TWI238453B - Substrate processing equipment - Google Patents
Substrate processing equipment Download PDFInfo
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- TWI238453B TWI238453B TW092126222A TW92126222A TWI238453B TW I238453 B TWI238453 B TW I238453B TW 092126222 A TW092126222 A TW 092126222A TW 92126222 A TW92126222 A TW 92126222A TW I238453 B TWI238453 B TW I238453B
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- C—CHEMISTRY; METALLURGY
- 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
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- 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
- C23C16/455—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 characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
- C23C16/45563—Gas nozzles
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- C—CHEMISTRY; METALLURGY
- 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
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- 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
- C23C16/455—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 characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
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- H10P72/0402—
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Abstract
Description
1238453 玫、發明說明: 【發明所屬之技術領域】 特別是關於對基板施以成 本發明係有關基板處理裝置 膜等處理之基板處理裝置。 【先前技術】 在今曰的超高速半導體裝置中, -士 匕者食次小化製程之進歩 的同時,〇· 1 // m以下之閘極具说如山从 ㈣長逐漸成為可能。-般隨著德 小化之同時,半導體裝置動 木此 又動作速度亦提高,但於如此相 §微小化之半導體裝置中邊 七 ^者微小化使閘極長之縮短, 有必要使閘極絕緣膜之膜厚按照比例原則減少。 但閘極長一旦成為01/zm以下,閉極絕緣膜之厚度於如 目前使用熱氧化膜之時,亦必須設定為!〜2 nm或以下,作 在如此極薄之閉極絕緣膜中,會增大通道電流,其結果是 無法回避閘極漏電流增大之問題。 因為如此之情況’自以往即提案比電容率係較熱氧化膜 甚^,因此對於閘極絕緣膜適用實際膜厚雖大,但換算成 熱氧化膜時膜厚小之Ta2〇5或AH Zr〇2、Hf〇2,此外如 H〇4或咖〇4等之高電介f材料。#由使用如此之高電 介質^料,一旦閘極長為以下,則儘管是在非常短 超门速半導體裝置,亦可使用1〇疆左右之物理上的膜厚 甲’極、邑緣膜,並可控制通道效果所造成之閘極漏電流。 例如以往所知之丁^仏膜,係可藉由cvd法將 及〇2作為氣相原料而形成。典型之場合為,cVD製程係在 減壓%王兄了,約48(rc、或在其以上之溫度來實行。如此形1238453 Description of the invention: [Technical field to which the invention belongs] In particular, the present invention relates to a substrate processing apparatus for processing a substrate, such as a film, on a substrate. [Previous technology] In today's ultra-high-speed semiconductor devices, while the fighters are making progress in the miniaturization process, gates below 0.1 m can be said to be possible from a long distance. -Generally, with the miniaturization of the semiconductor device, the moving speed of the semiconductor device has also increased. However, in such a miniaturized semiconductor device, the miniaturization of the semiconductor device shortens the gate length, and it is necessary to make the gate electrode shorter. The film thickness of the insulating film is reduced in accordance with the principle of proportionality. However, once the gate length becomes less than 01 / zm, the thickness of the closed-pole insulating film must also be set to the same as when a thermal oxide film is currently used! To 2 nm or less, the channel current is increased in such a very thin closed-pole insulating film. As a result, the problem of an increase in gate leakage current cannot be avoided. Because of this situation, it has been proposed that thermal oxide films are more specific than permittivity. Therefore, although the actual film thickness is large for gate insulating films, Ta205 or AH Zr with small film thickness when converted to thermal oxide films 〇2, Hf〇2, and other high dielectric f materials such as H04 or Ca04. # By using such a high dielectric material, once the gate length is below, even if it is a very short super gate speed semiconductor device, a physical film thickness of about 10 Å can be used. And can control the gate leakage current caused by the channel effect. For example, a conventionally known Ding film can be formed by using the cvd method and O 2 as a gas phase raw material. The typical occasion is that the cVD process is performed at a decompression percentage of about 28%, or about 48 (rc, or above).
0\87\87879.DOC 1238453 成之Ta2〇5膜,進—步在氧氣氛圍中被熱處理,結果,解除 了膜中氧欠缺的情% ’而膜本身亦結晶化。如此結晶化^ Ta2〇S膜,顯示出了大的比電容率。 由提昇通道區域中之載波電流移動性之觀點,可在高兩 介質閘極氧化膜及矽基板間,隔著1 nm以下,較佳為〇 以下厚度之極薄的基底氧化膜。基底氧化膜必須為非常 薄,其厚度若厚,則與在閘極絕緣膜使用高電介質膜之饮 果相抵消。另-方面,如此非常薄的基底氧㈣,必須二 致地覆蓋住矽基板表面,且須要求不會形成界面位準等之 缺陷。 自以往起,薄問極氧化膜-般係藉切基板之急速熱氧 化(RTO)處理(例如,參照專利文獻1}所形成,但若想形成 期望之1 nm以下厚度之熱氧化膜,則,必須降低膜形成時之 處理溫度。但是’以如此低溫所形成之熱氧化膜,容易含 有界面位準等之缺陷,不適合作為高電介質閘極氧化膜之 基底氧化膜。 圖1係顯示含有高電介質閘極絕緣膜之半導體裝置1〇之 構成圖。 參照圖1,半導體裝置10係形成於矽基板丨丨上,而於矽基 板11上,隔著基底氧化膜12形成有Ta2〇5、Ah〇3、Zr〇2、 Hf〇2、ZrSi〇4、HfSi〇4等之高電介質閘極氧化膜13,此外 於前述高電介質間極氧化膜13上形成有閘極電極14。 於圖1之半導體裝置10中,於前述基底氧化膜層12之表面 部伤,在保持矽基板丨丨與基底氧化膜丨2間之界面平坦性之 O:\87\87879.DOC -8- 1238453 咏 '雜氮(N)而形成氧氮化膜12A。藉由於基底氧化膜 ,中形成比電各率較矽氧化膜大之氧氮化膜12 A,可更加減 夕基底氧化膜丨2之熱氧化膜換算膜厚。 先引所忒明,有關高速半導體裝置1〇中,前述基底氧 化膜12之較佳厚度為儘可能地薄。 — 仁為了均勻地且安定地形成1 nm以下,例如〇·8 nm以 下,進而對應2〜3原子層之〇.4nm左右之厚度之基底氧化膜 12,較以往更來得困難。 另外,為實現於基底氧化膜12上所形成之高電介質閘極 絶緣膜13之機能,係藉由熱處理以結晶化所堆積之高電介 貝膜13,且必須進行缺氧補償,但對於高電介質膜丨3進行 如此之熱處理時,因基底氧化膜12之膜厚會增大,故藉由 使用高電介質閘極絕緣膜13減少閘極絕緣膜之實際膜厚, 實貝上即相互抵銷了。 隨著如此熱處理之基底氧化膜12之膜厚增大,暗示了在 矽基板11與基底氧化膜12之界面,氧原子及矽原子之相互 擴散,與隨著此之硅酸鹽過渡層的形成,或者因氧對矽基 板中的侵入而使基底氧化膜丨2成長之可能性。隨著如此基 底氧化膜12之熱處理而來之膜厚增大問題,特別是基底氧 化膜12之膜厚’在作為基底氧化膜時希望能減低至期望數 之原子層以下膜厚之時,會成為非常迫切之問題。 特許文獻1特開平5-47687號公報 【發明内容】 本發明係以提供解決上述課題之新穎且有用之基板處理 O:\87\87879.DOC -9 - 1238453 裝置為目的。 本發明更詳細之目的係在於提供一種基板處理裝置,可 於矽基板表面,安定地形成非常薄且典型為2〜3原子層分之 厚度之氧化膜,進而將其氮化並形成氧氮化膜。曰刀 此外,本發明更詳細之目的係在於提供一種包含美 理裝置之叢集型基板處㈣、、統,可於石夕基板表面,:定: 形成非书薄且典型為2〜3原子層分之厚度之氧化膜,進而使 其安定地氮化。 此外,本發明之其他課題之目的,係在於提供一種基板 處理裝置’可解決如上述之課題,構成為可謀求氧化膜之 均性、產量之改善與污染的防止。 本發明為達成上述目的具有如以下之特徵。 根據本發明’氣體嘴射部係由處理容器之-側起朝向被 =於保持構件之被處理基板噴射氣體,而被設置於處理 U他側之排氣口’則排出通過被處理基板之氣體,藉 此可以謀求氧化膜之均一性、產量之改善與污染的防止, 同了可以特疋之流速(層流),自一個方向安定地提供氣體 至被保持於處理空間内之被處理基板表面,安定被處理基 板之成膜處理,且可有效率地進行而提高生產性。 f外根據本發明,藉由於水平方向配置成一列的複數 —^體喷射口,使得處理空間全體之氣流可保持於一致, 女疋破處理基板之成膜處理,且可有效率地進行而提高生 產性。 卜根據本發明,藉由於氣體喷射部連接個別供給不0 \ 87 \ 87879.DOC 1238453 into a Ta205 film, which is further heat-treated in an oxygen atmosphere. As a result, the oxygen deficiency in the film is removed, and the film itself crystallizes. The crystalline Ta20S film thus crystallized showed a large specific permittivity. From the viewpoint of improving the carrier current mobility in the channel region, an extremely thin base oxide film with a thickness of 1 nm or less, preferably 0 or less, may be interposed between the dielectric oxide film and the silicon substrate of the upper two dielectric layers. The base oxide film must be very thin. If it is thick, it will be offset by the use of a high dielectric film for the gate insulating film. On the other hand, such a very thin base oxide must cover the surface of the silicon substrate uniformly, and it must be required that defects such as interface levels are not formed. Conventionally, thin interlayer oxide films are generally formed by rapid thermal oxidation (RTO) processing of a cut substrate (for example, refer to Patent Document 1), but if a thermal oxide film with a thickness of 1 nm or less is desired, It is necessary to reduce the processing temperature when the film is formed. However, a thermal oxide film formed at such a low temperature is likely to contain defects such as interface levels, and is not suitable as a base oxide film for a high-dielectric gate oxide film. Structure diagram of a semiconductor device 10 with a dielectric gate insulating film. Referring to FIG. 1, a semiconductor device 10 is formed on a silicon substrate, and Ta205 and Ah are formed on the silicon substrate 11 via a base oxide film 12. 〇3, Zr〇2, Hf〇2, ZrSi〇4, HfSi〇4 and other high-dielectric gate oxide film 13, in addition to the aforementioned high-dielectric interlayer oxide film 13, a gate electrode 14 is formed. In the semiconductor device 10, the surface of the aforementioned base oxide film layer 12 is damaged, and the flatness of the interface between the silicon substrate 丨 and the base oxide film 丨 2 is maintained. O: \ 87 \ 87879.DOC -8-1238453 Nitrogen (N) forms the oxynitride film 12A. The bottom oxide film is formed with an oxynitride film 12 A having a larger specific electrical rate than the silicon oxide film, which can further reduce the thickness of the thermal oxide film of the base oxide film 丨 2. It will be explained first about the high-speed semiconductor device. In 10, the preferable thickness of the aforementioned base oxide film 12 is as thin as possible. — In order to form uniformly and stably below 1 nm, for example, below 0.8 nm, and further corresponding to 0.4 nm of the 2 to 3 atomic layer The thickness of the base oxide film 12 on the left and right is more difficult than in the past. In addition, in order to realize the function of the high-dielectric gate insulating film 13 formed on the base oxide film 12, the high-electricity accumulated by crystallization is heat-treated. The dielectric film 13 must be compensated for lack of oxygen, but when such a heat treatment is performed on the high dielectric film 3, the thickness of the base oxide film 12 will increase. Therefore, the gate is reduced by using the high dielectric gate insulating film 13 The actual film thickness of the polar insulating film cancels each other out. As the film thickness of the base oxide film 12 thus heat-treated increases, it implies that at the interface between the silicon substrate 11 and the base oxide film 12, oxygen atoms and silicon Atomic diffusion With the formation of this silicate transition layer, or the possibility of the base oxide film growing due to the intrusion of oxygen into the silicon substrate, the problem of increasing the film thickness due to the heat treatment of the base oxide film 12 In particular, when the thickness of the base oxide film 12 is desired to be reduced to a desired number of atomic layers or less when used as the base oxide film, it becomes a very urgent problem. Patent Document 1 JP-A-5-47687 [ SUMMARY OF THE INVENTION The present invention aims to provide a novel and useful substrate processing device O: \ 87 \ 87879.DOC -9-1238453 which solves the above-mentioned problems. A more detailed object of the present invention is to provide a substrate processing device which can be used in On the surface of the silicon substrate, a very thin oxide film with a thickness of typically 2 to 3 atomic layers is formed stably, and then it is nitrided to form an oxynitride film. In addition, a more detailed object of the present invention is to provide a cluster substrate including a aesthetic device, which can be used on the surface of a Shixi substrate. It is intended to form a non-book thin and typically 2 ~ 3 atomic layer. An oxide film with a thickness of 1%, which in turn makes it nitride in a stable manner. Further, another object of the present invention is to provide a substrate processing apparatus' that can solve the above-mentioned problems and is configured to improve the uniformity of the oxide film, improve the yield, and prevent pollution. To achieve the above object, the present invention has the following features. According to the present invention, the 'gas nozzle ejection part ejects gas from the side of the processing container toward the substrate to be processed which is held on the holding member, and the exhaust port provided on the other side of the processing unit' exhausts the gas passing through the substrate to be processed. In this way, the uniformity of the oxide film, the improvement of the yield, and the prevention of pollution can be achieved. At the same time, it can provide a stable flow rate (laminar flow) from one direction to the surface of the substrate to be processed held in the processing space. It stabilizes the film formation process of the substrate to be processed, and can be efficiently performed to improve productivity. According to the present invention, the plural-body spray ports arranged in a row in the horizontal direction can keep the air flow in the entire processing space uniform, and the film-forming treatment of the processing substrate can be efficiently performed and improved. Productive. According to the present invention, the individual supply
O:\87\87879.DOC -10- 1238453 ㈣類氣體之複數個的氣體供給管路,可例如選擇性地安 定供給氮化氣體或氧化氣體,且可對處理空間中被處理基 板附近之區域,安定供給任意之氣體。 另:’根據本發明’由於排氣口係形成為較被處理基板 更加寬廣之長方形狀,故可提高通過被處理基板之氣體之 排氣效率,由此點亦可使處理空間全體之氣流保持於一 致’女定被處理基板之成膜處自,且可有效率土也進行而提 高生產性。 另外,根據本發明,由於排氣口係由處理容器另一側之 底部連通至延伸形成於下方之排氣途徑,故可提高通過被 處理基板之氣體之排氣效率,由此點亦可使處理空間全體 之氣流保持於一致,安定被處理基板之成膜處理且可有效 率地進行。 【實施方式】 以下圖式說明有關本發明之實施形態。 圖2係顯示本發明之基板處理裝置之一實施例構成之前 視圖。圖3係顯示本發明之基板處理裝置之—實施例構成之 側視圖。圖4為沿著圖2中A_A線之橫剖面圖。 =圖2至圖4所示,基板處理|置2()如後述,係構成為可 1續進行石夕基板之紫外光自由基氧化處理,與使用如此的 I外光自由基氧化處理所形成之氧化膜 < 高頻遠距離電漿 之自由基氮化處理。 基板處理裝置2G之主要構成,係包含:内部劃分成處理 空間之處理容器22、於特定溫度加熱被插入於處理容器22O: \ 87 \ 87879.DOC -10- 1238453 A plurality of gas supply lines of tritium gas can selectively and stably supply nitriding gas or oxidizing gas, for example, and can be applied to the area near the substrate to be processed in the processing space. , Stable supply of any gas. In addition, according to the present invention, since the exhaust port is formed in a wider rectangular shape than the substrate to be processed, the exhaust efficiency of the gas passing through the substrate to be processed can be improved, thereby maintaining the air flow in the entire processing space. Since the film formation of the substrate to be processed is uniform, it can also be performed efficiently to improve productivity. In addition, according to the present invention, since the exhaust port is connected from the bottom of the other side of the processing container to an exhaust path extending downward, the exhaust efficiency of the gas passing through the substrate to be processed can be improved. The airflow in the entire processing space is kept uniform, and the film formation processing of the substrate to be processed is stable and can be performed efficiently. [Embodiment] The following drawings explain embodiments of the present invention. Fig. 2 is a front view showing the structure of an embodiment of a substrate processing apparatus of the present invention. Fig. 3 is a side view showing the structure of an embodiment of the substrate processing apparatus of the present invention. FIG. 4 is a cross-sectional view taken along line A_A in FIG. 2. = As shown in Fig. 2 to Fig. 4, the substrate treatment | set 2 () is formed as described later, and can be formed by the UV light radical oxidation treatment of the Shi Xi substrate, and formed by using such an external light radical oxidation treatment. The oxide film < free radical nitriding treatment of high-frequency long-distance plasma. The main structure of the substrate processing apparatus 2G includes a processing container 22 which is internally divided into a processing space, and is inserted into the processing container 22 by heating at a specific temperature.
O:\87\87879.DOC -11 - 1238453 内部之被處理基板(石夕基板)之加熱部24、被搭載於處理容器 22上部之紫外線照射部26、供給氮自由基之遠距離電漿部 27、令被處理基板旋轉之旋轉驅動部28、使被插入處理空 間之被處理基板昇降之升降桿機構30、為減壓處理容器^ 内部之排氣路徑32,及為供給氣體(氮氣、氧氣等之製程氣 體)於處理容器22内部之氣體供給部34。 另外,基板處理裝置20係具有為支持上述各主要構成部 之框36。框36為立體地組合鐵架者,由被置放於地面之台 狀之底部框38、由底部框38之後部而被豎立成垂直方向之 垂直框40, 4卜由垂直框40之中間部起延伸於水平方向而被 橫向架設之中間框42,及由垂直框40, 41之上端部橫向架設 於水平方向之上部框44所構成。 於底部框38搭載有冷卻水供給部46、包含電磁閥之排氣 用閥48a,48b、渦輪分子幫浦5〇、真空管路51、紫外線照射 部26之電源單位52、升降桿機構3〇之驅動部136及氣體供給 部34等。 於垂直框40之内部形成有可穿插各種電纜線之電纜線導 管40a。另外,於垂直框41之内部形成有排氣導管4u。此 外,在被固定於垂直框40中間部之托架58上安裝有緊急停 止開關60,而在被固定於垂直框41中間部之托架62上則安 裝有由冷卻水進行溫度調整之溫度調整器64。 於中間框42上係支持有:上述處理容器22、紫外線照射 部26、遠距離電漿部27、旋轉驅動部28、升降桿機構3〇、 及UV燈控制器57。另外,於上部框44上則搭載有:可連通 O:\87\87879.DOC -12- 1238453 自氣體供給部34所拉出之複數條氣體管路58之氣體箱66、 離子測量控制器68、進行壓力控制之APC控制器70及控制 滿輪分子幫浦5〇之TMP控制器72等。 圖5係顯示被配置於處理容器22下方之機器構成之前視 圖。圖6係顯示被配置於處理容器22下方之機器構成之俯視 圖。圖7係顯示被配置於處理容器22下方之機器構成之側視 圖。圖8A係顯示排氣路徑32之構成之俯視圖;而圖8B則顯 不排氣路徑32之構成之前視圖;圖扣為沿著β·β線之縱剖 面圖。 如圖5至圖7所示,於處理容器22之後部下方設置有排出 處理容器22内部氣體之排氣路徑32。該排氣路徑32係被安 裝成與橫向尺寸與形成於處理容器22内部之處理空間之橫 向I幅大致相同而形成之長方形排氣口 74連通。 如此,由於排氣口 74係延伸形成為對應處理容器22内部 之橫向寬幅尺寸之長度,故自處理容器22之前部22a側供給 至内部之氣體,會如後述般,通過處理容器22内部流向後 方,以一定流速(層流)朝排氣路徑32有效率地排氣。 如圖8A〜圖8C所示,排氣路徑32係具有:被連通至排氣 口 74之長方形開口部32a、開口部32a之左右側面朝向下方 而傾斜成錐形狀之錐形部32b、在錐形部32b之下端處通路 面積被集中之底部32c、由底部32c向前方突出之乙字型之主 排氣管32d、開口於主排氣管32d下端之排出口 32e及向錐形 部32b之下部32f開口之分流用排出口叫。排出口仏被連 通至涡輪分子幫浦50之吸氣口。另外,分流用排出口叫被 O:\87\87879.DOC -13- 1238453 連通至分流管路5 1 a。 如圖5至圖7所示’由處理容器22之排氣口 排出之氣 體’係精由渦輪分子幫浦5〇之吸引力,自形成為長方形之 開口部32a流入,通過錐形部32b至底部32c,再經由主排氣 管3M與排出口 326被引導至渦輪分子幫浦5〇。 , 渦輪分子幫浦50之吐出管5〇a係經由間術被連通至真空 管路5卜因此’充填於處理容器22内部之氣體,當閥偽二 打開時則經由渦輪分子幫浦5Q向真空管路51排出。另外, 於排氣路徑32之分流用排出口叫係連接有a流管路仏, 而該分流管路5U會因閥48b之打開而與真空管路5i連通。 在此,說明有關構成本發明重要部分之處理容器Μ及其 周邊機器之構成。 [處理容器22之構成] 圖9係擴大顯示處理容器2 2及其周邊機器之側面縱剖面 3圖為從上方所見到拿掉蓋子構件82之處理容器22内 部之俯視圖。 如圖9與圖1〇所示,處理容器22係藉由蓋子構件82閉塞住 至80上部開口之構成,其内部成為製程空間(處理空間)84。 處理谷器22在前部22a形成有可供給氣體之供給口 22g, 而後。卩22b則形成有搬送口 94。於供給口 22g設置有後述之 氣體噴射噴嘴部93,而於搬送口 94則連通有後述之閘極閥 96 〇O: \ 87 \ 87879.DOC -11-1238453 The heating section 24 of the substrate to be processed (Shiyu substrate) inside, the ultraviolet irradiation section 26 mounted on the upper part of the processing container 22, and the long-distance plasma supply section for supplying nitrogen radicals 27. Rotary drive unit 28 for rotating the substrate to be processed, a lifting rod mechanism 30 for lifting and lowering the substrate to be processed inserted into the processing space, an exhaust path 32 for the pressure reduction processing container ^, and a supply gas (nitrogen, oxygen) Etc.) in the gas supply portion 34 inside the processing container 22. The substrate processing apparatus 20 includes a frame 36 for supporting the above-mentioned main components. The frame 36 is a three-dimensionally assembled iron frame. The bottom frame 38 is placed on the floor in the shape of a table, and the vertical frame 40 is erected in the vertical direction from the rear of the bottom frame 38. The middle portion of the vertical frame 40 The middle frame 42 extending in the horizontal direction and being horizontally erected is formed by the upper ends of the vertical frames 40 and 41 being horizontally erected in the horizontal upper frame 44. The bottom frame 38 is equipped with a cooling water supply unit 46, exhaust valves 48a and 48b including a solenoid valve, a turbo molecular pump 50, a vacuum line 51, a power supply unit 52 of the ultraviolet irradiation unit 26, and a lifting rod mechanism 30. The driving section 136, the gas supply section 34, and the like. A cable guide 40a is formed inside the vertical frame 40 through which various cables can be inserted. An exhaust duct 4u is formed inside the vertical frame 41. In addition, an emergency stop switch 60 is mounted on a bracket 58 fixed to the middle portion of the vertical frame 40, and a bracket 62 fixed to the middle portion of the vertical frame 41 is provided with temperature adjustment by cooling water.器 64。 64. Supported on the middle frame 42 are the processing container 22, the ultraviolet irradiation section 26, the remote plasma section 27, the rotation driving section 28, the lifter mechanism 30, and the UV lamp controller 57. In addition, the upper frame 44 is equipped with a gas box 66 and an ion measurement controller 68 that can communicate with O: \ 87 \ 87879.DOC -12-1238453. A plurality of gas lines 58 are pulled from the gas supply unit 34. APC controller 70 for pressure control and TMP controller 72 for controlling full-round molecular pump 50. FIG. 5 is a front view showing the configuration of a machine disposed below the processing container 22. As shown in FIG. FIG. 6 is a plan view showing the structure of a machine arranged below the processing container 22. As shown in FIG. FIG. 7 is a side view showing the structure of a machine arranged below the processing container 22. As shown in FIG. Fig. 8A is a plan view showing the structure of the exhaust path 32; Fig. 8B is a front view showing the structure of the exhaust path 32; and the figure is a longitudinal sectional view taken along the line β · β. As shown in FIGS. 5 to 7, an exhaust path 32 for exhausting the gas inside the processing container 22 is provided below the rear portion of the processing container 22. The exhaust path 32 is installed so as to communicate with a rectangular exhaust port 74 having a lateral dimension substantially the same as the horizontal I of the processing space formed inside the processing container 22. In this way, since the exhaust port 74 is extended to correspond to the width and width of the inside of the processing container 22, the gas supplied to the inside from the front 22a side of the processing container 22 will flow through the inside of the processing container 22 as described later. In the rear, the air is efficiently exhausted toward the exhaust path 32 at a constant flow rate (laminar flow). As shown in FIGS. 8A to 8C, the exhaust path 32 includes a rectangular opening portion 32a communicating with the exhaust port 74, a left and right side surfaces of the opening portion 32a, and a tapered portion 32b inclined in a tapered shape toward the lower side. The bottom 32c where the passage area is concentrated at the lower end of the shaped portion 32b, the B-shaped main exhaust pipe 32d protruding forward from the bottom 32c, the discharge port 32e opening at the lower end of the main exhaust pipe 32d, and the lower portion of the tapered portion 32b The 32f opening is called a discharge port. The exhaust port 仏 is connected to the suction port of the turbo molecular pump 50. In addition, the shunt outlet is called O: \ 87 \ 87879.DOC -13- 1238453 and is connected to the shunt line 5 1 a. As shown in FIG. 5 to FIG. 7, the “gas exhausted from the exhaust port of the processing container 22” is attracted by the turbo molecular pump 50 and flows in from the rectangular opening 32 a and passes through the tapered portion 32 b to The bottom 32c is guided to the turbo molecular pump 50 through the main exhaust pipe 3M and the discharge port 326. The turbo tube 50a of the turbomolecular pump 50 is connected to the vacuum line 5 via interstitial gas. Therefore, the gas filled in the processing container 22 is opened to the vacuum line via the turbomolecular pump 5Q when the valve 2 is opened. 51 is discharged. In addition, a shunting discharge port in the exhaust path 32 is connected to an a-flow pipe 仏, and the shunting pipe 5U is communicated with the vacuum pipe 5i due to the opening of the valve 48b. Here, the configuration of the processing container M and its peripheral devices constituting an important part of the present invention will be described. [Configuration of the processing container 22] Fig. 9 is an enlarged side view of the processing container 22 and its peripheral devices. Fig. 9 is a plan view of the inside of the processing container 22 with the lid member 82 removed from above. As shown in FIG. 9 and FIG. 10, the processing container 22 is closed by a cover member 82 to an upper opening of 80, and the inside thereof becomes a process space (processing space) 84. The processing trough 22 is formed with a gas supply port 22g in the front portion 22a, and thereafter.卩 22b is formed with a transfer port 94. The supply port 22g is provided with a gas injection nozzle section 93 described later, and the transfer port 94 is communicated with a gate valve 96 described later.
圖11為處理容器22之俯視圖。圖12為處理容器22之前視 圖。圖13為處理容器22之仰視圖。圖14為沿著圖12中C-C O:\87\87879.DOC -14- 1238453 線之縱剖面圖。圖1 5 Aα口 1 為處理谷态22之右側視圖。圖16為處 理容器22之左側視圖。 如圖11至圖16所示,於處理容器22之底部22c設置有:被 插入加熱部24之開口 73,及前述開口成長方形之排氣口 74。於排氣口 74連通有前述之排氣路徑32。另外,室8〇與 蓋子構件82,係例如切割加工鋁合金,並加工成如上述之 形狀者。 另外,於處理容器22之右側面22e係安裝有:為窺視製程 空間84之第卜第2窗口 75, 76,及為測定製程空間84之溫度 之感應器單元77。 於本實施例中,由於在右側面22e中央之左側配置有形成 為橢圓形之第1窗口 75,而右側面22e中央之右側配置有形 成為圓形之第2窗口 76,因而可由兩方面直接目視被保持於 製程空間84之被處理基板w之狀態,故有利於觀測被處理 基板W之成膜狀況等。 另外’窗口 75, 76之構成為在插入有熱電偶等之溫度測定 器具時,可由處理容器22拆掉。 另外,於處理容器22之左側面22d,係安裝有為測定製程 空間84之壓力之感應器單元85。於該感應器單元85設置有 測定範圍不同的3個壓力計85a〜85c,可高精密度地測定製 程空間84之壓力變化。 另外,於形成製程空間84之處理容器22之内壁之四個角 落,設置有形成為R形狀之彎曲部22h,其不僅可藉由該彎 曲部22h迴避應力集中,並可發揮使由氣體噴射噴嘴部93所 O:\87\87879 DOC -15- 1238453 射喷出之氣體流安定之作用。 [紫外線照射部26之構成] 如圖8至圖11所示,紫外線照射部26係被安裝於蓋子構件 82之上面。於該紫外線照射部26之筐體26a内部,以特定間 隔平行地配置有形成為圓筒狀之2根紫外線光源(UV燈)86, 87 〇 該务外線光源86,87具有發出波長為172 nm之紫外線之 特性’被設置於經由形成於蓋子構件82之橫向延伸之長方 形開口 82a,82b,可對與保持於製程空間84之被處理基板w 上面相對之製程空間84之前半側(於圖8左半部)區域照射紫 外線之位置。 另外’由延伸成直線狀之紫外線光源86, 87照射在被處理 基板W上之紫外線之強度分佈並不一致,而是因被處理基 板W之半徑方向之位置而變化,一方是越往被處理基板ψ 之外周圍側則越減少,另一方則是越往内周圍側則越減 少。如此紫外線光源86, 87雖在被處理基板w上形成單獨且 單調地變化之紫外線強度分佈,但對於被處理基板w之紫 外線強度分佈之變化方向則成相反。 因此,藉由UV燈控制器57的控制來最適化紫外線光源86, 87之驅動能量,故可在被處理基板w上實現非常地一致之 紫外線強度分佈。 另外,如此的驅動能量之最適值,係變化對紫外線光源 86, 87之驅動輸出而評估成膜結果,來求得最適值。 另外,被處理基板W與紫外線光源86, 87之圓筒狀圓筒芯FIG. 11 is a plan view of the processing container 22. FIG. 12 is a front view of the processing container 22. FIG. 13 is a bottom view of the processing container 22. Fig. 14 is a longitudinal sectional view taken along line C-C O: \ 87 \ 87879.DOC -14-1238453 in Fig. 12. Figure 1 5 Aα port 1 is a right side view of processing valley state 22. FIG. 16 is a left side view of the processing container 22. As shown in Figs. 11 to 16, the bottom 22c of the processing container 22 is provided with an opening 73 inserted into the heating section 24, and an exhaust opening 74 having a rectangular opening as described above. The above-mentioned exhaust path 32 is communicated with the exhaust port 74. The chamber 80 and the lid member 82 are made of, for example, a cut aluminum alloy and processed into a shape as described above. In addition, on the right side 22e of the processing container 22, a second window 75, 76 for peeping the process space 84, and a sensor unit 77 for measuring the temperature of the process space 84 are mounted. In this embodiment, since the first window 75 formed in an oval shape is arranged on the left side in the center of the right side 22e, and the second window 76 is formed in a circle on the right side of the center of the right side 22e, it can be directly visually viewed from two aspects. The state of the substrate w to be processed held in the process space 84 is advantageous for observing the film formation status of the substrate W to be processed. The windows 75 and 76 are configured so that they can be removed by the processing container 22 when a temperature measuring instrument such as a thermocouple is inserted. In addition, a sensor unit 85 for measuring the pressure in the process space 84 is mounted on the left side 22d of the processing container 22. The sensor unit 85 is provided with three pressure gauges 85a to 85c having different measurement ranges, and the pressure change in the process space 84 can be measured with high precision. In addition, four corners of the inner wall of the processing container 22 forming the process space 84 are provided with a curved portion 22h formed in an R shape, which can not only avoid stress concentration by the curved portion 22h, but also can exert a gas injection nozzle portion. 93 O: \ 87 \ 87879 DOC -15-1238453 Stabilization of gas flow from jets. [Configuration of the ultraviolet irradiation section 26] As shown in Figs. 8 to 11, the ultraviolet irradiation section 26 is mounted on the cover member 82. Inside the housing 26a of the ultraviolet irradiation section 26, two ultraviolet light sources (UV lamps) 86, 87 formed in a cylindrical shape are arranged in parallel at a specific interval. The external light sources 86, 87 have a wavelength of 172 nm. The characteristic of ultraviolet rays is provided through the rectangular openings 82a, 82b formed in the lateral extension of the cover member 82, and can face the front half of the process space 84 opposite to the upper surface of the substrate w held in the process space 84 (left of FIG. 8). (Half) area where the ultraviolet rays are exposed. In addition, the intensity distribution of the ultraviolet rays irradiated by the ultraviolet light sources 86 and 87 which are linearly irradiated on the substrate W to be processed is not uniform, but varies depending on the radial position of the substrate W to be processed. The outer side of ψ decreases, and the other side decreases toward the inner side. In this way, although the ultraviolet light sources 86, 87 form a single and monotonically changing ultraviolet intensity distribution on the substrate w to be processed, the direction of change of the ultraviolet intensity distribution of the substrate w to be processed is opposite. Therefore, by controlling the UV lamp controller 57 to optimize the driving energy of the ultraviolet light sources 86, 87, a very uniform ultraviolet intensity distribution can be achieved on the substrate w to be processed. In addition, the optimum value of such driving energy is obtained by changing the driving output of the ultraviolet light sources 86, 87 and evaluating the film formation results to obtain the optimum value. In addition, the cylindrical core of the substrate W to be processed and the ultraviolet light sources 86 and 87
O:\87\87879.DOC -16- 1238453 中心之距離,例如係設定成50〜300 mm,較佳為loo〜200 mm 左右。 圖17係擴大顯示紫外線光源86,87之安裝構造之縱剖面 圖。 如圖17所示,紫外線光源86,87係被保持於相對於紫外線 照射部26筐體26a之底部開口 2_6b之位置。並且,底部開口 26b係形成為於相對於被保持在製程空間料之被處理基板 w上面之位置處開口,且橫向寬幅尺寸較紫外線光源%, 全長更長之長方形。 於底部開口 26b之邊緣部26c,安裝有由透明石英所形成 之透明窗88。透明窗88將由紫外線光源86, 87所照射之紫外 線透射入製程空間84,並且具有可承受製程空間料減壓時 之壓力差之強度。 另外,於透明窗88下面邊緣部,形成有抵接被安裝於底 部開口 26b之邊緣部26c之溝内之密封構件(〇環)的之密封 面88a。該密封面88a係由為保護密封構件89之塗層或由黑 石英所形成。藉此,密封構件89之材質不會分解,可防止 劣化保護密封性能,同時並防止密封構件89之材質侵入至 製程空間84。 另外,於透明窗88上面邊緣部與不銹鋼製之防護罩88b 抵接’以提高鎖緊構件91夾住透明窗88時之強度,防止因 鎖緊時之擠壓力造成透明窗88破損。 另外,於本實施例中,係將紫外線光源86, 87與透明窗88 配置為於與由氣體噴射喷嘴部93所喷射之氣體流之流動方O: \ 87 \ 87879.DOC -16- 1238453 The center distance, for example, is set to 50 ~ 300 mm, preferably about loo ~ 200 mm. Fig. 17 is a longitudinal sectional view showing the mounting structure of the ultraviolet light sources 86 and 87 in an enlarged manner. As shown in Fig. 17, the ultraviolet light sources 86 and 87 are held at positions 2-6b with respect to the bottom opening of the housing 26a of the ultraviolet irradiation section 26. In addition, the bottom opening 26b is formed as a rectangle that is open at a position above the substrate w to be held in the process space, and has a width in a lateral direction that is larger than that of the ultraviolet light source and a longer rectangular shape. A transparent window 88 made of transparent quartz is attached to the edge portion 26c of the bottom opening 26b. The transparent window 88 transmits ultraviolet rays irradiated by the ultraviolet light sources 86, 87 into the process space 84, and has a strength capable of withstanding the pressure difference when the process space material is decompressed. In addition, a sealing surface 88a is formed on the lower edge portion of the transparent window 88 to abut a sealing member (o-ring) mounted in the groove of the edge portion 26c of the bottom opening 26b. The sealing surface 88a is formed of a coating for protecting the sealing member 89 or of black quartz. Thereby, the material of the sealing member 89 will not be decomposed, the deterioration of the protective sealing performance can be prevented, and the material of the sealing member 89 can be prevented from penetrating into the process space 84. In addition, the upper edge portion of the transparent window 88 is in contact with a protective cover 88b made of stainless steel to increase the strength of the locking member 91 when the transparent window 88 is sandwiched, and prevent the transparent window 88 from being damaged due to the pressing force during the locking. In addition, in this embodiment, the ultraviolet light sources 86, 87 and the transparent window 88 are arranged so as to flow with the gas flow sprayed by the gas spray nozzle portion 93.
O:\87\87879.DOC -17- 1238453 向垂直而延伸之方向,但不限於此,例如亦可配置成使紫 外線光源86, 87與透明窗88延伸於氣體流之流動之方向。 [氣體喷射喷嘴部93之構成] 如圖9與圖10所示,處理容器22在開口於前部22a之供給 口 22g處,設置有對製程空間84内部喷射氮氣或氧氣之氣體 喷射喷嘴部93。該氣體喷射喷嘴部93係如後述,在製程空 間84之檢向方向配置有一列的複數個喷射口 93a,可使由複 數個的喷射口 93a所喷射之氣體,以層流狀態通過被處理基 板W表面,而在製程空間84内部產生安定的氣流。 另外,閉塞製程空間84之蓋子構件82之下面與被處理基 板w之距離,係例如被設定成5〜1〇〇 mm,較理想為25〜85 mm左右。 [加熱部24之構成] 如圖9與圖1〇所示,加熱部24之構成為具備有:鋁合金製 之底座no、被固定於底座uo上之透明之石英鐘罩112、被 收容於石英鐘罩112之内部空間113之Sic加熱器114、由不 透明石英所形成之熱反射構件(反射器)116、由被裝載於石 英鈿罩112上面之siC加熱器114所加熱之siC基板設置台 (加熱構件)118。 因此,SiC加熱器U4與熱反射構件116係由石英鐘罩112 之内部空間113所隔離,可防止在製程空間84之污染。另 外,於洗淨步驟,因僅需洗淨被露出於製程空間84内之Sic 基板設置台118即可,故可省略洗淨Sic加熱器114與熱反射 構件116之作業。O: \ 87 \ 87879.DOC -17- 1238453 extends in a vertical direction, but it is not limited to this. For example, it can be configured such that the ultraviolet light sources 86, 87 and the transparent window 88 extend in the direction of the gas flow. [Configuration of Gas Injection Nozzle Section 93] As shown in FIG. 9 and FIG. 10, the processing container 22 is provided with a gas injection nozzle section 93 for injecting nitrogen or oxygen into the process space 84 at the supply port 22g opened at the front section 22a. . The gas injection nozzle portion 93 is a row of a plurality of injection ports 93a arranged in the direction of detection of the process space 84 as will be described later. The gas ejected from the plurality of injection ports 93a can pass through the substrate to be processed in a laminar flow state. W surface, and a stable airflow is generated inside the process space 84. In addition, the distance between the lower surface of the cover member 82 and the substrate w to be processed in the closed process space 84 is set to, for example, 5 to 100 mm, and more preferably 25 to 85 mm. [Configuration of Heating Section 24] As shown in FIGS. 9 and 10, the heating section 24 is configured to include a base made of aluminum alloy, a transparent quartz bell cover 112 fixed to the base uo, and housed in a quartz clock. Sic heater 114 in the inner space 113 of the cover 112, a heat reflecting member (reflector) 116 formed of opaque quartz, and a siC substrate setting table (heating) Component) 118. Therefore, the SiC heater U4 and the heat reflecting member 116 are separated by the internal space 113 of the quartz bell cover 112, which can prevent contamination in the process space 84. In addition, in the cleaning step, it is only necessary to clean the Sic substrate setting stand 118 exposed in the process space 84, so that the operation of cleaning the Sic heater 114 and the heat reflection member 116 can be omitted.
O:\87\87879.DOC -18- 1238453 被處理基板W係由保持構件120保持在相對於SiC基板設 置台118之上方。另一方面,siC加熱器114被裝載於熱反射 構件116之上面,而SiC加熱器114所發散之熱係放射至SiC 基板设置台11 8,且熱反射構件116所反射之熱亦放射至sic 基板設置台118。此外,本實施例之SiC加熱器114係在稍稍 離開SiC基板設置台118之狀態下加熱至約7〇〇。〇。 S i C基板設置台118因其熱傳導率佳,故可有效率地將來 自SiC加熱器114之熱傳達至被處理基板w,並消除被處理 基板W邊緣部份與中心部份之溫度差,防止被處理基板w 因溫度差而彎曲。 [旋轉驅動部28之構成] 如圖9與圖1〇所示,旋轉驅動部28係由以下所構成:在sic 基板設置台118之上方保持被處理基板W之保持構件12〇、 被固定於底座110下面之外殼122、對在由外殼122所劃分之 内部空間124内結合於保持構件120之軸120d之陶竟軸126 進行旋轉驅動之馬達128、及傳達馬達128之旋轉之磁鐵聯 結器130。 於旋轉驅動部28中,保持構件120之軸120d係貫通112石 英鐘罩並結合於陶瓷軸126,而於陶瓷轴126與傳達馬達128 之旋轉轴間則是經由磁鐵聯結器1 30以非接觸之方式傳達 驅動能量,故使旋轉驅動系統之構成變得簡潔,亦有助於 裝置全體之小型化。 保持構件120自120d上端起,具有於水平方向延伸成放射 狀之臂部12 0 a〜12 0 c。被處理基板W以被裝載於保持構件 O:\87\87879.DOC -19- 1238453 120之/部120a〜120c之狀恶保持著。如此,被保持之被處 理基板W與保持構件120—起由傳達馬達128以特定之旋轉 速度來旋轉,藉此可平均因114SiC加熱器發熱之溫度分 佈,並使來自紫外線光源86, 87所照射之紫外線之強度分佈 均一,且可對表面施以均一之成膜。 [升降桿機構3〇之構成] 如圖9與圖1〇所示,升降桿機構3〇係被設置於室8〇之下方 且112石英鐘罩之側面,由被插入於室⑽内之昇降臂1 32、 被連結於昇降臂132之昇降軸134、使昇降軸134昇降之驅動 部136所構成。昇降臂132係例如由陶莞或石英所形成,如 圖10所不,具有:結合著昇降軸134上端之結合部I32a,及 包圍s〗c基板設置台118外周之環狀部132b。並且,於昇降 臂132,在圓周方向上以12()度之間隔,設置有由環狀部⑽ 之内周起向中心延伸之3支抵接銷138a〜138c。 抵接銷138a〜138c會下降至喪合由sic基板設置台118之 外周向中心延伸而形成之溝118a〜i i8c之位置,藉由昇降臂 m上昇而再移動至SlC基板設置台ιΐ8之上方。另外,抵接 銷138a〜138c係配置成不干涉到較sie基板設置台中 ^ I伸於外周側所形成之保持構件之臂部l2〇a〜12〇c。 什降’ 132其搬送自冑機98之機械臂在取出被處理基板 W之別係使上述抵接銷13 8a〜138c抵接於被處理基板W之 下面二再由保持構件12()之臂部⑽㈠⑽拿起被處理基板 W藉此’搬运自動機98之機械臂可移動至被處理基板W 之下方而可以降下昇降臂132來搬送並保持被處理基板O: \ 87 \ 87879.DOC -18-1238453 The substrate W to be processed is held by the holding member 120 above the SiC substrate setting table 118. On the other hand, the siC heater 114 is mounted on the heat reflection member 116, and the heat emitted by the SiC heater 114 is radiated to the SiC substrate setting stage 118, and the heat reflected by the heat reflection member 116 is also radiated to sic. SUB Board Setting Stage 118. In addition, the SiC heater 114 of this embodiment is heated to about 700 in a state where it is slightly separated from the SiC substrate mounting table 118. 〇. The Si IC substrate setting table 118 has good thermal conductivity, so it can efficiently transfer heat from the SiC heater 114 to the substrate w to be processed, and eliminate the temperature difference between the edge portion and the center portion of the substrate W to be processed. The substrate w to be processed is prevented from being bent due to a temperature difference. [Structure of Rotary Drive Unit 28] As shown in FIGS. 9 and 10, the rotary drive unit 28 is configured by a holding member 12 for holding a substrate W to be processed above the sic substrate setting table 118, and is fixed to A housing 122 below the base 110, a motor 128 for rotationally driving a ceramic shaft 126 coupled to a shaft 120d of the holding member 120 in an internal space 124 divided by the housing 122, and a magnet coupling 130 for transmitting the rotation of the motor 128 . In the rotation driving part 28, the shaft 120d of the holding member 120 is passed through the 112 quartz clock cover and is coupled to the ceramic shaft 126, and the ceramic shaft 126 and the rotation shaft of the transmission motor 128 are connected in a non-contact manner through the magnet coupling 1 30. The method transmits driving energy, so that the structure of the rotary driving system is simplified, and it contributes to the miniaturization of the entire device. The holding member 120 has arm portions 12 0 a to 12 0 c extending in a radial direction from the upper end of 120 d. The substrate W to be processed is mounted on the holding member O: \ 87 \ 87879.DOC -19-1238453 120 / 120a to 120c. In this way, the substrate W to be processed and the holding member 120 are rotated by the transmission motor 128 at a specific rotation speed, thereby averaging the temperature distribution generated by the 114SiC heater and irradiating the light from the ultraviolet light sources 86, 87. The intensity distribution of ultraviolet rays is uniform, and the surface can be uniformly formed into a film. [Configuration of the lifting rod mechanism 30] As shown in FIG. 9 and FIG. 10, the lifting rod mechanism 30 is provided below the chamber 80 and on the side of the 112 quartz bell cover, and the lifting arm is inserted into the chamber. 1 32. A lifting shaft 134 connected to the lifting arm 132 and a driving part 136 for lifting the lifting shaft 134 are formed. The elevating arm 132 is formed of, for example, pottery or quartz, as shown in FIG. 10, and includes a joint portion I32a that is connected to the upper end of the elevating shaft 134, and an annular portion 132b that surrounds the outer periphery of the substrate mounting platform 118. In addition, three contact pins 138a to 138c extending from the inner periphery of the ring-shaped portion 向 toward the center are provided in the lifting arm 132 at intervals of 12 () degrees in the circumferential direction. The abutting pins 138a to 138c will descend to the positions of the grooves 118a to i i8c formed by extending from the peripheral center of the sic substrate setting table 118, and then move to the top of the SlC substrate setting table ι8 by raising the lifting arm m. . In addition, the contact pins 138a to 138c are arranged so as not to interfere with the arm portions 120a to 120c of the holding member formed on the outer peripheral side of the sie substrate setting table. In addition, when the robot arm of the conveyor 98 is used to take out the substrate W to be processed, the above-mentioned contact pins 13 8a to 138c are brought into contact with the lower surface of the substrate W, and the arm is held by the holding member 12 (). The ministry picked up the substrate W to be processed, so that the robot arm of the transfer robot 98 can be moved below the substrate W to be processed, and the lifting arm 132 can be lowered to carry and hold the substrate to be processed.
O:\87\87879.DOC 1238453 w。 [石英墊圈100之構成] 如圖9與圖1〇所示,於處理交哭? 处理奋杰22之内部,為遮蔽紫外線 而安裝有例如由白色等之不读日日r # +透明石央所形成之石英墊圈 100。又,石英墊圈100係如祛辦、, , a 货如後所述,為组合下部盒體102、 側面盒體104、上部盒體106及舍霜 巴復石央鐘罩112外周之圓筒 狀盒體108之構成。 該石英墊圈100,藉由覆蓋形成製程空間84之處理容器22 與蓋子構件82之内壁,可得到防止處理容器22與蓋子構件 82之熱膨脹之隔熱效果,並防止處理容器22與蓋子構件μ 之内壁因紫外線而氧化,且具有防止金屬污染之任務。 [遠距離電漿部27之構成] 如圖9與圖10所示,於製程空間料供給氮自由基之遠距離 電漿部27,係被安裝於處理容器22之前部22a,並經由供給 管路90連通至處理容器22之供給口 92。 於該遠距離電漿部27中,供給有Ar等之惰性氣體與氮氣 體,藉由電漿將此活性化,可形成氮自由基。如此所形成 之氮自由基會沿著被處理基板w之表面流動而氮化基板表 面。 另外’於其他之氮氣體,亦可實施使用〇2、NO、n20、 NH3氣體等之氧化、氮氧化自由基製程。 [閘極閥96之構成] 如圖9與圖10所示,於處理容器22之後部設置有為搬送被 處理基板W之搬送口 94。該搬送口 94係由閘極閥96所閉塞O: \ 87 \ 87879.DOC 1238453 w. [Structure of Quartz Gasket 100] As shown in Fig. 9 and Fig. 10, do you cry during processing? Inside the processing Fenjie 22, a quartz washer 100 formed of, for example, a white non-reading day r # + transparent stone center is installed to shield ultraviolet rays. In addition, the quartz gasket 100 is a cylindrical box body formed by combining the lower case body 102, the side case body 104, the upper case body 106, and the Sheshuangpao stone central bell cover 112 as described later. Composition of 108. The quartz washer 100 covers the inner walls of the processing container 22 and the lid member 82 forming the process space 84, and can obtain a thermal insulation effect to prevent the thermal expansion of the processing container 22 and the lid member 82, and prevent the processing container 22 and the lid member μ. The inner wall is oxidized by ultraviolet rays and has the task of preventing metal pollution. [Configuration of the long-distance plasma unit 27] As shown in FIG. 9 and FIG. 10, the long-range plasma unit 27 that supplies nitrogen radicals to the process space is installed at the front portion 22a of the processing container 22 and passes through the supply pipe. The path 90 communicates with the supply port 92 of the processing container 22. An inert gas such as Ar and a nitrogen gas are supplied to the long-distance plasma unit 27, and the plasma is activated to form nitrogen radicals. The nitrogen radicals thus formed will flow along the surface of the substrate w to be processed to nitride the surface of the substrate. In addition, it is also possible to carry out oxidation and nitridation radical processes using 02, NO, n20, NH3 gas and the like in other nitrogen gas. [Structure of Gate Valve 96] As shown in FIGS. 9 and 10, a transfer port 94 for transferring the substrate W to be processed is provided at the rear of the processing container 22. The transfer port 94 is closed by a gate valve 96
O:\87\87879DOC • 21 - 1238453 住,僅於搬送被處理基板W時由閘極閥96之打開動作而開 放。 於閘極閥96之後方設置有搬送自動機98。並且,配合閘 極閥96之打開動作,搬送自動機98之機械臂會由搬送口舛 進入至製程空間84之内部,並進行送被處理基板%之交換 作業。 、 [上述各構成部之詳細] (1)在此,詳細說明關於上述氣體噴射噴嘴部93之構成。 圖18係擴大顯示氣體喷射噴嘴部93之構成之縱剖面圖。 圖W係擴大顯示氣體喷射喷嘴部93之構成之橫剖面圖。圖 20係擴大顯示氣體喷射喷嘴部93之構成之前視圖。 如圖18至圖20所示,氣體噴射喷嘴部%於前面中央,具 有可連通上述遠距離電聚部27之供給管路9〇之連通孔 而於連通孔92之上方,則絲有複數㈣射口 93〜〜%於橫 方向配設成一列之喷嘴板叫〜叫。喷射口 93〜〜%心係例 如為直徑1 _的小孔,而以1〇麵之間隔設置。 ’雖設有包含小孔之噴射口 例如亦可為以細小狹縫做為噴射 另外,於本實施例中 93ai〜93an ’但不限於此, 口之構成。 另外,噴嘴板93bl,b3係被鎖緊於氣體喷射喷嘴部… Γ。因A ’自喷射口 9 一η所嘴射之氣體會由氣^ 射喷嘴部93之壁面流向前方。 例如’在嘴射口 93a丨〜93a祐部·番从μ 1δ又置於管狀之喷嘴管路時, 自喷射口 93a 1〜93an所嗔射之齑鲈_立 、耵之虱體一部份會發生回流至噴$O: \ 87 \ 87879DOC • 21-1238453, only when the substrate W to be processed is transported, the gate valve 96 is opened to open. A transfer robot 98 is provided behind the gate valve 96. In addition, in cooperation with the opening operation of the gate valve 96, the robot arm of the transfer robot 98 enters into the processing space 84 through the transfer port 舛, and performs the exchange operation of sending the processed substrate%. [Details of the above-mentioned components] (1) Here, the structure of the gas injection nozzle portion 93 will be described in detail. FIG. 18 is a longitudinal sectional view showing an enlarged configuration of the gas injection nozzle portion 93. FIG. FIG. W is a cross-sectional view showing the structure of the gas injection nozzle section 93 in an enlarged manner. Fig. 20 is an enlarged front view showing the configuration of the gas injection nozzle portion 93. As shown in FIGS. 18 to 20, the gas injection nozzle portion is located at the center of the front surface, and has a communication hole that can communicate with the supply pipe 90 of the long-distance electropolymerization portion 27 and above the communication hole 92. The nozzle plates 93 ~~% are arranged in a row in a horizontal direction. The ejection ports 93 ~~% are, for example, small holes with a diameter of 1 mm, and are arranged at intervals of 10 planes. 'Although a spray port including a small hole is provided, for example, a small slit may be used for spraying. In addition, in this embodiment, 93ai ~ 93an' is not limited to this, and the configuration of the port is not limited thereto. In addition, the nozzle plates 93bl and b3 are locked to the gas injection nozzle portion ... Γ. Since A ', the gas emitted from the nozzle 9 through the nozzle 9 will flow forward from the wall surface of the gas injection nozzle portion 93. For example, when the mouth firing port 93a 丨 ~ 93a, Yubei Fanfan μ 1δ is placed in the tube of the nozzle tube, the part of the perch which is shot from the ejection port 93a 1 ~ 93an is a part of the body Reflow to spray will occur
CH87\87879.DOC -22- 1238453 官路之後方,而在製程空間84產生氣體滯留,引發被處理 基板W周邊之氣體流不安定之問題。 但於本實施例中,因射喷孔93ai〜93an為形成於氣體噴射 喷嘴部93之壁面之構成,故不會產生如此之氣體返·回到喷 嘴後方之現象,可保持於安定被處理基板w周邊氣體流之 層流狀悲。藉此,可均一地形成被處理基板W上之成膜。 另外’在各噴嘴板931^〜93133相對之内壁,形成有具有使 氣體滯留之機能之凹部93ci〜93C3。因該凹部93q〜93h係被 設置於喷射口 之上流,故可平均自各喷射口 93ai〜93an所噴射之氣體之流速。藉此,能平均於製程空間 84全區域之流速。 此外,各凹部93〜〜93〇3可連通貫穿氣體喷射喷嘴部93之 供給孔93(^〜93(13。又,中央之氣體供給孔93(j2不與連通孔 92父又而形成於錯開之位置,折彎成彎曲形狀。 並且,於中央之氣體供給孔931,藉由第i質量控制器97a 而被控制其流量之氣體經由氣體供給管路992而被供應。 又,於被配置於氣體供給孔931左右之氣體供給孔93dl, 934,藉由第2質量控制器97b而被控制其流量之氣體經由 氣體供給管路99!、993而被供應。 另外,第1質量控制器97a與第2質量控制器97b,係經由 氣體供給管路9%、與氣體供給部34連接,並將來自氣體 供給部34所供給之氣體流量控制於預先所設定之流量。 第1質量控制器97a與第2質量控制器97b所供給之氣體, 係經由氣體供給管路99i〜993到達氣體供給孔93dl〜93d3,而 O:\87\87879.DOC -23- 1238453 再由噴射口 93a丨〜93an喷向製程 充填於各凹部93ci〜93c3後 空間84。 /私工間84内之氣體’為了可由延伸於處理容器22之前 部22a之橫向寬幅方向之各喷嘴板9扑1〜兜匕之射喷孔 叫〜93an向製程空間84之全區域噴射,在製程空間84之全 區域以特定流速(層流)流向處理容器22之後部22b側。 ,外,於處理容器22之後部22b側,由於延伸於後部22b 之杈向寬幅方向之長方形排1口74呈現開口,《製程空間 84内之氣體變成流向後方,照特定流速(層流)朝排氣路徑^ 排氣。 另外,於本實施例中,因可控制2個系統之流量,故例如 亦可以第1質量㈣器97a與第2質量控制器97b控制不同之 流量。 藉此,設定使供給於製程空間84内之氣體流量(流速)不 同’亦可使製程空間84内之氣體濃度分佈變化。此外,亦 可以第1貝里控制器97a與第2質量控制器97b供給不同種類 之氣體,例如亦可以第1質量控制器97a進行氮氣體之流量 控制’而以第2質量控制器97b進行氧氣體之流量控制。 使用之氣體例如可為含氧氣體、含氮氣體及稀有氣體等。 (2)在此,詳細說明關於加熱部以之構成。 圖21係擴大顯示加熱部24構成之縱剖面圖。圖22係擴大 顯示加熱部24之仰視圖。 、如_及圖22所示,加熱部24係於链合金製之底座ιι〇裝 載石英4里罩112,經由凸緣140固定於處理容器22之底部CH87 \ 87879.DOC -22- 1238453 is behind the official road, and gas retention occurs in the process space 84, causing the problem of unstable gas flow around the substrate W to be processed. However, in this embodiment, since the injection nozzle holes 93ai to 93an are formed on the wall surface of the gas injection nozzle portion 93, such a phenomenon that the gas returns and returns to the rear of the nozzle does not occur, and it can be maintained on a stable substrate to be processed. w The laminar flow of surrounding gas flow. Thereby, the film formation on the to-be-processed substrate W can be formed uniformly. In addition, recesses 93ci to 93C3 having a function of retaining gas are formed on the inner wall of each of the nozzle plates 931 to 93133. Since the recesses 93q to 93h are provided above the injection ports, the flow velocity of the gas injected from each of the injection ports 93ai to 93an can be averaged. As a result, the flow velocity over the entire area of the process space 84 can be averaged. In addition, each of the recesses 93 to 933 can communicate with the supply hole 93 (^ ~ 93 (13.13) which penetrates the gas injection nozzle section 93, and the central gas supply hole 93 (j2 is not formed in a staggered manner with the communication hole 92). The gas supply hole 931 in the center is supplied with the gas whose flow rate is controlled by the i-th mass controller 97a through the gas supply pipe 992. It is also arranged in The gas supply holes 93dl and 934 around the gas supply hole 931 are supplied with gas whose flow rate is controlled by the second mass controller 97b through the gas supply lines 99! And 993. In addition, the first mass controller 97a and The second quality controller 97b is connected to the gas supply unit 34 via a gas supply line 9%, and controls the flow rate of the gas supplied from the gas supply unit 34 to a preset flow rate. The first quality controller 97a and The gas supplied by the second quality controller 97b reaches the gas supply holes 93dl ~ 93d3 through the gas supply pipes 99i ~ 993, and O: \ 87 \ 87879.DOC -23-1238453 is sprayed from the injection ports 93a 丨 ~ 93an. Filling each recess 93ci ~ 93c3 in the process Space 84. / The gas in the private room 84 is so that the nozzle plate 9 extending in the widthwise direction of the front portion 22a of the processing container 22 can be blown 1 ~ the blast hole of the pocket is called ~ 93an to the entire process space 84 The area spray flows to the rear portion 22b side of the processing container 22 at a specific flow rate (laminar flow) in the entire area of the process space 84. Outside, on the rear portion 22b side of the processing container 22, the branch extending to the rear portion 22b extends in a wide direction. The rectangular port 1 has an opening 74, and the gas in the process space 84 becomes backward, and exhausts toward the exhaust path according to a specific flow rate (laminar flow). In addition, in this embodiment, the flow of the two systems can be controlled Therefore, for example, the first mass converter 97a and the second mass controller 97b can be used to control different flow rates. Thus, by setting the flow rate (flow rate) of the gas supplied to the process space 84 to be different, the flow rate in the process space 84 can also be adjusted. The gas concentration distribution changes. In addition, the first Bailey controller 97a and the second mass controller 97b can be supplied with different types of gases. For example, the first mass controller 97a can be used to control the flow of nitrogen gas, and the second mass The controller 97b controls the flow rate of the oxygen gas. The gas used may be, for example, an oxygen-containing gas, a nitrogen-containing gas, or a rare gas. (2) Here, the structure of the heating section will be described in detail. A longitudinal sectional view of 24. FIG. 22 is a bottom view showing the heating section 24 in an enlarged manner. As shown in FIG. 22 and FIG. 22, the heating section 24 is mounted on a chain alloy base. 140 fixed to the bottom of the processing container 22
O:\87\87879.DOC -24- 1238453 22c。並且,於石英鐘罩112之内部空間113,收容有加 熱器114與熱反射構件116。因此,SlC加熱器114與熱反射 構件116,與處理容器22之製程空間84隔離,不與製程空間 84之氣體接觸,而為不會產生污染之構成。 sic基板設置台118係被載置於與Sic加熱器114相對之石 英鐘罩112上,並可藉由高溫計119來測定溫度。該高溫計 119係藉由隨著SlC基板設置台118被加熱而產生之熱電效 果來測定SiC基板設置台118之溫度者,而於控制電路中, 由藉由高溫計119所檢測之溫度信號來推測被處理基板w 之溫度,再根據該推測溫度控制Sic加熱器114之發熱量。 另外石英鐘罩112之内部空間π 3,如後述於處理容器 22之製程空間84減壓時,減壓系統作動並同時減壓以使與 製程空間84之壓力差變小。因此,石英鐘罩112不必考慮減 C γ驟時之壓力差而加大殼厚(例如3 左右),熱容量小 即可’也因此可提尚加熱時之反應性。 底座U0形成為圓盤狀,於中央具有穿插有保持構件120 之軸120d之中央孔142,而於内部則設置有在圓周方向延伸 而形成之冷卻水用之第1水路144。因底座11〇為鋁合金製, 其熱膨脹率雖大,但可藉由在第1水路144流動冷卻水來冷 卻。 另外,凸緣140為組合介於底座11〇與處理容器22之底部 22c間之第丨凸緣146,與嵌合於第丨凸緣之内周之第2凸 緣148之構成。於第丨凸緣146之内周面,係設置有在圓周方 向延伸而形成之冷卻水用之第2水路15〇。O: \ 87 \ 87879.DOC -24-1238453 22c. A heater 114 and a heat reflecting member 116 are housed in an inner space 113 of the quartz bell cover 112. Therefore, the SlC heater 114 and the heat reflecting member 116 are isolated from the process space 84 of the processing container 22, and are not in contact with the gas in the process space 84, and have a structure that does not cause pollution. The sic substrate setting table 118 is placed on the stone bell cover 112 opposite to the Sic heater 114, and the temperature can be measured by a pyrometer 119. The pyrometer 119 measures the temperature of the SiC substrate setting table 118 by the thermoelectric effect generated as the SlC substrate setting table 118 is heated, and in the control circuit, the temperature signal detected by the pyrometer 119 is used to The temperature of the substrate w to be processed is estimated, and the amount of heat generated by the Sic heater 114 is controlled based on the estimated temperature. In addition, when the internal space π 3 of the quartz bell cover 112 is decompressed in the process space 84 of the processing container 22 as described later, the decompression system operates and decompresses simultaneously to reduce the pressure difference with the process space 84. Therefore, the quartz bell cover 112 does not need to take into account the decrease in the pressure difference of C γ and increase the thickness of the shell (for example, about 3), and the heat capacity is small, and thus the reactivity during heating can be improved. The base U0 is formed in a disc shape, and has a central hole 142 in the center through which the shaft 120d of the holding member 120 is inserted, and a first water passage 144 for cooling water formed in the circumferential direction is provided inside. The base 11 is made of aluminum alloy, and although its thermal expansion coefficient is large, it can be cooled by flowing cooling water through the first water passage 144. In addition, the flange 140 is a combination of a first flange 146 between the base 11 and the bottom 22c of the processing container 22, and a second flange 148 fitted on the inner periphery of the first flange. On the inner peripheral surface of the first flange 146, a second water path 15o for cooling water formed by extending in the circumferential direction is provided.
O:\87\87879.DOC -25- 1238453 上冷卻水供給部46所供給之冷卻水,係藉由在上述水路 144與150流動,冷卻由Sic加熱器114發熱所加熱之底座11〇 與凸緣140 ’並抑制底座110與凸緣14〇之熱膨脹。 另外,於底座110下面設置有:連通有使冷卻水流入於水 路144之第1流入管路152之第1流入口 154,與連通有排出通 過水路144之冷卻水之流出管路156之第1流出口 158。此 外,於底座110下面之外周附近’在圓周方向設置有複數個 (例如8〜12處左右)用於穿插鎖緊於第1凸緣146之螺栓160之 安裝孔162。 另外,於底座110下面之半徑方向上之中間位置附近設置 有:包含測定SiC加熱器114之溫度用之熱電偶之溫度感應 器164,與供給電源至SiC加熱器114之電源纜線連接用端子 166a〜166f。又,在SiC加熱器114形成有3個區域,而電源 纜線連接用端子166a〜166f則分別設置有供給電源至各區 域之+側端子、一側端子。 另外,於凸緣140下面設置有:連通有使冷卻水流入於水 路150之第2流入管路168之第2流入口 170,與連通有排出通 過水路150之冷卻水之流出管路172之第2流出口 174。 圖23係擴大顯示第2流入口 170,及第2流出口 174之安裝 構造之縱剖面圖。圖24係擴大顯示凸緣140之安裝構造之縱 剖面圖。 如圖23所示,於第1凸緣146係設置有可連通第2流入口 170之L字形之連通孔146a。該連通孔146a之邊緣部則被連 通至水路150。又,第2流出口 174亦以與上述第2流入口 170 O:\87\87879.DOC -26- 1238453 相同之構成被連通至水路1 5 〇。 由於水路150係在凸緣140之内部延伸形成於圓周方向, 故藉由冷卻凸緣140,亦間接地冷卻在第丨凸緣146之階狀部 146b與底座110間所挾持之石英鐘罩112之突出部η。之溫 度。藉此,石英鐘罩112之突出部112&可在半徑方向抑制熱 膨脹。 … 如圖23及圖24所示,於石英鐘罩112之突出部112&下面, 在圓周方向於特定間隔設置有複數個位置決定孔丨78。該位 置決定孔178係嵌合被螺入於底座11〇上面之栓176之孔,但 熱膨脹率大之底座110,在半徑方向熱膨脹時為不增加突出 4 112a之負荷’故形成為較栓1 %之外徑更大之大口徑。 即’僅能容許栓176與位置決定孔178之間隙部份,對石英 鐘罩112之突出部112a之底座110之熱膨脹。 另外’因石英鐘罩112之突出部H2a,對第!凸緣146之階 狀部146b設置有半徑方向之間隙,故因此點之故亦僅能容 許間隙之份之底座110之熱膨脹。 石英鐘罩112之突出部U2a下面,係藉由被安裝於底座 110上面之密封構件(〇環)180而密封,石英鐘罩112之突出 部112a上面,則藉由被安裝於第1凸緣146之密封構件(〇環) 182而密封。 此外,第1凸緣146與第2凸緣148之上面,係藉由被安裝 於處理容器22之底部22c之密封構件(〇環)1 84,186所密 封。而第2凸緣148之下面,則是藉由被安裝於底座11〇上面 之密封構件(〇環)188所密封。 O:\87\87879.DOC -27- 1238453 此由於在底座Π〇與凸緣140之間及凸緣140與處理容 器22之底部22(:之間成為雙重密封構造,無論其中何者的密 封構件有破損時亦可由其他密封構件來密封住,故更能提 咼處理容器22與加熱部24間密封構造之信賴性。 例如,石英鐘罩112破裂時或突出部112a產生裂痕時,可 由被配置於較突出部丨12a更外側之密封構件18〇,確保石英 鐘罩112内部之氣密性,並阻止處理容器22内之氣體流出至 外部。 或者,即使是接近加熱部24之密封構件180, 182產生劣化 時,亦可藉由安裝於較加熱部24更為遠遠之位置處之外側 密封構件186, 188,維持處理容器22與底座11〇間之密封性 能而’故亦能防止因長年變化之氣體漏洩。 如圖21所示,SiC加熱器114於石英鐘罩112之内部空間 中,係被載置於熱反射構件116之上面,且藉由立在底 座110上面之複數個夾鉗機構190,而被保持於特定高度。 該夹钳機構190係具有··抵接於熱反射構件116下面之外 筒190a,貫通外筒i9〇a並抵接於Sic加熱器114上面之軸 190b,及對著軸190b擠壓外筒190a之螺旋彈簧192。 並且,由於夾鉗機構190之構成係以螺旋彈簧192之彈菩 力夾住SiC加熱器114與熱反射構件丨16,故例如即使在搬運 時有所振動,SiC加熱器114與熱反射構件116亦能保持不會 接觸到石英鐘罩112。另外,因上述螺旋彈簧1 92之彈著力 為經常保持作用著,故亦可防止因熱膨脹而引起之螺絲鬆 弛,SiC加熱器114與熱反射構件Π6可被保持於不會鬆動之 O:\87\87879.DOC -28- 1238453 安定狀態。 另外,各夾鉗機構190係構成為可對底座110調整SiC加熱 器114與熱反射構件116之高度位置於任意位置,藉由調整 複數個夾鉗機構190之高度位置,能保持於SiC加熱器114與 熱反射構件116之水平。 此外,於石英鐘罩112之内部空間113中安裝有:SiC加熱 器114之各端子,與用於電連接被穿插於底座110之電源規 線連接用端子166a〜166f之連接構件194 a〜194f (但,於圖21 圖示有連接構件194a、194c)。 圖2 5係擴大顯不夹甜機構1 9 0上端部之安裝構造之縱剖 面圖。 如圖25所示,夾钳機構190係鎖緊被栓入於穿插於熱反射 構件116之穿插孔116a與SiC加熱器114之穿插孔U4e之轴 190b上端之螺母193,經由墊片195於軸方向擠壓L字形塾片 197, 199並挾持SiC加熱器114。O: \ 87 \ 87879.DOC -25- 1238453 The cooling water supplied by the cooling water supply unit 46 flows through the water channels 144 and 150 to cool the base 11 heated by the Sic heater 114 and the convex The edge 140 'prevents thermal expansion of the base 110 and the flange 14o. In addition, a first inlet 154 communicating with a first inflow pipe 152 for cooling water to flow into the water passage 144 and a first outlet 156 communicating with the cooling water outflow through the water passage 144 are provided below the base 110. Outlet 158. In addition, a plurality of mounting holes 162 (for example, about 8 to 12 locations) are provided in the circumferential direction near the outer periphery of the lower surface of the base 110 for inserting and locking the bolt 160 of the first flange 146. In addition, a temperature sensor 164 including a thermocouple for measuring the temperature of the SiC heater 114 is provided near a middle position in the radial direction below the base 110, and a terminal for connecting a power cable to the power supply to the SiC heater 114 is provided. 166a ~ 166f. In addition, three areas are formed in the SiC heater 114, and the power supply cable connection terminals 166a to 166f are respectively provided with a + side terminal and a side terminal for supplying power to each area. In addition, a second inflow port 170 communicating with a second inflow pipe 168 for cooling water to flow into the waterway 150 and a second outflow pipe 172 communicating with the cooling water discharged through the waterway 150 are provided below the flange 140. 2flow outlet 174. Fig. 23 is a longitudinal sectional view showing the mounting structure of the second inflow port 170 and the second outflow port 174 in an enlarged manner. Fig. 24 is a longitudinal sectional view showing the mounting structure of the flange 140 in an enlarged manner. As shown in FIG. 23, the first flange 146 is provided with an L-shaped communication hole 146a that can communicate with the second inlet 170. An edge portion of the communication hole 146a is connected to the water path 150. In addition, the second outflow port 174 is also connected to the water passage 150 with the same structure as the second inflow port 170 O: \ 87 \ 87879.DOC -26-1238453. Since the waterway 150 is formed in the circumferential direction extending inside the flange 140, the cooling of the flange 140 also indirectly cools the quartz bell cover 112 held between the stepped portion 146b of the first flange 146 and the base 110. Protrusion η. Temperature. Thereby, the protruding portion 112 & of the quartz bell cover 112 can suppress thermal expansion in the radial direction. ... As shown in Figs. 23 and 24, a plurality of position determining holes 78 are provided below the protruding portion 112 & of the quartz bell cover 112 at a predetermined interval in the circumferential direction. This position determining hole 178 is a hole for the bolt 176 which is screwed into the base 11, but the base 110 with a large thermal expansion coefficient does not increase the load of the protrusion 4 112a when thermally expanding in the radial direction, so it is formed as a bolt 1 The larger the diameter, the larger the diameter. That is, only the gap between the pin 176 and the position determining hole 178 is allowed to thermally expand to the base 110 of the protruding portion 112a of the quartz bell cover 112. In addition, because of the protruding portion H2a of the quartz bell cover 112, right! The stepped portion 146b of the flange 146 is provided with a gap in the radial direction. Therefore, the point can only allow the thermal expansion of the base 110 due to the gap. The underside of the protruding portion U2a of the quartz bell cover 112 is sealed by a sealing member (0 ring) 180 mounted on the base 110, and the upper portion of the protruding portion 112a of the quartz bell cover 112 is mounted on the first flange 146. The sealing member (〇ring) 182 is sealed. The upper surfaces of the first flange 146 and the second flange 148 are sealed by a sealing member (o-ring) 1,84,186 attached to the bottom 22c of the processing container 22. The lower surface of the second flange 148 is sealed by a sealing member (o-ring) 188 mounted on the upper surface of the base 11o. O: \ 87 \ 87879.DOC -27- 1238453 This is due to the double sealing structure between the base Π0 and the flange 140 and between the flange 140 and the bottom 22 (:) of the processing container 22, whichever is the sealing member. If it is damaged, it can be sealed by other sealing members, so it can improve the reliability of the sealing structure between the processing container 22 and the heating portion 24. For example, when the quartz bell cover 112 is broken or the protrusion 112a is cracked, it can be placed in the A sealing member 18 outside the protruding portion 12a ensures the airtightness of the inside of the quartz bell cover 112 and prevents the gas in the processing container 22 from flowing to the outside. Or, even if the sealing members 180, 182 are close to the heating portion 24, At the time of deterioration, the outer sealing members 186 and 188 can be installed further away from the heating section 24 to maintain the sealing performance between the processing container 22 and the base 110, thereby preventing the long-term changes. Gas leakage. As shown in FIG. 21, the SiC heater 114 is placed on the heat reflecting member 116 in the internal space of the quartz bell cover 112, and by a plurality of clamp mechanisms 190 standing on the base 110, The clamp mechanism 190 has an outer cylinder 190a abutting on the lower surface of the heat reflecting member 116, a shaft 190b penetrating the outer cylinder i90a and abutting on the upper surface of the Sic heater 114, and The coil spring 192 of the outer cylinder 190a is pressed against the shaft 190b. Moreover, since the structure of the clamp mechanism 190 is configured to sandwich the SiC heater 114 and the heat reflection member 16 with the spring force of the coil spring 192, for example, even during transportation, With some vibration, the SiC heater 114 and the heat reflecting member 116 can also keep from contacting the quartz bell cover 112. In addition, since the spring force of the coil spring 192 is constantly maintained, it can also be prevented from being caused by thermal expansion. The screws are loosened, and the SiC heater 114 and the heat reflecting member Π6 can be kept in a stable state of O: \ 87 \ 87879.DOC -28- 1238453. In addition, each clamp mechanism 190 is configured to adjust the base 110 The height positions of the SiC heater 114 and the heat reflection member 116 are at arbitrary positions. By adjusting the height positions of the plurality of clamp mechanisms 190, the level of the SiC heater 114 and the heat reflection member 116 can be maintained. In addition, the quartz bell cover 112 Inside Each of the terminals 113 is provided with connection members 194 a to 194f for connecting the terminals of the SiC heater 114 to the power gauge wire connection terminals 166a to 166f that are inserted in the base 110 (however, as shown in FIG. 21) Connecting members 194a, 194c). Fig. 25 is a longitudinal sectional view of the mounting structure of the upper end of the enlarged display device 190, as shown in Fig. 25. As shown in Fig. 25, the clamp mechanism 190 is locked and inserted into the heat-inserting mechanism. The nut 193 on the upper end of the shaft 190b of the reflection member 116 through the insertion hole 116a and the SiC heater 114 through the insertion hole U4e presses the L-shaped cymbals 197, 199 in the axial direction through the gasket 195 and holds the SiC heater 114.
SiC加熱器114,於穿插孔114e插入有L字形之墊片197 199之圓筒部197a,199a,而於圓筒部197a,199a内則穿插有 夹鉗機構190之軸190b。並且,L字形塾片197,199之突出部 197b,199b係抵接於SiC加熱器114之上面、下面。 夾钳機構190之軸190b,係藉由上述螺旋彈簧192之彈簧 力而被施予向下方之力,且夾鉗機構19〇之外筒19〇a藉由上 述螺旋彈簧192之彈簧力而被施予向上方之力。如此,使螺 旋彈簧192之彈簧力產生做為夾鉗力之作用,故熱反射構件 116與SiC加熱器114安定地被保持著,可防止因搬運時之振 O:\87\87879.DOC -29- 1238453 動所引起之破損。In the SiC heater 114, cylindrical portions 197a and 199a of L-shaped gaskets 197 and 199 are inserted into the insertion holes 114e, and shafts 190b of the clamp mechanism 190 are inserted into the cylindrical portions 197a and 199a. The protruding portions 197b and 199b of the L-shaped cymbals 197 and 199 are in contact with the upper and lower surfaces of the SiC heater 114. The shaft 190b of the clamp mechanism 190 is applied with a downward force by the spring force of the coil spring 192, and the outer mechanism 19o of the clamp mechanism 19o is clamped by the spring force of the coil spring 192. Give upward force. In this way, the spring force of the coil spring 192 is generated as a clamping force, so the heat reflecting member 116 and the SiC heater 114 are stably held, which can prevent vibration due to transportation. O: \ 87 \ 87879.DOC- 29-1238453 damage caused by movement.
SiC加熱器114之穿插孔114e,係較L字形之塾片19?a 197b之圓筒部197c,197d之口徑大,故設有間隙。因此,在 因SiC加熱器114之發熱而產生之熱膨脹,使穿插孔丨丨钟與 軸190b相對地變位時,穿插孔U4e可在抵接[字形塾片197, 199之突出部i97b,199b之狀態下於水平方向錯位,防止隨 著熱膨脹之應力的發生。 (3)在此,針對SiC加熱器114說明。 如圖26所不,SiC加熱器114係由:中心部形成為圓形狀 之第1發熱部114a,及包圍住第1發熱部114a之外周而形成 為圓弧狀之第2、第3發熱部114b,114c所構成。又,於sic 加熱器114中心係設置有:被穿插保持構件12〇之軸12〇d之 穿插孔114d。 發熱部114a〜114c係並列地連接至發熱控制電路196,再 由溫度調整器198控制於所設定之任意溫度。於發熱控制電 路196中,係藉由控制由電源2〇〇供給至發熱部1143〜114(:之 電壓’來控制自SiC加熱器114所放射之發熱量。 另外’若因發熱部114a〜114c之容量不同則會增大電源 200之負擔,故於本實施例中,可設定使各發熱部U4a〜114c 之容量(2 KW)成為相同之電阻。 發熱控制電路196係可選擇:控制方法I,同時使發熱部 114a〜114c通電並發熱;控制方法^,配合被處理基板w之 溫度分佈狀況,使中心之第1發熱部丨14a,或外側之第2、 第3發熱部U4b,114c之其中一者發熱;控制方法瓜,配合 O:\87\87879.DOC -30- 1238453 被處理基板W之溫度變化,同時使發熱部U4a〜114c發熱, 及使第1發熱部114a或第2、第3發熱部114b,114c之任一發 敎〇 被處理基板W在藉由上述保持構件120保持之狀態,邊旋 轉邊由各發熱部1丨4a〜114c發熱而被加熱之際,會因外周側 與中心部份之溫度差而使周邊部份朝上方彎翹。但,於本 貝加例中,由於SiC加熱器114係經由熱傳導率佳之以匚基板 °又置台11 8來加熱被處理基板w,故被處理基板w全體是以 來自SiC加熱器114之熱來加熱,可將被處理基板w之周邊 部份與中心部份之溫度差抑制到最小,以防止被處理基板 W的彎翹。 (4)在此,詳細說明有關U2石英鐘罩之構成。 圖27A係顯示石英鐘罩112之構造之俯視圖。圖27b係顯 示石英鐘罩112之構造之縱剖面圖。圖28A為從上方所見石 英鐘罩112之構造之立體圖;圖28B為從下方所見石英鐘罩 112之構造之立體圖。 如圖27A、圖27B與圖28A、圖28B所示,石英鐘罩112由 透明石英所形成,其係具有:於前述突出部112&上方形成 之圓筒部112b、覆蓋圓筒部112b上方之頂板U2c、延伸於 較頂板112c中央之下方之中空部U2d、及為補強被橫向架 设於突出部112a所形成之開口之梁部1 i2e。 由於突出部U2a與頂板112e承受荷重,故形成為較圓筒 部112b為厚。又,石英鐘罩112因延伸於縱方向之中空部 112d與延伸於橫方向之梁部U2e在内部 人入 s文可提咼上 O:\87\87879.DOC -31 - 1238453 下方向與半徑方向之強度。 另外,於梁部112e之中間位置可結合中空部U2d之下端 部份,而中空部112d内之穿插孔112f亦貫通梁部112e。於該 穿插孔112f可穿插保持構件120之軸120d。 並且’於石英鐘罩112之内部空間113插入有前述Sic加熱 器與熱反射構件116。又,雖SiC加熱器U4與熱反射構 件Π6形成為圓盤狀,但為可分割成圓弧狀之構成,可避開 梁部112e並於被插入内部空間113後組裝。 此外’於石英鐘罩112之頂板112c有3處(120度間隔)突 出’其係為支持SiC基板設置台118之輪轂U2g〜U2i。因 此’由輪較i12g〜112im支持之Sic基板設置台118,係被載 置成務从自頂板Π 2c突出之狀態。因此,即使處理容器22 之内部壓力有變化,或因產生溫度變化之Sic基板設置台 118變動至下方時,亦可防止接觸到頂板丨丨2c。 另外,石英鐘罩112之内部壓力,係如後述為進行藉由減 壓系統進行排氣流量的控制,使與處理容器22之製程空間 84之壓力差成為50 Torr以下,故可將石英鐘罩112之厚度製 作成比較薄。因此,由於可將頂板112(:之厚度做成薄約6〜1〇 mm左右,故使得石英鐘罩112之熱容量變小並可藉由提高 加熱柃之熱傳導效率提昇反應性。另外,本實施例之石英 鐘罩Π2,係設計成具有可承受1〇〇T〇rr壓力之強度。 圖29係顯示減壓系統之排氣系統構成之系統圖。 如圖29所示,處理容器22之製程空間料,係如前所述, 閥48a打開後,經由被連通至排氣口”之排氣路徑32,藉由The insertion hole 114e of the SiC heater 114 is larger in diameter than the cylindrical portions 197c and 197d of the L-shaped cymbals 19? A 197b, so a gap is provided. Therefore, when the insertion hole 丨 丨 the clock and the shaft 190b are relatively displaced due to the thermal expansion caused by the heat generated by the SiC heater 114, the insertion hole U4e can abut the [protrusion i97b of the zigzag cymbals 197, 199] In the state of 199b, it is displaced in the horizontal direction to prevent the occurrence of stress due to thermal expansion. (3) Here, the SiC heater 114 will be described. As shown in FIG. 26, the SiC heater 114 is composed of a first heat generating portion 114a having a circular center portion and a second and third heat generating portions having an arc shape surrounding the outer periphery of the first heat generating portion 114a. 114b, 114c. Further, a center of the sic heater 114 is provided with a through hole 114d through which the shaft 12o of the holding member 12o is inserted. The heat generating sections 114a to 114c are connected in parallel to the heat generating control circuit 196, and then controlled by the temperature adjuster 198 to an arbitrary set temperature. In the heat generation control circuit 196, the amount of heat emitted from the SiC heater 114 is controlled by controlling the voltage supplied from the power source 200 to the heat generation sections 1143 to 114 (:). In addition, if the heat generation sections 114a to 114c Different capacity will increase the load of the power supply 200, so in this embodiment, the resistance (2 KW) of each heating unit U4a ~ 114c can be set to the same resistance. The heating control circuit 196 is optional: control method I At the same time, the heating parts 114a to 114c are energized and generate heat; the control method ^ matches the temperature distribution of the substrate w to be processed, so that the first heating part 14a in the center, or the second and third heating parts U4b, 114c of the outer side One of them generates heat; the control method is to match O: \ 87 \ 87879.DOC -30-1238453 to the temperature change of the substrate W to be processed, while heating the heating portions U4a to 114c, and heating the first heating portion 114a or the second and second portions. Any one of the third heat generating sections 114b and 114c. When the substrate W to be processed is heated by the heat generating sections 1a to 114c while rotating while being held by the holding member 120, the substrate W may be heated by the outer periphery. The temperature difference between the side and the center makes the periphery However, in this example, since the SiC heater 114 heats the substrate w to be processed through the substrate with a good thermal conductivity, the substrate ° is set at 11 °, so the entire substrate w is processed from SiC. The heating by the heater 114 can minimize the temperature difference between the peripheral portion and the central portion of the substrate w to be processed to prevent warping of the substrate W to be processed. (4) Here, the U2 quartz clock will be described in detail The structure of the cover. Fig. 27A is a top view showing the structure of the quartz bell cover 112. Fig. 27b is a longitudinal sectional view showing the structure of the quartz bell cover 112. Fig. 28A is a perspective view of the structure of the quartz bell cover 112 seen from above; Fig. 28B is a view from below A perspective view of the structure of the quartz bell cover 112. As shown in FIGS. 27A, 27B, 28A, and 28B, the quartz bell cover 112 is formed of transparent quartz, and has a cylindrical portion 112b formed above the protruding portion 112 & The top plate U2c above the cylindrical portion 112b, the hollow portion U2d extending below the center of the top plate 112c, and the beam portion 1i2e which is laterally stretched over the opening formed by the protruding portion 112a. Because the protruding portion U2a It bears the load with the top plate 112e, so it is thicker than the cylindrical portion 112b. In addition, the quartz bell cover 112 extends in the longitudinal hollow portion 112d and the beam portion U2e in the horizontal direction. O: \ 87 \ 87879.DOC -31-1238453 Downward and radial strength. In addition, the middle part of the beam part 112e can be combined with the lower end of the hollow part U2d, and the through hole 112f in the hollow part 112d is also Through the beam portion 112e. The shaft 120d of the holding member 120 can be inserted into the insertion hole 112f. Further, the aforementioned Sic heater and the heat reflecting member 116 are inserted into the inner space 113 of the quartz bell cover 112. Further, although the SiC heater U4 and the heat reflecting member Π6 are formed in a disc shape, they are divided into arcs, and can be assembled after being inserted into the inner space 113 without the beam portion 112e. In addition, 'the top plate 112c of the quartz bell cover 112 is protruded at three places (120-degree intervals)', it is a hub U2g to U2i which supports the SiC substrate setting stand 118. Therefore, the Sic substrate setting stand 118 supported by the wheels i12g to 112im is placed in a state protruding from the top plate Π 2c. Therefore, even if the internal pressure of the processing container 22 is changed, or the Sic substrate setting table 118 is changed downward due to a temperature change, contact with the top plate 2c can be prevented. In addition, the internal pressure of the quartz bell cover 112 is to control the exhaust flow rate by a pressure reduction system as described later, so that the pressure difference from the process space 84 of the processing container 22 becomes 50 Torr or less. The thickness is made relatively thin. Therefore, since the thickness of the top plate 112 (: can be made as thin as about 6 to 10 mm, the thermal capacity of the quartz bell cover 112 can be reduced and the reactivity can be improved by increasing the heat conduction efficiency of the heating element. In addition, this embodiment The quartz bell cover Π2 is designed to have a strength that can withstand 100 Torr pressure. Figure 29 is a system diagram showing the structure of the exhaust system of the pressure reduction system. As shown in Figure 29, the process space of the processing container 22 As described above, after the valve 48a is opened, it is connected to the exhaust port 32 through the exhaust path 32.
O:\87\87879.DOC -32- 1238453 渦輪分子幫浦50之吸引力而減壓。此外,被連接至渦輪分 子幫浦50之排氣口之真空管路5丨下游,連通至吸引被排氣 氣體之幫浦(MBP) 201。 石英4里罩112之内部空間11 3係經由排氣管路202而被連 接至分流管路51a,而由旋轉驅動部28之外殼122所劃分成 之内部空間1 24,則經由排氣管路2〇4被連接至分流管路 51a 〇 排氣管路202係設置有:測定内部空間1丨3壓力之壓力計 205、 及於石英鐘罩112之内部空間U3減壓之際會打開之閥 206。 又,於分流管路5 ia,如前述係設置有閥48b,且設有 分流閥48b之分歧管路208。而於該分歧管路2〇8設有:在減 壓步驟之初期階段所打開之閥21〇、及為能較閥48b更集中 流量之可變隔膜211。 另外,於渦輪分子幫浦5 0之排氣側設有:開關用之閥 212、測定排氣側之壓力之壓力計214。並且,於渦輪軸清 除用之N2線連通至渦輪分子幫浦5 〇之渦輪管路21 6上設置 有:逆止閥218、隔膜220及閥222。 另外’上述閥206、210、212、222係包含電磁閥,依據 來自控制電路之控制信號而打開。 在如上述所構成之減壓系統中,於進行處理容器22、石 英鉍罩112與旋轉驅動部28之減壓步驟時,並非一口氣地減 壓,而是階段地減壓,使其漸漸地接近真空而減壓。 首先,以打開被設置於石英鐘罩112之排氣管路2〇2之閥 206 ’使石英鐘罩112之内部空間113與製程空間84之間經由 O:\87\87879.DOC -33- 1238453 排氣路徑32成為連通狀態,進行壓力之均一化。藉此,使 知在減壓步驟之開始階段之石英鐘罩丨12之内部空間11 3與 製程空間84間之壓力差變小。 其次’使被設置於上述分歧管路208之閥210打開,由可 4隔膜2 11進行被集中之小流量之減壓。之後,使被設於分 流官路5 1 a之閥48b打開,並階段性地增大排氣流量。 另外’比較由壓力計205所測定之石英鐘罩112之壓力, 與由感應态單元8 5之壓力計8 5 a〜8 5 c所測定之製程空間8 4 之壓力,當兩壓力差為50 Torr以下時,即令閥48b打開。藉 此’於減壓步驟,緩和作用於石英鐘罩n2之内外之壓力 差’並使不需要之應力不會作用於石英鐘罩112以進行減壓 步驟。 並且,於經過特定時間後使閥48a打開,並增大渦輪分子 幫浦50之吸引力所造成之排氣流量,減壓處理容器22、石 英鐘罩112與旋轉驅動部28之内部直到變為真空為止。 (5)在此,針對上述保持構件12〇之構成做說明。 圖30A係顯示保持構件120構成之俯視圖;圖3〇B係顯示 保持構件120構成之側面圖。 如圖3 0 A、圖3 0 B所示,保持構件12 0係由支持被處理基 板W之臂部120a〜120c,及可結合臂部120a〜120c之軸i2〇d 所構成。臂部120a〜120c為防止於製程空間84之污染,且為 了不遮蔽住來自SiC基板設置台118之熱,而由透明石英所 形成,以軸120d之上端為中心軸而以120度間隔在水平方向 成放射狀延伸。 OA87\87879.DOC -34- 1238453 此外,於臂部12〇a〜i2〇c之長方向之中間位置,突出有抵 接於被處理基板W下面之輪轂12〇e〜i2〇g。因此,被處理基 板W係由其抵接輪轂12(^〜12〇§之3點所支持。 如此’由於保持構件120為以點接觸支持被處理基板…之 構成,故對SiC基板設置台118可僅以些許之距離保持被處 理基板w於離開之位置。又,Sic基板設置台118與被處理 基板w之離開距離,例如為丨〜汕mm,較佳為3〜1〇 mm左右。 即’被處理基板W成為以浮在Sic基板設置台118上方之 狀恶旋轉,比起直接被載置於Sic基板設置台118者,來自 SiC基板設置台118之熱可更均一地放射,不易產生周邊部 伤與中心部份之溫度差,亦可防止因溫度差而產生之被處 理基板W之彎輕。 因被處理基板W係被保持在自SiC基板設置台U8離開之 位置,故即使因溫度差而產生彎翹,亦不會接觸到sic基板 設置台118,而隨著定常時之溫度均一化,可恢復至原來之 水平狀態。 另外,保持構件120之軸i2〇d係以不透明石英形成為棒 狀,牙插於上述SiC基板設置台118與石英鐘罩丨12之穿插孔 112f並延伸於下方。如此,雖保持構件12〇為在製程空間84 内保持被處理基板W者,但因係由石英所形成,故亦無須 擔心由金屬製品所造成之污染。 (6)在此,詳細說明有關上述旋轉驅動部28之構成。 圖3 1係顯示被配置於加熱部24下方之旋轉驅動部28之構 成之縱剖面圖。圖32則擴大顯示旋轉驅動部28之縱剖面圖。 O:\87\87879.DOC -35- 1238453 如圖31與圖32所示,在加熱部24之底座110下方鎖緊有用 於支持旋轉驅動部28之托架230。於該托架230係設有··旋 轉位置檢測機構232,及托架冷卻機構234。 此外’於托架230下方插入有穿插固定了保持構件12〇之 軸120d之陶瓷軸126,可藉由螺栓240來固定保持了可轉動 地支持陶瓷軸126之陶瓷軸承236, 237之固定側之外殼122。 於外殼122内,因旋轉部份係由陶瓷軸126與陶瓷軸承236, 237所構成,故可防止金屬之污染。 外设122係具有:穿插有螺栓240之凸緣242,及延伸形成 於凸緣238下方之有底筒狀之間隔壁244。於間隔壁2料之外 周面’設置有可連通前述減壓系統之排氣管路2〇4之排氣孔 246,而外殼122之内部空間124之氣體,係於前述減壓系統 之減壓步驟中,被排氣而減壓。因此,可防止製程空間84 内之氣體沿著保持構件12 0之軸12 0 d流出於外部。 此外’於内部空間124收容有磁鐵聯結器13〇之從動側磁 鐵248。該從動側磁鐵248為防止污染,係由在陶瓷軸126外 周所嵌合之磁鐵罩250所覆蓋住,並安裝成不會與内部空間 124之氣體接觸。 磁鐵罩250係由鋁合金形成為環狀之護罩,在内部形成有 收谷用之環狀空間。收容成内部不會搖晃之.狀態。另外, 磁鐵罩250之接合部份係以電子射束溶接成無間隙結合,係 不會如錫焊般地流出銀而造成污染地加工。 此外’於外殼122之外周,嵌合地設置有形成為筒狀之氛 圍側旋轉部252,經由軸承254, 255可旋轉地支持著。並且, O:\87\87879 DOC -36- 1238453 於氛圍側旋轉部252之内周,安裝有磁鐵聯結器130之驅動 側磁鐵2 5 6。 氛圍側旋轉部252下端部252a係經由傳達構件257可結合 馬達12 8之驅動軸12 8 a。因此,馬達12 8之旋轉驅動能量, 係經由被設在氛圍側旋轉部252之驅動側磁鐵256,與被設 在外殼122内部之從動側磁鐵248間之磁力,被傳達至陶究 軸126並傳達到保持構件120與被處理基板W。 另外,於氛圍側旋轉部252之外側,安裝有檢測氛圍側旋 轉部252旋轉之旋轉檢測單元258。該旋轉檢測單元258係由 被安裝在氛圍側旋轉部252下端部外周之圓盤狀之狹縫板 260, 261,與光學性地檢測狹縫板260, 261之旋轉量之光斷 續器262, 263所構成。 光斷續器262,263係由軸承架264被固定在固定側之外殼 122。並且,於旋轉檢測早元258中,因由一對的光斷續器 262, 263可同時檢測出配合旋轉速度之脈衝,故藉由比較兩 脈衝能提高旋轉檢測精密度。 圖3 3 A係顯示托架冷卻機構2 3 4構成之橫剖面圖,圖3 3 b 則顯示托架冷卻機構234構成之側面圖。 如圖33A、圖33B所示,托架冷卻機構234在托架23〇之内 部,形成有於圓周方向延伸之冷卻水用之水路23〇a。並且, 於水路230a之一端連通有冷卻水供給孔23〇b,而在水路 23 0a之另一端則連通有冷卻水供給排出孔23〇c。 自冷卻水供給部46所供給之冷卻水,由冷卻水供給孔 230b起通過水路230a後,由於是從冷卻水供給排出孔23以 O:\87\87879.DOC -37- 1238453 排出,故可冷卻托架230全體。 圖34係顯示旋轉位置檢測機構232構成之橫剖面圖。 如圖34所示,於托架230之一側面安裝有發光元件266, 而在托架230之另一侧面則安裝有接受來自發光元件266之 光之受光元件268。 另外,於托架230中央,在上下方向貫穿可穿插保持構件 120之軸120d之中央孔230d,而在該中央孔230d處設有交叉 般在橫方向貫穿之貫通孔230e,230f。 發光元件266係被插入在一方之貫通孔230e之邊緣部,而 受光元件268則被插入於另一方之貫通孔230f之邊緣部。於 貫通孔230e與23Of間由於穿插有軸120d,故可由受光元件 268之輸出變化檢測出軸120d之旋轉位置。 (7)在此,詳細說明有關旋轉位置檢測機構232之構成 與作用。 圖35A係顯示旋轉位置檢測機構232之非檢測狀態之圖, 而圖35B則顯示旋轉位置檢測機構232之檢測狀態之圖。 如圖35A所示,保持構件120之軸120d於外周被施以切線 方向之倒角加工。在發光元件266與受光元件268之中間位 置轉動時,該倒角加工部120i會與自發光元件266所發出之 光平行。 此時,來自發光元件266之光,通過倒角加工部120i之旁 邊而被照射到受光元件268。藉此,受光元件268之輸出信 號S會變成ON並傳達至旋轉位置判定電路270。 如圖35B所示,當保持構件120之軸120d轉動,倒角加工 O:\87\87879.DOC -38- 1238453 部12〇1之位置自中間位置偏離時,來自發光元件的光會 被軸120d所遮蔽,使得對旋轉位置判定電路27〇之輸出信號 s變成OFF。 圖36A係顯示旋轉位置檢測機構232之受光元件之輸 出信號s之波形圖,而圖36B則是從旋轉位置判定電路27〇 所輸出之脈衝信號p之波形圖。 如圖36A所示,受光元件268因軸I20d之轉動位置,使得 來自發光元件266的光之受光量(輸出信號s)成放射線狀變 化。於旋轉位置判定電路270中,設定對該輸出信號s之閥 值Η,當輸出信號s成為閥值η以上時則輸出脈衝p。 該脈衝Ρ係做為檢測保持構件12〇轉動位置之檢測信號而 被輪出。即係如圖1〇所示,旋轉位置判定電路27〇判定保持 構件120之臂部120a〜120c不會干涉到昇降臂132之抵接銷 13 8a〜13 8c,且在未干涉到搬送自動機98之機械臂之位置, 而輸出該檢測信號(脈衝P)。 (8)在此,根據由上述旋轉位置判定電路27〇所輸出之 檢測信號(脈衝P),針對進行控制電路之旋轉位置控制處理 作說明。 圖3 7是為了說明控制電路所進行之旋轉位置控制處理之 流程圖。 如圖37所示,控制電路於S11中,當有指示被處理基板… 轉動之控制信號時,則前進至S12使馬達128啟動。接著, 前進至S13,確認受光元件268之信號是否為on。當在sn 受光元件268之信號為ON時,則前進至S14,自檢測信號(脈 O:\87\87879.DOC -39- 1238453 街)之周期汁异出保持構件12〇與被處理基板w之轉動數。 接著,前進至Sl5,確認保持構件12〇與被處理基板1之 轉動數4否為預先所設定之目標轉動數仙。於仍,當保 ^構件120與被處理基板W之轉動數η為達到目標轉動數na 衧,則返回上述S13,再度確認馬達128之轉動數是否有上 昇0 另外,於上述S15中,當,由於保持構件12〇與被 理基板W之轉動數n達到目標轉動數仙,故前進至⑴, 處 確認是否有馬達停止之控制信號。於sn,當無馬達停止之 控制信號時則返回上述313,而當有馬達停止之控制信號時 則前進至川,令馬達停止。緊接著,在si9確認受光元件 268之信號是否為〇N,不斷的重複直到受光元件⑽之传號 變成〇N為止。 "〜 如此,保持構件12〇之臂部120a〜120c不會干涉到昇降臂 132之抵接銷138a〜138e ’且可使其停止在未干涉到搬 動機98之機械臂之位置。 、 另外,於上述旋轉位置控制處王里中,雖係說明了使用由 來自受光元件268之輸出信號之周期求出轉動數之方法之 情形,但例如亦可積算由前述光斷續器262,263所輸 號求出轉動數。 ° 122之側面所形成 (9)在此’詳細說明有關於處理容器 之窗口 75, 76之構成。 圖38為從上方所見窗口 75、 3 9係擴大顯示窗口 7 5之橫剖面 76之安裝處之橫剖 圖。圖40係擴大顯 面圖。圖 示窗口 76 O:\87\87879.DOC -40· 1238453 之橫剖面圖。 女圖38、圖39所示,第1窗口 75係可供給氣體於處理容器 内F所幵》成之製程空間84,由於被減壓成真空,故成氣 密性更高之構成。 ~ 固口 75為具有透明石英272,與遮蔽紫外線UV之玻璃274 之一重構造。透明石英272係於抵接於窗口安裝部276之狀 恶下,第1窗框278由小螺釘277栓住而固定於窗口安裝部 276。於窗口安裝部276之外面,安裝有氣密地密封住與透 明石央272之間之密封構件(〇環)280。此外,於第1窗框278 之外面,於使UV玻璃274抵接之狀態下,由小螺釘284拴住 固定第2窗框282。 如此,窗口 75藉由UV玻璃274可遮蔽由紫外光源(UV燈) 86, 87所照射之紫外線,防止其洩漏至製程空間以之外部, 並藉由密封構件280之密封效果,防止被供給至製程空間84 之氣體流出於外部。 另外’貫穿處理容器22側面之開口 286,係以向著處理容 器22之中央,亦即向著被保持於保持構件120之被處理基板 W之中心,斜斜地貫穿。因此,窗口 75係被設置在從處理 容器22之側面中心偏離之位置,但形成為於橫向可看得較 寬廣之橢圓形狀,而可由外部確認被處理基板界之狀態。 另外,第2窗口 76係與上述窗口 75為相同之構成,具有透 明石英292,與遮蔽紫外線uV玻璃294之二重構造。透明石 英292係以抵接於窗口安裝部296之狀態,將第1窗框298以 小螺釘297鎖住並固定於窗口安裝部296。於窗口安裝部296 O:\87\87879.DOC -41 - U38453 之-夕卜 面安装有氣密地密封住與透明石英292之間之密封構 f r\ ts \ —00此外,於第1窗框298之外面,以使uv玻璃294 狀!,用小螺釘304鎖住並固定第2窗框3。2。 87戶日_ 口 76藉由UV玻璃294遮蔽由紫外光源(UV燈)86, 户、、射之i外線防止其洩漏至製程空間84之外部,並藉 户ί構件300之密封效果,防止被供給至製程空間討之氣 體流出於外部。 、、另:’於本實施例中,雖係以處理容器22之側面配置一 气、了5’ 76之構成做為例子作說明,但不限於此,亦可 又置3個以上的窗口,或者當然亦可設置在側面以外之場 所。 〇〇)在此,說明關於構成石英墊圈100之各盒體1〇2, 1〇4 106, 108 。 ’ 圖9與圖1〇所不,石英塾圈1〇〇為組合下部盒體⑽、側 面盒體104、上部盒體1〇6與1〇8圓筒狀盒體之構成,其各自 ,由不透明石英所形成’以保護崔呂合金製之處理容器如 叉氣體與紫外線傷害,並防止因處理容器22之金屬污染為 目的而設置。 圖41Α係顯示下部盒體1〇2構成之俯視圖,圖彻係顯示 下部盒體102構成之側面圖。 如圖41Α、圖41Β所示,下部盒體1〇2其輪廓形狀係形成 為對應處理容器22之内壁形狀之板狀,而於其中央則形 有相對於SiC基板設置台118與被處理基板^圓形開口 310。該圓形開口 310形成為可插入圓筒狀盒體1〇8之尺寸, O:\87\87879.DOC -42- 1238453 <内周以120度間’设置有用於插入保持構件i 之臂部 120a〜120c之前端部之凹部31〇a〜31〇c。 另外,凹部31〇a〜31〇c之位置,係保持構件12〇之臂部 12〇a〜120c不會干涉到昇降臂Π2之抵接銷13心〜13^,且不 干涉到搬送自動機98之機械臂之位置。 另外,於下部盒體1〇2設置有相對於形成在處理容器22 底部之排氣π74之長方形開σ312。此外,下部盒體1〇2在 下面於非對稱位置設置有決定位置用之突起31扣,3141)。 另外,於上述圓形開口310之内周,形成有嵌合後述圓筒 狀盒體108之突起之凹部310de此外,於下部盒體1〇2之邊 緣部,设置有喪合於側面盒體104之階狀部3 1 5。 圖42A係顯示側面盒體1〇4構成之俯視圖,圖42β為側面 盒體104之前視圖,圖42C為側面盒體1〇4之後視圖,圖42〇 為側面盒體104之左側視圖,圖42E為側面盒體1〇4之右側視 圖。 如圖42A〜圖42E所示,側面盒體1〇4其外形狀係形成為對 應處理容器22之内壁形狀,四角落成R字狀之大致四角形之 框形狀.。在内側形成有製程空間84。 另外,側面盒體104於正面104a設置有:與前述氣體噴射 噴嘴部93之複數個的射喷口 93a相對並於橫方向延伸之細 長形之狹縫316’及設置在與被連通至遠距離電漿部27之連 通孔92相對之位置之u字形開口 317。又,於本實施例中, 係狹縫3丨6與開口 317為連通之構成,但亦可形成為各自獨 立之開口。 O:\87\87879 DOC -43- 1238453 另外,側面盒體104在背面i〇4b上,於與搬送口 94相對之 位置形成有前述搬送自動機98之機械臂通過之凹部Μ 8。 另外,側面盒體1 04在左側面丨〇4c,形成有相對於前述感 應器單元85之圓形孔319,在右側面1〇4(1,則形成有相對於 前述窗口 75, 76,與感應器單元77之孔32〇〜322。 圖43A係顯示上部盒體1〇6構成之仰視圖,圖43β則顯示 上部盒體106構成之側面圖。 如圖43A、圖43B所示,上部盒體1〇6其輪廓形狀形成為 對應處理容器22之内壁形狀之板狀,而於㈣紫外線光源 (uv燈)86, 87之位置則形成有長方形開口 324, 325。此外, 於上部盒體106之邊緣部設置有嵌合側面盒體1〇4之階狀部 326。 另外,上部盒體106設有對應蓋子構件82之形狀之圓形孔 3 27〜329,與長方形之四角孔33〇。 圖44A係顯示圓筒狀盒體1〇8構成之俯視圖,圖44b為圓 筒狀盒體108之側面縱剖面圖,圖44(:則是圓筒狀盒體ι〇8 之側面圖。 如圖44A〜圖44C所示,圓筒狀盒體1〇8形成為如覆蓋住石 英鐘罩112之外周之筒狀,於上端邊緣部設有被插入昇降臂 132之抵接銷138a〜138c之凹部i〇8a〜1〇8c。此外,圓筒狀盒 體108於上端部之外周,形成有嵌合下部盒體1〇2之凹= 310d之配合位置用之突起i〇8d。 (11)在此’說明關於升降桿機構3〇之密封構造。 圖45係擴大顯示升降桿機構3〇之縱剖面圖。圖46則擴大 O:\87\87879.DOC -44 - 1238453 顯示升降桿機構3 0之密封構造之縱剖面圖。 如圖45與圖46所示,升降桿機構3〇係構成為由驅動部136 令昇降軸134昇降使被插入室8〇内之昇降臂132昇降之際, 由蛇腹形狀之伸縮管332覆蓋住被插入室8〇之貫通孔8〇a内 之幵降軸134之外周,防止在室8〇内之污染。 伸縮官332其蛇腹部份為可伸縮之形狀,例如由鎳鉻鐵耐 熱合金或耐蝕鎳合金等所形成。另外,貫通孔8〇a由被穿插 昇降軸134之蓋子構件34〇所閉塞住。 此外,於藉由螺栓334鎖住昇降軸134之上端之昇降臂132 之連接構件336,係嵌合固定有圓筒形狀之陶瓷蓋338。該 陶瓷蓋338為延伸形成於較連接構件336更下方,係被設置 成由覆蓋住伸縮管332之周圍而不在室80内直接露出。 因此,伸縮管332於製程空間84在使昇降臂132上昇之際 會延伸至上方,而由陶瓷所形成之圓筒狀蓋338所覆蓋住。 故,伸縮官332藉由可昇降地被插入貫通孔8〇a之圓筒狀蓋 338,而不會直接曝晒在製程空間料之氣體與熱中,故可防 止因氣體與熱而造成劣化。 (12)以下,說明關於使用基板處理裝置2〇,進行被處理 基板W表面之紫外光自由基氧化處理,與之後所進行之遠 距離電漿自由基氮化處理。 [紫外光自由基氧化處理] 圖47A係顯示使用圖2之基板處理裝置2〇,進行被處理基 板W之自由基氧化情形之側面圖及俯視圖,圖47B係顯示圖 47A構成之俯視圖。O: \ 87 \ 87879.DOC -32-1238453 The attraction of turbo molecular pump 50 reduces pressure. In addition, the vacuum line 5 丨 connected to the exhaust port of the turbo molecular pump 50 is connected to a pump (MBP) 201 that sucks exhaust gas. The internal space 11 3 of the quartz 4 cover 112 is connected to the branch line 51 a through the exhaust line 202, and the internal space 1 24 divided by the housing 122 of the rotary driving section 28 is connected to the exhaust line The 204 is connected to the branch line 51a. The exhaust line 202 is provided with a pressure gauge 205 that measures the pressure in the internal space 1 and 3, and a valve 206 that opens when the internal space U3 of the quartz bell cover 112 is decompressed. Further, the branch line 5 ia is provided with the branch line 208 having the valve 48b and the branch valve 48b as described above. The branch pipe 20 is provided with a valve 21 and a variable diaphragm 211 which can be opened in the initial stage of the pressure reducing step, and can be more concentrated than the valve 48b. In addition, on the exhaust side of the turbo molecular pump 50, a valve 212 for opening and closing and a pressure gauge 214 for measuring the pressure on the exhaust side are provided. In addition, a turbine line 21 6 that communicates with the N2 line for turbine shaft cleaning to the turbo molecular pump 50 is provided with a check valve 218, a diaphragm 220, and a valve 222. In addition, the above-mentioned valves 206, 210, 212, and 222 include solenoid valves and are opened in accordance with a control signal from a control circuit. In the decompression system configured as described above, when the decompression steps of the processing container 22, the quartz bismuth cover 112, and the rotary driving unit 28 are performed, the pressure is not decompressed at one go, but gradually decompressed to gradually reduce the pressure. Close to vacuum and decompress. First, the valve 206 ′ provided in the exhaust pipe 200 of the quartz bell cover 112 is opened, so that the internal space 113 and the process space 84 of the quartz bell cover 112 are discharged through O: \ 87 \ 87879.DOC -33-1238453. The air path 32 is in a connected state, and the pressure is uniformized. Thereby, the pressure difference between the internal space 11 3 and the process space 84 of the quartz bell cover 12 at the beginning of the decompression step is made small. Secondly, the valve 210 provided in the branch line 208 is opened, and the concentrated small-flow decompression is performed by the separable diaphragm 2 11. After that, the valve 48b provided in the diverting official path 5 1 a is opened, and the exhaust flow rate is increased stepwise. In addition, 'compare the pressure of the quartz bell cover 112 measured by the pressure gauge 205 with the pressure of the process space 8 4 measured by the pressure gauges 8 5 a to 8 5 c of the inductive state unit 8 5 when the pressure difference is 50 Torr In the following case, the valve 48b is opened. By this, in the decompression step, the pressure difference acting on the inside and outside of the quartz bell cover n2 is relaxed, and unnecessary stress is not applied to the quartz bell cover 112 to perform the decompression step. In addition, the valve 48a is opened after a certain time has elapsed, and the exhaust gas flow rate caused by the attraction of the turbo molecular pump 50 is increased. The inside of the pressure reduction processing container 22, the quartz bell cover 112, and the rotation driving portion 28 is reduced to a vacuum. until. (5) Here, the structure of the said holding member 120 is demonstrated. Fig. 30A is a plan view showing the structure of the holding member 120; Fig. 30B is a side view showing the structure of the holding member 120. As shown in FIGS. 30A and 30B, the holding member 120 is composed of arm portions 120a to 120c supporting the substrate W to be processed, and an axis i20d that can be combined with the arm portions 120a to 120c. The arm portions 120a to 120c are formed of transparent quartz to prevent contamination in the process space 84 and not to shield the heat from the SiC substrate setting table 118. The upper end of the axis 120d is used as the center axis at a horizontal interval of 120 degrees. The direction extends radially. OA87 \ 87879.DOC -34-1238453 In addition, at the middle position in the longitudinal direction of the arm portions 120a to i2oc, the hubs 120e to i20g abutting on the substrate W to be processed protrude. Therefore, the substrate W to be processed is supported by the abutting hub 12 (^ ~ 12〇§ 3 points). Thus, since the holding member 120 is configured to support the substrate to be processed with point contact, the stage 118 is provided for the SiC substrate. It is possible to maintain the separated position of the substrate w to be processed only by a small distance. In addition, the separation distance between the Sic substrate setting table 118 and the substrate to be processed w is, for example, 丨 ~ Shan mm, preferably about 3 to 10 mm. 'The substrate W to be processed has a vicious rotation floating above the Sic substrate setting table 118. Compared with those directly placed on the Sic substrate setting table 118, the heat from the SiC substrate setting table 118 can be more uniformly radiated, and it is not easy to generate. The temperature difference between the peripheral wound and the central part can also prevent the substrate W from being bent due to the temperature difference. Since the substrate W to be processed is maintained at a position separated from the SiC substrate setting table U8, Warping occurs due to the temperature difference, and it will not contact the sic substrate setting table 118, and it can be restored to the original horizontal state as the temperature is uniform at a constant time. In addition, the axis i2od of the holding member 120 is made of opaque quartz. Formed into rods, It is inserted into the above-mentioned SiC substrate setting table 118 and the quartz bell cover 112f and extends below. In this way, although the holding member 120 holds the substrate W to be processed within the process space 84, it is formed of quartz. Therefore, there is no need to worry about contamination caused by metal products. (6) Here, the structure of the above-mentioned rotary driving section 28 will be described in detail. FIG. 31 shows the structure of the rotary driving section 28 arranged below the heating section 24. Vertical sectional view. Figure 32 is an enlarged longitudinal sectional view of the rotary drive section 28. O: \ 87 \ 87879.DOC -35- 1238453 As shown in Figure 31 and Figure 32, it is useful to lock under the base 110 of the heating section 24 A bracket 230 supporting the rotation driving portion 28. A rotation position detecting mechanism 232 and a bracket cooling mechanism 234 are provided on the bracket 230. In addition, a holding member 12 is inserted and fixed below the bracket 230. The ceramic shaft 126 of the shaft 120d can be fixed by a bolt 240 to hold the housing 122 on the fixed side of the ceramic bearings 236, 237 that rotatably support the ceramic shaft 126. Inside the housing 122, the ceramic shaft is used for the rotating part. 126 and ceramic bearings 236, 237 Therefore, the metal can be prevented from being contaminated. The peripheral device 122 includes a flange 242 with bolts 240 interposed therebetween and a bottomed cylindrical partition wall 244 extending below the flange 238. It is provided on the peripheral surface of the partition wall 2 There is an exhaust hole 246 which can communicate with the exhaust line 204 of the aforementioned decompression system, and the gas in the internal space 124 of the casing 122 is decompressed by being exhausted in the decompression step of the aforementioned decompression system. Therefore, the gas in the process space 84 can be prevented from flowing to the outside along the axis 12 0 d of the holding member 12 0. Further, a driven side magnet 248 of the magnet coupling 13 is housed in the internal space 124. The driven-side magnet 248 is covered with a magnet cover 250 fitted on the outer periphery of the ceramic shaft 126 to prevent contamination, and is mounted so as not to contact the gas in the internal space 124. The magnet cover 250 is a ring-shaped cover formed of an aluminum alloy, and a ring-shaped space for valley harvesting is formed inside. Contained in a state that will not shake. In addition, the joint portion of the magnet cover 250 is welded with an electron beam to form a gap-free connection, and it does not flow out of silver like soldering to cause contamination. In addition, on the outer periphery of the housing 122, a cylindrical-shaped surrounding-side rotating portion 252 is fitted and fitted, and is rotatably supported by bearings 254, 255. In addition, O: \ 87 \ 87879 DOC -36-1238453 is provided on the inner periphery of the atmosphere-side rotating portion 252 with the driving-side magnet 2 5 6 of the magnet coupling 130. The lower end portion 252a of the atmosphere-side rotating portion 252 is connected to the drive shaft 12 8a of the motor 12 8 via the transmission member 257. Therefore, the rotational driving energy of the motor 128 is transmitted to the ceramic shaft 126 through the magnetic force between the driving-side magnet 256 provided in the atmosphere-side rotating portion 252 and the driven-side magnet 248 provided inside the housing 122. It is transmitted to the holding member 120 and the substrate W to be processed. Further, a rotation detection unit 258 for detecting the rotation of the atmosphere-side rotating portion 252 is mounted outside the atmosphere-side rotating portion 252. The rotation detection unit 258 is a disc-shaped slit plate 260, 261 mounted on the outer periphery of the lower end portion of the atmosphere-side rotation portion 252, and a photo interrupter 262 that optically detects the rotation amount of the slit plate 260, 261. , 263. The photointerrupters 262 and 263 are fixed to the housing 122 by the bearing frame 264. Furthermore, in the rotation detection early element 258, since a pair of optical interrupters 262, 263 can simultaneously detect pulses matching the rotation speed, the accuracy of rotation detection can be improved by comparing the two pulses. FIG. 3 A is a cross-sectional view showing the structure of the bracket cooling mechanism 2 3 4, and FIG. 3 3 b is a side view showing the structure of the bracket cooling mechanism 234. As shown in Figs. 33A and 33B, the bracket cooling mechanism 234 is formed inside the bracket 23o with a water channel 23a for cooling water extending in the circumferential direction. A cooling water supply hole 23b is communicated with one end of the water path 230a, and a cooling water supply discharge hole 23c is communicated with the other end of the water path 230a. The cooling water supplied from the cooling water supply unit 46 passes through the water passage 230a from the cooling water supply hole 230b, and is discharged from the cooling water supply discharge hole 23 at O: \ 87 \ 87879.DOC -37- 1238453, so it can be discharged. The entire cooling bracket 230. FIG. 34 is a cross-sectional view showing the configuration of the rotation position detecting mechanism 232. As shown in FIG. 34, a light emitting element 266 is mounted on one side of the bracket 230, and a light receiving element 268 that receives light from the light emitting element 266 is mounted on the other side of the bracket 230. In the center of the bracket 230, a central hole 230d through which the shaft 120d of the holding member 120 can be inserted is penetrated in the up-down direction, and through-holes 230e, 230f are formed in the central hole 230d to cross in the transverse direction. The light emitting element 266 is inserted into the edge portion of the one through hole 230e, and the light receiving element 268 is inserted into the edge portion of the other through hole 230f. Since the shaft 120d is interposed between the through holes 230e and 23Of, the rotation position of the shaft 120d can be detected from the output change of the light receiving element 268. (7) Here, the configuration and function of the rotational position detection mechanism 232 will be described in detail. FIG. 35A is a diagram showing a non-detection state of the rotation position detection mechanism 232, and FIG. 35B is a diagram showing a detection state of the rotation position detection mechanism 232. As shown in FIG. 35A, the shaft 120d of the holding member 120 is chamfered in the tangential direction on the outer periphery. When the intermediate position between the light-emitting element 266 and the light-receiving element 268 is rotated, the chamfered portion 120i is parallel to the light emitted from the light-emitting element 266. At this time, the light from the light-emitting element 266 is irradiated to the light-receiving element 268 through the side of the chamfered portion 120i. Thereby, the output signal S of the light receiving element 268 is turned ON and transmitted to the rotation position determination circuit 270. As shown in FIG. 35B, when the axis 120d of the holding member 120 rotates and the position of the chamfering process O: \ 87 \ 87879.DOC -38-1238453 part 1201 deviates from the middle position, the light from the light emitting element will be subjected to the axis It is shielded by 120d, so that the output signal s of the rotation position determination circuit 270 becomes OFF. Fig. 36A is a waveform diagram showing the output signal s of the light receiving element of the rotation position detecting mechanism 232, and Fig. 36B is a waveform diagram of the pulse signal p output from the rotation position determination circuit 27o. As shown in FIG. 36A, the light-receiving element 268 rotates on the axis I20d, so that the light-receiving amount (output signal s) of the light from the light-emitting element 266 changes radially. The rotational position determination circuit 270 sets a threshold value 对该 for the output signal s, and outputs a pulse p when the output signal s becomes equal to or greater than the threshold value η. The pulse P is turned out as a detection signal for detecting the rotation position of the holding member 120. That is, as shown in FIG. 10, the rotation position determining circuit 27 determines that the arms 120a to 120c of the holding member 120 will not interfere with the contact pins 13 8a to 13 8c of the lifting arm 132, and does not interfere with the transfer robot. Position of the robotic arm 98, and outputs the detection signal (pulse P). (8) Here, based on the detection signal (pulse P) output from the rotation position determination circuit 270, the rotation position control processing of the control circuit will be described. Fig. 37 is a flowchart for explaining the rotational position control process performed by the control circuit. As shown in FIG. 37, the control circuit is in S11. When there is a control signal instructing the substrate to be processed ..., it proceeds to S12 to start the motor 128. Next, the process proceeds to S13 to check whether the signal of the light receiving element 268 is on. When the signal of the light receiving element 268 is ON, the process proceeds to S14, and the periodicity of the self-detection signal (pulse O: \ 87 \ 87879.DOC -39-1238453 Street) is different from the holding member 12o and the substrate w to be processed. The number of rotations. Next, the process proceeds to S15, and it is confirmed whether the number of rotations 4 of the holding member 12 and the substrate 1 to be processed is a target number of rotations set in advance. Yu still, when the rotation number η of the protection member 120 and the substrate W to be processed reaches the target rotation number na 则, return to the above S13, and confirm again whether the rotation number of the motor 128 has increased by 0. In addition, in the above S15, when, Since the number of rotations n of the holding member 12 and the substrate W reaches the target number of rotations, the process proceeds to ⑴ to check whether there is a control signal for the motor to stop. In sn, when there is no control signal for motor stop, it will return to the above 313, and when there is a control signal for motor stop, it will advance to Sichuan to stop the motor. Next, it is checked at si9 whether the signal of the light receiving element 268 is ON, and it is repeated until the signal of the light receiving element ⑽ becomes ON. " In this way, the arm portions 120a to 120c of the holding member 120 will not interfere with the abutment pins 138a to 138e of the lifting arm 132, and can be stopped at a position where the robot arm 98 does not interfere. In addition, in the above-mentioned rotary position control section Wang Lizhong, although the method of using the period of the output signal from the light receiving element 268 to determine the number of rotations has been described, for example, the numbers input by the aforementioned optical interrupters 262, 263 may be accumulated. Find the number of rotations. ° 122 side (9) Here, the structure of the windows 75 and 76 of the processing container will be described in detail. Fig. 38 is a cross-sectional view of the installation position of the cross section 76 of the enlarged display window 75 as seen from the top of the windows 75 and 39. Figure 40 is an enlarged view. Figure window 76 O: \ 87 \ 87879.DOC -40 · 1238453 cross section. As shown in Fig. 38 and Fig. 39, the first window 75 is a process space 84 formed by a gas that can be supplied to the processing container F. Since it is decompressed to a vacuum, it has a more airtight structure. ~ Solid mouth 75 is a heavy structure with transparent quartz 272 and a glass 274 that shields UV rays. The transparent quartz 272 is in contact with the window mounting portion 276, and the first window frame 278 is fixed to the window mounting portion 276 by a small screw 277. A sealing member (o-ring) 280 that air-tightly seals between the window mounting portion 276 and the transparent center 272 is installed. In addition, the second window frame 282 is fastened by a small screw 284 on the outer surface of the first window frame 278 while the UV glass 274 is in contact with the second window frame 278. In this way, the window 75 can shield the ultraviolet light irradiated by the ultraviolet light source (UV lamp) 86, 87 by the UV glass 274, prevent it from leaking to the outside of the process space, and prevent the supply to the window by the sealing effect of the sealing member 280. The gas in the process space 84 flows out. In addition, the opening 286 penetrating through the side surface of the processing container 22 penetrates obliquely toward the center of the processing container 22, that is, toward the center of the processing substrate W held by the holding member 120. Therefore, the window 75 is provided at a position deviated from the center of the side surface of the processing container 22, but is formed in an elliptical shape which can be seen in a wide width in the lateral direction, and the state of the boundary of the substrate to be processed can be confirmed from the outside. In addition, the second window 76 has the same structure as the above-mentioned window 75, and has a double structure of transparent quartz 292 and ultraviolet-shielding uV glass 294. The transparent stone 292 is in a state of being in contact with the window mounting portion 296, and the first window frame 298 is locked and fixed to the window mounting portion 296 with a small screw 297. At the window mounting part 296 O: \ 87 \ 87879.DOC -41-U38453, a sealing structure fr \ ts \ —00 which is hermetically sealed with transparent quartz 292 is installed on the surface of the U38453. In addition, on the first window The outside of the frame 298 to make the uv glass 294! , Use small screws 304 to lock and fix the second window frame 3.2. 87 households day_mouth 76 is shielded by ultraviolet light source (UV lamp) 86, UV, UV light 294, UV and UV light outside to prevent it from leaking to the outside of the process space 84, and the sealing effect of the member 300 to prevent The gas supplied to the process space flows out. …, And: “In this embodiment, although the configuration of 5 ′ 76 is arranged on the side of the processing container 22 as an example, it is not limited to this, and three or more windows may be placed, or Of course, it can also be installed in a place other than the side. 〇〇) Here, the respective cases 10, 102, 108, 108 constituting the quartz gasket 100 will be described. 9 and FIG. 10, the quartz ring 100 is a combination of a lower case ⑽, a side case 104, an upper case 10 and a 108 cylindrical case, each of which is composed of The opaque quartz is formed for the purpose of protecting the processing container made of Cui Lu alloy such as fork gas and ultraviolet rays, and preventing metal pollution of the processing container 22. Fig. 41A is a plan view showing the structure of the lower case 102, and Fig. 41A is a side view showing the structure of the lower case 102. As shown in FIG. 41A and FIG. 41B, the lower box body 102 is formed in a plate shape corresponding to the shape of the inner wall of the processing container 22, and at the center thereof, a SiC substrate setting table 118 and a substrate to be processed are formed. ^ Circular opening 310. The circular opening 310 is formed in a size that can be inserted into the cylindrical box body 108, and O: \ 87 \ 87879.DOC -42-1238453 < an arm for inserting the holding member i is provided at an inner periphery of 120 degrees The recesses 31a to 31c at the ends before the portions 120a to 120c. In addition, the positions of the recessed portions 31〇a to 31〇c, the arm portions 120a to 120c of the holding member 12o do not interfere with the contact pins 13 of the lifter arm 2 and 13 ^, and do not interfere with the transfer robot Position of the robotic arm 98. In addition, a rectangular opening σ312 is provided in the lower case 102 with respect to the exhaust gas π74 formed at the bottom of the processing container 22. In addition, the lower case 102 is provided with a projection 31 for determining the position at an asymmetric position below, 3141). In addition, a concave portion 310de is formed on the inner periphery of the circular opening 310 to fit a protrusion of the cylindrical case 108 described later. In addition, an edge portion of the lower case 10 is provided with a side case 104. Of step-like part 3 1 5. 42A is a plan view showing the side box body 104, FIG. 42β is a front view of the side box 104, FIG. 42C is a rear view of the side box 104, and FIG. 42 is a left side view of the side box 104, FIG. 42E It is a right side view of the side box body 104. As shown in Figs. 42A to 42E, the outer shape of the side box body 104 is formed into a substantially rectangular frame shape corresponding to the inner wall shape of the processing container 22 and the four corners are R-shaped. A process space 84 is formed on the inside. In addition, the side box 104 is provided on the front surface 104a with an elongated slit 316 'opposite to the plurality of gas injection nozzles 93a of the gas injection nozzle portion 93 and extending in the horizontal direction, and is provided to be connected to a long-distance electrical connection. A u-shaped opening 317 at a position opposite to the communication hole 92 of the slurry portion 27. In this embodiment, the slits 3 and 6 and the opening 317 are connected to each other, but they may be formed as separate openings. O: \ 87 \ 87879 DOC -43- 1238453 In addition, the side box 104 is formed with a recess M 8 through which the robot arm of the aforementioned transfer robot 98 passes, at a position opposite to the transfer port 94 on the back surface 104b. In addition, the side box 104 is formed with a circular hole 319 corresponding to the aforementioned sensor unit 85 on the left side and 04c, and on the right side 104 (1, it is formed with respect to the aforementioned windows 75, 76, and Holes 32 ~ 322 of the sensor unit 77. Fig. 43A is a bottom view showing the structure of the upper box 106, and Fig. 43β is a side view showing the structure of the upper box 106. As shown in Figs. 43A and 43B, the upper box The outline of the body 106 is formed into a plate shape corresponding to the shape of the inner wall of the processing container 22, and rectangular openings 324 and 325 are formed at positions of ultraviolet light sources (uv lamps) 86 and 87. In addition, the upper case 106 The edge portion is provided with a stepped portion 326 for fitting the side box body 104. In addition, the upper box body 106 is provided with circular holes 3 27 to 329 corresponding to the shape of the cover member 82, and rectangular rectangular hole 33. FIG. 44A is a plan view showing the structure of the cylindrical box body 108, FIG. 44b is a side longitudinal sectional view of the cylindrical box body 108, and FIG. 44 (: is a side view of the cylindrical box body 08. As shown in FIG. 44A to FIG. 44C, the cylindrical box body 108 is formed in a cylindrical shape such as to cover the outer periphery of the quartz bell cover 112. Concave portions 008a to 108c of the contact pins 138a to 138c inserted into the lifting arm 132 are provided on the upper edge portion. In addition, the cylindrical case 108 is formed with a fitting lower case 1 on the outer periphery of the upper end. Concavity of 〇2 = protrusion io8d for mating position of 310d. (11) Here, the sealing structure of the lifting rod mechanism 30 will be described. Fig. 45 is an enlarged longitudinal sectional view of the lifting rod mechanism 30. Fig. 46 O: \ 87 \ 87879.DOC -44-1238453 shows a longitudinal sectional view of the sealing structure of the lifter mechanism 30. As shown in FIGS. 45 and 46, the lifter mechanism 30 is constituted by the driving section 136 command When the lifting shaft 134 is raised and lowered to raise and lower the lifting arm 132 inserted into the chamber 80, the bellows-shaped telescopic tube 332 covers the outer periphery of the lower shaft 134 in the through hole 80a of the inserted chamber 80 to prevent Contamination in the chamber 80. The telescopic officer 332 has a telescopic shape, for example, formed of a nickel-chromium heat-resistant alloy or a corrosion-resistant nickel alloy. In addition, the through-hole 80a is covered by a cover inserted into the lifting shaft 134. The member 34 is closed. In addition, the lifting arm 13 at the upper end of the lifting shaft 134 is locked by a bolt 334 The connecting member 336 of 2 is fitted with a cylindrical ceramic cover 338 fitted and fixed. The ceramic cover 338 is formed to extend below the connecting member 336 and is provided to cover the periphery of the telescopic tube 332 instead of the chamber 80. Therefore, the telescopic tube 332 in the process space 84 is extended to the upper side when the lifting arm 132 is raised, and is covered by a cylindrical cover 338 formed of ceramic. Therefore, the telescopic official 332 can be raised and lowered by The cylindrical cover 338 inserted into the through hole 80a is not directly exposed to the gas and heat of the process space material, so the deterioration due to the gas and heat can be prevented. (12) The following is a description of the use of the substrate processing apparatus 20 to perform the ultraviolet radical oxidation treatment on the surface of the substrate W to be processed and the long-distance plasma radical nitridation treatment performed thereafter. [Ultraviolet Radical Oxidation Treatment] Fig. 47A is a side view and a plan view showing the radical oxidation of the substrate W to be processed using the substrate processing apparatus 20 of Fig. 2, and Fig. 47B is a plan view showing the structure of Fig. 47A.
O:\87\87879.DOC -45- 1238453 如圖47A所示,於前述製程空間84中,可由氣體喷射喷嘴 部93供給氧氣體,並於沿著被處理基㈣之表面流動後, 經由排氣口 74、满輪分子幫浦5()與幫浦2〇1排氣。藉由使用 渦輪分子幫浦50 ’前述製程空間84之製程廢力,係被設定 在因基板W之氧自由基之氧化所需之1〇-3〜1〇-6丁。汀之範圍。 同時,較理想的係藉由驅動產生172 nm2波長之紫外光 之紫外線光源86, 87’而在如此形成之氧氣流中形成氧自由 基所开/成之氧自由基在延著前述被處理基板%之表面流 動之際,會氧化旋轉之基板表面。藉由因如此之被處理基 板W之氧自由基之氧化,在石夕基板表面,可安定且再現性 佳地形成i nm以下之膜厚非常薄之氧化膜,特別是相當於 2〜3原子層之約ο·# nm膜厚之氧化膜。 如圖47B所示,可知紫外線光源86,87為延伸於與氧氣流 方向交又之方向之管狀光源,渦輪分子幫浦別會經由排氣 口 74排出製程空間84之氣體。另一方面,由前述排氣心 直接通至幫浦50之圖47B中以點線所示之排氣路徑係藉由 關閉住閥48b而被遮蔽。 圖48係顯示於圖2之基板處理裝置如中,藉由圖、圖 47B之"步驟設定基板溫度於4赋,並_邊使紫外光照射強 度與乳氣流量,或氧分壓作各種變化一邊於石夕基板表面形 成石夕氧化膜之情形時,膜厚與氧化時間之關係"但於在圖 48之實驗中’係在自由基氧化之前除去石夕基板表面之自然 ’又有時’於紫外光激發氮自由基中除去殘留於基 板表面之碳,此外,更於Ar氛圍中,藉由進行於約9赃之O: \ 87 \ 87879.DOC -45- 1238453 As shown in FIG. 47A, in the aforementioned process space 84, oxygen gas can be supplied from the gas injection nozzle portion 93, and after flowing along the surface of the substrate to be processed, it is discharged through Air port 74, full-wheel molecular pump 5 () and pump 201 are exhausted. By using the turbo molecular pump 50 'process waste force of the aforementioned process space 84, it is set at 10-3 to 10-6 d, which is required for the oxidation of oxygen radicals of the substrate W. Ting range. At the same time, it is desirable to drive the ultraviolet light source 86, 87 'which generates ultraviolet light with a wavelength of 172 nm2 to generate oxygen radicals formed / formed by oxygen radicals in the thus-formed oxygen stream to extend the substrate to be processed. When the% surface flows, the rotating substrate surface is oxidized. As a result of the oxidation of the oxygen radicals of the substrate W to be processed, an extremely thin oxide film with a thickness of less than 1 nm can be formed on the surface of the Shixi substrate with stability and reproducibility, especially equivalent to 2 to 3 atoms. The thickness of the layer is about ο · # nm. As shown in FIG. 47B, it can be seen that the ultraviolet light sources 86, 87 are tubular light sources extending in a direction intersecting with the direction of the oxygen flow, and the turbo molecular pump will exhaust the gas in the process space 84 through the exhaust port 74. On the other hand, the exhaust path shown by the dotted line in FIG. 47B that leads directly from the aforementioned exhaust core to the pump 50 is blocked by closing the valve 48b. Fig. 48 shows the substrate processing apparatus shown in Fig. 2. As shown in Fig. 47B, the substrate temperature is set to 4 °, and the ultraviolet light irradiation intensity and breast gas flow rate, or the oxygen partial pressure are variously adjusted. In the case where the Shiyu substrate is formed on the surface of the Shiyu substrate, the relationship between the film thickness and the oxidation time is "but in the experiment shown in Fig. 48," the nature of removing the surface of the Shixi substrate before the free radical oxidation "has The carbon remaining on the surface of the substrate is removed in the UV light excited nitrogen radicals. In addition, in an Ar atmosphere,
O:\87\87879.DOC -46- 1238453 高溫熱處理,平坦化基板表面。另外,作為前述紫外線光 源86,87係使用波長為1 72 nm之激分子燈。 參照圖48,系列1之資料,係顯示將紫外光照射強度設定 於紫外光源24B之窗面之基準強度(5〇 mW/cm2)之5%,製程 壓力設定成665 mPa(5m Torr)、氧氣流量設定成30 SCCM時 之氧化時間與氧化膜厚之關係,而系列2之資料,則顯示將 紫外光強度設定成0,製程壓力設定成133Pa (1 T〇rr)、氧氣 流量設定成3SLM之情形之氧化時間與氧化膜厚之關係。 又’系列3之資料,係顯示將紫外光強度設定成〇,製程壓 力設定成2.66Pa(20m Torr),氧氣流量設定成150 SCCM之情 形之氧化時間與氧化膜厚之關係,而系列4之資料,則顯示 將紫外光強度設定成1 〇〇%,即設定成前述基準強度,製程O: \ 87 \ 87879.DOC -46- 1238453 High temperature heat treatment to flatten the substrate surface. In addition, as the ultraviolet light source 86, 87, an excimer lamp having a wavelength of 1 72 nm was used. Referring to FIG. 48, the data of Series 1 shows that the intensity of ultraviolet light irradiation is set to 5% of the reference intensity (50mW / cm2) of the window surface of the ultraviolet light source 24B, and the process pressure is set to 665 mPa (5m Torr) and oxygen. The relationship between the oxidation time and the oxide film thickness when the flow rate is set to 30 SCCM, and the data of Series 2 shows that the ultraviolet light intensity is set to 0, the process pressure is set to 133Pa (1 Torr), and the oxygen flow rate is set to 3SLM. The relationship between the oxidation time and the thickness of the oxide film. The data of Series 3 shows the relationship between the oxidation time and the thickness of the oxide when the ultraviolet light intensity is set to 0, the process pressure is set to 2.66Pa (20m Torr), and the oxygen flow rate is set to 150 SCCM. Data, it shows that the UV light intensity is set to 100%, that is, set to the aforementioned reference intensity.
壓力設定成2.66Pa(20m Torr)、氧氣流量設定成150 SCCM 之情形之氧化時間與氧化膜厚之關係。此外,系列5之資 料’係顯示將紫外光強度設定成基準強度之2〇%,製程壓 力設定成2.66Pa(20m Torr)、氧氣流量設定成150 SCCM之情 形之氧化時間與氧化膜厚之關係,而系列6之資料,則顯示 將紫外光強度設定成基準強度之2〇%,製程壓力約為67Pa (〇·5 Torr)、氧氣流量為〇.5SLm時之氧化時間與氧化膜厚之 關係。此外,系列7之資料,係顯示將紫外光強度設定成基 準強度之20%,製程壓力設定成665Pa (5 T〇rr)、氧氣流量 設定成2SLM時之氧化時間與氧化膜厚之關係,而系列8之 資料,則顯示將紫外光強度設定成基準強度之5%,製程壓 力為2.66Pa(20m Torr)、氧氣流量為150SCCM時之氧化時間 O:\87\87879.DOC -47- 1238453 與氧化膜厚之關係。 於圖48之實驗中,氧化膜之膜厚係由xps法所求得,但 刖並又有可夂取如此低於i麵非常薄的氧化膜膜厚之統 一的方法。 因此本發明之發明者,對在圖的所示之所觀察之Sl2p軌道 之XPS光譜’進行本底修正與3/2及1/2旋轉狀態之分離修 正,而以圖50所示所得結果之Si2p3/2XPS光譜為主,依^及 H. Lu, et al., Appl. Phys, Lett. 71 (1997), pp.2764) 之教示使用於式⑴所不之式與係數求出氧化膜之膜厚d。 d=又 sina · ιη 口 χ+/(^ j 〇+)+1;]· (1) λ = 2· 96 β = 0. 75 但於式⑴中1為圖55所示之XPS光譜之測出角,於圖 示之例中,被設定成30。。又數!中,!、對應氧化膜之光 料值之積分強度PWWx),係對應圖5〇中於 102〜104eV之能量區域所能見到之峰值。另一方面,广為 對應100eV附近之能量區域中,對應起因於發基板之光譜峰 值之積分強度。 曰 再度參照圖48可確認,相對於紫外光戶、 ” 7ti度小,四 形成之氧自由基密度小之情形下(系列丨,2, 3, 8),雖最初 化膜之氧化膜厚為〇 nm者,但隨著氧化時間氧化膜厚會 漸地持續增加者,在將紫外光照射光度設定為基準強^ 20%以上之系列4, 5, 6, 7中,如於圖51概略所示,氧化膜 長於成長開始後會在大致到達〇·4 nm之膜厚之時停滯,' O:\87\87879.DOC -48- 1238453 在經過某種程度的停滯時間後,會再急速的開始成長。 圖以或圖51之關係,係意味著於石夕基板表面°之氧化處 理,可安定地形成〇·4 nm左右之膜厚非常薄的氧化膜。又, 如於圖48所見,可知由於如此之停滯時間持續了某種程 J ’故所形成之氧化膜具有相同之厚度。即,根據本發:: 月b於石夕基板上形成厚度約〇·4 nm之相同厚度之氧化膜。 圖52A、圖52B係概略地顯示於該矽基板上形成薄氧化膜 之製程。於該等圖中,須注意已非常地單純化矽⑽)基板 上之構造。 參照圖52A,於矽基板表面每丨個矽原子結合2個氧原子, 而形成有1原子層之氧層。於其代表性之狀態中,基板表面 之石夕原子係由基板内部的2财原子與基板表面的2個氧原 子所定位,形成副氧化物。 對此,於圖52B之狀態中,矽基板最上層之矽原子係由# 個氧原子所定位,取得安定的Si4+之狀態。可能係由於此一 理由,於圖52A之狀態中快速地進行氧化,變成為圖细之 狀態中氧化停滯。於圖52B之狀態之氧化膜之厚度為〇·4 nm ,此係與於圖48所觀察到之停滯狀態之氧化膜厚一致。 於圖50之XPS光譜,於氧化膜厚為〇lnm或〇 2nm之情況 下:於ΗΠ〜104eV之能量範圍中可見之低峰值係對應圖52八 之副氧化物,而在氧化膜厚超過〇3 nm之情形下,由於在 該能量範圍所顯示之峰值係、起因糾4+,故可認為顯示超過 1原子層之氧化膜的形成者。 如此於0.4 nm之膜厚上之氧化膜厚停滯現象,並不限定 O:\87\87879.DOC -49- 1238453 於圖47A,圖47B之uv〇2自由基氧化製程,應為只要可以良 好精細度形成同樣薄的氧化膜之氧化膜形成方法,皆可見 到相同之情況。 由圖52B之狀態更加繼續氧化,則會使氧化膜之厚度再度 增大。 又 圖53係顯示在由使用如此之基板處理裝置20之圖47A、圖 47B之紫外光自由基氧化製程所形成之氧化膜上,形成厚度 為〇·4 nmiZrSi04x膜與電極膜(參照後面所說明之圖 54B),對所得到之積層構造,所求得之熱氧化膜換算膜厚 Teq與漏洩電流Ig之關係。但,圖53之漏洩電流特性係於前 述電極膜與矽基板間,以平帶電壓Vfb為基準,以施加之狀 態測定Vft-uv之電壓。為了比較,於圖53亦顯示有熱氧 化膜之漏洩電流特性。另外,圖示之換算膜厚係關於組合 氧化膜與ZrSiOx膜之構造者。 參照圖53可知,省略氧化膜時,亦即於氧化膜膜厚為〇打⑺ 之情形下,漏洩電流密度超過熱氧化膜之漏洩電流密度, 又熱氧化膜換算膜厚Teq亦變成約17 nm左右之比較大之 值。 對此,可知若使氧化膜之膜厚由〇 nm增大至〇·4 nm,則 熱氧化膜換异膜厚Teq之值開始減少。於如此之狀態中,氧 化膜會成介於矽基板與ZrSl〇x膜之間,其物理膜厚實際上 應疋增大但換异膜厚Teq卻呈現減少,此點在矽基板上直接 形成ZrCh膜之情形下,意味著如圖54八所示,大規模地產生 Zr向著矽基板中的擴散或是Sl向著ZrSi〇x膜中的擴散,在矽 O:\87\87879.DOC -50- 1238453 基板與之間形成有厚界面層。對此,可考慮如圖 別所示,藉由使厚度Q.4nm之氧化膜介在其中,可抑制如 此之界面層的形成’結果減少換算膜厚者。隨之,可知漏 ^電流之值亦隨著氧化膜之厚度減少。但圖54A、圖54B係 顯示出如此所形成之實驗材料之概略的剖面,並且顯示在 矽基板44 1上形成有氧化膜442,而於氧化膜上則形成有 ZrSiOx膜443之構造。 另方面^如述氧化膜之膜厚超過0.4 nm,則熱氧化 膜換算膜厚之值會開始再度增大。於氧化膜之膜厚超過〇·4 nm之範圍,隨著膜厚之增大漏洩電流之值亦會減少,可想 成其換算膜厚的增大係起因於氧化膜之物理膜厚的增大。 如此,在圖48所觀察到之氧化膜成長所停滞之〇·4 近之膜厚,係對應包含氧化膜與高電介質膜之系之換算膜 厚之最小值,可得知藉由圖52(B)所示之安定的氧化膜,可 有效地阻止Zr等之金屬元素對矽基板中的擴散,並且即使 氧化膜的厚度更大,其金屬元素之擴散阻止效果亦不會提 高許多。 此外’可知使用0.4 nm厚度之氧化膜時之漏洩電流之 值,係較對應之厚度之熱氧化膜之漏洩電流之值小約2位 數,藉由使用如此構造之絕緣膜於MOS電晶體之閘極絕緣 膜中,可最小化閘極漏洩電流。 另外’於圖4 8或5 1所说明之氧化膜成長〇 · 4 nm之停滯現 象之結果,即使如圖55A所示於矽基板441上所形成之氧化 膜442存在著最初之膜厚未變化之凹凸,在氧化膜成長之 O:\87\87879.DOC -51 - 1238453 :::厚增大係如圖55B所示停滞在〇·4議之附近,故藉由 、,滯期間内繼續氧化膜成長’可得到如圖55c所示非常地 平坦、相同臈厚的氧化膜442。 如先前所說明,對於非常薄之氧化膜,目前尚未有統一 之膜厚測定方法。因此,圖55C之氧化膜料2之膜厚值可能 ^因測定方法相異而有所不同。但由先前所說明之理由可, 付知,在氧化膜成長中發生停;帶之厚度為2原子層份之厚 度,故,可認為較理想之氧化膜442之膜厚約為2原子層份 子度於該較理想之厚度係為於氧化膜442整體確保有2 _ 原子層份之厚度,而有在某部份形成有3原子層份厚度區域 之If开^。即,可認為較理想之氧化膜442之厚度實際上是2〜3 原子層之範圍。 [遠距離電漿自由基氮化處理] 圖56係顯示於基板處理裝置2〇所使用之遠距離電漿部 之構成。 如圖56所示,遠距離電漿部27係於内部形成有氣體循環籲 通路27a、與此連通之氣體入口 27b、及氣體出口 76c之典型 的包含有由鋁構成之區塊27A,而在前述區塊27A之一部份 形成有鐵氧體磁心27B。 於前述氣體循環通路27a、氣體入口 27b及氣體出口 27c之 内面,係配設有氟素樹脂加工27d,由捲繞在前述鐵氧體磁 心27B之線圈供給頻率為400 kHz之高頻,而於前述氣體循 環通路27a内形成電漿27C。 隨著電漿27C之激發,於前述氣體循環通路27a中雖形成 O:\87\87879.DOC -52- 1238453 有氮自由基與氮離子,但氮離子會 通一際消失,故由前述氣趙出、:::=趙德環 自由基N/。此外,於圖56之構成 ^放出氮 述氣體出口 27C之離子過渡器27e,而::= 置接地於前 叩除去如氮離子等之 電粒子,而於前述製程空間84僅供給有氮自由基。 即使在未使前述離子過濾、器27e接地之情形下,前述離子卜過 遽me之構造亦有作為擴散板❹,可充分地除去 子等之帶電粒子。 圖57係顯示由遠距離電漿部27所形成之離子數與電子能 量之關係,與微波電漿源之比較。 如圖57所示,在由微波激發電漿之情形下,會促進氮分 子之氮離子化,而形成有量多的氮離子。對此,在由5〇〇kHz 以下之高頻激發電漿之情形下,會大幅度地減少所形成之 氮離子數。在以微波進行電漿處理時,如圖58所示,則需 要1.33\103〜1.33\106?&(10-1〜10-4丁〇]:1:)的高真空,高頻電 漿處理’係可以13.3〜13·3 kPa (0· 1〜1〇〇 Torr)之比較高之壓 力來進行。 以下之表1,係顯示在由微波激發電漿之情形,與由高頻 激發電漿之情形間,離子化能量變換效率、放電可能壓力 範圍、電漿消耗電力及製程氣體流量的比較。 表1Relationship between oxidation time and oxide film thickness when pressure is set to 2.66Pa (20m Torr) and oxygen flow rate is set to 150 SCCM. In addition, the data of Series 5 'shows the relationship between the oxidation time and the oxide film thickness when the ultraviolet light intensity is set to 20% of the reference intensity, the process pressure is set to 2.66Pa (20m Torr), and the oxygen flow rate is set to 150 SCCM. The data of Series 6 shows the relationship between the oxidation time and the thickness of the oxide film when the UV intensity is set to 20% of the reference intensity, the process pressure is about 67Pa (0.5 Torr), and the oxygen flow rate is 0.5SLm. . In addition, the data of Series 7 shows the relationship between the oxidation time and the oxide film thickness when the ultraviolet light intensity is set to 20% of the reference intensity, the process pressure is set to 665Pa (5 Torr), and the oxygen flow rate is set to 2SLM. The data of Series 8 shows the oxidation time when the UV intensity is set to 5% of the reference intensity, the process pressure is 2.66Pa (20m Torr), and the oxygen flow rate is 150SCCM O: \ 87 \ 87879.DOC -47- 1238453 and Relationship between oxide film thickness. In the experiment of Fig. 48, the film thickness of the oxide film is obtained by the XPS method, but there is no uniform method to obtain such a very thin oxide film thickness below the i-plane. Therefore, the inventor of the present invention performs background correction and separation correction of 3/2 and 1/2 rotation states on the observed XPS spectrum of the Sl2p orbit shown in the figure, and uses the result shown in FIG. 50 The Si2p3 / 2XPS spectrum is mainly used in accordance with the teachings of H. Lu, et al., Appl. Phys, Lett. 71 (1997), pp. 2764) to calculate the oxide film using the formulas and coefficients of formula ⑴. Film thickness d. d = also sina · ιη 口 χ + / (^ j 〇 +) + 1;] · (1) λ = 2. 96 β = 0.75 But in formula ⑴ 1 is the measurement of the XPS spectrum shown in Figure 55 The exit angle is set to 30 in the example shown in the figure. . Count again! in,! The integral intensity corresponding to the light value of the oxide film (PWWx) corresponds to the peak value that can be seen in the energy region of 102 ~ 104eV in Fig. 50. On the other hand, in the energy region corresponding to the vicinity of 100 eV, the integrated intensity corresponding to the spectral peak value of the hair substrate is corresponding. Referring to FIG. 48 again, it can be confirmed that, compared with the UV light household, "7ti degree is small and the density of oxygen radicals formed in the four is small (series 丨, 2, 3, 8), although the oxide film thickness of the initial film is 〇nm, but the thickness of the oxide film will continue to increase with the oxidation time, in the series 4, 5, 6, 7 set the ultraviolet light irradiation intensity to a reference intensity ^ 20% or more, as schematically shown in Figure 51 It is shown that the oxide film stagnates when it reaches a film thickness of approximately 0.4 nm after the beginning of growth. 'O: \ 87 \ 87879.DOC -48-1238453 after a certain degree of stagnation time, it will sag again. It begins to grow. The relationship between the figure and FIG. 51 means that the oxidation treatment on the surface of the Shi Xi substrate ° can form a very thin oxide film with a thickness of about 0.4 nm. Also, as shown in FIG. 48, It can be seen that the oxidized film formed with the same thickness has the same thickness because such a dwell time lasts for a certain period of time. That is, according to the present invention: the oxide of the same thickness of about 0.4 nm is formed on the Shi Xi substrate Fig. 52A and Fig. 52B are diagrams schematically showing a system for forming a thin oxide film on the silicon substrate. In these figures, you must pay attention to the structure on the silicon substrate). Referring to FIG. 52A, each silicon atom on the surface of the silicon substrate is combined with 2 oxygen atoms to form a 1-atom layer of oxygen. In its typical state, the Shi Xi atom on the substrate surface is positioned by the two rich atoms inside the substrate and two oxygen atoms on the substrate surface to form a secondary oxide. In this state, in the state of FIG. 52B, The silicon atom in the uppermost layer of the silicon substrate is positioned by # oxygen atoms to obtain a stable state of Si4 +. It may be because of this reason that the oxidation is rapidly performed in the state of Fig. 52A, and the oxidation is stopped in the state shown in the figure. The thickness of the oxide film in the state of FIG. 52B is 0.4 nm, which is consistent with the oxide film thickness in the stagnant state observed in FIG. 48. In the XPS spectrum of FIG. 50, the oxide film thickness is 0.01 nm or In the case of 〇2nm: the low peak visible in the energy range of ΗΠ ~ 104eV corresponds to the secondary oxide shown in Figure 52, and when the oxide film thickness exceeds 〇3 nm, the peak value displayed in this energy range Department and cause correction 4+, so it can be considered to show Formation of an oxide film over 1 atomic layer. The phenomenon of stagnation of the oxide film thickness at a film thickness of 0.4 nm is not limited to O: \ 87 \ 87879.DOC -49-1238453 as shown in Figure 47A and Figure 47B. 2 The free radical oxidation process should be the same as long as the oxide film formation method can form the same thin oxide film with good fineness. From the state of Fig. 52B, if the oxidation is continued, the thickness of the oxide film will increase again. Fig. 53 shows the formation of a thickness of 0.4 nmiZrSi04x film and electrode film on the oxide film formed by the ultraviolet light radical oxidation process of Figs. 47A and 47B using such a substrate processing apparatus 20. The illustrated FIG. 54B) shows the relationship between the obtained thermal oxide film conversion film thickness Teq and the leakage current Ig for the obtained laminated structure. However, the leakage current characteristics in Fig. 53 are measured between the aforementioned electrode film and the silicon substrate, and the voltage of Vft-uv is measured based on the flat band voltage Vfb as a reference. For comparison, the leakage current characteristics of the thermal oxidation film are also shown in FIG. 53. In addition, the conversion film thickness shown in the figure refers to a structure that combines an oxide film and a ZrSiOx film. Referring to FIG. 53, when the oxide film is omitted, that is, when the thickness of the oxide film is 0 h, the leakage current density exceeds the leakage current density of the thermal oxide film, and the thermally converted film thickness Teq also becomes about 17 nm. The larger value from left to right. In this regard, it is understood that if the film thickness of the oxide film is increased from 0 nm to 0.4 nm, the value of the thermal oxide film exchange film thickness Teq starts to decrease. In such a state, the oxide film is formed between the silicon substrate and the ZrSlOx film. The physical film thickness should actually increase but the transmutation film thickness Teq decreases, which is directly formed on the silicon substrate. In the case of the ZrCh film, it means that diffusion of Zr into the silicon substrate or Sl into ZrSi0x film occurs on a large scale as shown in Fig. 54. In silicon O: \ 87 \ 87879.DOC -50 -1238453 A thick interface layer is formed between the substrate and the substrate. In this regard, as shown in the figure, it is considered that the formation of the interface layer can be suppressed by interposing an oxide film having a thickness of Q.4 nm therebetween. As a result, the converted film thickness can be reduced. It follows that the value of the leakage current also decreases with the thickness of the oxide film. However, Figs. 54A and 54B show a schematic cross-section of the experimental material thus formed, and a structure in which an oxide film 442 is formed on the silicon substrate 44 1 and a ZrSiOx film 443 is formed on the oxide film. On the other hand, if the film thickness of the oxide film exceeds 0.4 nm, the value of the film thickness converted from the thermal oxide film will start to increase again. When the film thickness of the oxide film exceeds 0.4 nm, the value of the leakage current will decrease as the film thickness increases. It can be thought that the increase in the converted film thickness is due to the increase in the physical film thickness of the oxide film. Big. In this way, the film thickness near 0.4 that the stagnation of the oxide film growth observed in FIG. 48 corresponds to the minimum value of the converted film thickness of the system including the oxide film and the high-dielectric film. It can be seen from FIG. 52 ( The stable oxide film shown in B) can effectively prevent the diffusion of metal elements such as Zr into the silicon substrate, and even if the thickness of the oxide film is larger, the effect of preventing the diffusion of metal elements will not be much improved. In addition, it can be seen that the value of the leakage current when using an oxide film with a thickness of 0.4 nm is about two digits smaller than the value of the leakage current of a thermal oxide film with a corresponding thickness. By using the insulating film thus structured in a MOS transistor, In the gate insulation film, the gate leakage current can be minimized. In addition, as a result of the stagnation phenomenon of the oxide film growth of 0.4 nm illustrated in FIG. 4 8 or 51, even if the oxide film 442 formed on the silicon substrate 441 as shown in FIG. 55A has the original film thickness unchanged. The unevenness in the growth of the oxide film is O: \ 87 \ 87879.DOC -51-1238453 ::: Thickness increase is stagnated around 0.4 as shown in Figure 55B, so it continues with the delay period. The oxide film is grown, and as shown in FIG. 55c, the oxide film 442 is very flat and has the same thickness. As explained previously, there is currently no uniform film thickness measurement method for very thin oxide films. Therefore, the film thickness value of the oxide film material 2 in FIG. 55C may vary depending on the measurement method. However, for the reasons explained earlier, it is known that the stoppage occurs during the growth of the oxide film; the thickness of the belt is 2 atomic layers, so it can be considered that the ideal film thickness of the oxide film 442 is about 2 atomic layers. In this preferred thickness, the thickness of the 2 _ atomic layer is ensured in the whole of the oxide film 442, and if the thickness of a 3 atomic layer thickness region is formed in a certain part. That is, it can be considered that the ideal thickness of the oxide film 442 is actually in the range of 2 to 3 atomic layers. [Remote Plasma Free Radical Nitriding] FIG. 56 shows the configuration of a remote plasma unit used in the substrate processing apparatus 20. As shown in FIG. 56, the long-distance plasma unit 27 is a block 27A made of aluminum, which typically includes a gas circulation channel 27a, a gas inlet 27b, and a gas outlet 76c connected thereto. A part of the aforementioned block 27A is formed with a ferrite core 27B. A fluorine resin processing 27d is provided on the inner surfaces of the gas circulation path 27a, the gas inlet 27b, and the gas outlet 27c. A high frequency of 400 kHz is supplied from a coil wound around the ferrite core 27B. A plasma 27C is formed in the gas circulation path 27a. With the excitation of plasma 27C, although O: \ 87 \ 87879.DOC -52-1238453 is formed in the aforementioned gas circulation path 27a, there are nitrogen radicals and nitrogen ions, but nitrogen ions will disappear for a while. Zhao Chu, ::: = Zhao Dehuan radical N /. In addition, the structure of FIG. 56 ^ ion transition device 27e emitting nitrogen gas outlet 27C, and :: = is placed on the front to remove electric particles such as nitrogen ions, and only nitrogen radicals are supplied in the aforementioned process space 84 . Even if the ion filter and the device 27e are not grounded, the structure of the ion 过 me also functions as a diffusion plate ❹, and can sufficiently remove charged particles such as ions. Fig. 57 shows the relationship between the number of ions and the energy of the electrons formed by the remote plasma unit 27 and the comparison with the microwave plasma source. As shown in Fig. 57, when the plasma is excited by the microwave, nitrogen ionization of the nitrogen molecules is promoted, and a large amount of nitrogen ions are formed. On the other hand, when the plasma is excited at a high frequency below 500 kHz, the number of nitrogen ions formed is greatly reduced. When the plasma treatment is performed by microwave, as shown in FIG. 58, a high vacuum and high frequency plasma of 1.33 \ 103 ~ 1.33 \ 106? (10-1 ~ 10-4 丁 〇): 1 :) are required. The processing can be performed at a relatively high pressure of 13.3 to 13.3 kPa (0.1 to 100 Torr). Table 1 below shows the comparison of ionization energy conversion efficiency, possible discharge pressure range, plasma power consumption, and process gas flow between the case where the plasma is excited by microwaves and the case where the plasma is excited by high frequencies. Table 1
離子化能量變 換效率 放電可能 壓力範圍 電漿 消耗電力 製程 氣體流量 微 波 l.OOxlO'2 0.1m〜0·1 Torr 1 〜500W 0〜100 SCCM 高 頻 l.OOxlO"7 0.1 〜100 Torr 1 〜10kW 0.1 〜10SLM O:\87\87879.DOC -53- 1238453 參照表1’可知關於離子化能量變換效率,相對於在微波 激發之情形時約為lxl0-2左右,於RF激發之情形則減少至 約IxlO·7為止’另外,關於放電可能廢力,相對於為微波激 發之 〇· 1ΙΏ Torr〜〇·1 T〇rr 门 、丄 丄on· U33mPa〜13.3Pa)左右,汉匕數發之情 形則是〇.1〜1〇〇丁01^〇3_31^〜13.3]^^)左右。隨之,電漿消 耗電力係RF激發時較微波激發時為大,而製程氣體流量係 RF激發時亦較微波激發時大出很多。 於基板處理裝置20中,係以氮自由基仏*而非氮離子來進 行氧化膜之氮化處理,因此被激發之氮離子數量少較為理 想。又,由最小化被加諸於被處理基板之損害之觀點來看, 亦是被激發之氮離子數量少較為理想。此外,於基板處理 裝置20中,以被激發之氮自由基數量少,於高電介質閘極 絕緣膜下非常薄之最多2〜3原子層左右厚度之基底氧化 膜,非常適合於氮化。 圖59A、圖59B係分別顯示使用基板處理裝置2〇進行被處 理基板W之自由基氮化時之側面圖與俯視圖。 如圖59A、圖59B所示,於遠距離電漿部27供給有Ar氣體 與氮氣體,故以數100 kHz之頻率藉由高頻激發電漿,形成 氮自由基。而被形成之氮自由基係延著前述被處理基板w 之表面流動,經由前述排氣口 74與幫浦201被排出。結果, 前述製程空間84可被設定於適合基板w之自由基氮化之 l-3 3Pa〜i3.3kPa (0.01〜100 Torr)範圍的製程壓力。如此被形 成之氮自由基會在延著前述被處理基板W之表面流動之 際,氮化被處理基板W之表面。 O:\87\87879.DOC -54- 1238453 於圖59A、圖59B之氮化步驟中,於氮化步驟之前的清淨 步驟中,前述閥48a與212為被開放,藉由關閉閥48a使前述 製程空間84之壓力減壓至133xl{rl〜133xl〇_4匕之壓力為 止,殘留於製程空間84中之氧及水分會被清除,但於其後 之氮化處理中,其閥48a與212被關閉,而渦輪分子幫浦 則不包含於製程空間84之排氣路徑。 如此,藉由使用基板處理裝置2〇,可在被處理基板…之 表面形成非常薄之氧化膜,並進一步氮化其氧化膜表面。 圖60A係顯示使用遠距離電漿部27,並以表2所示條件氮 化藉由基板處理裝置2〇在矽基板上進行熱氧化處理而形成 之2·〇 nm厚之氧化膜時之前述氧化膜中之氮濃度分佈,圖 60B則顯示於相同氧化膜中之氮濃度分佈與氧濃度分佈之 關係圖。Ionization energy conversion efficiency discharge possible pressure range plasma consumption power process gas flow microwave l.OOxlO'2 0.1m ~ 0 · 1 Torr 1 ~ 500W 0 ~ 100 SCCM high frequency l.OOxlO " 7 0.1 ~ 100 Torr 1 ~ 10kW 0.1 ~ 10SLM O: \ 87 \ 87879.DOC -53- 1238453 With reference to Table 1 ', it can be seen that the ionization energy conversion efficiency is about lxl0-2 in the case of microwave excitation, and reduced to RF in the case of RF excitation. About IxlO · 7 'In addition, regarding the possible wasteful force of the discharge, compared with the microwave excitation (0.1 · 1 Torr ~ 0 · 1 Torr gate, 丄 丄 on · U33mPa ~ 13.3Pa), the number of Chinese daggers is several. It is about 0.1 ~ 1〇〇 丁 01 ^ 〇3_31 ^ ~ 13.3] ^^). As a result, the plasma power consumption is greater in RF excitation than in microwave excitation, and process gas flow is much larger in RF excitation than in microwave excitation. In the substrate processing apparatus 20, the nitridation treatment of the oxide film is performed with a nitrogen radical 仏 * instead of a nitrogen ion, so it is desirable that the number of excited nitrogen ions is small. From the viewpoint of minimizing the damage to be applied to the substrate to be processed, it is also desirable that the number of excited nitrogen ions is small. In addition, in the substrate processing apparatus 20, the base oxide film with a small number of excited nitrogen radicals and a thickness of about 2 to 3 atomic layers under the high dielectric gate insulating film is very suitable for nitriding. 59A and 59B are a side view and a plan view, respectively, when radical nitridation of the substrate W to be processed is performed using the substrate processing apparatus 20. As shown in Figs. 59A and 59B, Ar gas and nitrogen gas are supplied to the long-range plasma unit 27. Therefore, the plasma is excited by a high frequency at a frequency of several hundred kHz to form nitrogen radicals. The formed nitrogen radicals flow along the surface of the substrate w to be processed, and are discharged through the exhaust port 74 and the pump 201. As a result, the aforementioned process space 84 can be set to a process pressure in the range of 1-3 Pa to i3.3 kPa (0.01 to 100 Torr) suitable for radical nitridation of the substrate w. The nitrogen radicals thus formed will nitrate the surface of the substrate W to be processed while flowing along the surface of the substrate W to be processed. O: \ 87 \ 87879.DOC -54- 1238453 In the nitriding step of Fig. 59A and Fig. 59B, in the cleaning step before the nitriding step, the aforementioned valves 48a and 212 are opened, and the aforementioned valve is closed by closing the valve 48a The pressure in the process space 84 is reduced to the pressure of 133xl {rl ~ 133xl0_4. The oxygen and moisture remaining in the process space 84 will be removed. However, in the subsequent nitriding treatment, the valves 48a and 212 will be removed. Is turned off, and the turbo molecular pump is not included in the exhaust path of the process space 84. In this way, by using the substrate processing apparatus 20, a very thin oxide film can be formed on the surface of the substrate to be processed, and the surface of the oxide film can be further nitrided. FIG. 60A shows the foregoing when a long-range plasma unit 27 is used and nitrided under a condition shown in Table 2 by a substrate processing apparatus 20 to perform a thermal oxidation process on a silicon substrate to form an oxide film having a thickness of 2.0 nm. The distribution of nitrogen concentration in the oxide film. FIG. 60B shows the relationship between the distribution of nitrogen concentration and the distribution of oxygen concentration in the same oxide film.
氮流i Ar流量 電漿電力 壓力 溫度 破波 •Ο— 15 SCCMj - 120W 8.6m Torr 500°C 向頻 50 SCCM 2SLM 2kW 1 Torr 700°C 參照表2,於使用基板處理裝置20進行RF氮化處理之際, 對製程空間84内,以50SCCMi流量供給氮或2SLM之流量 供給Ar,在1 Torr (133pa)之壓力下進行氮化處理,但於氮 化處理開始前暫時將製程空間84之内壓減壓至1〇·6 τ〇ΓΓ (1.33x10 Pa)左右為止,並充分地清除殘留於内部之氧或 水伤。因此,於以前述i T〇rr&右之壓力所進行之氮化處理 之際,於製程空間84中,其殘留氧可由Ar或氮來稀釋,殘 留氧濃度,故殘留氧之熱力學上之活動度變的非常地小。Nitrogen flow i Ar flow Plasma power pressure temperature breaking wave 〇— 15 SCCMj-120W 8.6m Torr 500 ° C Directional frequency 50 SCCM 2SLM 2kW 1 Torr 700 ° C Refer to Table 2 for RF nitriding using a substrate processing device 20 During the process, nitrogen was supplied into the process space 84 at a flow rate of 50 SCCMi or Ar was supplied at a flow rate of 2 SLM. Nitriding treatment was performed at a pressure of 1 Torr (133pa), but the process space 84 was temporarily left before the nitriding process started. The pressure is reduced to about 10.6 τ〇ΓΓ (1.33x10 Pa), and oxygen or water damage remaining inside is fully removed. Therefore, in the nitriding treatment performed under the aforementioned pressure of i Torr & right, in the process space 84, the residual oxygen can be diluted by Ar or nitrogen, and the residual oxygen concentration, so the thermodynamic activity of the residual oxygen The degree becomes very small.
O:\87\87879.DOC -55- 1238453 對此,在使用微波電漿之氮化處理中,氮化處理時之處 壓力係與清除壓為同樣程度,故可認為於電漿氛圍申, 殘留氧係具有高熱力學上活動度者。 參照圖60A,於藉由微波激發電漿而氮化之情形時,其被 導入於氧化膜中之氮的濃度為有限的,故可知實質上並未 進行氧化膜之氮化。對此如同本實施例般,於藉由rf激發 電漿而氮化之情形時,可知於氧化膜中其氮濃度會隨著深 度呈現線性變化,而在表面附近則達到將近2〇%之濃度。 圖61係顯示使用XPS (X射線光譜)所進行之圖6〇a之測定 原理。 參照圖61,於矽基板411上形成氧化膜412之試驗材料, 係由X射線以特定角度斜斜地照射,·再由檢測器Det 1、 DET2以各種角度檢測被激發之χ射線光譜。此時,例如由 被設定成90。之深檢測角之檢測器DET1中,其於激發χ射線 之氧化膜412内之路徑短,故於以前述檢測器DET1所檢測 之X射線光譜中包含有許多氧化膜412之下部資訊,相對於 此’在被設定成淺檢測角之檢測器DET2中,其於激發χ射 線之氧化膜412中之路徑長,故檢測器DET2主要是檢測氧 化膜412表面附近之資訊。 圖60B係顯示於前述氧化膜中之氮濃度與氧濃度之關 係。但圖60B中,氧濃度係由對應〇ls執道之χ射線強度所 表不。 參照圖60Β,在如本發明般以rf遠距離電漿進行氧化膜 氮化之情形中,隨著氮濃度的增大會使氧濃度減少,故可O: \ 87 \ 87879.DOC -55- 1238453 In this regard, in the nitriding process using a microwave plasma, the pressure at the time of the nitriding process is the same as the removal pressure, so it can be considered in the plasma atmosphere. Residual oxygen system has high thermodynamic activity. Referring to Fig. 60A, in the case where the plasma is nitrided by microwave excitation, the concentration of nitrogen introduced into the oxide film is limited, so it can be seen that nitriding of the oxide film is not substantially performed. In this case, as in this embodiment, when the plasma is nitrided by rf excitation, it can be known that the nitrogen concentration in the oxide film changes linearly with the depth, and reaches a concentration of nearly 20% near the surface. . Figure 61 shows the measurement principle of Figure 60a using XPS (X-ray spectroscopy). Referring to FIG. 61, a test material for forming an oxide film 412 on a silicon substrate 411 is irradiated obliquely by X-rays at a specific angle, and then the detectors Det 1, DET2 detect the excited X-ray spectrum at various angles. At this time, for example, is set to 90. In the detector DET1 with a deep detection angle, the path in the oxide film 412 of the excited x-ray is short, so the X-ray spectrum detected by the aforementioned detector DET1 contains a lot of information about the lower part of the oxide film 412. In the detector DET2 which is set to a shallow detection angle, the path in the oxide film 412 that excites x-rays is long, so the detector DET2 mainly detects information near the surface of the oxide film 412. Fig. 60B shows the relationship between the nitrogen concentration and the oxygen concentration in the aforementioned oxide film. However, in Fig. 60B, the oxygen concentration is represented by the x-ray intensity corresponding to the ols. Referring to FIG. 60B, in the case where the oxide film is nitrided with rf remote plasma as in the present invention, the oxygen concentration decreases as the nitrogen concentration increases, so
O:\87\87879.DOC -56- 1238453 於氧化膜中氮原子會置換氧原子。對此,在以微波電浆 進订氧化膜氮化之情形巾,無法見到如此之置換關係,亦 不見氧濃度隨著氮濃度而降低之關係。另夕卜特別是於圖 60B中’在由微波氮化導入5〜6%的氮之例中可見到氧濃度 的曰加Λ係思味著隨著氮化而引起氧化膜之增加。隨著 如此之微波氮化之氧濃度的增加,係於高真Μ進行微波 W ’故可認為殘留於處理空間中之氧或水份並非藉由如 南頻遠距離電職化情形之^氣體與氮氣體來稀釋,而是 因在氛圍中具有高活動度者。 圖62係顯不於基板處理裝置2〇形成厚度為4入(〇4 與 7A(0.7 nm)之氧化膜,並由使用前述遠距離電漿部之圖 59A、圖59B之氮化步驟,將#氮化時之氮化時間與膜中之 辰度之關係。又圖63係顯示對隨著圖62之氮化處理之氮 對氧化膜膜表面之偏析情形。另外,於圖62、圖63亦顯示 出以急速熱氧化處理將氧化膜形成為5人(〇·5 nm)*7A (〇7 nm)的厚度之情形。 多…、圖62,膜中之氮濃度係任一氧化膜皆會隨著氮化處 理牯間而一起上昇,但特別是在具有對應由紫外光自由基 氧化所形成之2原子層份之〇 4nm膜厚之氧化膜的情形,或 具有接近於此之〇·5 nm膜厚之熱氧化膜的情形時,由於氧 化膜薄’故於相同成膜條件下膜中之氮濃度會變高。 圖63係顯示於圖6丨分別將檢測器DET丨及DET2設定成%。 及90之檢測角所檢測出之氮濃度之結果。 由圖63可知,圖63之縱軸係以90。之檢測角所得到由分散O: \ 87 \ 87879.DOC -56-1238453 In the oxide film, the nitrogen atom will replace the oxygen atom. For this reason, in the case where the oxide film is nitrided with a microwave plasma, such a replacement relationship cannot be seen, and a relationship that the oxygen concentration decreases with the nitrogen concentration cannot be seen. In addition, particularly in FIG. 60B, in the case where 5 to 6% of nitrogen is introduced by microwave nitriding, the addition of oxygen concentration Δ is considered to increase the oxide film with nitriding. With the increase of the oxygen concentration of such microwave nitridation, the microwave W is performed at high true M, so it can be considered that the oxygen or water remaining in the processing space is not caused by the gas in the long-range electric frequency as in the south frequency. Dilute with nitrogen gas, but because of high activity in the atmosphere. FIG. 62 shows the formation of an oxide film with a thickness of 4 in. (0 4 and 7A (0.7 nm)) in the substrate processing apparatus 20, and the nitriding step of FIG. 59A and FIG. 59B using the aforementioned long-range plasma unit #The relationship between the nitriding time and the degree of crystallization in the film. Fig. 63 shows the segregation of nitrogen on the oxide film surface with the nitriding treatment of Fig. 62. In addition, Figs. It also shows that the oxide film is formed to a thickness of 5 persons (0.5 nm) * 7A (〇7 nm) by a rapid thermal oxidation treatment. Many ..., Fig. 62, the nitrogen concentration in the film is that of any oxide film It will rise together with nitriding treatment, but especially when it has an oxide film with a thickness of 0.4 nm corresponding to the 2-atomic layer formed by ultraviolet radical oxidation, or has an oxide film close to this. In the case of a thermally oxidized film with a film thickness of 5 nm, the nitrogen concentration in the film will increase under the same film formation conditions because the oxide film is thin. Figure 63 shows in Figure 6 丨 Detectors DET 丨 and DET2 are set respectively The results are shown in Fig. 63, and the vertical axis of Fig. 63 is 90%. Angular obtained by dispersion
O:\87\87879.DOC -57- 1238453 在臈全體之氮原子而來之x射線光譜強度之值,除3〇。之檢 測角所付到之由偏析於膜表面之氮原子之X射線光譜強度 所得到者,並將此;t義為氮偏析率。在該值為以上之㈣ 下,會產生對表面之氮偏析。 多…、圖63,藉由紫外光激發氧自由基處理而將氧化膜之 ,厚形成為7A之情形下,其氮偏析率成為1以上,氮原子於 取初之表面偏析’可認為是如圖i中之氧氮化膜UA之狀態 者另外,可知在進行9〇秒間之氮化處理後,於膜中之分 佈大致相同。又可知即使是其他之膜,以輝之氮化處理, 亦會使氮原子之財分佈變成大致相同。 w於圖64之實驗中,在基板處理裝置2〇,針對H)片晶圓(晶 圓#1〜晶圓#10),重複進行前述紫外光自由基氧化處理及遠 距離電水虱化處理。圖64係顯示如此得到之氧氮化膜之每 個晶圓之膜厚變動。但,圖64之結果係關於在基板處理裝 置2〇驅動紫外線光源86, _進行紫外光自由基氧化處理 之際,形成由XPS測定所求得之氧化膜厚度為〇·4聰之氧化 、接著將如此所形成之氧化膜,藉由驅動前述遠距離 電水^27進订1化處理,變換成包含約4%氮原子之氧氮化 膜之情形者。 >照圖64’縱軸係顯示對於如此所求得之氧氮化膜以相 ®對稱所求得之膜厚,但由圖6何知所求得之膜厚係大惠 安定於 8Α (〇·8 nm)。 圖65係顯示藉由基板處理裝置2〇,於石夕基板上藉由使用 紫外線光源86, 87之自由基氧化處理形成膜厚為〇4咖之O: \ 87 \ 87879.DOC -57-1238453 The value of the x-ray spectral intensity from the nitrogen atoms in the whole plutonium, divided by 30. The detection angle is obtained from the X-ray spectral intensity of nitrogen atoms segregated on the film surface, and t is the nitrogen segregation rate. Above this value, nitrogen segregation on the surface occurs. Many ..., Fig. 63. In the case where the oxide film is formed to a thickness of 7A by ultraviolet light-excited oxygen radical treatment, the nitrogen segregation rate becomes 1 or more. The nitrogen atom segregates at the initial surface. In the state of the oxynitride film UA in FIG. 1, it can be seen that the distribution in the film after the nitriding treatment for 90 seconds is approximately the same. It can also be seen that even with other films, the nitridation treatment with glow can make the distribution of nitrogen atoms substantially the same. In the experiment shown in FIG. 64, in the substrate processing apparatus 20, for the HD wafer (wafer # 1 to wafer # 10), the aforementioned ultraviolet light radical oxidation treatment and long-range electric water lice treatment were repeated. . Fig. 64 shows the variation in film thickness of each of the wafers of the oxynitride film thus obtained. However, the results shown in FIG. 64 relate to the formation of an oxide film having a thickness of 0.4 Satoshi when the ultraviolet light source 86 is driven by the substrate processing apparatus 20, and the ultraviolet light radical oxidation treatment is performed. The oxide film formed in this way is converted into a case of an oxynitride film containing about 4% nitrogen atoms by driving the aforementioned long-distance electro-water ^ 27 into an order process. > According to FIG. 64 ', the vertical axis shows the film thickness obtained by phase symmetry for the oxynitride film thus obtained, but the film thickness obtained from FIG. 6 is determined by Da Hui An at 8A ( 0.8 nm). FIG. 65 shows that a substrate thickness of 0 μm is formed on a substrate of Shi Xi by a radical oxidation treatment using an ultraviolet light source 86, 87 on a substrate of Shi Xi.
O:\87\87879.DOC -58- 1238453 氧化膜後’藉由遠距離電漿部27將其加以氮化之情形,所 得的因氮化之膜厚增加之調查結果。 參照圖65,可知最初(進行氮化處理前)膜厚約為〇38打㈤ 之氧化膜,係在氮化處理中導入4〜7%之氮原子之時,膜厚 、、’勺增大至0.5nm為止。另一方面,在氮化處理中導入約15〇/〇 之氮原子時,其膜厚約增大至13 nm為止,於該情形時可 認為被導入之氮原子通過氧化膜侵入至矽基板中而形成氮 化膜。 於圖65中係以▲顯示有關僅導入一層份之氮於厚度為 0.4 nm之氧化膜中之理想的模型構造中之氮濃度與膜厚之 關係。 參照圖65,於該理想的模型構造中,氮原子導入後之膜 厚約變成0.5 nm,該情形時之膜厚增加約為〇lnm,而氮濃 度約為12%。若以該模型為基準,則結論為··藉由基板處 里哀置20進行氧化膜之氮化時,其膜厚增加以抑制在相同 程度之0.1〜0.2 nm者為較理想。另外此時亦可預估被取入於 膜中之氮原子量最大為丨2〇/〇左右。 另外,於以上之說明中,係說明使用基板處理裝置2〇而 幵乂成非ψ薄之基底氧化膜之例,但本發明並未限定於如此 特定之實施例,亦可適用在矽基板或矽膠層上,形成所希 望膜厚之高品質氧化膜、氮化膜或氮氧化膜。 乂上以較佳之實施例說明了本發明,但本發明並未限 定於上述之特定實施例,於揭示在申請專利範圍之要旨内 白可作各種變化、變更。O: \ 87 \ 87879.DOC -58- 1238453 After oxidizing the film ′ In the case of nitriding it by the remote plasma unit 27, the result of investigation of the increase in film thickness due to nitridation is obtained. Referring to FIG. 65, it can be seen that the initial (before nitriding) oxide film having a thickness of about 0.38 ㈤ is an increase in film thickness when nitrogen atoms of 4 to 7% are introduced during the nitriding process. Up to 0.5nm. On the other hand, when a nitrogen atom of about 15/0 is introduced during the nitridation process, the film thickness is increased to about 13 nm. In this case, it can be considered that the introduced nitrogen atom penetrates into the silicon substrate through the oxide film. A nitride film is formed. In Fig. 65, the relationship between the nitrogen concentration and the film thickness in the ideal model structure for the introduction of only one layer of nitrogen in an oxide film with a thickness of 0.4 nm is shown by ▲. Referring to FIG. 65, in this ideal model structure, the film thickness after the introduction of nitrogen atoms becomes about 0.5 nm, in this case, the film thickness increases by about 0.1 nm, and the nitrogen concentration is about 12%. If this model is used as a reference, it is concluded that when the oxide film is nitrided by placing 20 on the substrate, it is desirable that the film thickness be increased to suppress the same degree of 0.1 to 0.2 nm. In addition, the maximum amount of nitrogen atoms that can be taken into the film at this time can be estimated to be about 20/0. In addition, in the above description, an example in which a substrate processing device 20 was used to form a non-ψ thin base oxide film was described. However, the present invention is not limited to such a specific embodiment, and can be applied to a silicon substrate or a silicon substrate. On the silicon layer, a high-quality oxide film, nitride film, or oxynitride film with a desired film thickness is formed. The invention has been described above with reference to preferred embodiments, but the invention is not limited to the specific embodiments described above, and various changes and modifications may be made within the spirit of the scope of the patent application.
O:\87\87879.DOC -59- 1238453 【圖式簡單說明】 圖1係顯示含有高電介質閘極絕緣膜之半導體裝置之 成圖。 圖2係顯示本發明之基板處理裝置之一實施例構成之 視圖。 、圖3係顯示本發明之基板處理裝置之一實施例構成之側 視圖。 圖4為沿著圖2中A-A線之橫剖面圖。 圖5係顯示配置於處理容器22下方之機器構成之前視圖。 圖6係顯示配置於處理容器22下方之機器構成之俯視圖。 圖7係顯示配置於處理容器22下方之機器構成之側視圖。 圖8 A係顯示排氣路徑32之構成之俯視圖。 圖8B係顯示排氣路徑32之構成之前視圖。 圖8C為沿著b-b線之縱剖面圖。 圖9係擴大顯示處理容器22及其周邊機器之側面縱剖面 圖。 圖10為從上方所見拿掉蓋子構件82後之處理容器22内部 之俯視圖。 圖π為處理容器22之俯視圖。 圖為處理容器22之前視圖。 圖13為處理容器22之仰視圖。 圖14為沿著圖12中C-C線之縱剖面圖。 圖15為處理容器22之右側視圖。 圖16為處理容器22之左側視圖。 O:\87\87879.DOC -60- 1238453 圖17係擴大顯示紫外線光源86、87之安裝構造之縱剖面 圖。 圖1 8係擴大顯示氣體噴射噴嘴部93之構成之縱剖面圖。 圖19係擴大顯示氣體噴射喷嘴部93之構成之橫剖面圖。 圖20係擴大顯示氣體噴射噴嘴部93之構成之前視圖。 圖21係擴大顯示加熱部24之構成之縱剖面圖。 圖22係擴大顯示加熱部24之仰視圖。 圖2 3係擴大顯不第2流入口 17 0 ’及第2流出口 17 4之安穿 構造之縱剖面圖。 圖24係擴大顯示凸緣140之安裝構造之縱剖面圖。 圖25係擴大顯示夾鉗機構190之上端部之安裝構造之縱 剖面圖。 圖26係顯示SiC加熱器114,及SiC加熱器114之控制系統 構造之圖。 圖27A係顯示石英鐘罩H2之構造之俯視圖。 圖27B係顯示石英鐘罩112之構造之縱剖面圖。 圖28A為從上方所見石英鐘罩112之構造之立體圖。 圖28B為從下方所見石英鐘罩112之構造之立體圖。 圖29係顯示減壓系統之排氣系統構成之系統圖。 圖30A係顯示保持構件12〇構成之俯視圖。 圖30B係顯示保持構件12〇構成之側面圖。 圖31係顯示配置於加熱部24下方之旋轉驅動部28之構成 之縱剖面圖。 圖32係擴大顯示旋轉驅動部“之縱剖面圖。O: \ 87 \ 87879.DOC -59- 1238453 [Brief Description of the Drawings] Figure 1 is a drawing showing a semiconductor device containing a high-dielectric gate insulating film. Fig. 2 is a view showing the structure of an embodiment of a substrate processing apparatus of the present invention. Fig. 3 is a side view showing the structure of one embodiment of the substrate processing apparatus of the present invention. Fig. 4 is a cross-sectional view taken along line A-A in Fig. 2. FIG. 5 is a front view showing the configuration of a machine disposed below the processing container 22. FIG. 6 is a plan view showing the structure of a machine disposed below the processing container 22. FIG. 7 is a side view showing the configuration of a machine disposed below the processing container 22. FIG. 8A is a plan view showing the configuration of the exhaust path 32. FIG. FIG. 8B is a front view showing the configuration of the exhaust path 32. FIG. Fig. 8C is a longitudinal sectional view taken along line b-b. Fig. 9 is an enlarged longitudinal sectional view of the processing container 22 and its peripheral devices. Fig. 10 is a plan view of the inside of the processing container 22 with the lid member 82 removed from above. FIG. Π is a plan view of the processing container 22. The figure shows a front view of the processing container 22. FIG. 13 is a bottom view of the processing container 22. Fig. 14 is a longitudinal sectional view taken along the line C-C in Fig. 12. FIG. 15 is a right side view of the processing container 22. FIG. 16 is a left side view of the processing container 22. O: \ 87 \ 87879.DOC -60- 1238453 Fig. 17 is a longitudinal sectional view showing the installation structure of the ultraviolet light sources 86 and 87 in an enlarged manner. FIG. 18 is a longitudinal sectional view showing the structure of the gas injection nozzle section 93 in an enlarged manner. FIG. 19 is a cross-sectional view showing the structure of the gas injection nozzle section 93 in an enlarged manner. FIG. 20 is an enlarged front view showing the configuration of the gas injection nozzle portion 93. FIG. FIG. 21 is a longitudinal sectional view showing an enlarged configuration of the heating section 24. FIG. 22 is an enlarged bottom view of the heating unit 24. Fig. 2 is a longitudinal cross-sectional view of the enlarged penetration structure of the second inflow port 17 0 ′ and the second outflow port 17 4. FIG. 24 is a longitudinal sectional view showing the mounting structure of the flange 140 in an enlarged manner. Fig. 25 is a longitudinal sectional view showing the mounting structure of the upper end portion of the clamp mechanism 190 on an enlarged scale. FIG. 26 is a diagram showing the structure of the SiC heater 114 and the control system of the SiC heater 114. FIG. Fig. 27A is a plan view showing the structure of the quartz bell cover H2. Fig. 27B is a longitudinal sectional view showing the structure of the quartz bell cover 112. FIG. 28A is a perspective view of the structure of the quartz bell cover 112 seen from above. FIG. 28B is a perspective view of the structure of the quartz bell cover 112 seen from below. Fig. 29 is a system diagram showing the structure of an exhaust system of a pressure reduction system. FIG. 30A is a plan view showing the configuration of the holding member 12o. Fig. 30B is a side view showing the configuration of the holding member 12o. FIG. 31 is a longitudinal sectional view showing the configuration of the rotation driving section 28 disposed below the heating section 24. As shown in FIG. Fig. 32 is a longitudinal sectional view showing an enlarged "rotation drive unit".
O:\87\87879.DOC -61 - 1238453 圖33A係顯示托架冷卻機構234構成之橫剖面圖。 圖33B係顯示托架冷卻機構234構成之側面圖。 圖34係顯示旋轉位置檢測機構232構成之橫剖面圖。 圖3 5 A係顯示旋轉位置檢測機構2 3 2之非檢測狀態之圖。 圖35B係顯示旋轉位置檢測機構232之檢測狀態之圖。 圖36A係顯示旋轉位置檢測機構232之受光元件268之輸 出信號S之波形圖。 圖36B為從旋轉位置判定電路270所輸出之脈衝信號P之 波形圖。 圖37為說明控制電路所進行旋轉位置控制處理之流程 圖。 圖38為從上方所見窗口 75、76之安裝處之橫剖面圖。 圖39係擴大顯示窗口 75之橫剖面圖。 圖40係擴大顯示窗口 76之橫剖面圖。 圖41A係顯示下部盒體102構成之俯視圖。 圖41B係顯示下部盒體102構成之側面圖。 圖42A係顯示側面盒體104構成之俯視圖。 圖42B係顯示側面盒體104構成之前視圖。 圖42C係顯示側面盒體104構成之後視圖。 圖42D係顯示側面盒體104構成之左側視圖。 圖42E係顯示側面盒體104構成之右側視圖。 圖43A係顯示上部盒體106構成之仰視圖。 圖43B係顯示上部盒體106構成之側面圖。 圖44A係顯示圓筒狀盒體108構成之俯視圖。 O:\87\87879.DOC -62- 1238453 圖44B係顯示圓筒狀盒體1〇8構成之側面縱剖面圖。 圖44c係顯示圓筒狀盒體1〇8構成之側面圖。 圖45係擴大顯示升降桿機構3〇之縱剖面圖。 圖46為擴大顯示升降桿機構儿之密封構造之縱剖面圖。 圖47A係顯示使用圖2之基板處理裝置2〇, 板歡自由編情形之㈣及侧。 圖47B係顯示圖47A之構成之俯視圖。 圖48係顯示使用基板處理裝置,所進行之基板氧化處 理步驟之圖。 圖9係顯示根據本發明所使用之之膜厚測定方法之 圖。 圖5〇係顯不根據本發明所使用之xps之膜厚測定方法之 其他圖。 圖51係概略地顯不藉由基板處理裝置2〇形成氧化膜之 際所觀/則到氧化膜厚成長之停滞現象之圖。 圖52A係顯不於矽基板表面之氧化膜形成過程1之圖。 圖52B係顯不於矽基板表面之氧化膜形成過程2之圖。 圖53係顯不於本發明第丨實施例中,所得到之氧化膜之漏 洩電流特性之圖。 圖54A為說明圖53之漏洩電流特性原因之圖。 圖54B為說明圖5 3之漏洩電流特性原因之圖。 圖55A係顯示於基板處理裝置川所產生之氧化膜形成步 驟1之圖。 圖55B係顯不於基板處理裝置2〇所產生之氧化膜形成步O: \ 87 \ 87879.DOC -61-1238453 Fig. 33A is a cross-sectional view showing the structure of the bracket cooling mechanism 234. Fig. 33B is a side view showing the structure of the bracket cooling mechanism 234. FIG. 34 is a cross-sectional view showing the configuration of the rotation position detecting mechanism 232. FIG. 3A is a diagram showing the non-detection state of the rotational position detecting mechanism 2 3 2. FIG. 35B is a diagram showing a detection state of the rotation position detecting mechanism 232. Fig. 36A is a waveform diagram showing an output signal S of the light receiving element 268 of the rotation position detecting mechanism 232. FIG. 36B is a waveform diagram of the pulse signal P output from the rotation position determination circuit 270. Fig. 37 is a flowchart illustrating a rotational position control process performed by the control circuit. Figure 38 is a cross-sectional view of the installation location of the windows 75, 76 seen from above. Fig. 39 is a cross-sectional view of the enlarged display window 75. Fig. 40 is a cross-sectional view of the enlarged display window 76. FIG. 41A is a plan view showing the structure of the lower case 102. FIG. FIG. 41B is a side view showing the structure of the lower case 102. FIG. FIG. 42A is a plan view showing the configuration of the side box body 104. FIG. FIG. 42B is a front view showing the structure of the side box body 104. FIG. FIG. 42C is a rear view showing the configuration of the side box body 104. FIG. FIG. 42D is a left side view showing the structure of the side box 104. FIG. 42E is a right side view showing the structure of the side box 104. FIG. FIG. 43A is a bottom view showing the structure of the upper case 106. FIG. FIG. 43B is a side view showing the structure of the upper case 106. FIG. FIG. 44A is a plan view showing the configuration of the cylindrical case 108. FIG. O: \ 87 \ 87879.DOC -62- 1238453 Fig. 44B is a side longitudinal sectional view showing the structure of a cylindrical box body 108. Fig. 44c is a side view showing the configuration of the cylindrical case body 108. Fig. 45 is an enlarged longitudinal sectional view of the lifter mechanism 30. Fig. 46 is a longitudinal sectional view showing an enlarged seal structure of the lift lever mechanism. FIG. 47A shows the side and the side of the case where the board is freely edited using the substrate processing apparatus 20 of FIG. 2. Fig. 47B is a plan view showing the structure of Fig. 47A. Fig. 48 is a diagram showing the substrate oxidation processing steps performed using a substrate processing apparatus. Fig. 9 is a diagram showing a film thickness measurement method used in accordance with the present invention. Fig. 50 is a diagram showing another method for measuring the film thickness of xps used in accordance with the present invention. Fig. 51 is a diagram schematically showing a stagnation phenomenon observed until the oxide film thickness grows when the oxide film is formed by the substrate processing apparatus 20. FIG. 52A is a diagram showing an oxide film formation process 1 on the surface of a silicon substrate. FIG. 52B is a view showing an oxide film formation process 2 on the surface of the silicon substrate. Fig. 53 is a graph showing the leakage current characteristics of the obtained oxide film in the first embodiment of the present invention. FIG. 54A is a diagram illustrating the cause of the leakage current characteristic of FIG. 53. FIG. 54B is a diagram explaining the cause of the leakage current characteristic of FIG. 53. FIG. Fig. 55A is a diagram showing an oxide film forming step 1 generated in the substrate processing apparatus. FIG. 55B shows an oxide film formation step generated by the substrate processing apparatus 20
O:\87\87879.DOC -63- 1238453 驟2之圖。 圖550係顯示於基板處理裝置2〇所產生之氧化膜形成步 驟3之圖。 圖56係顯示於基板處理裝㈣所使用之遠距離電激源構 成之圖。 圖57為比較RF遠距離電漿與微波電漿特性之圖。 圖58為比較RF遠距離電漿與微波電漿特性之其他圖。 圖59A係顯示使用基板處理裝置2〇所進行之氧化膜之氮 化處理之側面圖。 圖59B係顯示使用基板處理裝置2()所進行之氧化膜之氮 化處理之俯視圖。 圖60A係顯示使用遠距離電漿部27,以表2所示條件對藉 由基板處理裝置20在石夕基板上以熱氧化處理形成之2.0 nm 厚之氧化膜’進行氮化時之前述氧化膜中之氮濃度分佈圖。 _係顯示於相同氧化膜中之氮濃度分佈與氧濃度分 佈之關係圖。 圖61係顯示在本發明所使用之又“之概略圖。 ,圖62係顯不根據氧化膜之遠距離電聚之氮化時間與膜中 氮濃度之關係圖。 圖63係顯示氧化膜之氮化時間與氮之膜内分佈之關係 圖。 圖64係顯示根據氧化膜之氮化處理所形成之整個氧氮化 膜之晶圓之膜厚變動圖。 圖65係顯示隨著因本實施例之氧化膜氮化處理之膜厚增O: \ 87 \ 87879.DOC -63-1238453 Picture of step 2. FIG. 550 is a view showing an oxide film forming step 3 generated in the substrate processing apparatus 20. FIG. Fig. 56 is a diagram showing the composition of a long-distance electric source used in the substrate processing apparatus. Figure 57 is a graph comparing the characteristics of RF long-range plasma and microwave plasma. Fig. 58 is another graph comparing the characteristics of RF long-range plasma and microwave plasma. Fig. 59A is a side view showing the nitriding treatment of the oxide film using the substrate processing apparatus 20. Fig. 59B is a plan view showing the nitriding treatment of the oxide film using the substrate processing apparatus 2 (). FIG. 60A shows the aforementioned oxidation when nitriding the 2.0 nm-thick oxide film 'formed on the Shixi substrate by the substrate processing apparatus 20 by thermal oxidation treatment using the remote plasma unit 27 under the conditions shown in Table 2. Distribution of nitrogen concentration in the film. _ Is a graph showing the relationship between the nitrogen concentration distribution and the oxygen concentration distribution in the same oxide film. Fig. 61 is a schematic diagram showing the "" used in the present invention. Fig. 62 is a graph showing the relationship between the nitriding time and the nitrogen concentration in the film based on the long-distance electropolymerization of the oxide film. The relationship between the nitriding time and the nitrogen distribution in the film. Figure 64 shows the film thickness variation of the entire oxynitride film formed by the nitriding process of the oxide film. Film thickness increase
O:\87\87879.DOC -64- 1238453 加圖。 【圖式代表符號說明】 10半導體裝置 ’ 11 Si基板 12基底氧化膜 12 A氧氮化膜 13高電介質膜 14 閘極電極 20基板處理裝置 22處理容器 22a前部 22b後部 22c底部 22d左側面 22e 右側面 22g供給口 24加熱部 26 紫外線照射部 26a 筐體 26b底部開口 26c 邊緣部 27遠距離電漿部 27a氣體循環通路 27b 氣體入口 128 馬達 128a驅動軸 130磁鐵聯結器 132昇降臂 134 昇降軸 136 驅動部 138a〜138c抵接銷 140 凸緣 142 中央孔 144 第1水路 146 第1凸緣 146a L字形之連通孔 146b 階狀部 148 第2凸緣 150 第2水路 152第1流入管路 154 第1流入口 156流出管路 158 第1流出口 160螺栓 162安裝孔 164溫度感應器 O:\87\87879.DOC -65- 1238453 27c 氣體出口 166a〜166f電源纜線連接用端子 27d 氟素樹脂加工 170 第2流入口 27e 離子過濾器 174 第2流出口 27A 區塊 176 栓 27B 鐵氧體磁心 178 位置決定孔 27C 電漿 180 密封構件(0環) 28 旋轉驅動部 182 密封構件(0環) 30 升降桿機構 184 密封構件(0環) 32 排氣路徑 186 密封構件(0環) 32a 開口部 188 密封構件(0環) 32b 錐形部 190 夾钳機構 32c 底部 190a 外筒 32d 主排氣管 190b 軸 32e 排出口 192 螺旋彈簧 32f 下部 193 螺母 32g 分流用排出口 195 墊片 34 氣體供給部 196 發熱控制電路 36 框 197, 199 L字形墊片 38 底部框 197a,199a 圓筒部 40,41 垂直框 197b,199b 突出部 40a 電纜線導管 197c,197d 圓筒部 41a 排氣導管 198 溫度調整器 42 中間框 200 電源 44 上部框 201 幫浦 O:\87\87879.DOC -66 1238453 46 冷卻水供給部 48a,48b 電磁閥之排氣用閥 50渦輪分子幫浦 50a 吐出管 51真空管路 51a分流管路 52 電源單位 57 UV燈控制器 58 氣體管路 60緊急停止開關 62托架 64溫度調整器 66氣體箱 68離子測量控制器 70 APC控制器 72 TMP控制器 74排氣口 75 第1窗口 76 第2窗口 77感應器單元 80 室 80a貫通孔 82蓋子構件 84製程空間(處理空間) 202排氣管路 204排氣管路 205 壓力計 206 閥 208 分歧管路 210 閥 211 可變隔膜 212 閥 214壓力計 216 渦輪管路 218 逆止閥 220 隔膜 222 閥 230托架 230a 冷卻水用之水路 230b 冷卻水供給孔 230c 冷卻水供給排出孔 230d 中央孔 230e,230f 貫通孔 232旋轉位置檢測機構 234托架冷卻機構 236, 237 陶瓷軸承 238 凸緣 240螺栓 O:\87\87879.DOC -67- 1238453 85感應器單元 85a〜85c壓力計 86, 87外線光源(紫外線光源) 88透明窗 88a 密封面 88b 防護罩 89密封構件(〇環) 90供給管路 91鎖緊構件 92供給口 93氣體喷射喷嘴部 93al〜93an 喷射口 93bl〜93b3 喷嘴板 93cl〜93c3 凹部 93dl〜93d3 供給孔 94搬送口 96閘極閥 97a第1質量控制器 97b第2質量控制器 98搬送自動機 991〜995 氣體供給管路 100石英墊圈 102 下部盒體 104側面盒體 242 凸緣 244 間隔壁 246排氣孔 248 從動側磁鐵 250磁鐵罩 252氛圍側旋轉部 252a下端部 254,255 軸承 256 驅動側磁鐵 257傳達構件 258旋轉檢測單元 260,261 狹縫板 262, 263 光斷續器 264軸承架 266發光元件 268 受光元件 268 受光元件 270旋轉位置判定電路 272 透明石英 274 UV玻璃 276 窗口安裝部 277 小螺釘 278 第1窗框 280密封構件 O:\87\87879 DOC 68- 1238453 282 第2窗框 284 小螺釘 286 開口 292 透明石英 294 UV玻璃 296 窗口安裝部 297 小螺釘 298 第1窗框 300密封構件(0環) 302 第2窗框 304小螺釘 310圓形開口 310a〜310c 凹部 310d 凹部 312開口(長方形) 314a,314b 突起 315'階狀部 316狹缝 317 開口 318 凹部 319 圓形孔 320〜322 孔 324, 325 長方形開口 104a 正面 104b 背面 106 上部盒體 108 圓筒狀盒體 108 a〜108c 凹部 108d 突起 110底座 112石英鐘罩 112a突出部 112b 圓筒部 112c頂板 112d 中空部 112e梁部 112f 穿插孔 112g〜112i輪轂 113 内部空間 114 SiC加熱器 114a第1發熱部 114b,114c第2,第3發熱部 114d 穿插孔 114e 穿插孔 116熱反射構件(反射器) 116a 穿插孔 118 SiC基板設置台(加熱構件)326階狀部 O:\87\87879.DOC -69- 1238453 119 高溫計 120保持構件 120a〜120c 臂部 120d保持構件 120e〜120g輪轂 120i 倒角加工部 122 外殼 124 内部空間 126 陶瓷軸 327〜329 圓形孔 330 四角孔 332伸縮管 334螺栓 336連接構件 338 陶瓷蓋 340蓋子構件 411 矽基板 412氧化膜 441 矽基板 442 氧化膜 443 ZrSiOx O:\87\87879.DOC -70-O: \ 87 \ 87879.DOC -64- 1238453 [Illustration of Symbols] 10 semiconductor device 11 Si substrate 12 base oxide film 12 A oxynitride film 13 high dielectric film 14 gate electrode 20 substrate processing device 22 processing container 22a front 22b rear 22c bottom 22d left side 22e Right side 22g supply port 24 heating section 26 ultraviolet irradiation section 26a cabinet 26b bottom opening 26c edge section 27 remote plasma section 27a gas circulation path 27b gas inlet 128 motor 128a drive shaft 130 magnet coupling 132 lift arm 134 lift shaft 136 Drive sections 138a to 138c abut pin 140 flange 142 center hole 144 first water passage 146 first flange 146a L-shaped communication hole 146b stepped portion 148 second flange 150 second water passage 152 first inflow pipe 154 first 1 inlet 156 outlet pipe 158 1st outlet 160 bolt 162 mounting hole 164 temperature sensor O: \ 87 \ 87879.DOC -65- 1238453 27c gas outlet 166a ~ 166f terminal for power cable connection 27d fluorine resin processing 170 2nd inlet 27e ion filter 174 2nd outlet 27A block 176 plug 27B ferrite core 178 position determining hole 27C plasma 180 seal member (0 ring) 28 rotary drive Portion 182 Seal member (0 ring) 30 Lifting rod mechanism 184 Seal member (0 ring) 32 Exhaust path 186 Seal member (0 ring) 32a Opening portion 188 Seal member (0 ring) 32b Tapered portion 190 Clamp mechanism 32c Bottom 190a Outer cylinder 32d Main exhaust pipe 190b Shaft 32e Discharge port 192 Coil spring 32f Lower 193 Nut 32g Diversion port 195 Gasket 34 Gas supply unit 196 Heating control circuit 36 Frame 197, 199 L-shaped gasket 38 Bottom frame 197a, 199a cylindrical part 40, 41 vertical frame 197b, 199b protruding part 40a cable duct 197c, 197d cylindrical part 41a exhaust duct 198 temperature regulator 42 middle frame 200 power supply 44 upper frame 201 pump O: \ 87 \ 87879. DOC -66 1238453 46 Cooling water supply unit 48a, 48b Exhaust valve for solenoid valve 50 Turbo molecular pump 50a Discharge pipe 51 Vacuum line 51a Divert line 52 Power supply unit 57 UV lamp controller 58 Gas line 60 Emergency stop switch 62 bracket 64 temperature regulator 66 gas box 68 ion measurement controller 70 APC controller 72 TMP controller 74 exhaust port 75 first window 76 second window 77 sensor unit 80 chamber 80a penetrates Hole 82 Cover member 84 Process space (processing space) 202 Exhaust line 204 Exhaust line 205 Pressure gauge 206 Valve 208 Branch line 210 Valve 211 Variable diaphragm 212 Valve 214 Pressure gauge 216 Turbine line 218 Check valve 220 Diaphragm 222 Valve 230 Bracket 230a Water passage for cooling water 230b Cooling water supply hole 230c Cooling water supply discharge hole 230d Central hole 230e, 230f Through hole 232 Rotary position detection mechanism 234 Bracket cooling mechanism 236, 237 Ceramic bearing 238 Flange 240 Bolt O: \ 87 \ 87879.DOC -67- 1238453 85 sensor unit 85a ~ 85c pressure gauge 86, 87 external light source (ultraviolet light source) 88 transparent window 88a sealing surface 88b protective cover 89 sealing member (〇ring) 90 supply pipe Road 91 locking member 92 supply port 93 gas injection nozzle section 93al ~ 93an injection port 93bl ~ 93b3 nozzle plate 93cl ~ 93c3 recess 93dl ~ 93d3 supply hole 94 transfer port 96 gate valve 97a first quality controller 97b second quality control Device 98 transfer automatic machine 991 ~ 995 gas supply line 100 quartz gasket 102 lower case 104 side case 242 flange 244 partition wall 246 exhaust hole 248 driven side magnet 250 magnet cover 252 atmosphere Side rotation portion 252a Lower end portion 254, 255 Bearing 256 Drive side magnet 257 Transmission member 258 Rotation detection unit 260, 261 Slot plate 262, 263 Photointerrupter 264 Bearing frame 266 Light emitting element 268 Light receiving element 268 Light receiving element 270 Rotation position determination circuit 272 Transparent quartz 274 UV glass 276 Window mounting section 277 Small screw 278 First window frame 280 Seal member O: \ 87 \ 87879 DOC 68- 1238453 282 Second window frame 284 Small screw 286 Opening 292 Transparent quartz 294 UV glass 296 Window mounting section 297 Small Screw 298 1st window frame 300 sealing member (0 ring) 302 2nd window frame 304 small screw 310 circular opening 310a ~ 310c recessed portion 310d recessed portion 312 opening (rectangular) 314a, 314b protrusion 315 'stepped portion 316 slit 317 opening 318 recess 319 round hole 320 ~ 322 holes 324, 325 rectangular opening 104a front 104b back 106 upper case 108 cylindrical case 108 a ~ 108c recess 108d protrusion 110 base 112 quartz bell cover 112a protrusion 112b cylinder 112c top plate 112d Hollow section 112e Beam section 112f Insertion hole 112g ~ 112i Hub 113 Internal space 114 SiC heater 114a First heating section 114b, 114c 2, the third heating part 114d through the socket 114e through the socket 116 thermal reflection member (reflector) 116a through the socket 118 SiC substrate setting table (heating member) 326 step-shaped part O: \ 87 \ 87879.DOC -69- 1238453 119 pyrometer 120 holding member 120a ~ 120c arm 120d holding member 120e ~ 120g hub 120i chamfered portion 122 housing 124 internal space 126 ceramic shaft 327 ~ 329 round hole 330 corner hole 332 telescopic tube 334 bolt 336 connection member 338 Ceramic cover 340 cover member 411 silicon substrate 412 oxide film 441 silicon substrate 442 oxide film 443 ZrSiOx O: \ 87 \ 87879.DOC -70-
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| JP2002278200A JP2004119523A (en) | 2002-09-24 | 2002-09-24 | Substrate processing equipment |
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| TW200421433A TW200421433A (en) | 2004-10-16 |
| TWI238453B true TWI238453B (en) | 2005-08-21 |
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| TW092126222A TWI238453B (en) | 2002-09-24 | 2003-09-23 | Substrate processing equipment |
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| AU (1) | AU2003266566A1 (en) |
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| TWI775073B (en) * | 2020-05-07 | 2022-08-21 | 台灣積體電路製造股份有限公司 | Method and apparatus for light curing |
| TWI792020B (en) * | 2019-08-16 | 2023-02-11 | 家登精密工業股份有限公司 | Quick-release valve module, reticle pod provided with quick-release valve module, and method for quickly providing quick-release valve module on reticle pod |
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| JP5409903B2 (en) * | 2010-05-17 | 2014-02-05 | 株式会社アルバック | Vacuum processing apparatus, processing object processing method, and film forming apparatus |
| JP2019047042A (en) * | 2017-09-05 | 2019-03-22 | 東芝メモリ株式会社 | Semiconductor manufacturing equipment |
| CN113628987B (en) * | 2020-05-07 | 2025-03-28 | 台湾积体电路制造股份有限公司 | Light curing method and device |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JPH0377315A (en) * | 1989-08-21 | 1991-04-02 | Daiwa Handotai Sochi Kk | Semiconductor manufacturing apparatus using mo-cvd method |
| JP3035953B2 (en) * | 1990-02-22 | 2000-04-24 | ソニー株式会社 | (III)-(V) Group Compound Semiconductor Vapor Phase Growth Method |
| JP3338884B2 (en) * | 1993-09-20 | 2002-10-28 | 株式会社日立製作所 | Semiconductor processing equipment |
| JP2000068215A (en) * | 1998-08-18 | 2000-03-03 | Shin Etsu Handotai Co Ltd | Method for growing vapor phase thin film and device therefor |
-
2002
- 2002-09-24 JP JP2002278200A patent/JP2004119523A/en active Pending
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2003
- 2003-09-22 WO PCT/JP2003/012086 patent/WO2004030066A1/en not_active Ceased
- 2003-09-22 AU AU2003266566A patent/AU2003266566A1/en not_active Abandoned
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI792020B (en) * | 2019-08-16 | 2023-02-11 | 家登精密工業股份有限公司 | Quick-release valve module, reticle pod provided with quick-release valve module, and method for quickly providing quick-release valve module on reticle pod |
| TWI775073B (en) * | 2020-05-07 | 2022-08-21 | 台灣積體電路製造股份有限公司 | Method and apparatus for light curing |
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| Publication number | Publication date |
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| JP2004119523A (en) | 2004-04-15 |
| AU2003266566A1 (en) | 2004-04-19 |
| WO2004030066A1 (en) | 2004-04-08 |
| TW200421433A (en) | 2004-10-16 |
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