the lower strip of light. The radiation is adjusted by an adjustment unit not shown in the figure, and the adjustment unit is passed through a predetermined parameter. Adjustments are made; this design is known, for example, from the above-mentioned patent application DE-A_199 05 524, which is based on the adjustment technique of the patent 'in order to avoid repetition, and will not be repeated here. The temperature measuring device for measuring the temperature of the wafer is a pyrometer 13, which is mounted on the side of the lower long tube and is mounted toward the side of the long strip 8 below the wafer. The measurement range of the pyrometer 13 includes the above-mentioned long strip paper scale applicable to the Chinese National Standard (CNS) A4 specification (21〇X 297 mm) -11 - 1283445 A7 V. Invention description (9·) ^ Line of Spectral Gap Steel. For example, the pyrometer i3 can measure light rays with a length of 2·7 μm. Therefore, the pyrometer 13 can basically only measure 2 wafers: the radiated radiation, or the unfiltered light of the lower nuclear strip lamp 8, and the τ heating lamp 11 radiates and is reflected by the wafer. The radiation of the radiation emitted by the first heating lamp 11 is adjusted to the right, and the light beam emitted by the unadjusted wafer is distinguished from the radiation of the reading tube reflected by the wafer. The light beam of the twisted lamp U of the lower strip lamp 8 is adjusted to fall within the measurement range of the pyrometer, that is, on the side of the wafer radiation, and is distinguished from it, so In the conventional system, the light-emitting wavelength of the long strip lamp above it also falls on the measuring wavelength range of the pyrometer (4), and the weaving core can be the servant signal_background-radiation relationship of the surplus. a red light source pyrometer is disposed on the side of the pyrometer 13 disposed toward the crystal I® direction, and the installation direction is toward the lower long light tube 8 without filtering and adjusting at least - plus Pour u to confirm the strength of the miscellaneous wire. The light intensity of the directly measured heating lamp U, and the radiation intensity emitted by the second heating lamp 11 and reflected by the wafer 3 and measured by the pyrometer 13, the light intensity due to the crystal The round light adjustment is so different that it can be distinguished, and the reflectivity of the wafer will be measured by the step-by-step method. The reflectivity can be used to infer the emissivity of the wafer. The emissivity of the wafer is very important in determining the wafer temperature, because the data of the measured wafer light ray and no emissivity can not calculate the inferred wafer. temperature. The other factor that determines the emissivity is the penetration rate, which is the penetration of the wafer at the measured wavelength. - The transmittance of the semiconductor crystal is usually very high. This paper size applies to the Chinese National Standard (CNS) A4 specification (1⁄2 X 297 public)' -Γ . C Please read the notes on the back and fill in this page. Intellectual Property Bureau employee consumption cooperative printed 1283445
、發明說明(10·) 氏,例如像南度摻雜金屬層之晶圓,基本上在計算過程中可 被忽略,所以通常不必另外確定其透率。但也可以讓放射 率維持一定值(放射率=1 _穿透率_反射率),如此便可以 十分精確地僅由反射率之測量值來計算出反射率。 此外,晶圓之穿透率也可以其他方式測量。針對該目 的’也可另外增設-圖中未示出之第二高溫計,該高溫計例 i可朝向與下方長條燈料目反之晶圓面裝設,並且也測量在 波長2·7μιη範圍之輻射線。因為上方長條燈管之燈泡有濾光 功此’所以不會測量到該波長範圍内之輻射線,基本上除了 晶圓本身之輻射線,也只有下方長條燈管之未經就處理之 ^熱k 11之射線會穿透過晶圓,而被該高溫計接收測 I。但由於該輕射線如上所述已進行過調整處理,所以基本 上可以使其與晶圓輕射線區分開來。又因為下方長條燈管8 <未經濾光處理之加紐11之触線強度已為習知,所以 可以藉此決定晶圓之穿透率。 · 當然下方長紐管8之H絲處理之&熱燈u所放 射之-小雜鱗線’也可能㈣次反麟錄室之反射壁 牆而被晶®上歉高溫制量。但是鋪射量基本上不大, 而可以略不計’或者也可在_之妓鮮測量作業就將 其考慮進來校正。 ,根據反射率及穿透率之資訊,可以精確得知晶圓3之放 射率。在得知由高溫計13或由圖巾辆出之上方高溫計所 測得之晶®放射讀值之後,可_常精準地測得晶圓之溫 度。由於晶圓輻射線與加熱燈輻射線之間之輻射訊號-背景- 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -η. (請先閲讀背面之注意事項- Φ 項再填 · I I 1 I I I I ^ — — — — · 窝本頁) 經濟部智慧財產局員工消費合作社印製 1283445 經濟部智慧財產局員工消費合作社印製 A7 五、發明說明(11·) 輕射關係狀況,藉由設計模式有了十分良好之改善,因而即 使在晶圓3溫度偏低,亦即晶圓溫度較低時,該方法也同樣 適用。 根據該習知之溫度,方可適當地調節加熱裝置。在此所 採行本發明較佳之實施形式中,僅應用上方長條燈管7之經 濾光處理之加熱燈10來進行溫度調節作業,且在必要時也 可連同運用下方長條燈管8之經遽光處理之加熱燈來進行 溫度_作業。下核紐管8之未域光處理之加熱燈 11將保持在一定值或調整至一預定數值。藉此可以避免加 熱:k輕射鈿度有突躍昇高之狀況,此加熱燈輕射線使用於晶 圓反射率及穿透率測量。用於反射率及穿透率測量之加熱燈 輻射線基本上應維持一定值,如此將可以較精準地確定晶圓 溫度。 ^ 圖二顯示一根據本發明之另一實施形式之快速加熱裝 置。居快速加熱裝置乃由一外室2〇所組成,其橫切面可以 疋任意幾合圖形之金屬室或鋼質室。該外室亦可以是角狀或 圓形。室内牆最好採用一高反光層,可以部份或完全反光。 該室壁牆上裝設有一小型開口 21,以利待測量之輻射線由 皇内部照射出來。通過該開口,待測量之輕射線會直接射在 位於後方,且圖中未示出之輻射測量裝置,最好採用高溫 计,或經過一導引裝置’例如光纖,將其導向該測量裝置。 为力彳在A封蓋及室底部之内邵或在其上側,裝設有上方 長條燈管27及下方長條燈管28形式之加熱裝置。最好裝設 同樣可放射可見光之長條燈管27、28及加熱燈29、30。尤 — — Ί — ---装-------丨訂--------- (請先閱讀背面之注意事項再填寫本頁)Description of the Invention (10·), for example, a wafer like a south doped metal layer is basically negligible during the calculation, so it is usually not necessary to additionally determine its transmittance. However, it is also possible to maintain the emissivity at a certain value (emissivity = 1 _ transmittance _ reflectance), so that the reflectance can be calculated very accurately only from the measured value of the reflectance. In addition, the transmittance of the wafer can also be measured in other ways. For this purpose, a second pyrometer, not shown, may be additionally provided. The pyrometer example i may be mounted toward the bottom of the strip and opposite to the wafer surface, and also measured at a wavelength of 2·7 μηη. Radiation. Because the bulb of the upper strip lamp has a filtering function, the radiation in the wavelength range will not be measured. Basically, except for the radiation of the wafer itself, only the lower strip tube is not processed. ^The heat k 11 rays will penetrate the wafer and be measured by the pyrometer. However, since the light beam has been subjected to the adjustment process as described above, it can be substantially distinguished from the wafer light beam. Moreover, since the intensity of the contact line of the underlying strip 8 <unfiltered button 11 is already known, the transmittance of the wafer can be determined by this. · Of course, the H-wire treatment of the lower long tube 8 and the small-scale scaly line that is emitted by the heat lamp u may also be a high-temperature production by the Crystal®. However, the amount of paving is basically not large, but it can be ignored or it can be taken into account in the fresh measuring operation. According to the information of the reflectance and the transmittance, the transmittance of the wafer 3 can be accurately known. The temperature of the wafer can be accurately measured after knowing the crystallographic readings measured by the pyrometer 13 or by the upper pyrometer. Radiation signal between the radiation of the wafer and the radiation of the heater lamp - Background - This paper scale applies to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) - η. (Please read the notes on the back - Φ Refilling · II 1 IIII ^ — — — — · 窝 ) ) ) ) ) 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 834 The situation is very well improved by the design pattern, so the method is equally applicable even when the temperature of the wafer 3 is low, that is, when the wafer temperature is low. The heating device can be appropriately adjusted according to the conventional temperature. In the preferred embodiment of the invention, only the filter-heated heating lamp 10 of the upper strip lamp 7 is used for the temperature adjustment operation, and if necessary, the lower strip lamp 8 can be used together. The temperature-working is performed by a calendering heat lamp. The heat lamp 11 of the lower nucleus tube 8 which is not field light treated will remain at a certain value or be adjusted to a predetermined value. In this way, heating can be avoided: a slight increase in the lightness of the k-light, which is used for the measurement of the crystal reflectance and the transmittance. The heater lamp used for reflectance and transmittance measurement should be maintained at a certain value so that the wafer temperature can be determined more accurately. Figure 2 shows a rapid heating device in accordance with another embodiment of the present invention. The rapid heating device consists of an outer chamber 2〇, and its cross section can be used for any metal or steel chamber. The outer chamber can also be angular or circular. The interior wall preferably uses a highly reflective layer that can be partially or completely reflective. A small opening 21 is mounted on the wall of the chamber to allow the radiation to be measured to be illuminated by the interior of the emperor. Through the opening, the light rays to be measured are directly incident on the rear, and the radiation measuring device not shown in the figure is preferably guided by a pyrometer or via a guiding device such as an optical fiber. In order to force the inside of the A cover and the bottom of the chamber or on the upper side thereof, a heating device in the form of an upper long tube 27 and a lower long tube 28 is installed. It is preferable to install the long tubes 27, 28 and the heating lamps 29, 30 which are also capable of radiating visible light.尤— Ί — ---装-------丨定--------- (Please read the notes on the back and fill out this page)
1283445 A7 B7 五、發明說明(l2·) (請先«讀背面之注意事項再填寫本頁) 其是長條燈管分別包含有多個鎢-鹵素燈29、30作為加熱燈 之用。與第一實施例不同的是,加熱燈29、30之所有燈泡 之組成物質對加熱燈之整個光譜輻射線,基本上均可穿透。 同時其燈形可以是桿狀或任意安裝之點狀加熱燈。下方長條 燈管28可以採用桿狀加熱燈,而上方長條燈管27採用點狀 加熱燈裝設,或以相反方式裝設。長條燈管27、28也可以 都採用相同之加熱燈形式裝設。在長條燈管27、28都採用 相同之桿狀加熱燈裝設之狀況下,則其裝設方式可以是兩桿 狀加熱燈27、28彼此上下平行裝設,或上下彼此交錯裝設, 若是兩桿狀燈管27、28彼此以上下交錯之方式裝設,則最 好是以正交直角方式裝設。 在長條燈管27及28之間裝設有一待處理之基板33, 該基板最好係由矽組成之圓盤狀半導體晶圓。該晶圓33可 以是未鍍層或已鍍層及/或未經植入作業處理之基板。但基 本上取好採用已鍍層之晶圓。其中最好採用鐘有C〇或η, 或者鍵有兩者混合鍍層之晶圓,因為如此可使其穿透係數 (穿透率)在溫度為350°C時小於0.15。該圓盤狀晶圓33之頂 面35及底面36乃分別以與長條燈管27及28平行之方式裝 i 設。 部 | 位於上方長條燈管27與晶圓33之頂面35之間裝設有 | 一板狀透明隔絕體38。以同樣方式位於基板33之底面% 異 與下方長條燈管28之間也裝設有—透明隔絕體39。該隔絕 | 體38及39橫跨過整個室20,以至於將該室2〇之内部空間 | .分隔成二份。尤其是放置有基板33之室2〇内部,為被隔絕 ί 本紙張尺度適用中國國家標準(CNS)A4規格(21G X 297公釐)'------- -15-1283445 A7 B7 V. INSTRUCTIONS (l2·) (Please read the note on the back and fill out this page.) It is a long lamp that contains a plurality of tungsten-halogen lamps 29 and 30 as heating lamps. In contrast to the first embodiment, the constituent materials of all of the bulbs of the heating lamps 29, 30 are substantially transparent to the entire spectral radiation of the heating lamp. At the same time, the lamp shape can be a rod-shaped or arbitrarily mounted point heating lamp. The lower strip lamp 28 can be a rod-shaped heater lamp, and the upper strip tube 27 is mounted by a spot heating lamp or in the opposite manner. The long tubes 27, 28 can also be mounted in the same heating lamp. In the case where the long tube lamps 27 and 28 are all mounted by the same rod-shaped heating lamp, the mounting manner may be that the two rod-shaped heating lamps 27 and 28 are installed in parallel with each other, or are staggered with each other. If the two rod-shaped tubes 27 and 28 are arranged to be interlaced with each other, it is preferable to mount them in an orthogonal right angle manner. A substrate 33 to be processed is disposed between the long tubes 27 and 28, and the substrate is preferably a disk-shaped semiconductor wafer composed of tantalum. The wafer 33 can be an unplated or plated and/or substrate that has not been implanted. However, it is basically preferable to use a coated wafer. Among them, it is preferable to use a wafer having a C 〇 or η, or a combination of the two, because the penetration coefficient (penetration) is less than 0.15 at a temperature of 350 °C. The top surface 35 and the bottom surface 36 of the disc-shaped wafer 33 are mounted in parallel with the elongated tubes 27 and 28, respectively. A plate-shaped transparent insulator 38 is disposed between the upper strip tube 27 and the top surface 35 of the wafer 33. In the same manner, a transparent insulating body 39 is also disposed between the bottom surface of the substrate 33 and the lower long light tube 28. The insulation | body 38 and 39 spans the entire chamber 20 such that the interior space of the chamber 2 is divided into two. In particular, the inside of the chamber 2 where the substrate 33 is placed is isolated. ί This paper scale applies the Chinese National Standard (CNS) A4 specification (21G X 297 mm)'------- -15-
1283445 五、發明說明(13·) 體38及39.所分隔之處理室42。在處理室幻内部將可建立 -適合於處轉敎高壓或紐處輯境,其巾可能包括有 部份之刺激氣體,如此隔絕方式將可避免其干擾或污染長條 燈管27及28之加熱燈29、30或室2〇有反光功能之内牆^ 相應於此必須另外裝設進氣口及氣體排放口,此兩者在圖二 中並未示出。 ~ 上方隔絕體38乃用於吸收預定波長或由上方長條燈管 27所放射之加熱輻射裝置之光譜波長範圍,基板33頂面將 可藉此加熱輕射裝置加熱,該加熱輕射裝置具有圭少一光譜 波長缺口。可藉由相應之濾光器,其為鍍有一或多鍍層之隔 絕體38,或者一或多個濾光薄膜來達成該吸收效果,該濾 光薄膜乃附在透光基質,亦即透光板上。該透光基質最好採 用石英玻璃。 若採用濾光薄膜之設計模式,該薄膜基本上不一定需要 附著在透光板上或是直接與該透光板接觸。濾光薄膜也可以 與透光板保持一定之空間距離,且甚至可將其安置在更靠近 上方長條燈管27之位置上,做為透明板。在下列敘述中, 將僅以「隔絕體38」來統稱該分開裝設之濾光薄膜及透光 板。 透過該鍍層及薄膜之設計,將可以阻隔加熱輻射裝置預 足之光波長範圍。在此乃指一或多個波長區間及/或離散 之單一波長。 圖二所示之本發明較佳之實施形式中,板狀之透明隔絕 體38乃由含有氫氧元素之石英玻璃所製成。該類石英玻璃 τ _家標準(CNS)A4規格⑽χ挪公楚)1283445 V. INSTRUCTIONS (13·) The processing chambers 42 separated by bodies 38 and 39. In the interior of the processing room, it will be established - suitable for switching to high pressure or new location, the towel may include part of the stimulating gas, so that it can avoid interference or pollute the long tubes 27 and 28 The inner wall of the heating lamp 29, 30 or the chamber 2 has a reflective function. Accordingly, the air inlet and the gas discharge port must be separately provided, which are not shown in FIG. The upper insulating body 38 is for absorbing a spectral wavelength range of a predetermined wavelength or a heating radiation device radiated by the upper elongated tube 27, and the top surface of the substrate 33 can be heated by the heating light-emitting device, the heating light-emitting device having Gui Shaoyi has a spectral wavelength gap. The absorption effect can be achieved by a corresponding filter, which is an insulator 38 plated with one or more plating layers, or one or more filter films, which are attached to the light-transmitting substrate, that is, light-transmitting. On the board. The light-transmitting substrate is preferably quartz glass. If the design mode of the filter film is adopted, the film does not necessarily need to be attached to the light-transmitting plate or directly contact the light-transmitting plate. The filter film can also maintain a certain spatial distance from the light-transmitting plate, and can even be placed closer to the upper long tube 27 as a transparent plate. In the following description, the separately disposed filter film and light-transmitting plate will be collectively referred to only as "insulator 38". Through the design of the coating and the film, it is possible to block the wavelength range of light that is preheated by the heating radiation device. This refers to one or more wavelength intervals and/or discrete single wavelengths. In the preferred embodiment of the invention illustrated in Figure 2, the plate-shaped transparent insulator 38 is made of quartz glass containing hydroxide elements. This type of quartz glass τ _ home standard (CNS) A4 specifications (10) χ 公 公 Chu)
It-----Ί — lill^w ^ ill----訂-----――丨 (請先閲讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 -16- 1283445 Α7 Β7 五、發明說明(14· > 之特性在於可以吸收介於2·6μιη至2·8μπι之波長範圍之紅 外線,藉此可使加熱輻射裝置之波長光譜中形成一缺口。而 石英板之鍍層及濾光薄膜之固定作業過程中可能出現許多 困難,也可藉由採用該含有氫氧元素之石英板來避免。 因為吸收了部份加熱輻射線,隔絕體38之溫度將會增 高,所以也必須對其進行冷卻作業,否則高溫隔絕體邛本 身也將會放射熱輻射線,這將影響基板33原本預期之溫度 變化曲線。 & 為了冷卻隔絕體38及有需要時冷卻隔絕體39,需另外 裝$又一冷卻氣脂:,經由途一隔絕體而向外流至處理室42之 外部。當然也可以藉由裝設在隔絕體38、39内之冷卻管路 來讓冷卻氣體在其間流通而進行冷卻作業。在此類情況下, 亦可使用冷卻流體,例如油來進行冷卻。若隔絕體38乃例 如由一透光板及與其分開裝設之一或多個濾光薄膜所組 成’則冷卻媒介也可流動於薄膜及透光板之間。 經濟部智慧財產局員工消費合作社印製 由長條燈T 27所產生之預定波長之部份熱輕射線會被 隔絕體38阻絕,相對地,這些波長對下方隔絕體%而言則 是透明的。最好採用一般石英玻璃所製成之薄板。 在裝置運作之過程中,上方長條燈管27將放射熱輕射 線,藉此可將晶目33加熱至一預定溫度。該加熱輕射線乃 由不同波長之光稍城。在圖二巾顯示該加鋪射線兩種 不同波長之練行㈣線,射光線44‘絲為2加 之光線,光線45則表π波長為2·3μ:ηι之光線。 波長為2·7μΐΏ之光線可藉由含有氫氧元素之石英板所 1283445 五、發明說明(15. 38吸收’亦即光線44無法穿透隔絕體犯, 收阻絕。相反地,光線45之波姻不在隔絕體38 ^㈣内’所以可以毫無阻礙地穿透過去。根據圖示說 明’先線也確實穿透下方之隔絕體%,且反射至外室2〇之 反光内壁上,再-对透過隔絕體%而打在晶圓%上。因 33本妓高反雜,所以对—小部份之光線μ 曰在曰曰圓33上被吸收’其餘大部份則被反射。這也是為什 麼加熱輕射線會有如此高密度輕射線之其中一個原因。如圖 所了 H有多次反射發生,每一次反射都會有部份光線會被 阳圓吸收。最後光線45抵達室2〇内之開口 2卜而到達輕 射測量器。 下^健管28之加鍊3。,其絲應料成比上方 長條k笞27之加^^燈29之輕射弱。此外再將加教惨3〇之 ,線進行些微驗。長舰管28之輻航譜最好與長條 =27之無射光蹲相同。長條燈管28經調整之轉射線可以 毫無阻礙地穿透隔絕體39。同樣地,其中包括有一波長為 之光線49,及波長為2 3μιη之絲48。兩種光線均 可無阻礙地穿透隔絕體39,其中大部份乃由基板%反射, 而打在外室20内之開口 21上。 高溫之晶圓33也同樣放射輕射線。在圖二中,晶圓輻 射線乃由虛線表示,其中光線W表示波長為2加之光線, 光線52則表示波長為2·3μχη之光線。 ,他在圖二中可看出波長為2.3_及2 7μπι時,高溫計所 測得之輻射訊號-背景-輻射關係狀況。波長為2 7哗時所測 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱〉 -18 閲 訂 秦 1283445 Α7 Β7 經濟部智慧財產局員工消費合作社印製 五、發明說明(I6·) 得之輕射訊號·背景·輕射關係狀況應比波長為2·3μη1時所測 得之輻射訊號-背景-輻射關係狀況為佳,因為大部份之波長 轉射線係由Jl方長條燈管之祕絲職生,軸晶圓所放 射之該波長之輻射線則不易區分得出。 決定晶圓之溫度過程中,乃採用高溫計來測量波長為 2.7μπι之輻射線。在該波長可得到良好之介於晶圓輕射線及 晶圓反射輻射線之間之輻射訊號-背景_輕射關係狀況,因為 僅有下方絲燈管28產生該預定波長之縣線可被高溫計 所測得。在下核鎌緣調整處理之加熱贿射線之狀況 下’可以讓日日日®輻鱗解地透過±述方式與日%gJ反射輕射 線分,。下方長條燈管之加熱燈輻射線強度將如上所述,藉 由-局溫計或以其他方式得知,例如也可藉由測量由加熱燈 所消耗之電量來計算。再度以上述方式得知晶圓之反射^ 進而求得其放解。根據該放辨及晶_雜可以再 得知晶圓溫度。 /尤其是在製歧處理鍍有^或^騎之晶圓過程中, 採用本發’親之方式係十分助。目為a%為一良 好之電導體’㈣圓經f進行Cq之鍍層作業及加熱作 以便可以產生〇)Si2之電導效果。而產生CQSi2之過程必須 在溫度介於4GGt至5GGX之隨t ’脚_溫度之設定 也必須可在溫度低於wc之狀況下侧其溫度。 在二述之發明巾騎糊祕的—些特性。其中包括立 表面之高反射率。如圖三所示,鍍有c。之晶圓穿透率非常 低而且基本上為定值’所料f $外進行·確認作業 本紙張尺度剌中_緖準(CNS)A4規格--------- I:----ΗΙΙ1ΙΦ Μ • 1 I _ϋ n IV «I n 訂--------- φ (請先閲讀背面之注意事項再填寫本頁) -1Q - 濟 部 智 慧 財 產 局 消 費 合 作 社 印 製 1283445 五、發明說明(1*7·〉 11 ,目讀率相反射率之函數方式表示。尤其虛線 Z表示放射率錢值時之曲線。由左至右遞減,因料透 =反射率及放射率之總合在任何時間點都是卜在該曲線 八、不同晶圓在不同穿透率之穿透量乃標示出在圖塊中: =別為未崎之♦晶圓、已鍍層之晶圓及鐘有姑之晶圓。未 度層晶圓之穿透量明顯地大於0.15,而已鐘層之晶圓與鍍有 錄之卵圓,財透量卿顯地小於G15。鍍有狀晶圓乃特 別適合於战本發明之溫度_,目為不需糾進行反射率 之測量確認作業。 。在圖四巾,鍍杨之晶κ之溫度賴曲線乃藉由任意時 1匡間示出其中遠晶圓乃在一快速加 ”式進行處理作業。溫度昇高謹。c後, 溫狀態維持-段時間,接著再降溫。該溫度變化曲線乃一方 面由一直接與晶圓接觸之溫度計追縱(如曲線Α),而另一方 面也藉由另一高溫計進行測量作業(如曲線8),同時進行上 述(處理方式。明顯地發現,由高溫計所測得之溫度變化曲 線與由溫度制得之溫度變化曲線性極高。兩溫度變化 曲線幾近重疊一致,尤其是在溫度低於3〇(rc<狀況下。開 始時,高溫計雖有輕微之起伏,但在加熱程序開始後,該輕 微之起伏狀況便會消失,兩溫度變化曲線便重疊一致。高溫 計所測得之溫度變化曲線在冷卻過程中會出現有一短暫之 咼學值’該高學值乃為加熱燈測試之結果。 實際運作上,也有穿透率大於0.15之晶圓,例如像是 圖二中之未鍵層之校準晶圓。因為穿透率、放射率及反射率 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) -70- — ΓΙ—ι,^,ΙΙΊ — — I — 1 —· I 着 1 1 I I 1 II (請先閲讀背面之注意事項再填寫本頁)It-----Ί- lill^w ^ ill----book------丨 (please read the notes on the back and fill out this page) Printed by the Intellectual Property Office of the Intellectual Property Office of the Ministry of Economic Affairs - 16- 1283445 Α7 Β7 V. Description of the Invention (14· > It is characterized in that infrared rays in a wavelength range of from 2. 6 μm to 2·8 μm can be absorbed, whereby a gap can be formed in the wavelength spectrum of the heating radiation device. There may be many difficulties in the fixing operation of the quartz plate coating and the filter film, and it can also be avoided by using the quartz plate containing the hydrogen and oxygen element. Because part of the heating radiation is absorbed, the temperature of the insulator 38 will be Increased, so it must also be cooled, otherwise the high temperature insulation body itself will also radiate heat radiation, which will affect the expected temperature curve of the substrate 33. & Cooling insulation for cooling the insulation 38 and if necessary The body 39 needs to be additionally charged with another cooling grease: it flows outward to the outside of the processing chamber 42 via an insulator. Of course, it can also be cooled by the cooling pipelines installed in the insulators 38, 39. Gas in between Cooling operation is carried out in this case. In such cases, a cooling fluid, such as oil, may also be used for cooling. If the insulating body 38 is composed, for example, of a light-transmitting plate and one or more filter films separately provided therefrom 'The cooling medium can also flow between the film and the light-transmissive plate. The Ministry of Economic Intelligence's Intellectual Property Bureau employee consumption cooperative prints a part of the predetermined light wavelength generated by the long strip light T 27, which is blocked by the body 38. In contrast, these wavelengths are transparent to the lower % of the insulator. It is preferable to use a thin plate made of ordinary quartz glass. During the operation of the device, the upper long tube 27 will emit heat and light rays. The crystallite 33 can be heated to a predetermined temperature. The heated light ray is slightly different from the light of different wavelengths. In Figure 2, the towel shows two different wavelengths of the practice line (four) line, and the light ray 44' is 2 In addition to the light, the light 45 is π wavelength of 2·3μ: ηι. The light with a wavelength of 2·7μΐΏ can be obtained by a quartz plate containing hydrogen and oxygen elements 1283445 V. Description of the invention (15. 38 absorption 'that is, light 44 can not penetrate On the contrary, the wave of light 45 is not in the body of the body 38 ^ (four) 'so can penetrate the past without any hindrance. According to the illustration, the 'first line does penetrate the % of the insulator below, And reflected to the reflective inner wall of the outer chamber 2〇, and then hit the wafer % by the penetration of the insulator. Because 33 is high, it is a small part of the light μ 曰 in the circle 33 The upper part is absorbed. The rest is reflected. This is one of the reasons why there is such a high-density light beam when heating light rays. As shown in the figure, H has multiple reflections, and each reflection will have some light. It is absorbed by the sun circle. The last light 45 reaches the opening 2 in the chamber 2 and reaches the light gauge. Add the chain 3 of the lower tube 28 . The wire should be made to be lighter than the upper strip k笞27 plus ^^ lamp 29. In addition, the teachings will be miserable, and the line will be micro-tested. The aeronautical spectrum of the long hull tube 28 is preferably the same as that of the long strip = 27. The adjusted beam of light from the elongated tube 28 can penetrate the insulator 39 without hindrance. Similarly, it includes a light beam 49 having a wavelength and a filament 48 having a wavelength of 23 μm. Both types of light penetrate the insulator 39 unimpeded, with most of it being reflected by the substrate and hitting the opening 21 in the outer chamber 20. The high temperature wafer 33 also emits light rays. In Fig. 2, the wafer radiation is indicated by a broken line, wherein the light W represents a light having a wavelength of 2 and the light 52 represents a light having a wavelength of 2·3 μχ. In Figure 2, he can see the radiation signal-background-radiation relationship measured by the pyrometer when the wavelength is 2.3_ and 2 7μπι. The wavelength of the paper measured at the wavelength of 2 7 适用 applies to the Chinese National Standard (CNS) A4 specification (210 X 297 public 〉 -18) Read Qin 1283445 Α 7 Β 7 Ministry of Economic Affairs Intellectual Property Bureau employee consumption cooperative printing 5, invention description ( I6·) The light-light signal, background, and light-radiation relationship should be better than the measured radiation-background-radiation relationship when the wavelength is 2·3μη1, because most of the wavelengths are transmitted by the Jl side. The filament of the long tube, the radiation of the wavelength emitted by the shaft wafer is not easy to distinguish. In determining the temperature of the wafer, a pyrometer is used to measure the radiation with a wavelength of 2.7 μm. This wavelength can obtain a good radiation signal-background-light relationship between the wafer light ray and the reflected radiation of the wafer, because only the lower wire tube 28 produces the predetermined wavelength of the county line can be pyrometer Measured. Under the condition of heating the bribe ray under the adjustment of the lower core rim, it can be used to make the day and the day radiantly dissipate through the ± ray method and the day %gJ to reflect the light ray. The heating lamp of the lower strip tube Radiation intensity will be as above It can be calculated by measuring the amount of electricity consumed by the heating lamp, for example, by measuring the amount of electricity consumed by the heating lamp. The reflection of the wafer is again obtained in the above manner, and then the solution is obtained. The wafer temperature can be known by the resolution and crystal. / Especially in the process of disposing the wafer with ^ or ^ riding, it is very helpful to use the method of 'pro-family'. The target is a%. A good electrical conductor '(4) circle is subjected to Cq plating operation and heating so that the conductance effect of 〇)Si2 can be produced. The process of producing CQSi2 must be set at a temperature of 4 GGt to 5 GGX with a t _ foot _ temperature and must be at a temperature lower than wc. In the second description of the invention of the towel to ride the secret - some characteristics. This includes the high reflectivity of the facade. As shown in Figure 3, it is plated with c. The wafer penetration rate is very low and basically the value is 'followed by the f$. · Confirm the operation of the paper scale 剌 绪 绪 (CNS) A4 specification --------- I:-- --ΗΙΙ1ΙΦ Μ • 1 I _ϋ n IV «I n 订--------- φ (please read the notes on the back and fill out this page) -1Q - Jishang Intellectual Property Bureau Consumer Cooperative Printed 1283445 V. Description of the invention (1*7·〉 11), the function of the phase reflectance phase reflectance is expressed as a function. Especially the dotted line Z represents the curve of the emissivity money value. It decreases from left to right, due to the permeability = reflectivity and emissivity The sum of the points at any point in time is in the curve. 8. The penetration of different wafers at different penetration rates is indicated in the block: = Do not be the swaddle of the wafer, the coated wafer And Zhong Yougu's wafer. The penetration of un-layered wafers is significantly greater than 0.15, while the wafers of the clock layer and the plated ovals are significantly smaller than the G15. It is especially suitable for the temperature of the invention. It is not necessary to correct the reflectivity measurement and confirm the operation. In the figure four, the temperature of the yttrium-plated crystal κ is based on In the meantime, it is shown that the far-wafer is processed in a fast-adding manner. After the temperature rises, the temperature is maintained for a period of time, and then the temperature is lowered. The temperature change curve is on the one hand The thermometer directly in contact with the wafer is traced (such as curve Α), while on the other hand, the measurement operation (such as curve 8) is performed by another pyrometer, and the above (the processing method is clearly found, by the pyrometer The measured temperature change curve and the temperature change made by temperature are extremely high. The two temperature change curves are nearly identical, especially at temperatures below 3 〇 (rc< condition. At the beginning, the pyrometer is slightly The undulations, but after the heating process begins, the slight undulations will disappear and the two temperature profiles will overlap. The temperature curve measured by the pyrometer will have a short dropout value during the cooling process. The high value is the result of the heat lamp test. In practice, there are also wafers with a penetration rate greater than 0.15, such as the unbonded calibration wafer in Figure 2. Because of penetration, emissivity and reflection This paper size applies to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) -70- — ΓΙ—ι,^,ΙΙΊ — — I — 1 —· I 1 1 II 1 II (Please read the back Please fill out this page again)
1283445 發明說明(I8·) 之總合總是卜所以可以在上述方法外,另外進行晶圓之穿 透測I作業,以便與所測得之反射率—起來計算放射率及晶 圓溫度。 為了達成該目的,則必須在第一實施例中加裝另一高溫 計,且經由相應之開口裝設在室20内上方長條燈管27之上 方位置’並朝向晶圓33之方向。 在圖五中,曲線c乃顯示含錢氧元素之±方石英板4 之穿透值。可以清楚地看見,在波長介於2·7μπι至2·8μιη 义範圍内,石英板之穿透值幾近零,亦即對該波長範圍内之 輻射線而言,該石英減不可穿透。而在該波長範圍内,也 會有一些波長之輻射線會被下方輻射測量體測量而可求出 晶圓反射率,再進一步藉以測得放射率。為了確定溫度之反 射率及穿透率之間之關連性,必須嚴格地確定晶圓穿透率係 在該波長範圍内所測量。但是,卻因為上方石英板38在該 波長範圍内不透光,所以利用該波長並無法得出所要之穿透 率。 有鑑於該光線之穿透量必須在其他波長範圍内測量, 便藉此資料由外插法求得其所尋求之穿透量。基於該目的 將在上方高溫計開啟一濾光器,該濾光器之穿透量變化與波 長相關,如圖五中之曲線D所示。在石英板4不透光之波 長範圍内,該濾光器有極高之透光性。反而在較低及較高之 波長範圍内’該滤光器係不透光。 雖裝有含有氫氧元素之石英板38及濾光器,石英板38 之吸收範圍之左方及右方兩波長光譜區域中,仍有在長條燈 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) I ♦裝---------------· (請先閱讀背面之注意事項再填寫本頁) 以 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 A7 B7 J283445 五、發明說明(I9·) 管27上方之高溫計可測得之波長,藉由上述方式可將其切 斷。為了制實際轉之方式所選擇之縣財,其滤光器 曲、,泉及石英曲線涵蓋之面積範圍在石英之吸收範圍兩側相 當。 日日圓之牙透量與波長之間只會呈現極弱或近似之線性 關係’例如在圖五中〜晶圓範例中所示之穿透率曲線E,藉 此可^測量石英之吸收範圍左方之波長區域之穿透晶圓之 穿透量’同樣也可以測量石英之吸收範圍右方之波長區域之 «晶圓之穿透量。由於晶圓穿透量與波長之間只會呈現極 弱或近似之線性關係,所以可以透過一中間值或近似值得知 石英之吸收範圍内在該特定光譜波長之穿透值。透過組合進 行♦透值測量及上述晶圓反射率之測量可以精確得知放射 率,這方法在晶圓之穿透值大於〇·15之狀況下也適用。如 此便可在溫度低於4〇〇°C直到接近300°C之範圍·間進行一可 靠之溫度控制。 在上述之穿透測量方式中’下方長條燈管之加熱燈必須 .進行調整,讓上方長條燈管及下方長條燈管之加熱燈輻射線 可以彼此區分開來。在經由相應之調整並且加熱燈輻射線可 以彼此分開之狀況下,可利用一位於下方長條燈管28之下 之輕射測量器,例如一高溫計來進行輕射測量作業。根據上 述之方式’將測量到由上方長條燈管所放射並經由調整之轉 射線,並分別與下方長條燈管輻射線及晶圓輻射線區分開 來。經過多次反射後,而被高溫計所測得之輻射線可在系統 校準過程中校正,或在確定穿透率之過程中忽略不計。 國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁) 裝---—!—訂--------_ 經濟部智慧財產局員工消費合作社印製 1283445 Α7 Β7 五、發明說明(2〇·) 因為在第一實施例中,當下方長條燈管保持定值或調整 到一足之預定值時,調節晶圓溫度之上方長條燈管將進行加 熱運作,所以建議採用第一實施例來進行穿透率之測量。反 射及穿透之測量曲線基本上呈一等值或一習知之燈源輻射 強度變化。相反地,調節溫度之加熱燈,其加熱燈輻射線強 度乃變化十分迅速,以至有突增之狀況產生,這將阻礙反射 值及穿透值之測量。 雖然本發明根據較佳之實施例來做說明,但本發明並不 偈限於用在該具體之實施例。例如,用於測量加熱燈輻射線 強度之裝置也可以其他測量裝置取代,例如根據加熱燈所消 耗之電流來計算之高溫計。此外,上述之實施形式之各個特 徵可以適當方式交換或組合運用。 —•I I Ί !Ί I - I! β 看! >41^- (請先閲讀背面之注意事項再填窝本頁) 經濟部智慧財產局員工消費合作社印製 j尺 張 紙 I本 一公 197 -2 X 10 2 /IV 格 規 Α4 S) Ν (C 標 家 1283445 A7 B7 五、發明説明(22·) 45 光線 48 光線 49 光線 51 光線 52 光線 (請先聞讀背面之注意事項再填寫本頁) 經濟部智慧財產局員工消費合作社印製 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) -25-1283445 Description of the Invention (I8·) The total sum is always so that in addition to the above method, a wafer penetration test I can be performed to calculate the emissivity and the crystal temperature from the measured reflectance. In order to achieve this, it is necessary to add another pyrometer in the first embodiment and mount it in the direction above the upper elongated tube 27 in the chamber 20 via the corresponding opening and toward the wafer 33. In Fig. 5, the curve c shows the penetration value of the ± square quartz plate 4 containing the oxygen element. It can be clearly seen that in the range of wavelengths ranging from 2·7 μm to 2·8 μm, the penetration value of the quartz plate is almost zero, that is, the quartz is impenetrable for the radiation in the wavelength range. In this wavelength range, there are also some wavelengths of radiation that can be measured by the underlying radiation measuring body to determine the reflectivity of the wafer, and further to measure the emissivity. In order to determine the correlation between the reflectance of temperature and the transmittance, it is necessary to strictly determine the wafer transmittance measured in this wavelength range. However, since the upper quartz plate 38 is opaque in this wavelength range, the desired transmittance cannot be obtained by using this wavelength. In view of the fact that the amount of penetration of the light must be measured in other wavelength ranges, the data is extrapolated to find the amount of penetration sought. For this purpose, a filter is turned on in the upper pyrometer, and the change in the amount of penetration of the filter is related to the wavelength, as shown by curve D in Fig. 5. The filter has a very high light transmittance in the wavelength range in which the quartz plate 4 is opaque. Instead, the filter is opaque in the lower and higher wavelength ranges. Although it is equipped with a quartz plate 38 and a filter containing hydrogen and oxygen elements, the left and right wavelength regions of the absorption range of the quartz plate 38 are still applicable to the Chinese National Standard (CNS) in the strip light scale. A4 size (210 X 297 mm) I ♦ Pack---------------· (Please read the notes on the back and fill out this page) Printed A7 B7 J283445 V. Description of the Invention (I9·) The wavelength at which the pyrometer above the tube 27 can be measured can be cut by the above method. In order to make the actual choice of the county, the area covered by the filter, spring and quartz curve is equivalent to the absorption range of the quartz. There is only a very weak or nearly linear relationship between the tooth penetration of the Japanese yen and the wavelength 'for example, the transmittance curve E shown in the example of the wafer in the figure 5, which can be used to measure the absorption range of the quartz. The penetration of the through-wafer in the wavelength region of the square can also measure the amount of penetration of the wafer in the wavelength region to the right of the absorption range of the quartz. Since the amount of wafer penetration and the wavelength will only exhibit a very weak or nearly linear relationship, the value of the breakthrough in the absorption range of the quartz at the specific spectral wavelength can be known by an intermediate value or an approximation. The emissivity can be accurately determined by combining the ♦ fugitive measurement and the above-mentioned wafer reflectance measurement. This method is also applicable when the wafer penetration value is greater than 〇·15. Thus, a reliable temperature control can be performed between temperatures below 4 〇〇 ° C and up to approximately 300 ° C. In the above-mentioned penetration measurement mode, the heating lamp of the lower strip lamp must be adjusted so that the radiation lamps of the upper strip lamp and the lower strip lamp can be distinguished from each other. A light-emitting measuring device, such as a pyrometer, located below the underlying light tube 28, may be utilized for light-light measurement operations, with corresponding adjustments and heating lamp radiation that may be separated from one another. According to the above method, the radiation emitted from the upper long tube and adjusted by the adjustment will be measured and distinguished from the lower long tube radiation and the wafer radiation, respectively. After multiple reflections, the radiation measured by the pyrometer can be calibrated during system calibration or ignored during the determination of penetration. National Standard (CNS) A4 specification (210 X 297 mm) (Please read the note on the back and fill out this page) Pack----! —订--------_ Ministry of Economic Affairs Intellectual Property Bureau Staff Consumer Cooperative Printed 1283445 Α7 Β7 V. Invention Description (2〇·) Because in the first embodiment, when the lower strip lamp remains fixed Or, when adjusting to a predetermined value, the strip lamp above the wafer temperature will be heated, so it is recommended to use the first embodiment to measure the transmittance. The measurement curve of reflection and penetration is substantially an equivalent or a known variation of the source radiation intensity. Conversely, the temperature of the heating lamp, the intensity of the radiation of the heating lamp changes very rapidly, so that a sudden increase occurs, which will hinder the measurement of the reflection value and the penetration value. Although the present invention has been described in terms of preferred embodiments, the invention is not limited to the specific embodiments. For example, the means for measuring the intensity of the radiation of the heating lamp can also be replaced by other measuring means, such as a pyrometer calculated from the current consumed by the heating lamp. Furthermore, the various features of the above-described embodiments may be interchanged or combined in an appropriate manner. —•I I Ί !Ί I - I! β Look! >41^- (Please read the note on the back and fill in the nest page) Ministry of Economic Affairs Intellectual Property Bureau employee consumption cooperative printed j-sheet paper I this one public 197 -2 X 10 2 /IV grid rule 4 S) Ν (C Standard 1283445 A7 B7 V. Invention Description (22·) 45 Light 48 Light 49 Light 51 Light 52 Light (please read the note on the back and fill out this page) Printed by the Intellectual Property Office of the Ministry of Economic Affairs This paper scale applies to the Chinese National Standard (CNS) A4 specification (210X297 mm) -25-
Claims (1)
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TW91109849A TWI283445B (en) | 2001-05-23 | 2002-05-10 | Method and apparatus for thermally treating substrates |
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US9449858B2 (en) | 2010-08-09 | 2016-09-20 | Applied Materials, Inc. | Transparent reflector plate for rapid thermal processing chamber |
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US4891499A (en) * | 1988-09-09 | 1990-01-02 | Texas Instruments Incorporated | Method and apparatus for real-time wafer temperature uniformity control and slip-free heating in lamp heated single-wafer rapid thermal processing systems |
US5155336A (en) * | 1990-01-19 | 1992-10-13 | Applied Materials, Inc. | Rapid thermal heating apparatus and method |
US5154512A (en) * | 1990-04-10 | 1992-10-13 | Luxtron Corporation | Non-contact techniques for measuring temperature or radiation-heated objects |
EP0612862A1 (en) * | 1993-02-24 | 1994-08-31 | Applied Materials, Inc. | Measuring wafer temperatures |
US5650082A (en) * | 1993-10-29 | 1997-07-22 | Applied Materials, Inc. | Profiled substrate heating |
US5444815A (en) * | 1993-12-16 | 1995-08-22 | Texas Instruments Incorporated | Multi-zone lamp interference correction system |
DE4414391C2 (en) * | 1994-04-26 | 2001-02-01 | Steag Rtp Systems Gmbh | Method for wave vector selective pyrometry in rapid heating systems |
US5960158A (en) * | 1997-07-11 | 1999-09-28 | Ag Associates | Apparatus and method for filtering light in a thermal processing chamber |
US6310328B1 (en) * | 1998-12-10 | 2001-10-30 | Mattson Technologies, Inc. | Rapid thermal processing chamber for processing multiple wafers |
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2002
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US9449858B2 (en) | 2010-08-09 | 2016-09-20 | Applied Materials, Inc. | Transparent reflector plate for rapid thermal processing chamber |
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