TW201215250A - Plasma processing device and plasma processing method - Google Patents

Plasma processing device and plasma processing method Download PDF

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Publication number
TW201215250A
TW201215250A TW100110999A TW100110999A TW201215250A TW 201215250 A TW201215250 A TW 201215250A TW 100110999 A TW100110999 A TW 100110999A TW 100110999 A TW100110999 A TW 100110999A TW 201215250 A TW201215250 A TW 201215250A
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Taiwan
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plasma
electromagnetic wave
wafer
microwave
gas
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TW100110999A
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Chinese (zh)
Inventor
Shigenori Ozaki
Nobuhiko Yamamoto
Yutaka Fujino
Atsushi Ueda
Junichi Kitagawa
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Tokyo Electron Ltd
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Publication of TW201215250A publication Critical patent/TW201215250A/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32Gas-filled discharge tubes
    • H01J37/32431Constructional details of the reactor
    • H01J37/32733Means for moving the material to be treated
    • H01J37/32752Means for moving the material to be treated for moving the material across the discharge
    • H01J37/32761Continuous moving
    • H01J37/32779Continuous moving of batches of workpieces
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32Gas-filled discharge tubes
    • H01J37/32009Arrangements for generation of plasma specially adapted for examination or treatment of objects, e.g. plasma sources
    • H01J37/32192Microwave generated discharge

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Plasma Technology (AREA)

Abstract

The disclosed plasma processing device (100) is provided with: a processing vessel (1); a table (3) that supports a plurality of wafers (W); and a plurality of microwave introduction units (27) that introduce electromagnetic waves for causing the generation of plasma at a plurality of sites within the processing vessel (1). The configuration is such that each of the wafers (W) carried on the carrying region (SR) of the table (3) can move relatively in a manner so as to pass through a position facing the microwave-transmitting region of the transmitting plate (28) of at least one of the microwave introduction units (27). The transmitting plates (28) can be disposed in a manner so that the time integral value of plasma density and/or the integral value of plasma irradiation time is the same at any position over the wafers.

Description

201215250 六、發明說明: 【發明所屬之技術領域】 本發明是有關往處理容器引導預定頻率的電磁波,使 產生電漿來電漿處理被處理體之電漿處理裝置及電漿處理 方法。 【先前技術】 對半導體晶圓等的被處理體,例如進行氧化處理或氮 化處理、CVD ( Chemical Vapor Deposition)處理、餓刻 處理等的電漿處理。電漿處理裝置有利用具有複數個縫隙 的平面天線來導入微波至處理容器內而使電漿生成的縫隙 天線方式的電漿處理裝置爲人所知。又,其他方式的電漿 處理裝置,有利用線圈狀的天線來導入高頻至處理容器內 而使電漿生成的感應稱合型電獎(Inductively^Coupled Plasma ; ICP)方式的電漿處理裝置爲人所知。如此的電 漿處理裝置可在處理容器內使高密度的電漿生成。 爲了朝次世代以後的裝置開發,例如一邊謀求對3次 元裝置加工或微細化的對應,一邊使生產性提升,而需要 一邊確保基板面內的處理的均一性,一邊處理複數的被處 理體,或使被處理體目前爲直徑3 00mm的基板大型化成 直徑450mm。因應於此,需要在對應於基板而大型化的 處理容器內使電漿密度的分布均一化。 在上述縫隙天線方式的電漿處理裝置中,產生於處理 容器內的電漿的密度控制是藉由縫隙的形狀或配置、處理 -5- 201215250 容器或微波導入窗的形狀設計等來進行。例如,爲了按照 處理內容來改變電漿密度的分布,需要更換成不同縫隙的 形狀或配置的平面天線。並且,在上述ICP方式的電漿處 理裝置中,也是爲了改變電漿密度的分布,而需要變換成 不同線圏形狀或配置的天線。但,此天線的更換是費時又 費力的大規模作業。 並且,在處理容器內所生成的電漿密度的分布,亦可 藉由例如改變微波的功率、處理壓力、氣體流量等的製程 參數來微調。但,該等的製程參數是無法與製程條件分割 ,因此可使製程參數變化的範圍的電漿密度分布的變化幅 度(界限)小,其效果有限。 而且,因平面天線、處理容器等的製作公差、組裝誤 差、同一款式的裝置間的機器差等的諸因素,而有在處理 容器內電漿的對稱性瓦解,電漿密度的分布偏心的情形發 生。此情況,並無簡易的方法來予以補正的手段,因此會 有需要平面天線的更換等大規模的裝置改變的問題。 可是,有爲了同時處理複數的大型基板,而設置複數 的微波導入窗,且使對應於各微波導入窗,在各個的下方 設置試料台之電漿處理裝置被提案(例如專利文獻1)。 更有從複數的微波導入窗來分別導入微波而形成電漿,藉 此對一片的大型基板進行均一的電漿處理之電漿處理裝置 被提案(例如專利文獻2)。並且,在具有複數的天線及 複數的微波導入窗的裝置中,可按各天線供給不同電力的 微波之電漿處理裝置也被提案(例如專利文獻3)。201215250 VI. Description of the Invention: [Technical Field] The present invention relates to a plasma processing apparatus and a plasma processing method for guiding electromagnetic waves of a predetermined frequency to a processing container to cause plasma to be processed into a processed object. [Prior Art] For the object to be processed such as a semiconductor wafer, for example, plasma treatment such as oxidation treatment, nitrogenation treatment, CVD (Chemical Vapor Deposition) treatment, or starving treatment is performed. The plasma processing apparatus is known in the art of a slit antenna type plasma processing apparatus which uses a planar antenna having a plurality of slits to introduce microwaves into a processing container to generate plasma. Further, in another type of plasma processing apparatus, there is a plasma processing apparatus of an Inductively Coupled Plasma (ICP) type in which a high frequency is introduced into a processing container by a coil-shaped antenna to generate plasma. Known. Such a plasma processing apparatus can generate high density plasma in a processing vessel. For the development of the device after the next generation, for example, while improving the productivity of the three-dimensional device processing or miniaturization, it is necessary to process a plurality of processed objects while ensuring the uniformity of the processing in the substrate surface. Alternatively, the substrate to be processed is currently grown to a diameter of 450 mm in a substrate having a diameter of 300 mm. In response to this, it is necessary to uniformize the distribution of the plasma density in the processing container which is enlarged corresponding to the substrate. In the above-described slot antenna type plasma processing apparatus, the density control of the plasma generated in the processing container is performed by the shape or arrangement of the slit, the shape design of the container or the microwave introduction window, and the like. For example, in order to change the distribution of plasma density in accordance with the processing content, it is necessary to replace the planar antenna with a shape or configuration of a different slit. Further, in the plasma processing apparatus of the ICP method described above, in order to change the distribution of the plasma density, it is necessary to convert the antenna into a different coil shape or arrangement. However, the replacement of this antenna is a time-consuming and laborious large-scale operation. Further, the distribution of the plasma density generated in the processing vessel can be finely adjusted by, for example, changing process parameters such as microwave power, processing pressure, gas flow rate, and the like. However, these process parameters cannot be separated from the process conditions, so that the variation width (limit) of the plasma density distribution in the range in which the process parameters vary can be made small, and the effect is limited. Further, due to factors such as manufacturing tolerances of the planar antenna and the processing container, assembly errors, and machine differences between devices of the same type, there is a case where the symmetry of the plasma in the processing container collapses and the distribution of the plasma density is eccentric. occur. In this case, there is no simple way to correct the problem, and there is a problem that a large-scale device change such as replacement of a planar antenna is required. However, in order to simultaneously process a plurality of large-sized substrates, a plurality of microwave introduction windows are provided, and a plasma processing apparatus in which a sample stage is provided under each of the microwave introduction windows is proposed (for example, Patent Document 1). Further, a plasma processing apparatus in which a plurality of large-sized substrates are subjected to uniform plasma treatment is proposed (for example, Patent Document 2). Further, in a device having a plurality of antennas and a plurality of microwave introduction windows, a microwave plasma processing apparatus capable of supplying microwaves of different electric power for each antenna has also been proposed (for example, Patent Document 3).

S -6- 201215250 並且,爲了有效率地進行複數的處理工程,而在處理 容器內設置藉由隔壁所分割的複數個處理室,在其下方可 旋轉地配備用以載置複數的基板的載置台之處理裝置也被 提案(例如專利文獻4)。 而且,在縫隙天線方式的電漿處理裝置中,使用構成 可藉由鐵心調諧器來使微波的相位變化之複數的天線模組 ,作爲對處理容器內導入微波的機構之電漿處理裝置也被 提案(例如專利文獻5)。 先行技術文獻 專利文獻 專利文獻1 :日本國特開平8-255785號公報 專利文獻2 :日本國特開平1 0-92797號公報 專利文獻3 :日本國特開2004- 1 283 85號公報 專利文獻4 :日本國特開平6-204147號公報 專利文獻5 :日本國特開20 1 0- 1 70974號公報 【發明內容】 爲了調整處理容器內的電漿密度的分布,可想在處理 容器內使複數的電漿獨立產生有效。但,若各電漿的產生 部位及被處理體的配置爲固定,則會因鄰接的電漿彼此間 的距離或電漿的擴散程度,而在電漿密度產生高低的分布 ,反而會有難以謀求被處理體的面內的處理均一化的課題 201215250 本發明的目的是在處理容器內使複數的電漿產生之方 式的電漿處理裝置中,容易控制電漿密度的分布,而在被 處理體的面內實現所望的處理。 本發明的電漿處理.裝置,係具備: 可抽真空的處理容器,其係形成處理被處理體的處理 空間; 支撐裝置,其係於上述處理容器內支撐被處理體; 電磁波產生裝置,其係產生電磁波,該電磁波係用以 使電漿生成於上述處理容器內; 複數的電磁波導入單元,其係將在上述電磁波產生裝 置產生的電磁波導入至上述處理容器內;及 驅動裝置,其係以上述支撐裝置的中央作爲旋轉中心 ,使被該支撐裝置支撐的複數的被處理體及/或上述複數 的電磁波導入單元旋轉,而使環繞運動, 上述電磁波導入單元係具有電磁波導入窗,該電磁波 導入窗係面對上述處理空間而設置,使電磁波透過而導入 至上述處理容器內, 上述支撐裝置係具有載置複數的被處理體之載置台, 被載置於上述載置台的複數的被處理體係對上述電磁 波導入窗相對移動,以各個的被處理體至少通過一個上述 電磁波導入窗的電磁波透過區域的對向位置之方式構成。 又,本發明的電漿處理裝置,亦可在上述相對移動之 間,以一個的被處理體對於2個以上的上述電磁波導入窗 至少部分地依序通過對向的位置之方式構成。S -6-201215250 Further, in order to efficiently perform a plurality of processing projects, a plurality of processing chambers divided by the partition walls are provided in the processing container, and a plurality of substrates for mounting the plurality of substrates are rotatably provided below the processing chamber. A processing device for setting the table is also proposed (for example, Patent Document 4). Further, in the plasma processing apparatus of the slot antenna type, an antenna module constituting a plurality of phases which can change the phase of the microwave by the core tuner is used as a plasma processing apparatus for a mechanism for introducing microwaves into the processing container. Proposal (for example, Patent Document 5). CITATION LIST Patent Literature Patent Literature 1: Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. Japanese Patent Application Laid-Open No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. The plasma is produced independently. However, if the position where the plasma is generated and the arrangement of the object to be processed are fixed, the plasma density may be high or low due to the distance between adjacent plasmas or the degree of plasma diffusion. The problem of uniformizing the processing in the surface of the object to be processed 201215250 The object of the present invention is to easily control the distribution of the plasma density in the plasma processing apparatus in which a plurality of plasmas are generated in the processing container. The desired processing is achieved in-plane. The plasma processing apparatus of the present invention includes: a vacuum-processable processing container that forms a processing space for processing the object to be processed; a supporting device that supports the object to be processed in the processing container; and an electromagnetic wave generating device Generating electromagnetic waves for generating plasma in the processing container; a plurality of electromagnetic wave introducing units for introducing electromagnetic waves generated by the electromagnetic wave generating device into the processing container; and driving means for The center of the support device serves as a center of rotation, and a plurality of objects to be processed supported by the support device and/or the plurality of electromagnetic wave introduction units are rotated to cause a wraparound motion. The electromagnetic wave introduction unit has an electromagnetic wave introduction window, and the electromagnetic wave is introduced. The window system is provided to face the processing space, and electromagnetic waves are transmitted and introduced into the processing container. The supporting device has a mounting table on which a plurality of objects to be processed are placed, and a plurality of processed systems placed on the mounting table Relatively moving the electromagnetic wave introduction window to each of the processed bodies By introducing at least one of said electromagnetic waves through a window constituting the embodiment of the location area. Further, the plasma processing apparatus of the present invention may be configured such that one of the objects to be processed passes through the opposing positions at least partially in sequence with respect to the two or more electromagnetic wave introduction windows between the relative movements.

S -8- 201215250 又,本發明的電漿處理裝置,亦可在上述相對移動之 間,以一個的被處理體同時對於2個以上的上述電磁波導 入窗至少部分地通過對向的位置之方式構成。 又,本發明的電漿處理裝置中,上述複數的電磁波導 入窗係以藉由從各電磁波導入窗所導入的電磁波來生成的 電漿之電漿密度的時間性累計値及/或電漿照射時間的累 計値無論在一個被處理體的哪個位置皆形成相同之方式配 置。 又,本發明的電漿處理裝置,亦可更具備輔助性的電 磁波導入單元,其係對於上述相對移動的被處理體的軌道 ,具有設於偏離對向的位置之位置的電磁波導入窗。 又,本發明的電漿處理裝置,亦可具備複數的電磁波 導入單元,其係上述電磁波導入窗的面積相異。 又,本發明的電漿處理裝置,上述電磁波產生裝置亦 可對應於上述電磁波導入單元來個別地設置。 又,本發明的電漿處理裝置,供給至上述複數的電磁 波導入單元的電磁波的功率可個別地設定。 又,本發明的電漿處理裝置,從處於接近上述旋轉中 心的位置之內側的電磁波導入窗所導入的電磁波的功率與 從比該內側的電磁波導入窗更位於環繞半徑的外側之外側 的電磁波導入窗所導入的電磁波的功率相異。 本發明的電漿處理方法,係使用電漿處理裝置,經由 上述複數的電磁波導入窗來將電磁波導入至上述處理容器 內而使電漿生成,且在上述處理容器之中以被處理體至少 201215250 通過一個上述電磁波導入窗的電磁波透過區域的對向位置 之方式,一邊使被處理體對於上述電磁波導入窗相對移動 ’一邊以無論在被處理體上的那個位置,電漿密度的時間 性累計値及/或電漿照射時間的累計値皆形成相同的方式 進行電漿處理, 該電漿處理裝置係具備: 可抽真空的處理容器,其係形成處理被處理體的處理 空間; 支撐裝置’其係於上述處理容器內支撐被處理體; 電磁波產生裝置,其係產生電磁波,該電磁波係用以 使電漿生成於上述處理容器內; 複數的電磁波導入單元,其係將在上述電磁波產生裝 置產生的電磁波導入至上述處理容器內;及 驅勳裝置,其係以上述支撐裝置的中央作爲旋轉中心 ,使被該支撐裝置支撐的複數的被處理體及/或上述複數 的電磁波導入單元旋轉,而使環繞運動, 上述電磁波導入單元係具有電磁波導入窗,該電磁波 導入窗係面對上述處理空間而設置,使電磁波透過而導入 至上述處理容器內, 上述支撐裝置係具有載置複數的被處理體之載置台。 若根據本發明,則以被載置於支撐裝置的被處理體至 少通過一個電磁波導入窗的電磁波透過區域的對向位置之 方式設成可相對移動。而且,以無論在被處理體上的哪個 位置,電漿密度的時間性累計値及/或電漿照射時間的累Further, the plasma processing apparatus according to the present invention may be configured such that at least one of the objects to be processed simultaneously passes through the opposing position with respect to two or more electromagnetic wave introduction windows between the relative movements. Composition. Further, in the plasma processing apparatus of the present invention, the plurality of electromagnetic wave introduction windows are temporally accumulated 电 and/or plasma irradiation of the plasma density of the plasma generated by the electromagnetic waves introduced from the respective electromagnetic wave introduction windows. The accumulation of time is configured in the same way regardless of the position of a processed object. Further, the plasma processing apparatus of the present invention may further include an auxiliary electromagnetic wave introducing unit that has an electromagnetic wave introducing window provided at a position deviated from the opposing position with respect to the track of the object to be moved relatively. Further, the plasma processing apparatus of the present invention may further include a plurality of electromagnetic wave introducing units having different areas of the electromagnetic wave introducing windows. Further, in the plasma processing apparatus of the present invention, the electromagnetic wave generating device may be provided separately in accordance with the electromagnetic wave introducing unit. Further, in the plasma processing apparatus of the present invention, the power of the electromagnetic waves supplied to the plurality of electromagnetic wave introducing units can be individually set. Further, in the plasma processing apparatus of the present invention, the electromagnetic wave power introduced from the electromagnetic wave introduction window located inside the position close to the rotation center and the electromagnetic wave introduction from the outer side of the outer radius of the electromagnetic wave introduction window on the inner side are introduced. The power of the electromagnetic waves introduced by the windows is different. In the plasma processing method of the present invention, the plasma processing apparatus is used to introduce electromagnetic waves into the processing container through the plurality of electromagnetic wave introduction windows to generate plasma, and the processed object is at least 201215250 in the processing container. The temporal accumulation of the plasma density at the position on the object to be processed while the object to be processed is relatively moved to the electromagnetic wave introduction window by the opposite direction of the electromagnetic wave transmission region of the electromagnetic wave introduction window And/or the cumulative enthalpy of the plasma irradiation time is formed in the same manner for plasma treatment, the plasma processing apparatus comprising: a vacuumable processing container that forms a processing space for processing the object to be processed; The electromagnetic wave generating device is configured to generate electromagnetic waves for generating plasma in the processing container, and a plurality of electromagnetic wave introducing units to be generated in the electromagnetic wave generating device. Electromagnetic waves are introduced into the processing container; and the drive device is The center of the support device serves as a center of rotation, and a plurality of objects to be processed supported by the support device and/or the plurality of electromagnetic wave introduction units are rotated to cause a wraparound motion. The electromagnetic wave introduction unit has an electromagnetic wave introduction window, and the electromagnetic wave is introduced. The window system is provided to face the processing space, and electromagnetic waves are transmitted and introduced into the processing container. The supporting device has a mounting table on which a plurality of objects to be processed are placed. According to the present invention, the object to be processed placed on the supporting device is relatively movable so as to pass through at least the opposing position of the electromagnetic wave transmitting region of the electromagnetic wave introducing window. Moreover, regardless of the position on the object to be processed, the temporal accumulation of the plasma density and/or the fatigue of the plasma irradiation time

S -10- 201215250 計値皆形成相同的方式配置電磁波導入窗,藉 理體的面內之處理的均一性提升。並且,即使 線,或變更製程條件,還是可獨立控制處理容 分布。因此,可在處理容器內以所望的分布來 電漿。又,即使對應於被處理體的大型化來使 型化時,還使可藉由使複數的電磁波導入單元 磁波導入窗的面積、供給的電磁波的功率等變 地調節在處理容器內所生成的電漿分布。 【實施方式】 以下,參照圖面來詳細說明有關本發明之 。圖1是模式性地顯示本發明的實施形態的電 100的構成例的剖面圖。圖2A,2B是表示作 漿處理裝置100的支撐裝置的載置台的外觀的 3是電漿處理裝置100的微波導入單元的槪略 4A,4B,4C是表示使用於圖1的電漿處理裝: 面天線的平面圖。圖5是表示圖1的電漿處理 頂壁lc的下面的底面圖。 電漿處理裝置100的主要構成是具備: 處理容器1,其係構成氣密; 支撐搬送裝置2,其係於處理容器1內支 理體的半導體晶圓(以下簡稱「晶圓」)W; 氣體導入部15,其係導入氣體至處理容器 排氣裝置24,其係用以將處理容器1內 此可使被處 更換平面天 器內的電漿 安定地維持 處理容器大 的配置或電 化,來簡單 一實施形態 漿處理裝置 爲使用於電 立體圖。圖 構成圖。圖 置1 00的平 裝置100的 撐作爲被處 1內; 予以減壓排 -11 - 201215250 氣; 複數的微波導入單元27,其係設於處理容器1的上 部,將用以使產生電漿的微波導入至處理容器1內; 導波管37,其係一端被連接至微波導入單元27; 微波產生裝置39,其係被連接至此導波管的另一端 ,使微波產生;及 控制部50,其係作爲控制該等電漿處理裝置1 00的 各構成部的控制手段。 另外,藉由微波導入單元27、導波管37、及微波產 生裝置39來構成使處理氣體的電漿產生於處理容器1內 的電漿產生手段。 處理容器1是具有由鋁等的材質所構成的底壁la、 側壁1 b及頂壁1 c。 支撐裝置2是具有載置台3、支撐部4及驅動裝置5 。載置台3是在處理容器1的內部水平支撐複數片的晶圓 W。載置台3是藉由熱傳導性高的材質例如A1N等的陶瓷 材所構成。此載置台3是藉由從處理容器1的底壁la的 中央延伸至上方的圓筒狀的支撐部4所支撐。 又’載置台3是例如圖2A所示具有複數處(在圖2A 是5處)載置晶圓W的載置區域Sr。 又’載置台3.是藉由被連結至支撐部4的驅動裝置5 ’以支撐部4作爲轉軸(中心),構成可旋轉。在本實施 形態中’複數的載置區域SR是以載置台3的轉軸爲中心 配置成同心圓狀。因此,藉由載置台3旋轉,5個的載置S -10- 201215250 The electromagnetic wave introduction window is configured in the same way, and the uniformity of processing in the in-plane of the borrowing body is improved. Moreover, even if the line, or changing the process conditions, the processing capacity can be independently controlled. Therefore, the plasma can be distributed in the treatment vessel in a desired distribution. In addition, even when the shape of the object to be processed is increased, the area of the magnetic wave introduction window of the plurality of electromagnetic wave introduction means, the power of the supplied electromagnetic wave, and the like can be adjusted in the processing container. Plasma distribution. [Embodiment] Hereinafter, the present invention will be described in detail with reference to the drawings. Fig. 1 is a cross-sectional view schematically showing a configuration example of an electric device 100 according to an embodiment of the present invention. 2A and 2B are views showing the appearance of the mounting table of the supporting device of the slurry processing apparatus 100. 3 is a schematic diagram of the microwave introducing unit of the plasma processing apparatus 100, 4A, 4B, and 4C showing the plasma processing apparatus used in Fig. 1. : Plan view of the antenna. Fig. 5 is a bottom plan view showing the lower surface of the plasma treatment top wall 1c of Fig. 1. The main structure of the plasma processing apparatus 100 includes: a processing container 1 which is airtight; and a supporting transport apparatus 2 which is a semiconductor wafer (hereinafter referred to as "wafer") W of the processing body in the processing container 1; The gas introduction unit 15 introduces a gas into the processing container exhausting device 24 for maintaining the large arrangement or electrification of the processing container in the processing container 1 so that the plasma in the replaced planar device can be stably maintained. A simple embodiment of the slurry processing apparatus is used for an electro-optical image. Figure Composition diagram. The support of the flat device 100 of FIG. 1 is taken as the location 1; the decompression row -11 - 201215250 gas is applied; the plurality of microwave introduction units 27 are provided at the upper portion of the processing container 1 and are used to generate plasma. The microwave is introduced into the processing container 1; the waveguide 37 is connected to the microwave introducing unit 27 at one end; the microwave generating device 39 is connected to the other end of the waveguide to generate microwaves; and the control unit 50 It is used as a control means for controlling each component of the plasma processing apparatus 100. Further, the microwave introducing unit 27, the waveguide 37, and the microwave generating device 39 constitute a plasma generating means for generating plasma of the processing gas in the processing container 1. The processing container 1 is a bottom wall 1a, a side wall 1b, and a top wall 1c which are made of a material such as aluminum. The support device 2 has a mounting table 3, a support portion 4, and a drive device 5. The stage 3 is a wafer W horizontally supporting a plurality of sheets inside the processing container 1. The mounting table 3 is made of a material having a high thermal conductivity such as a ceramic material such as A1N. This mounting table 3 is supported by a cylindrical support portion 4 that extends from the center of the bottom wall 1a of the processing container 1 to the upper side. Further, the mounting table 3 is, for example, a mounting region Sr in which a plurality of places (5 in Fig. 2A) are placed on the wafer W as shown in Fig. 2A. Further, the mounting table 3 is configured to be rotatable by the driving device 5' coupled to the support portion 4 with the support portion 4 as a rotation axis (center). In the present embodiment, the plurality of mounting regions SR are arranged concentrically around the rotation axis of the mounting table 3. Therefore, by the rotation of the mounting table 3, five placements

S -12- 201215250 區域SR是在以支撐部4的轉軸爲中心的同一圓周上進行 環繞運動(公轉)。 另外’載置台3不必是單體,亦可按照載置的晶圓W 的片數來分割成複數。例如圖2B是表示在藉由驅動裝置 5來構成可旋轉的共通台部6設置藉由5個支撐部7所支 撐的5個台座8之載置台的變形例。5個的支撐部7及台 座8是在以台部6的轉軸爲中心的同一圓周上環繞運動( 公轉)。就此構成例而言,支撐裝置的構成是包含台部6 、支撐部7、台座8及驅動裝置5。 又,載置台3具備未圖示的加熱或冷卻機構,可將晶 圓W的溫度控制在例如2 5 °C (室溫)〜9 0 0 °C的範圍。 並且,在載置台3設有用以支撐晶圓W來使昇降的 晶圓支撐銷(未圖示)。各晶圓支撐銷是設成可對載置台 3的表面突没。 在處理容器1的頂壁lc的中央設有氣體導入部15。 氣體導入部15是具有圓筒形的噴嘴16,在其下面形成有 氣孔16a。此氣體導入部15是被連接至配管17。 氣體供給裝置18的構成是包含氣體供給源18a、及 被連接至此氣體供給源18a的配管17。在圖1是圖示一 個的氣體供給源1 8 a及配管1 7,但可按照氣體種類來設 置複數的氣體供給源18a及配管17。氣體供給源18a是 例如供給電漿生成用的Ar、Kr、Xe、He等的稀有氣體、 或氧化處理的氧氣體等的氧化性氣體、氮化處理的氮化氣 體等的處理氣體。並且,在CVD處理時,亦可構成供給 -13- 201215250 成膜原料氣體、使用於置換處理容器內環境時的N2、Ar 等的淨化氣體、使用於洗滌處理容器1內時的C1F3、NF3 等的洗滌氣體。在連接氣體供給源18a乃至氣體導入部 15的配管17的途中具備未圖示的質量流控制器及開閉閥 ,可進行所被供給之氣體的切換或流量等的控制。另外, 氣體供給裝置18可爲電漿處理裝置1〇〇的構成一部分, 或者外置的裝置。 並且,在處理容器1的側壁lb設有用以在電漿處理 裝置1〇〇與隣接的搬送室(未圖示)之間進行晶圓W的 搬出入的搬出入口 19、及開閉此搬出入口 19的閘閥20。 在處理容器1的底壁la複數處(在圖1是2處)形 成有排氣口 1 1。在此排氣口 Π連接排氣管1 2,經由此排 氣管12來連接至排氣裝置24»圖1是在底壁la設置2 處的排氣口 1 1,分別連接排氣裝置24。 排氣裝置24是例如具備APC閥、及作爲高速真空泵 的渦輪分子泵。如上述般,排氣裝置24是經由排氣管12 來連接至排氣口 11。藉由使排氣裝置24作動,處理容器 1內的氣體會經由排氣口 11及排氣管12來往外部排氣。 藉此,可將處理容器1內高速地減壓至例如〇.133Pa。 其次,一邊參照圖3〜圖5 —邊說明有關對處理容器 1內導入微波的機構。電漿處理裝置100是使在複數的微 波產生裝置39所產生的微波分別經由微波導入單元27來 供給至處理容器1內的構成。微波產生裝置39與微波導 入單元27之間是分別藉由導波管37來連接。S -12- 201215250 The area SR is a wraparound motion (revolution) on the same circumference centered on the rotation axis of the support portion 4. Further, the mounting table 3 does not have to be a single body, and may be divided into a plurality of pieces according to the number of wafers W placed thereon. For example, Fig. 2B shows a modification of the mounting table in which five pedestals 8 supported by the five support portions 7 are provided by the drive unit 5 to form the rotatable common table portion 6. The five support portions 7 and the pedestal 8 are circumferentially moved (revolved) on the same circumference centered on the rotation axis of the table portion 6. In this configuration example, the configuration of the support device includes the table portion 6, the support portion 7, the pedestal 8, and the drive device 5. Further, the mounting table 3 is provided with a heating or cooling mechanism (not shown), and the temperature of the crystal W can be controlled to, for example, a range of 25 ° C (room temperature) to 900 ° C. Further, the mounting table 3 is provided with a wafer supporting pin (not shown) for supporting the wafer W to be lifted and lowered. Each of the wafer support pins is provided so as to protrude from the surface of the mounting table 3. A gas introduction portion 15 is provided at the center of the top wall lc of the processing container 1. The gas introduction portion 15 is a nozzle 16 having a cylindrical shape, and a gas hole 16a is formed on the lower surface thereof. This gas introduction portion 15 is connected to the pipe 17. The gas supply device 18 is configured to include a gas supply source 18a and a pipe 17 connected to the gas supply source 18a. In Fig. 1, a gas supply source 18a and a pipe 17 are shown, but a plurality of gas supply sources 18a and pipes 17 can be provided in accordance with the type of gas. The gas supply source 18a is, for example, a processing gas such as a rare gas such as Ar, Kr, Xe, or He for plasma generation, an oxidizing gas such as an oxidized oxygen gas, or a nitriding gas. In addition, in the CVD process, it is possible to form a raw material gas for supplying -13 to 201215250, a purge gas such as N2 and Ar for use in the environment of the replacement processing container, and C1F3, NF3, etc. when used in the washing processing container 1. Washing gas. The mass flow controller (not shown) and the on-off valve are provided in the middle of the piping 17 that connects the gas supply source 18a to the gas introduction unit 15, and the switching of the supplied gas or the flow rate and the like can be controlled. Further, the gas supply device 18 may be a part of the composition of the plasma processing apparatus 1 or an external device. Further, the side wall 1b of the processing container 1 is provided with a carry-out port 19 for carrying in and out of the wafer W between the plasma processing apparatus 1 and an adjacent transfer chamber (not shown), and opening and closing the carry-out port 19 Gate valve 20. At the plurality of bottom walls la of the processing container 1 (2 in Fig. 1), an exhaust port 11 is formed. Here, the exhaust port Π is connected to the exhaust pipe 12, and is connected to the exhaust device 24 via the exhaust pipe 12. FIG. 1 is an exhaust port 1 at the bottom wall 1a, and is connected to the exhaust device 24, respectively. . The exhaust device 24 is, for example, an APC valve and a turbo molecular pump as a high-speed vacuum pump. As described above, the exhaust device 24 is connected to the exhaust port 11 via the exhaust pipe 12. By operating the exhaust unit 24, the gas in the processing container 1 is exhausted to the outside through the exhaust port 11 and the exhaust pipe 12. Thereby, the inside of the processing container 1 can be decompressed at a high speed to, for example, 〇.133Pa. Next, a mechanism for introducing microwaves into the processing container 1 will be described with reference to Figs. 3 to 5 . The plasma processing apparatus 100 is configured such that microwaves generated by the plurality of microwave generating devices 39 are supplied to the processing chamber 1 via the microwave introducing unit 27, respectively. The microwave generating device 39 and the microwave introducing unit 27 are connected by a waveguide 37, respectively.

S -14- 201215250 首先,說明有關作爲電磁波導入單元的微波導入單元 27。微波導入單元27的主要構成是具備透過板28、平面 天線3 1。 作爲使微波透過的電磁波導入窗之透過板28是配備 於支撐部13a上,該支撐部13a是被形成於頂壁lc。在 透過板28中,面向支撐部13a之間的處理容器1內的部 分會形成作爲電磁波透過區域的微波透過區域。透過板 28是由介電質例如石英或Al2〇3、A1N等的陶瓷所構成》 此透過板28與支撐部13a之間是經由密封構件29來氣密 地密封。因此,各透過板2 8是分別堵住頂壁1 c的開口, 保持處理容器1內的氣密性。 平面天線31是在透過板28的上方,設成與載置台3 的載置區域SR對向。平面天線31是呈圓板狀。另外,平 面天線31的形狀並非限於圓板狀,例如亦可爲四角板狀 。平面天線3 1是由例如表面被鍍金或銀的銅板或鋁板所 構成。平面天線31是具有放射微波的複數個縫隙狀的微 波放射孔32。微波放射孔32是以預定的圖案來貫通平面 天線3 1而形成。 各個的微波放射孔32是例如圖4A所示,呈細長的 長方形狀(縫隙狀)。另外,微波放射孔32的形狀亦可 爲圓形狀、圓弧狀等其他的形狀。而且,微波放射孔32 的配置形態並無特別加以限定,例如圖4B那樣,彎曲的 細長的複數個微波放射孔32全體配置成圓形,或圖4C那 樣細長的微波放射孔3 2亦可配置成從平面天線3 1的中心 -15- 201215250 放射狀地延伸。 在平面天線31之上連接導波管37的下端。在導波管 37的另一端側是經由匹配電路38來連接產生微波的微波 產生裝置39。 作爲電磁波產生裝置的微波產生裝置39是使預定頻 率的微波產生。微波的頻率是例如2.45GHz爲理想,其他 亦可使用800MHz〜1GHz (較理想是800MHz〜915MHz) 、8.35GHz、1 .98GHz 等。 導波管37是具有:從平面天線31朝上方延伸的剖面 圓形狀的圆形導波管37a、及經由模式變換器40來連接 至此圓形導波管3 7a的上端部之延伸於水平方向的矩形導 波管37b。模式變換器40是具有將以TE模式來傳播於矩 形導波管3 7b內的微波變換成TM模式的機能。藉由如此 的構造,微波是經由具有內導體(圖示省略)的圓形導波 管37a來往平面天線31傳播。 藉由以上那樣的構成,在微波產生裝置39所產生的 微波可經由導波管37來往微波導入單元27的平面天線 31傳播,且經由透過板28的微波透過區域來導入至處理 容器1內。另外,在本實施形態的電漿處理裝置1〇〇中, 作爲導入微波至處理容器1內的機構,並非限於圖3所示 的構成。例如,亦可適於利用在專利文獻5所揭示的微波 導入機構。 在本實施形態中,微波導入單元27是設置複數個。 圖5是由處理容器1的內部所見的頂壁lc的底面圖。在S -14- 201215250 First, the microwave introducing unit 27 as an electromagnetic wave introducing unit will be described. The main configuration of the microwave introducing unit 27 is to include a transmitting plate 28 and a planar antenna 31. The transmission plate 28, which is an electromagnetic wave introduction window for transmitting microwaves, is provided on the support portion 13a, and the support portion 13a is formed on the top wall lc. In the transmission plate 28, a portion of the processing container 1 facing the support portion 13a forms a microwave transmission region as an electromagnetic wave transmission region. The transmission plate 28 is made of a dielectric material such as quartz, Al2〇3, A1N or the like. The space between the transmission plate 28 and the support portion 13a is hermetically sealed via the sealing member 29. Therefore, each of the transmission plates 28 is an opening that blocks the top wall 1c, respectively, and maintains the airtightness in the processing container 1. The planar antenna 31 is disposed above the transmission plate 28 so as to face the mounting area SR of the mounting table 3. The planar antenna 31 has a disk shape. Further, the shape of the planar antenna 31 is not limited to a disk shape, and may be, for example, a square plate shape. The planar antenna 31 is composed of, for example, a copper plate or an aluminum plate whose surface is plated with gold or silver. The planar antenna 31 is a plurality of slit-shaped microwave radiation holes 32 having radiated microwaves. The microwave radiation holes 32 are formed by penetrating the planar antenna 31 in a predetermined pattern. Each of the microwave radiation holes 32 has an elongated rectangular shape (slit shape) as shown, for example, in Fig. 4A. Further, the shape of the microwave radiation holes 32 may be other shapes such as a circular shape or an arc shape. Further, the arrangement of the microwave radiation holes 32 is not particularly limited. For example, as shown in FIG. 4B, the curved plurality of elongated microwave radiation holes 32 are arranged in a circular shape, or the elongated microwave radiation holes 32 can be arranged as shown in FIG. 4C. Radially extending from the center -15-201215250 of the planar antenna 3 1 . The lower end of the waveguide 37 is connected above the planar antenna 31. On the other end side of the waveguide 37, a microwave generating device 39 that generates microwaves is connected via a matching circuit 38. The microwave generating device 39 as the electromagnetic wave generating means generates microwaves of a predetermined frequency. The frequency of the microwave is ideal, for example, 2.45 GHz, and other frequencies of 800 MHz to 1 GHz (more preferably 800 MHz to 915 MHz), 8.35 GHz, and 1.98 GHz may be used. The waveguide 37 is a circular waveguide 37a having a circular cross section extending upward from the planar antenna 31, and an upper end portion connected to the upper end portion of the circular waveguide 37a via the mode converter 40 extending in the horizontal direction Rectangular waveguide 37b. The mode converter 40 has a function of converting microwaves propagating in the rectangular waveguide 37b in the TE mode into the TM mode. With such a configuration, the microwave propagates through the planar waveguide 31 via the circular waveguide 37a having an inner conductor (not shown). With the above configuration, the microwave generated by the microwave generating device 39 can be transmitted to the planar antenna 31 of the microwave introducing unit 27 via the waveguide 37, and introduced into the processing container 1 via the microwave transmitting region of the transmitting plate 28. Further, in the plasma processing apparatus 1 of the present embodiment, the mechanism for introducing the microwave into the processing container 1 is not limited to the configuration shown in Fig. 3 . For example, it is also possible to use the microwave introduction mechanism disclosed in Patent Document 5. In the present embodiment, a plurality of microwave introduction units 27 are provided. Figure 5 is a bottom plan view of the top wall lc as seen from the inside of the processing container 1. in

S -16- 201215250 圖5中描繪有合計20個的透過板28。亦即,在本 態的電漿處理裝置100是設有合計20個的微波導 27。在圖5所例示的形態中,各微波導入單元27 是相同’透過板28的面積也是相等。以下的說明 透過板28的位置來說明微波導入單元27的配置。 作爲電磁波導入窗的透過板28並非限於圓形,例 爲矩形等的其他形狀。 如圖5所示,以能夠包圍頂壁1 c的中心〇 ( 與載置台3的轉軸的位置相同)之方式同心圓狀地 5個的透過板28,四重地配列於頂壁lc的徑方向 台3的徑方向)。首先,最內周的第1周是藉由 28A1、28B1、28C1、28D1、28E1 的 5 個所構成。 從內側算起第2周是藉由透過板2 8A2、2 8B2、 2 8D2、2 8E2的5個所構成。同樣,從內側算起第 藉由透過板 28A3、 28B3、 28C3、 28D3、 28E3 的 5 成。然後,最外周的第4周是藉由透過板2 8A4、 28C4、28D4、28E4的5個所構成。在此,透過板 2 8A4是以對1片的晶圓W進行電漿處理的觀點萍 群組,同樣,透過板28B1〜28B4、透過板28C1〜 透過板28D1〜28D4、透過板28E1〜28E4亦分別 組。有關此點更一邊參照圖6 —邊進行說明。 圖6是在載置台3的平面圖投影顯示與圖5同 28的配置。如上述般,在載置台3設有5處載置 的載置區域SR。載置台3是藉由使驅動裝置5驅 實施形 入單元 的構成 是根據 另外, 如亦可 在此是 配列有 (載置 透過板 其次, 28C2 ' 3周是 個所構 28B4、 28 A1 〜 :構成1 28C4、 構成群 透過板 晶圓W 動,在 -17- 201215250 圖6中的箭號所示的方向旋轉(自轉),因此各載置區域 SR是以載置台3的轉軸爲中心’在同方向環繞(公轉) 。在此,若例如針對透過板28A1〜28A4的群組來想,則 從最內側的透過板28A1到最外側的透過板28A4是對於 載置區域SR的環繞方向依序排列配置成弧狀。而且,透 過板28A1〜28A4是分別在各載置區域SR移動的期間, 配置成至少其一部分無論對於哪個載置區域SR皆上下互 相重疊。亦即,被載置於載置區域SR的晶圆W是對透過 板28A1〜28A4相對移動,構成可通過透過板28A1〜 2 8A4之中的至少一個微波透過區域的對向位置。在本實 施形態中,晶圓W是對透過板28A1〜28A4相對移動,構 成可通過透過板28A1〜28A4的微波透過區域的所有對向 位置。在此,所謂「對向位置」是意指使透過板28A1〜 2 8 A4的微波透過區域的面積朝向載置台3,原封不動垂 直投影時,該投影區域與載置區域SR (或在此被載置的 晶圓W )是至少部分地重疊。並且,透過板28A1〜28A4 是配置成無論在晶圓W上的哪個位置,電漿密度的時間 性累計値及/或電漿照射時間的累計値皆會形成相同。藉 由如此的配置,透過板28A1〜28A4是錯開時間依序一部 分或全體與載置區域SR上下重疊而去。同樣,透過板 28B1〜28B4、透過板 28C1〜28C4、透過板 28D1〜28D4 、透過板28E1〜28E4的各群組也是分別配置成弧狀,錯 開時間依序配置成一部分或全體會與載置區域SR上下重 疊而去。S-16-201215250 A total of 20 transmissive plates 28 are depicted in FIG. That is, in the plasma processing apparatus 100 of the present state, a total of 20 microwave guides 27 are provided. In the embodiment illustrated in Fig. 5, each of the microwave introduction units 27 is the same. The area of the transmission plate 28 is also equal. The following description explains the arrangement of the microwave introduction unit 27 by the position of the board 28. The transmission plate 28 as the electromagnetic wave introduction window is not limited to a circular shape, and is formed into other shapes such as a rectangle. As shown in Fig. 5, five transmissive plates 28 concentrically arranged so as to surround the center 〇 of the top wall 1 c (the same position as the rotational axis of the mounting table 3) are arranged in a quadruple direction in the radial direction of the top wall lc. The diameter direction of the table 3). First, the first week of the innermost circumference is composed of five of 28A1, 28B1, 28C1, 28D1, and 28E1. The second week from the inside is constituted by five of the transparent plates 2 8A2 , 2 8B2 , 2 8D2 , and 2 8E2 . Similarly, from the inside, it is passed through the transmission plates 28A3, 28B3, 28C3, 28D3, and 28E3. Then, the fourth week of the outermost circumference is constituted by five of the transmission plates 28A4, 28C4, 28D4, and 28E4. Here, the transmission plate 28A4 is a group of plasmas for processing one wafer W. Similarly, the transmission plates 28B1 to 28B4, the transmission plates 28C1 to 28B1 to 28D4, and the transmission plates 28E1 to 28E4 are also used. Grouped separately. This point will be further described with reference to FIG. Fig. 6 is a plan view showing the plan view of the mounting table 3 in the same manner as Fig. 5. As described above, the mounting table 3 is provided with the mounting area SR placed at five places. The mounting table 3 is configured such that the drive unit 5 is driven into the unit. Alternatively, it may be arranged here (the transmission plate is placed next, and 28C2' is a structure 28B4, 28 A1 〜: 1 28C4, the constituent group is rotated by the plate wafer W, and is rotated (rotated) in the direction indicated by the arrow in Fig. 6 in -17-201215250. Therefore, each of the mounting areas SR is centered on the rotating shaft of the mounting table 3 The direction is around (revolution). Here, for example, the group of the transmissive plates 28A1 to 28A4 is arranged in order from the innermost transmissive plate 28A1 to the outermost transmissive plate 28A4 in the circumferential direction of the placement area SR. In addition, the transmissive plates 28A1 to 28A4 are arranged such that at least some of the transmissive plates 28A1 to 28A4 are vertically overlapped with each other regardless of which of the mounting regions SR. The wafer W of the region SR is relatively moved to the transmissive plates 28A1 to 28A4, and constitutes an opposite position through at least one of the transmissive plates 28A1 to 28A4. In the present embodiment, the wafer W is transmissive. Board 28A1~28A4 The movement is configured to pass through all of the opposing positions of the microwave transmission regions of the transmission plates 28A1 to 28A4. Here, the "opposing position" means that the area of the microwave transmission region of the transmission plates 28A1 to 2 8 A4 is directed toward the mounting table 3. When the vertical projection is not performed, the projection area is at least partially overlapped with the placement area SR (or the wafer W placed thereon), and the transmission plates 28A1 to 28A4 are disposed on the wafer W. At which position, the cumulative time 电 of the plasma density and/or the cumulative 値 of the plasma irradiation time will be the same. With such a configuration, the transmission plates 28A1 to 28A4 are sequentially shifted in part or in whole and the mounting area SR Similarly, the respective groups of the transmission plates 28B1 to 28B4, the transmission plates 28C1 to 28C4, the transmission plates 28D1 to 28D4, and the transmission plates 28E1 to 28E4 are also arranged in an arc shape, and the staggered time is sequentially arranged in part or all. The experience overlaps with the placement area SR.

S -18- 201215250 藉由如此配置複數的透過板28,使載置台3預定次 數旋轉後的晶圓W的各部位之電漿照射的時間性累計値 形成相同,可在複數的晶圓W間及晶圓W的面內大致均 等地電漿處理。亦即,藉由從透過板28的微波透過區域 所放射的微波來生成作用於晶圓W的電漿的照射時間是 在晶圓W,表面的哪個部位皆形成時間平均大致相等的結 果。 另外,在處理容器1內,因爲在透過板28的微波透 過區域的正下方所生成的電漿會擴散而去,所以到達晶圓 W表面的電漿是具有比透過板28的微波透過區域的面積 更大的面積(水平剖面積)。此電漿擴散區域的面積也會 依照從透過板2 8到晶圓W表面的距離(間隙LG )而有所 不同。可考慮如此的電漿擴散來決定透過板28的配置。 並且,可理解使透過板28環繞,而取代使載置台3旋轉 來使環繞載置區域SR,也是同樣可行。亦即,只要使微 波導入單元27與載置區域SR相對移動於逆向的方向即可 ,哪一方移動皆可,或亦可使雙方移動。 電漿處理裝置1〇〇的各構成部是形成被連接至控制部 1 5 0來控制的構成。控制部5 0是電腦,例如圖7所示, 具備:具有CPU的控制器51、及被連接至此控制器51的 使用者介面5 2及記憶部5 3。控制器5 1是在電漿處理裝 置1 〇〇中統括控制例如氣體流量、壓力、微波輸出等製程 條件相關的各構成部(例如驅動部5、氣體供給裝置1 8、 排氣裝置24、微波產生裝置39等)之控制手段。 -19- 201215250 使用者介面52具有:工程管理者爲了管理電漿 裝置100而進行指令的輸入操作等的鍵盤、及使電漿 裝置100的運轉狀況可視化顯示的顯示器等。並且, 憶部53中保存有記錄控制程式(軟體)或處理條件 等的處方,該控制程式(軟體)是用以在製程控制君 的控制下實現被執行於電漿處理裝置1〇〇的各種處理 然後,因應所需,以來自使用者介面52的指示 從記憶部53叫出任意的處方,使執行於製程控制器 在製程控制器51的控制下,於電漿處理裝置100的 容器1內進行所望的處理。並且,上述控制程式及處 件資料等的處方可利用被儲存於電腦可讀取的記憶 54的狀態者,或從其他的裝置例如經由專線來使隨 送上線利用。電腦可讀取的記憶媒體5 4例如可舉 ROM、硬碟、SSD、軟碟、快閃記憶體、DVD、藍光 等。 其次,說明有關利用本實施形態的電漿處理裝置 的電漿處理的程序之一例。在此是舉使用含氮的氣體 處理氣體,將晶圓表面予以電漿氮化處理時爲例。首 例如從使用者介面52輸入指令,而使能夠在電漿處 置100進行電漿氮化處理。控制器51會接受此指令 出被保存於記憶部53或記錄媒體54的處方。然後, 夠在根據處方的條件下實行電漿氮化處理的方式,從 器51往電漿處理裝置1〇〇的各終端裝置例如驅動裝 、氣體供給裝置18、排氣裝置24、微波產生裝置39 處理 處理 在記 資料 § 51 者。 等, 51, 處理 理條 媒體 時傳 CD- 光碟 100 作爲 先, 理裝 ,讀 以能 控制 置5 等送S -18-201215250 By arranging the plurality of transmissive plates 28 in this manner, the time-accumulation of the plasma irradiation of each portion of the wafer W after the predetermined number of rotations of the mounting table 3 is formed in the same manner, and can be formed between the plurality of wafers W And plasma treatment is performed substantially uniformly in the plane of the wafer W. That is, the irradiation time for generating the plasma acting on the wafer W from the microwaves radiated from the microwave transmitting region of the transmitting plate 28 is the result of forming the time average of the wafer W at which portion of the surface is substantially equal. Further, in the processing container 1, since the plasma generated directly under the microwave transmitting region of the transmitting plate 28 is diffused, the plasma reaching the surface of the wafer W has a microwave transmitting region larger than the transmitting plate 28. Larger area (horizontal sectional area). The area of the plasma diffusion region also varies depending on the distance from the surface of the transmission plate 28 to the surface of the wafer W (gap LG). Such a plasma diffusion can be considered to determine the configuration of the transmission plate 28. Further, it is understood that it is equally feasible to surround the transmissive plate 28 instead of rotating the mounting table 3 so as to surround the mounting area SR. In other words, as long as the microwave introducing unit 27 and the mounting region SR are relatively moved in the reverse direction, either one can be moved or both can be moved. Each component of the plasma processing apparatus 1 is configured to be connected to the control unit 150. The control unit 50 is a computer. For example, as shown in Fig. 7, the control unit 50 includes a controller 51 having a CPU, a user interface 52 connected to the controller 51, and a memory unit 53. The controller 51 is configured to control various components (for example, the drive unit 5, the gas supply unit 18, the exhaust unit 24, and the microwave) in the plasma processing apparatus 1 to control process conditions such as gas flow rate, pressure, and microwave output. Control means for generating device 39, etc.). -19-201215250 The user interface 52 has a keyboard for inputting an instruction or the like for the management of the plasma device 100, and a display for visually displaying the operation state of the plasma device 100. Further, the memorandum portion 53 holds a prescription for recording a control program (software), a processing condition, and the like, and the control program (software) is for realizing various types of plasma processing apparatus 1 to be executed under the control of the process control. Processing, and then, according to the instruction from the user interface 52, an arbitrary prescription is called from the memory unit 53, so that the process controller is executed in the container 1 of the plasma processing apparatus 100 under the control of the process controller 51. Perform the desired processing. Further, the prescriptions of the control program, the device data, and the like can be used in the state of the memory 54 readable by the computer, or can be used by other devices, for example, via a dedicated line. The computer readable memory medium 5 4 can be, for example, a ROM, a hard disk, an SSD, a floppy disk, a flash memory, a DVD, a Blu-ray, or the like. Next, an example of a procedure for plasma treatment using the plasma processing apparatus of the present embodiment will be described. Here, an example is given in which a gas containing a nitrogen-containing gas is used to treat the surface of the wafer by plasma nitriding. For example, the command is input from the user interface 52, and the plasma nitriding process can be performed at the plasma place 100. The controller 51 accepts this command to issue a prescription stored in the storage unit 53 or the recording medium 54. Then, in a manner of performing plasma nitriding treatment under the conditions of the prescription, each of the terminal devices from the device 51 to the plasma processing apparatus 1 such as a driving device, a gas supply device 18, an exhaust device 24, and a microwave generating device 39 Processing is in the record § 51. Etc., 51, processing the management of the media, when the CD-CD 100 is used as the first, the dressing, reading to control, etc.

S -20- 201215250 出控制訊號。 然後,打開閘閥20,從搬出入口 1 9依序搬入例如複 數片的晶圓W至處理容器1內,載置於載置台3的載置 區域SR上。其次,使驅動裝置5驅動,令載置台3旋轉 ,使安定化至形成一定的旋轉速度爲止》 其次,一邊使排氣裝置24作動來將處理容器1內減 壓排氣,一邊從氣體供給裝置18使稀有氣體及含氮氣體 分別以預定的流量經由氣體導入部15來導入至處理容器 1內。而且,調整排氣量及氣體供給量來將處理容器1內 調節至預定的壓力。 其次,開啓(輸入)各微波產生裝置39的功率,使 產生微波。然後,預定的頻率例如2.45 GHz的微波會從各 微波產生裝置39分別經由匹配電路38來引導至導波管 37,依序通過矩形導波管37b及圓形導波管37a,供給至 平面天線板31。微波是在矩形導波管37b內以TE模式傳 播,此TE模式的微波是在模式變換器40被變換成TM模 式,在圓形導波管3 7a內朝微波導入單元27的平面天線 板31傳播而去。微波是從被貫通形成於平面天線板31的 孔之微波放射孔32經由透過板28來放射至處理容器1內 的晶圓W的上方空間。如此一來,微波會分別從各微波 導入單元27來導入至處理容器1內。 在本實施形態是例如配置20處的微波導入單元27, 利用經由各微波導入單元27來導入處理容器1的微波在 處理容器1內形成電磁場,例如被導入處理容器1內的不 -21 - 201215250 活性氣體及含氮氣體會被電漿化。利用此微波所被 電漿是藉由微波從平面天線板31的微波放射孔32 例如形成l〇1()/cm3〜1013/cm3的高密度,且在晶圓 爲大致2eV以下的低電子溫度之電漿。如此形成的 電漿是往底層膜的離子等所造成的電漿損傷少。然 由電漿中的活性種例如自由基或離子的作用來氮化 的矽表面,而形成矽氮化膜SiN的薄膜。另外,可 氮氣體而使用含氧氣體,藉此進行矽的氧化處理, 藉由使用成膜原料氣體來進行電漿CVD法的成膜。 一旦由控制器51送出使電漿處理終了的控制 則各微波產生裝置39的功率會被關閉(切掉)。 停止來自氣體供給裝置18的處理氣體的供給,將 器內抽真空。然後,使載置台3的旋轉停止,從處 1內依序搬出晶圓W,完成對複數片的晶圓W的同 處理。 圖8A、圖8B是直線性地顯示對圖5及圖6所 波導入單元27的透過板28A1〜28A4逆向地相對 晶圓W的軌跡。圖8A、圖8B中’ L1是表不與晶β 相對移動方向正交的方向(當相對移動方向爲圓軌 與其接線方向正交的方向)之透過板28Α1〜28Α4 者彼此間的間隔(透過板28Α1〜28Α4的微波透過 中心間的距離)。又,Μ是表示從最內側的透過板 的中心到最外側的透過板28Α4的中心的距離’ D 晶圓W的直徑。又,圖中的箭號是被載置於載置iS -20- 201215250 Control signal. Then, the gate valve 20 is opened, and, for example, a plurality of wafers W are sequentially loaded into the processing container 1 from the carry-out port 19, and placed on the mounting area SR of the mounting table 3. Then, the drive unit 5 is driven to rotate the mounting table 3 to stabilize the rotation speed of the mounting unit 3. Next, the exhaust unit 24 is operated to decompress the inside of the processing container 1 while exhausting the gas from the gas supply unit. 18 The rare gas and the nitrogen-containing gas are introduced into the processing container 1 through the gas introduction unit 15 at a predetermined flow rate. Further, the amount of exhaust gas and the amount of gas supplied are adjusted to adjust the inside of the processing container 1 to a predetermined pressure. Next, the power of each of the microwave generating devices 39 is turned on (input) to generate microwaves. Then, microwaves of a predetermined frequency, for example, 2.45 GHz, are guided from the respective microwave generating devices 39 to the waveguide 37 via the matching circuit 38, and sequentially supplied to the planar antenna through the rectangular waveguide 37b and the circular waveguide 37a. Board 31. The microwave is propagated in the TE mode in the rectangular waveguide 37b, and the TE mode microwave is converted into the TM mode in the mode converter 40, and the planar antenna plate 31 of the microwave introduction unit 27 is formed in the circular waveguide 37a. Spread away. The microwave is radiated from the microwave radiation hole 32 penetrating through the hole formed in the planar antenna plate 31 to the space above the wafer W in the processing container 1 via the transmission plate 28. In this manner, microwaves are introduced into the processing container 1 from the respective microwave introduction units 27, respectively. In the present embodiment, for example, the microwave introduction unit 27 is disposed at 20, and an electromagnetic field is formed in the processing container 1 by the microwave introduced into the processing container 1 via each of the microwave introduction units 27, for example, it is introduced into the processing container 1 not - 21 - 201215250 The reactive gas and the nitrogen-containing gas are plasmad. The plasma to be used by the microwave is formed by microwaves from the microwave radiation holes 32 of the planar antenna plate 31, for example, to a high density of l〇1 ()/cm3 to 1013/cm3, and a low electron temperature of approximately 2 eV or less on the wafer. Plasma. The plasma thus formed is less damaged by plasma caused by ions or the like of the underlying film. However, the surface of the tantalum nitride is formed by the action of an active species such as a radical or an ion in the plasma to form a thin film of the tantalum nitride film SiN. Further, an oxygen-containing gas can be used as the nitrogen gas to carry out oxidation treatment of the ruthenium, and film formation by a plasma CVD method can be carried out by using a film-forming material gas. Once the control for discharging the plasma treatment is sent by the controller 51, the power of each microwave generating device 39 is turned off (cut off). The supply of the process gas from the gas supply device 18 is stopped, and the inside of the device is evacuated. Then, the rotation of the mounting table 3 is stopped, and the wafer W is sequentially carried out from the inside of the space 1, and the same processing of the wafer W of the plurality of sheets is completed. Figs. 8A and 8B are linearly showing the trajectories of the transmissive plates 28A1 to 28A4 of the wave introducing unit 27 of Figs. 5 and 6 in the opposite direction to the wafer W. In Figs. 8A and 8B, 'L1 is the interval between the transmissive plates 28Α1 to 28Α4 in the direction orthogonal to the direction in which the crystal β is relatively orthogonal (the direction in which the relative movement direction is the direction in which the circular rail is orthogonal to the wiring direction). The distance between the centers of the microwaves of the plates 28Α1 to 28Α4). Further, Μ indicates the distance D from the center of the innermost transmissive plate to the center of the outermost transmissive plate 28Α4 D The diameter of the wafer W. Also, the arrow in the figure is placed on the mount i

激發的 放射, W附近 高密度 後、藉 晶圓w 取代含 且亦可 信號, 其次, 處理容 理容器 時電漿 示的微 移動的 面W的 道時, 的鄰接 區域的 :28A1 是表示 [域SRThe excited radiation, after the high density near W, is replaced by the wafer w and can also be signaled. Secondly, when the processing container is treated with the micro-moving surface W of the plasma, the adjacent region: 28A1 is expressed as [ Domain SR

S -22- 201215250 的定位置的晶圓W對透過板28A1〜28A4的移動方向,考 慮透過板28A1〜28A4的弧狀配置來直線性地顯示圖6所 示的環繞方向者。 首先,最內側的透過板28A1的中心與最外側的透過 板28A4的微波透過區域的中心位置,爲了避免在晶圓W 的端部位置P 1、P 3的電漿密度的時間性累計値相較於其 他的部位(例如晶圓W的中央位置P2 )降低,較理想是 使Μ與晶圓W的直徑D相同或更廣。亦即,M2D的關 係成立爲理想。在圖8Α是大致M = D,在圖88是M>D, 透過板28ΑΊ〜28A4的配置是圖8B較理想。並且,藉由 充分地取透過板28A1〜28 A4的相對移動方向(圓軌道時 是圓周方向)的配置間隔,可使晶圓W依序通過透過板 28A1〜28 A4的微波透過區域的對向位置。相反的,藉由 縮小透過板28 A1〜28 A4的相對移動方向的配置間隔,亦 可使透過板28A1〜28 A4的其中2個以上的透過板的微波 透過區域與晶圓W在相對移動中同時上下互相重疊。 並且,與依序相鄰配置於相對移動方向的透過板 28A1〜28A4的相對移動方向正交的方向(相對移動方向 爲圓軌道時,與其接線方向正交的方向)的間隔是設 定成在鄰接的透過板間不會有電漿密度的時間性累計値的 降低之情形。亦即,若間隔L i過小或過大,則即使考慮 了電漿的擴散,也會有電漿密度產生大的山部及小的谷部 ,在晶圓W的面內之處理的均一性降低的情況。相反的 ,在圖8A中,P1是只通過透過板28A1的微波透過區域 -23- 201215250 的正下方,P3是只通過透過板28A4的微波透過區域的正 下方,相對的,P2是通過透過板28A2及透過板28 A3的 雙方的微波透過區域的正下方,因此P2是電漿照射時間 要比PI、P3更多。當透過板28A1〜28A4的電漿密度爲 均一時,P2是例如在氮化處理中,氮摻雜量或氮化膜厚 會比PI、P3更大。因此,在PI,P2、P3,以電漿密度的 時間性累計値形成相同的方式,調節透過板28A1〜28A4 的大小或間隔L!、從透過板28 A〜28D到晶圓W表面的 最短距離(間隙LG)、各微波導入單元27的微波功率等 。而且,以無論在晶圓W上的哪個位置,電漿照射的時 間累計値皆會形成相同的方式,配置電漿源(透過板), 藉此可進行更均一的處理。 圖9〜圖14是表示與圖8A或圖8B同樣,模擬以預 定的間隔來配置4個透過板28A1〜28A4(直徑109mm) 時的電漿密度的時間性累計値的重疊結果。從各透過板 28A1〜28A4到晶圓W表面的最短距離(間隙LG)是設 爲89mm。晶圓W的直徑D是設爲300mm。圖9〜圖14 的縱軸是表示以通過時間來除以電子密度(電漿密度)的 時間性累計値的平均値,橫軸是表示垂直於晶圓W的移 動方向之方向的距離。並且,在圖9〜圖14的橫軸是重 疊顯示晶圓W的大,小(直徑)。 首先,圖 9 是 1^ = 90111111(1^ = 270111111) ,M<D 時。如 圖9所示,在和晶圓W與透過板的相對移動方向正交的 方向(當相對移動方向爲圓軌道時,意指與其接線方向正In the moving direction of the transmissive plates 28A1 to 28A4, the wafer W of the fixed position of S-22-201215250 is linearly displayed in the circumferential direction shown in Fig. 6 in consideration of the arc arrangement of the transmissive plates 28A1 to 28A4. First, the center of the innermost transmissive plate 28A1 and the center of the microwave transmitting region of the outermost transmissive plate 28A4 are arranged to avoid temporal accumulation of the plasma density at the end positions P 1 and P 3 of the wafer W. The lowering of the other portions (for example, the central position P2 of the wafer W) is preferably the same or wider than the diameter D of the wafer W. That is, the relationship of M2D is established as ideal. In Fig. 8A, it is substantially M = D, and in Fig. 88, M > D, the arrangement of the transmission plates 28A to 28A4 is preferable to Fig. 8B. Further, by sufficiently taking the arrangement intervals of the relative movement directions of the transmission plates 28A1 to 28A4 (the circumferential direction in the case of the circular orbit), the wafer W can be sequentially passed through the direction of the microwave transmission region of the transmission plates 28A1 to 28A4. position. Conversely, by narrowing the arrangement interval of the transmission plates 28 A1 to 28 A4 in the relative movement direction, the microwave transmission regions of the two or more transmission plates of the transmission plates 28A1 to 28 A4 may be relatively moved with the wafer W. At the same time, they overlap each other. Further, the interval between the directions in which the relative movement directions of the transmission plates 28A1 to 28A4 disposed adjacent to each other in the relative movement direction are orthogonal to each other (the direction in which the direction of movement is a circular orbit, the direction orthogonal to the direction of the connection) is set to be adjacent There is no time-dependent reduction in the plasma density between the plates. In other words, if the interval L i is too small or too large, even if the diffusion of the plasma is considered, there is a large mountain portion and a small valley portion in which the plasma density is generated, and the uniformity of the treatment in the plane of the wafer W is lowered. Case. In contrast, in Fig. 8A, P1 passes only directly below the microwave transmission region -23-201215250 of the transmission plate 28A1, and P3 passes directly under the microwave transmission region of the transmission plate 28A4, and P2 passes through the transmission plate. Both the 28A2 and the transparent plate 28A3 are directly under the microwave transmission region. Therefore, P2 has more plasma irradiation time than PI and P3. When the plasma density of the transmission plates 28A1 to 28A4 is uniform, P2 is, for example, in the nitriding treatment, the nitrogen doping amount or the nitride film thickness is larger than PI and P3. Therefore, in PI, P2, and P3, the size or interval L of the transmission plates 28A1 to 28A4 and the minimum of the surface from the transmission plates 28 A to 28D are adjusted in the same manner as the temporal accumulation of the plasma density. The distance (gap LG), the microwave power of each microwave introduction unit 27, and the like. Further, in any position on the wafer W, the cumulative time of plasma irradiation is formed in the same manner, and a plasma source (transmission plate) is disposed, whereby a more uniform process can be performed. In the same manner as in Fig. 8A or Fig. 8B, the result of superimposing the temporal accumulation of the plasma density when the four transmission plates 28A1 to 28A4 (diameter: 109 mm) are arranged at predetermined intervals is simulated. The shortest distance (gap LG) from the respective transmission plates 28A1 to 28A4 to the surface of the wafer W was set to 89 mm. The diameter D of the wafer W is set to 300 mm. The vertical axis of Figs. 9 to 14 is the average 値 indicating the temporal accumulation 値 of the electron density (plasma density) by the passage time, and the horizontal axis is the distance indicating the direction perpendicular to the moving direction of the wafer W. Further, the horizontal axis of Figs. 9 to 14 is a large and small (diameter) in which the wafer W is overlapped and displayed. First, Figure 9 is 1^ = 90111111 (1^ = 270111111), M<D. As shown in Fig. 9, in the direction orthogonal to the relative movement direction of the wafer W and the transmission plate (when the relative movement direction is a circular orbit, it means that the wiring direction is positive

S -24- 201215250 交的方向。以下同樣)之晶圓W的中央部分與端部的電 漿密度的合算値之比較下,中央部分高,端部下降,全體 形成山形。另一方面,圖 10是 Ι^ = 120ιηιη(Μ = 360ιηιη) ,M>D時。如圖1〇所示,與相對移動方向正交的方向之 晶圓W的中央部分與端部的電漿密度的合算値是大致均 等。和圖9的情況同樣,被配置於兩端的透過板28A1, 28A4的電漿密度是在外側下降。但是在偏離晶圓W的寬 度D的部分產生下降,在晶圓W的面內是被保持大致均 一的電漿密度》 圖 11 〜圖 13 是表示在 Li = 120mm(M = 360mm), M>D的設定下,使從透過板28A1〜28A4(亦即各對應的 微波導入單元27)的微波透過區域導入的微波功率變化 的情況。圖1 1是表示將從配置於外側的透過板28A1, 2 8A4導入的微波功率設爲1 000W,且將從配置於內側的 2個透過板28 A2,28 A3導入的微波功率設爲600W的情 況。電漿密度的合算値是在與相對移動方向正交的方向之 晶圓W的中央部分下降,端部較高。圖12是表示將從配 置於外側的透過板28A1,28A4導入的微波功率設爲 1000W,且將從配置於內側的2個透過板28A2,28A3導 入的微波功率設爲1 3 00W的情況。電漿密度的合算値是 在與相對移動方向正交的方向之晶圓W的中央部分變高 ,在端部變低。圖13是表示依透過板28A1 ’ 28A2’ 28A3,28A4的順序,將所導入的微波功率設定於400W、 600W、800W、1000W的情況。電漿密度的合算値是在與 -25- 201215250 相對移動方向正交的方向之晶圓 W的一端側(透過板 28A4側)高,在多端側(透過板28A1側)下降,產生一 方向的傾斜。 圖14是表示在Li = 90mm(M = 270mm) ,M<D的設定 下,使從透過板28A1〜28A4的微波透過區域導入的微波 功率變化的情況。圖14是將從配置於外側的透過板28A1 ,28A4導入的微波功率各設爲較大的l〇〇〇W,將從配置 於內側的2個透過板28A2,28A3導入的微波功率各設爲 較小的700W。但,因爲M<D,所以在與相對移動方向正 交的方向之晶圓W的端部的電漿密度的合算値的下降未 被改善。 由上述模擬結果亦可確認,爲了使到達晶圓W的面 內之電漿的密度均一化,實現處理的均一化,最好M2D 的關係成立。以上的說明是如圖8A及圖8B那樣晶圓W 爲直線運動時,但當晶圓 W爲公轉運動時,由於晶圓W 上的位置P 1與P3的速度不同,離公轉軸遠的側(外側) 的P3要比近的側(內側)的P 1速度快,因此需要例如圖 1 3那樣提高外側的電漿密度,使電漿密度的時間性累計 値形成均一。 如以上般,本實施形態的電漿處理裝置1〇〇是具備載 置晶圓W的複數個載置區域SR,以分別被載置於該複數 個載置區域SR的晶圓W至少通過一個微波導入單元27 的透過板28的微波透過區域的對向位置之方式形成可相 對移動。然後,以無論在晶II W上的哪個位置,電漿密S -24- 201215250 The direction of the handover. In the comparison between the central portion of the wafer W and the plasma density at the end portion, the central portion is high and the end portion is lowered, and the whole is formed into a mountain shape. On the other hand, Fig. 10 is Ι^ = 120ιηιη(Μ = 360ιηιη), M>D. As shown in Fig. 1A, the sum of the plasma densities of the central portion and the end portion of the wafer W in the direction orthogonal to the direction of movement is substantially uniform. Similarly to the case of Fig. 9, the plasma density of the transmission plates 28A1 and 28A4 disposed at both ends is lowered outward. However, a drop occurs in a portion deviating from the width D of the wafer W, and a substantially uniform plasma density is maintained in the plane of the wafer W. Fig. 11 to Fig. 13 are shown at Li = 120 mm (M = 360 mm), M> In the setting of D, the microwave power introduced from the microwave transmission regions of the transmission plates 28A1 to 28A4 (that is, the corresponding microwave introduction units 27) is changed. Fig. 11 shows that the microwave power introduced from the transmissive plates 28A1 and 28A4 disposed outside is set to 1 000 W, and the microwave power introduced from the two transmissive plates 28 A2 and 28 A3 disposed inside is set to 600 W. Happening. The total 电 of the plasma density is lowered in the central portion of the wafer W in the direction orthogonal to the relative movement direction, and the end portion is high. Fig. 12 shows a case where the microwave power introduced from the transmissive plates 28A1 and 28A4 disposed outside is 1000 W, and the microwave power guided from the two transmissive plates 28A2 and 28A3 disposed inside is set to 1 300 W. The total 电 of the plasma density is increased in the central portion of the wafer W in the direction orthogonal to the relative movement direction, and becomes lower at the end portion. Fig. 13 shows a case where the introduced microwave power is set to 400 W, 600 W, 800 W, and 1000 W in the order of the transmission plates 28A1' 28A2' 28A3, 28A4. The total density of the plasma density is higher on one end side (the side of the transmission plate 28A4) of the wafer W in the direction orthogonal to the direction of movement of -25 to 201215250, and is lowered on the multi-end side (the side of the transmission plate 28A1) to generate a direction. tilt. Fig. 14 is a view showing a state in which the microwave power introduced from the microwave transmission regions of the transmission plates 28A1 to 28A4 is changed under the setting of Li = 90 mm (M = 270 mm) and M < D. FIG. 14 shows that the microwave powers introduced from the transmissive plates 28A1 and 28A4 disposed outside are set to be larger, and the microwave powers to be introduced from the two transmissive plates 28A2 and 28A3 disposed inside are set. Smaller 700W. However, since M < D, the decrease in the plasma density of the end portion of the wafer W in the direction orthogonal to the relative moving direction is not improved. From the above simulation results, it was confirmed that in order to uniformize the density of the plasma reaching the surface of the wafer W and to achieve uniform processing, it is preferable that the relationship of M2D is established. The above description is as shown in FIG. 8A and FIG. 8B. When the wafer W is in a linear motion, when the wafer W is in the revolving motion, the speeds of the positions P1 and P3 on the wafer W are different, and the side far from the revolution axis is different. The P3 of the (outer side) is faster than the P1 of the near side (inner side). Therefore, it is necessary to increase the density of the plasma on the outer side as shown in Fig. 13, so that the temporal accumulation of the plasma density is uniform. As described above, the plasma processing apparatus 1A of the present embodiment includes a plurality of mounting regions SR on which the wafer W is placed, and at least one wafer W placed on the plurality of mounting regions SR is passed through at least one The microwave introduction unit 27 is formed to be relatively movable in such a manner as to oppose the position of the microwave transmission region of the transmission plate 28. Then, regardless of the position on the crystal II W, the plasma is dense

S -26- 201215250 度的時間性累計値及/或電漿照射時間的累計値皆形成相 同的方式配置電漿源(透過板),藉此可進行均一的處理 。因此,可使複數片的晶圓W間、及1片的晶圓W面內 的處理的均一性提升。並且,即使更換平面天線31,或 變更製程條件,還是可獨立控制處理容器1內的電漿分布 。因此,可在處理容器1內以所望的分布來安定地維持電 漿。又,即使對應於晶圓W的大型化來使處理容器1大 型化時,還使可藉由改變微波導入單元27的數量或配置 來簡單地調節在處理容器1內所生成的電漿分布。 其次,一邊參照圖15〜圖24,一邊舉幾個例子來說 明有關微波導入單元27的配置。在此也是依透過板來顯 示微波導入單元27的配置。圖15〜圖24是在載置台3 的平面圖投影顯示透過板28的配置。另外,在以下所示 的例子中是描繪3個或5個載置區域SR,但載置區域SR 的數量可爲任意。 圖15是表示在頂壁lc中,在與載置區域SR的環繞 軌道對向的位置,同心圓狀地配設4周、3群組 '合計12 個的透過板之例。首先,最內周的第1周是藉由透過板 1 1 1 A 1、1 1 1 B 1、1 1 1 C 1的3個所構成。其次,從內側算 起第2周是藉由透過板111A2、111B2、111C2的3個所 構成。同樣,從內側算起第3周是藉由透過板111A3、 111B3、111C3的3個所構成。然後,最外周的第4周是 藉由透過板111A4、111B4、111C4的3個所構成。透過 板111A1〜111A4是以對1片的晶圓W進行電漿處理的觀 -27- 201215250 點來構成1群組,同樣,透過板111B1〜1ΠΒ4、透過板 1 1 1 C 1〜1 1 1 C4亦分別構成群組。各群組的透過板1 1 1 A 1 〜111A4、透過板 111B1〜111B4、透過板 111C1〜111C4 是分別從內側往外側弧狀地且對箭號所示的載置區域SR 的環繞方向依序配列。並且,各群組的透過板111A1〜 111A4、透過板111B1〜111B4、透過板111C1〜111C4橫 渡載置區域SR的寬度方向(環繞的圓軌道的徑方向)配 列。藉由如此的配列,可對載置區域SR錯開時間依序將 複數的透過板的一部分或全體配列成上下重疊而去。圖 1 5所示的配列的基本想法是與圖5及圖6同樣,但在圖 1 5是群組數比圖5及圖6更少。此情況,藉由以無論在 晶圓W上的哪個位置,電漿密度的時間性累計値及/或電 漿照射時間的累計値皆會形成相同的方式來配置電漿源( 透過板),可進行均一的處理。並且,透過板的配設個數 可按照處理容器1的大小、載置區域SR(或晶圓W)的 數量、載置台3的旋轉速度、處理的內容(例如氧化、氮 化、成膜、蝕刻等)等來適當設定。 圖16是表示取代圖15的最內周的透過板111A1、 111B1、111C1,配置大面積的透過板112,且於頂壁lc 中,在與載置區域811的環繞軌道對向的位置,同心圓狀 地配設3周、3群組的透過板113A1,113A2,113A3、 113B1, 113B2, 113B3、 113C1, 113C2, 113C3 之合計 1 0個的透過板之例。 首先,在頂壁1C的中央是設有比周圍的透過板S -26- 201215250 degrees of time accumulation / and / or accumulation of plasma irradiation time are formed in the same way to configure the plasma source (transmission plate), so that uniform processing can be performed. Therefore, the uniformity of the processing in the wafer W of the plurality of wafers and the wafer W in one wafer can be improved. Further, even if the planar antenna 31 is replaced or the process conditions are changed, the plasma distribution in the processing container 1 can be independently controlled. Therefore, the plasma can be stably maintained in the processing container 1 with a desired distribution. Further, even when the processing container 1 is enlarged in accordance with the enlargement of the wafer W, it is possible to easily adjust the plasma distribution generated in the processing container 1 by changing the number or arrangement of the microwave introducing units 27. Next, the arrangement of the microwave introducing unit 27 will be described with reference to Figs. 15 to 24, to name a few. Here, the configuration of the microwave introduction unit 27 is also shown in accordance with the transmission plate. 15 to 24 are views showing the arrangement of the transmission plate 28 on the plan view of the mounting table 3. Further, in the example shown below, three or five placement areas SR are depicted, but the number of placement areas SR may be arbitrary. Fig. 15 is a view showing an example in which a total of twelve transparent plates are arranged four times in a concentric manner at a position facing the surrounding track of the mounting region SR in the top wall lc. First, the first week of the innermost circumference is constituted by three of the transmission plates 1 1 1 A 1 , 1 1 1 B 1 , and 1 1 1 C 1 . Next, the second week from the inside is constituted by three of the transmission plates 111A2, 111B2, and 111C2. Similarly, the third week from the inside is constituted by three of the transmission plates 111A3, 111B3, and 111C3. Then, the fourth week of the outermost circumference is constituted by three of the transmission plates 111A4, 111B4, and 111C4. The transmission plates 111A1 to 111A4 are formed by a group of -27-201215250 points for plasma treatment of one wafer W. Similarly, the transmission plates 111B1 to 1ΠΒ4 and the transmission plates 1 1 1 C 1 to 1 1 1 C4 also constitutes a group. The transmission plates 1 1 1 A 1 to 111A4 , the transmission plates 111B1 to 111B4 , and the transmission plates 111C1 to 111C4 of each group are sequentially curved from the inside to the outside and sequentially arranged in the circumferential direction of the placement area SR indicated by the arrow. Arranged. Further, the transmission plates 111A1 to 111A4, the transmission plates 111B1 to 111B4, and the transmission plates 111C1 to 111C4 of the respective groups are arranged in the width direction of the placement region SR (the radial direction of the surrounding circular orbit). By such an arrangement, a part or the whole of the plurality of transmissive plates can be arranged in a vertically overlapping manner with respect to the placement area SR. The basic idea of the arrangement shown in Fig. 15 is the same as that of Figs. 5 and 6, but in Fig. 15, the number of groups is less than that of Figs. 5 and 6. In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible. Further, the number of the transparent plates can be set according to the size of the processing container 1, the number of the mounting regions SR (or wafers W), the rotational speed of the mounting table 3, and the contents of the processing (for example, oxidation, nitridation, film formation, Etching, etc., etc. are set as appropriate. 16 is a view showing a transparent plate 112A1, 111B1, and 111C1 which are disposed on the innermost circumference of FIG. 15, and a large-area transmission plate 112 is disposed, and the top wall lc is concentric with the circumferential track of the mounting region 811. An example of a total of 10 transmission plates of the transmission plates 113A1, 113A2, 113A3, 113B1, 113B2, 113B3, 113C1, 113C2, and 113C3 of three groups and three groups is arranged in a circular shape. First, in the center of the top wall 1C, there is a transmissive plate than the surrounding

S -28- 201215250 113A1〜113A3、113B1 〜113B3、113C1〜113C3 更 透過板112。在透過板112的周圍,從內側算起第 藉由透過板113A1、113B1、及113C1的3個所構 2周是藉由113A2、113B2、113C2的3個所構成 周是藉由透過板113A3、113B3、113C3的3個所 透過板113A1〜113A3是以藉由與透過板112的組 1片的晶圓W進行電槳處理的觀點構成1群組,同 過板 113B1〜113B3、透過板 113C1〜113C3亦分 與透過板112的組合來構成群組。透過板112與各 透過板 113A1〜113A3、透過板 113B1〜113B3、 113C1〜113C3是分別從內側往外側弧狀地對箭號 載置區域SR的環繞方向依序配列。並且,各群組 板113A1〜113A3、透過板113B1〜113B3、透過板 〜11 3C3是分別橫渡載置區域SR的寬度方向(環 軌道的徑方向)配列。藉由如此的配列,可對載 Sr錯開時間依序將複數的透過板的微波透過區域 分或全體配列成上下重疊而去。就此例而言,環繞 載置區域SR (或晶圓W )的內側(轉軸側)是無 繞軌道上的哪個位置皆經常重疊於透過板112的微 區域的正下方。因此,可使載置區域SR(或晶圓 內側(轉軸側)的電漿密度比外側更高。 圖17是省略圖16的各群組的透過板的其中各 減少透過板的數量之例。另外,在圖丨7是描繪3 區域SR,但載置區域SR的數量可爲任意。首先, 大徑的 1周是 成,第 ,第3 構成。 合來對 樣,透 別藉由 群組的 透過板 所示的 的透過 1 1 3C 1 繞的圓 置區域 的一部 運動的 論在環 波透過 W)的 —個, 個載置 在頂壁 -29- 201215250 1C的中央設有大徑的透過板114。透過板114的周圍是在 與載置區域Sr的環繞軌道對向的位置,從內側算起第1 周設有透過板115A1、115B1及115C1的3個,第2周設 有透過板1 15A2、1 15B2、1 15C2的3個,合計設有7個 的透過板。透過板115A1、115A2是以藉由與透過板114 的組合來對1片的晶圓W進行電漿處理的觀點構成1群 組,同樣,透過板115B1、115B2、透過板115C1、I15C2 亦分別藉由與透過板1 1 4的組合來構成群組。透過板1 1 4 與各群組的透過板Π5Α1、115A2、透過板115B1、115B2 、透過板1 15C1、1 15C2是分別由內側往外側弧狀地對箭 號所示的載置區域SR的環繞方向依序配列。並且,各群 組的透過板115A1、115A2、透過板115B1、115B2、透過 板1 15C1、1 15C2是分別橫渡載置區域SR的寬度方向( 環繞的圓軌道的徑方向)配列。藉由如此的配列,可對載 置區域SR錯開時間依序將複數的透過板的微波透過區域 的一部分或全體配列成上下重疊而去。此例也是環繞運動 的載置區域SR或晶圓W的內側(轉軸側)無論在環繞軌 道上的哪個位置皆經常重疊於透過板114的微波透過區域 的正下方。因此,可使載置區域SR或晶圓W的內側(轉 軸側)的電漿密度比外側更高。 圖18是表示在頂壁lc中,在與載置區域SR的環繞 軌道對向的位置,同心圓狀地配設4周、合計16個的透 過板之例。首先,最內周的第1周是藉由透過板116A1、 1 16B1、1 16C1的3個所構成。其次,從內側算起第2周S -28- 201215250 113A1 to 113A3, 113B1 to 113B3, 113C1 to 113C3 are further transmitted through the board 112. Around the transmission plate 112, three of the three passes of the transmission plates 113A1, 113B1, and 113C1 from the inside are formed by the transmission plates 113A3 and 113B3 by the three sections 113A2, 113B2, and 113C2. The three transmission plates 113A1 to 113A3 of the 113C3 are grouped by the viewpoint of performing electric paddle processing on the wafer W of the group of the transmission plates 112, and the same plates 113B1 to 113B3 and the transmission plates 113C1 to 113C3 are also divided. The group is formed in combination with the transmissive plate 112. The transmission plate 112 and the transmission plates 113A1 to 113A3 and the transmission plates 113B1 to 113B3 and 113C1 to 113C3 are arranged in an arc-like manner from the inside to the outside in the circumferential direction of the arrow placement area SR. Further, each of the group plates 113A1 to 113A3, the transmission plates 113B1 to 113B3, and the transmission plates 11 to 11C3 are arranged in the width direction (the radial direction of the ring track) of the placement region SR. By such an arrangement, the microwave transmissive regions of the plurality of transmissive plates or the entire array can be sequentially arranged to overlap each other in the Sr shift time. In this case, the inner side (the axis side) of the surrounding placement area SR (or the wafer W) is which position on the unwound track often overlaps directly below the micro area of the transmission plate 112. Therefore, the plasma density of the mounting region SR (or the inner side of the wafer (the rotating shaft side) can be made higher than the outer side. Fig. 17 is an example in which the number of the transparent reflecting plates of the respective transparent plates of Fig. 16 is omitted. Further, in Fig. 7, the three regions SR are depicted, but the number of the placement regions SR may be arbitrary. First, one week of the large diameter is the first, third, and third configurations. The movement of a part of the circular area through the 1 1 3C 1 shown by the plate is transmitted through the W), and the large diameter is placed in the center of the top wall -29-201215250 1C. Through the board 114. The periphery of the transmission plate 114 is at a position facing the surrounding track of the mounting region Sr, and three of the transmission plates 115A1, 115B1, and 115C1 are provided on the first circumference from the inside, and the transmission plate 1 15A2 is provided on the second circumference. 3 of 15B2 and 1 15C2, and a total of seven transmissive plates are provided. The transmissive plates 115A1 and 115A2 are grouped by a plasma treatment of one wafer W by a combination with the transmissive plate 114. Similarly, the transmissive plates 115B1 and 115B2 and the transmissive plates 115C1 and I15C2 are respectively borrowed. The group is formed by a combination with the transmissive plate 1 1 4 . The transmission plate 1 1 4 and the transmission plates Π5Α1 and 115A2 of the respective groups, the transmission plates 115B1 and 115B2, and the transmission plates 1 15C1 and 1 15C2 are respectively curved outwardly from the inside to the outside of the placement area SR indicated by the arrow. The directions are arranged in order. Further, the transmission plates 115A1 and 115A2 and the transmission plates 115B1 and 115B2 and the transmission plates 1 15C1 and 1 15C2 of the respective groups are arranged in the width direction (the radial direction of the circular orbit) of the placement region SR. By such an arrangement, a part or the whole of the microwave transmission regions of the plurality of transmission plates can be arranged in a vertically overlapping manner with respect to the placement area SR. In this example, the mounting area SR of the surrounding motion or the inner side (the rotating shaft side) of the wafer W often overlaps directly below the microwave transmitting area of the transmitting plate 114 regardless of the position on the surrounding track. Therefore, the plasma density of the inner side (rotation side) of the mounting region SR or the wafer W can be made higher than the outer side. Fig. 18 is a view showing an example in which a total of 16 transparent plates are arranged concentrically at a position facing the surrounding track of the mounting region SR in the top wall 1c. First, the first week of the innermost circumference is constituted by three of the transmission plates 116A1, 16B1, and 16C1. Second, the second week from the inside

S -30- 201215250 是藉由透過板116A2、116B2、116C2的3個所構成。從 內側算起第3周是藉由透過板116A3、116B3、116C3、 116D的4個所構成。然後,最外周的第4周是藉由透過 板 1 16A4 ' 116B4、116C4、116E、116F、1 16G 的 6 個所 構成》如此,使外側(載置台3的外周)的透過板的個數 比頂壁1 c的中心側還設置更多。藉由如此的配列,可對 載置區域SR錯開時間依序將複數的透過板的微波透過區 域的一部分或全體配列成上下重疊而去。並且,藉由使外 側(載置台3的外周)的透過板的個數比頂壁1 c的中心 側還配置更多,可容易提高環繞速度變快的載置區域Sr (或晶圓W)的外側的電漿密度。此情況,以無論晶圓W 上的哪個位置,電漿密度的時間性累計値及/或電漿照射 時間的累計値皆形成相同的方式,配置電漿源(透過板) ,藉此可進行均一的處理。 圖19是表示在頂壁1C中,在與載置區域SR的環繞 軌道對向的位置,同心圓狀地配設4周、合計10個的透 過板之例。首先,最內周的第1周是藉由透過板117A、 11 7B的2個所構成。其次,從內側算起第2周是藉由透 過板11 8A、11 8B的2個所構成。從內側算起第3周是藉 由透過板119A、119B的2個所構成。然後,最外周的第 4周是藉由透過板120A、120B、120C、120D的4個所構 成。並且,使第1周〜第4周的透過板的面積變化,第1 周與第4周是相同大小,第2周是比第1周更大,第3周 是比第2周再更大。如此,可組合面積不同的透過板來配 -31 - 201215250 置。藉由如此的配列,可對載置區域sR錯開時間依序將 複數的透過板的微波透過區域的一部分或全體配列成上下 重疊而去。如此,將電漿源(透過板)配置成無論在晶圓 W上的哪個位置,電漿密度的時間性累計値及/或電漿照 射時間的累計値皆會形成相同,藉此可進行均一的處理。 圖20是在頂壁lc中,在與載置區域SR的環繞軌道 對向的位置,同心圓狀地使4周合計14個的透過板,不 是頂壁lc的全體,而是偏置於一部分之構成例。亦即, 最內周的第1周是藉由透過板121A、121B的2個所構成 。其次,從內側算起第2周是藉由透過板122A、122B、 122C的3個所構成。從內側算起第3周是藉由透過板 123A、123B、123C、123D的4個所構成。然後,最外周 的第4周是藉由透過板124A、124B、124C、124D、124E 的5個所構成。藉由使透過板與載置區域SR(或晶圓W )相對移動,不需要在頂壁lc的全域設置透過板,因此 如圖20所示可使透過板部分地偏在設置。此情況,藉由 以無論在晶圆W上的哪個位置,電漿密度的時間性累計 値及/或電漿照射時間的累計値皆會形成相同的方式來配 置電漿源(透過板),可進行均一的處理。並且,在頂壁 U中,在未設置透過板的區域(朝向圖20的紙面右半分 )例如可使用於配備膜厚測定裝置或氣體供給裝置等其他 的用途。 圖21是表示在頂壁lc中,在與載置區域SR的環繞 軌道對向的位置配置合計9個的橢圓形狀的透過板之例。S -30- 201215250 is constituted by three of the transmission plates 116A2, 116B2, and 116C2. The third week from the inside is constituted by four of the transmission plates 116A3, 116B3, 116C3, and 116D. Then, the fourth week of the outermost circumference is constituted by the six layers of the transmission plates 1 16A4 '116B4, 116C4, 116E, 116F, and 16G, so that the number of the transmission plates on the outer side (the outer circumference of the mounting table 3) is higher than the top. The center side of the wall 1 c is also set more. By such an arrangement, a part or the whole of the microwave transmission regions of the plurality of transmission plates can be arranged in a vertically overlapping manner with respect to the placement area SR. Further, by arranging the number of the transparent plates on the outer side (outer circumference of the mounting table 3) more than the center side of the top wall 1c, it is possible to easily increase the mounting area Sr (or wafer W) in which the surrounding speed is increased. The outer plasma density. In this case, the plasma source (transmission plate) can be configured in the same manner regardless of the position on the wafer W, the cumulative time of the plasma density, and/or the cumulative time of the plasma irradiation time. Uniform processing. Fig. 19 shows an example in which a total of ten transparent plates are arranged four times in a concentric manner at a position facing the surrounding track of the mounting region SR in the top wall 1C. First, the first week of the innermost circumference is constituted by two of the transmission plates 117A and 11 7B. Next, the second week from the inside is formed by passing through two of the plates 11 8A and 11 8B. The third week from the inside is constituted by two of the transmission plates 119A and 119B. Then, the fourth week of the outermost circumference is constituted by four of the transmission plates 120A, 120B, 120C, and 120D. Further, the area of the transmission plate from the first week to the fourth week is changed, and the first week and the fourth week are the same size, the second week is larger than the first week, and the third week is larger than the second week. . In this way, it is possible to combine the transmissive plates with different areas to match -31 - 201215250. According to such an arrangement, a part or the whole of the microwave transmission regions of the plurality of transmission plates can be arranged in a vertically overlapping manner with respect to the placement region sR. In this way, the plasma source (transmission plate) is disposed such that the position of the plasma density and/or the cumulative time of the plasma irradiation time are the same regardless of the position on the wafer W, thereby achieving uniformity. Processing. FIG. 20 is a transmissive plate in which the total length of four of four weeks is concentrically placed on the top wall lc at a position facing the surrounding track of the mounting area SR, not the entire top wall lc, but is offset to a part. A configuration example. That is, the first week of the innermost circumference is constituted by two of the transmission plates 121A and 121B. Next, the second week from the inside is constituted by three of the transmission plates 122A, 122B, and 122C. The third week from the inside is constituted by four of the transmission plates 123A, 123B, 123C, and 123D. Then, the fourth week of the outermost circumference is constituted by five of the transmission plates 124A, 124B, 124C, 124D, and 124E. By moving the transmissive plate and the placement region SR (or the wafer W) relative to each other, it is not necessary to provide the transmissive plate in the entire region of the top wall lc. Therefore, as shown in Fig. 20, the transmissive plate can be partially biased. In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible. Further, in the top wall U, a region where the transmission plate is not provided (toward the right half of the paper surface of Fig. 20) can be used for other purposes such as a film thickness measuring device or a gas supply device. Fig. 21 is a view showing an example in which a total of nine elliptical transmissive plates are disposed in a position facing the surrounding track of the mounting region SR in the top wall lc.

S -32- 201215250 亦即,最內周的第1周是藉由透過板125A、125B、125C 的3個所構成。其次,從內側算起第2周是藉由透過板 126A、126B、126C的3個所構成。從內側算起第3周是 藉由透過板127A、127B、127C的3個所構成。透過板 125A〜125C、126A〜126C、127A〜127C的長度方向的角 度爲任意,且亦可不一定中心要配置成同心圓狀。如此, 透過板的形狀不是一定限於圓形,例如除了橢圓形以外, 可爲四角形、長方形等的多角形的任意形狀。此情況,藉 由以無論在晶圓W上的哪個位置,電漿密度的時間性累 計値及/或電漿照射時間的累計値皆會形成相同的方式來 配置電漿源(透過板),可進行均一的處理。S -32 - 201215250 That is, the first week of the innermost circumference is constituted by three of the transmission plates 125A, 125B, and 125C. Next, the second week from the inside is constituted by three of the transmission plates 126A, 126B, and 126C. The third week from the inside is constituted by three of the transmission plates 127A, 127B, and 127C. The angles in the longitudinal direction of the transmission plates 125A to 125C, 126A to 126C, and 127A to 127C are arbitrary, and may not necessarily be arranged concentrically at the center. As described above, the shape of the transmission plate is not necessarily limited to a circular shape, and may be any shape of a polygonal shape such as a quadrangle or a rectangle, in addition to an elliptical shape. In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible.

圖22是表示在頂壁lc中,在與載置區域SR的環繞 軌道對向的位置,同心圓狀地配置3周、合計.6個的透過 板之構成例。亦即,最內周的第1周是藉由透過板128A 、128B的2個所構成。其次,從內側算起第2周是藉由 透過板129A、129B的2個所構成。最外周亦即從內側算 起第3周是藉由透過板13 0A、130B的2個所構成。就此 例而言,第2周的透過板129A、12 9B是構成比第1周的 透過板128A、1280、第3周的透過板130A、130B更大 面積。具體而言,透過板12 9A、129B是形成比載置區域 SR (或晶圓W )的面積更大,形成載置區域SR (或晶圓 W)的全體會重疊於透過板12 9A、129B的正下方。因此 ,就晶圓W的面內的處理的均一性的觀點而言,透過板 12 9A、129B爲主要的電漿生成部,第1周的透過板128A -33- 201215250 、128B、第3周的透過板130A、130B是補充透過板 12 9A、129B的輔助性電漿生成部。此情況,藉由以無論 在晶圓W上的哪個位置,電漿密度的時間性累計値及/或 電漿照射時間的累計値皆會形成相同的方式來配置電漿源 (透過板),可進行均一的處理。 在圖22是使具有作爲輔助性電漿生成部的機能之透 過板 128A、128B、透過板 13 0A、130B的各微波透過區 域與載置區域SR(或晶圓W)的軌道部分地上下重疊, 但考慮電漿的擴散,亦可設於偏離載置區域SR(或晶圓 W)的軌道之位置。將如此的例子顯示於圖23。 圖23是在頂壁lc中,在與載置區域SR的環繞軌道 對向的位置,同心圓狀地配置3周、合計6個的透過板之 構成例。亦即,最內周的第1周是藉由透過板131A、 131B的2個所構成。其次,從內側算起第2周是藉由透 過板132A、132B的2個所構成。最外周亦即從內側算起 第3周是藉由透過板133A、133B的2個所構成。第2周 的透過板132A、132B是構成比第1周的透過板131 A、 131B、第3周的透過板133A、133B更大面積。具體而言 ,透過板13 2A、13 2B是形成比載置區域SR(或晶圓W) 的面積更大,形成載置區域SR(或晶圓W)的大部分會 重疊於透過板13 2A、132B的正下方。因此,就晶圓W的 面內的處理的均一性的觀點而言,透過板13 2A、132B爲 主的電漿生成部,第1周的透過板131A、131B、第3周 的透過板133A、133B是補充透過板132A、132B的輔助Fig. 22 is a view showing an example of a configuration in which a total of six transparent plates are arranged three times in a concentric manner at a position facing the surrounding track of the mounting region SR in the top wall lc. That is, the first week of the innermost circumference is constituted by two of the transmission plates 128A and 128B. Next, the second week from the inside is constituted by two of the transmission plates 129A and 129B. The outermost circumference, that is, the third week from the inner side, is composed of two of the transmission plates 130A and 130B. In this example, the transmission plates 129A and 12 9B of the second week constitute a larger area than the transmission plates 128A and 1280 of the first week and the transmission plates 130A and 130B of the third circumference. Specifically, the transmission plates 12 9A and 129B are formed to have a larger area than the placement region SR (or the wafer W), and the entire formation region SR (or wafer W) is superposed on the transmission plates 12 9A and 129B. Just below. Therefore, from the viewpoint of the uniformity of the processing in the in-plane of the wafer W, the transmissive plates 12 9A and 129B are the main plasma generating portions, and the first reflecting plates 128A - 33 - 201215250 , 128B , and the third week The transmission plates 130A and 130B are auxiliary plasma generating units that supplement the transmission plates 12 9A and 129B. In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible. In Fig. 22, each of the microwave transmission regions having the transmission plates 128A and 128B and the transmission plates 130A and 130B having the functions of the auxiliary plasma generating portion and the rails of the placement region SR (or wafer W) are partially overlapped. However, considering the diffusion of the plasma, it may be located at a position away from the track of the mounting area SR (or the wafer W). An example of this is shown in FIG. Fig. 23 shows an example of a configuration in which a total of six transparent plates are arranged three times concentrically at a position facing the surrounding track of the mounting region SR in the top wall lc. That is, the first week of the innermost circumference is constituted by two of the transmission plates 131A and 131B. Next, the second week from the inside is constituted by two of the plates 132A and 132B. The outermost circumference, that is, from the inner side, is formed by the two transmission plates 133A and 133B. The transmission plates 132A and 132B of the second week are larger in area than the transmission plates 131 A and 131B of the first week and the transmission plates 133A and 133B of the third circumference. Specifically, the transmissive plates 13 2A and 13 2B are formed to have a larger area than the mounting region SR (or the wafer W), and most of the mounting region SR (or the wafer W) is superposed on the transmissive plate 13 2A. Directly below 132B. Therefore, from the viewpoint of the uniformity of the processing in the in-plane of the wafer W, the plasma generating portions mainly including the transmitting plates 13 2A and 132B, the transmitting plates 131A and 131B of the first week, and the transmitting plates 133A of the third week. 133B is supplementary to the auxiliary plate 132A, 132B

S -34- 201215250 性電漿生成部。在圖23中,具有作爲輔助性電漿生成部 的機能之透過板133A、133B雖未與載置區域SR (或晶圓 W)的軌跡部分地上下重疊,但在透過板133A、133B的 微波透過區域的正下方所生成的電漿會藉由擴散而擴散至 晶圓W的上方而去,因此可取得補充藉由從透過板132A 、132B的微波透過區域所導入的微波而生成的電漿之效 果。此情況,藉由以無論在晶圓W上的哪個位置,電漿 密度的時間性累計値及/或電漿照射時間的累計値皆會形 成相同的方式來配置電漿源(透過板),可進行均一的處 理。 圖24是與圖22同樣,組合大面積及小面積的透過板 之構成例。亦即,在頂壁lc中,在與載置區域811的環繞 軌道對向的位置,同心圓狀地配置有2個大面積透過板 135A、135B、及同心圓狀地配置4周、4個的透過板。小 面積透過板的最內周的第1周是透過板134A,從內側算 起第2周是透過板134B,從內側算起第3周是透過板 134C,最外周亦即從內側算起第4周是由透過板134D所 構成。就此例而言,大面積的透過板135A、135B是配合 導波管37的形狀來構成矩形。具體而言,透過板135A、 13 5B是形成比載置區域SR (或晶圓W)的面積更大,在 透過板135A、135B的正下方,藉由載置區域SR(或晶圓 W)相對移動,形成其全部可通過透過板135A、135B的 微波透過區域的正下方。因此,就晶圓W的面內的處理 的均一性的觀點而言,透過板135A、135B爲主要的電漿 -35- 201215250 生成部,第1周的透過板134A、第2周的透過板134B、 第3周的透過板134C、第4周的13 4D是補充透過板 135A、135B的輔助性電漿生成部。另外,在圖24中,具 有作爲輔助性電漿生成部的機能之透過板134A、134B、 134C、134D是使與載置區域SR (或晶圓W)的軌跡部分 地上下重疊,但如圖23的例子所說明,考慮電漿的擴散 ,透過板134A、134B、134C、134D亦可設於偏離載置區 域SR(或晶圓W)的軌跡之位置。此情況,藉由以無論 在晶圓W上的哪個位置,電漿密度的時間性累計値及/或 電漿照射時間的累計値皆會形成相同的方式來配置電漿源 (透過板),可進行均一的處理。 如圖5、6、圖15〜圖24所示,使載置區域SR (或 晶圓W)環繞運動時,在載置區域SR (或晶圓W)之中 接近轉軸的內周側的部位是移動速度會變慢,外周側的部 位是移動速度會變快。因此,如圖1 8所例示般,比起頂 壁1 c的內側部分,在頂壁1 c的外側部分配設更多的透過 板,亦有效容易提高移動速度快的載置區域SR的外周部 分的電漿密度。並且,比起頂壁lc的內側部分,更擴大 外側部分的透過板的面積,亦有效提高移動速度快的載置 區域SR的外周部分的電漿密度。而且,使來自配置於頂 壁lc的外側部分的透過板的微波功率的導入形成比配置 於內側部分的透過板更大,亦有效提高移動速度快的載置 區域SR的外周部分的電漿密度。又,如圖22及圖23所 示,藉由將成爲輔助性電漿生成部的透過板配置於頂壁S -34- 201215250 Plasma generation department. In FIG. 23, the transmission plates 133A and 133B having the function as the auxiliary plasma generating portion are not partially overlapped with the track of the placement region SR (or the wafer W), but the microwaves are transmitted through the transmission plates 133A and 133B. The plasma generated immediately below the transmission region is diffused and spread over the wafer W, so that the plasma generated by the microwaves introduced from the microwave transmission regions of the transmission plates 132A and 132B can be obtained. The effect. In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible. Fig. 24 is a view showing an example of a configuration in which a large-area and small-area transmission plate is combined as in Fig. 22; In other words, in the top wall lc, two large-area transmission plates 135A and 135B are arranged concentrically at positions facing the surrounding track of the mounting region 811, and four and four concentrically arranged. Through the board. The first week of the innermost area of the small-area transmission plate is the permeation plate 134A, and the second week from the inside is the permeation plate 134B, and the third week from the inside is the permeation plate 134C, and the outermost circumference is the inner side. 4 weeks is made up of the transmission plate 134D. In this case, the large-area transmission plates 135A and 135B are formed in a rectangular shape in accordance with the shape of the waveguide 37. Specifically, the transmissive plates 135A and 135B are formed to have a larger area than the mounting region SR (or the wafer W), and are disposed directly below the transmissive plates 135A and 135B by the mounting region SR (or wafer W). Relatively moving, all of them are formed to pass directly under the microwave transmitting region of the transmitting plates 135A, 135B. Therefore, from the viewpoint of the uniformity of the processing in the in-plane of the wafer W, the transmissive plates 135A and 135B are the main plasma-35-201215250 generating portion, the first reflecting plate 134A, and the second reflecting plate. 134B, the transmission plate 134C of the third week, and the 13 4D of the fourth week are auxiliary plasma generating units that supplement the transmission plates 135A and 135B. In addition, in FIG. 24, the transmission plates 134A, 134B, 134C, and 134D having the function as the auxiliary plasma generating portion partially overlap the track of the mounting region SR (or the wafer W), but as shown in the figure. As an example of 23, in consideration of the diffusion of the plasma, the transmission plates 134A, 134B, 134C, and 134D may be provided at positions deviated from the trajectory of the mounting region SR (or the wafer W). In this case, the plasma source (transmission plate) is configured in the same manner by which the cumulative time of the plasma density and/or the cumulative time of the plasma irradiation time are formed regardless of the position on the wafer W. Uniform processing is possible. As shown in FIGS. 5, 6, and 15 to 24, when the mounting region SR (or the wafer W) is moved around, the portion on the inner peripheral side of the rotating shaft is placed in the mounting region SR (or the wafer W). The moving speed will be slower, and the moving speed will be faster on the outer peripheral side. Therefore, as illustrated in Fig. 18, more of the transmissive plate is disposed on the outer portion of the top wall 1c than the inner portion of the top wall 1c, and it is also effective to easily increase the outer circumference of the mounting region SR having a fast moving speed. Part of the plasma density. Further, the area of the transmissive plate of the outer portion is enlarged more than the inner portion of the top wall lc, and the plasma density of the outer peripheral portion of the mounting region SR having a high moving speed is also effectively improved. Further, the introduction of the microwave power from the transmissive plate disposed at the outer portion of the top wall lc is made larger than that of the transmissive plate disposed on the inner portion, and the plasma density of the outer peripheral portion of the mounting region SR having a high moving speed is effectively increased. . Further, as shown in Figs. 22 and 23, the transmission plate serving as the auxiliary plasma generating portion is disposed on the top wall.

S -36- 201215250 1C的外側部分,亦有效提高移動速度快的載置區域SR的 外周部分的電漿密度。並且,藉由將電漿源(透過板)配 置成無論在晶圓W上的哪個位置,電漿密度的時間性累 計値及/或電漿照射時間的累計値皆會形成相同,可進行 均一的處理。 其次,一邊參照圖25〜圖30,一邊說明有關處理容 器1的氣體供給部及排氣部的構成。電漿處理裝置100是 在頂壁1C配設複數的微波導入單元27,因此相較於以往 那樣在處理空間的上方全域設置微波導入單元的構成,氣 體導入部位的配置的自由度高。可在頂壁lc配備有微波 導入單元27的部位以外的任意處設置氣體導入部15。圖 25是模式性地顯示電漿處理裝置100的處理容器1的內 部的氣流。另外,在圖25中,排氣裝置24是具備APC 閥(APC)及渦輪分子泵(TMP)。圖26是模式性地明 確顯示在與圖25相同的氣體導入部15的構成中,處理容 器1內的氣流與載置台3、載置區域SR、氣體導入部15 及排氣口 11的位置關係。在圖26中,氣體導入部15是 配設於頂壁lc的中央,在氣體導入部15的中心設有一個 的氣孔16。並且,在圖26中’在載置台3的下方圓環狀 地設置排氣口 11’因此從氣孔16噴射的氣體會如圖中箭 號所示般,在處理容器1內被均等地分配成放射狀,從排 氣口 11排氣。其途中’氣體會被均等地分配於在旋轉的 載置台3的載置區域Sr所載置的晶圓w的表面,可謀求 複數片的晶圓W間的處理均一化、及一片的晶圓w面內 -37- 201215250 的處理均一化。 圖27是表示氣體導入部及排氣部的別的構成例。在 圖27中,氣孔16a是設於頂壁lc的全域。亦即,除了頂 壁lc設有透過板28(電漿導入單元27)的地方以外,在 頂壁lc的全域形成有多數的氣孔16a。往各氣孔16a的 氣體導入的構成是例如可爲形成於頂壁lc的內部之氣體 流路,或配設於頂壁lc的上部之氣體分配器。並且,圖 27是在載置台3的下方4處配備排氣口 11,因此從各氣 孔16a噴射的氣體會被均等地分配於處理容器1內,從各 排氣口 11排氣。其途中,氣體會被均等地分配於在旋轉 的載置台3的載置區域SR所載置的晶圓W的表面,可謀 求複數片的晶圓W間的處理均一化、及一片的晶圓W面 內的處理均一化。另外,藉由在排氣口 11設置排氣分散 板,可取得更均等的氣流。 圖28〜圖30是表示氣體導入部及排氣部的另外別的 構成例。圖2 8〜圖3 0是模式性地明確顯示處理容器1 ( 在此是圖示省略)內的氣流與載置台3、載置區域SR、氣 體導入部及排氣口 1 1的位置關係。首先,若參照圖28, 則具有氣體導入構件1 6作爲氣體導入部,其係例如與載 置台3對向設置,且在載置台3的半徑方向呈長條形狀。 氣體導入構件16是具備用以導入氣體的噴嘴。例如在氣 體導入構件1 6的下面直列地形成有複數的氣孔1 6a。圖 28是將2根的氣體導入構件16直線狀地配置成該等的長 度方向會重疊於載置台3的直徑。The outer portion of the S-36-201215250 1C also effectively increases the plasma density of the outer peripheral portion of the mounting area SR where the moving speed is fast. Further, by arranging the plasma source (transmission plate) at any position on the wafer W, the temporal accumulation of the plasma density and/or the accumulation of the plasma irradiation time are all the same, and uniformity can be performed. Processing. Next, the configuration of the gas supply unit and the exhaust unit of the processing container 1 will be described with reference to Figs. 25 to 30 . In the plasma processing apparatus 100, a plurality of microwave introducing units 27 are disposed in the top wall 1C. Therefore, the microwave introducing unit is provided over the entire processing space as compared with the conventional one, and the degree of freedom in the arrangement of the gas introduction portions is high. The gas introduction portion 15 may be provided at any position other than the portion where the ceiling wall lc is provided with the microwave introduction unit 27. Fig. 25 is a view schematically showing the flow of the inside of the processing container 1 of the plasma processing apparatus 100. Further, in Fig. 25, the exhaust device 24 is provided with an APC valve (APC) and a turbo molecular pump (TMP). FIG. 26 is a view schematically showing the positional relationship between the airflow in the processing container 1 and the mounting table 3, the mounting region SR, the gas introduction portion 15, and the exhaust port 11 in the configuration of the gas introduction portion 15 similar to that of FIG. . In Fig. 26, the gas introduction portion 15 is disposed at the center of the top wall lc, and one air hole 16 is provided at the center of the gas introduction portion 15. Further, in Fig. 26, 'the exhaust port 11' is provided annularly below the mounting table 3, so that the gas ejected from the air hole 16 is equally distributed in the processing container 1 as indicated by an arrow in the figure. Radial, exhausted from the exhaust port 11. In the meantime, the gas is equally distributed on the surface of the wafer w placed on the mounting region Sr of the rotating mounting table 3, and the processing between the wafers W of a plurality of wafers can be uniformized, and a wafer can be processed. The processing of w-in-37-201215250 is uniform. Fig. 27 is a view showing another configuration example of the gas introduction portion and the exhaust portion. In Fig. 27, the air holes 16a are provided over the entire area of the top wall lc. That is, a plurality of air holes 16a are formed in the entire area of the top wall lc except for the place where the top wall lc is provided with the transmission plate 28 (the plasma introduction unit 27). The gas introduction structure to each of the air holes 16a may be, for example, a gas flow path formed inside the top wall lc or a gas distributor disposed on the upper portion of the top wall lc. Further, in Fig. 27, the exhaust port 11 is provided at the lower portion 4 of the mounting table 3, so that the gas ejected from each of the air holes 16a is evenly distributed in the processing container 1, and is exhausted from each of the exhaust ports 11. In the meantime, the gas is equally distributed to the surface of the wafer W placed on the mounting region SR of the rotating mounting table 3, and the processing between the wafers W of a plurality of wafers can be uniformized, and one wafer can be processed. The processing in the W plane is uniform. Further, by providing the exhaust gas dispersion plate at the exhaust port 11, a more uniform air flow can be obtained. Fig. 28 to Fig. 30 show other examples of the configuration of the gas introduction portion and the exhaust portion. Figs. 28 to 30 show the positional relationship between the airflow in the processing container 1 (not shown here), the mounting table 3, the mounting region SR, the gas introduction portion, and the exhaust port 1 1 in a schematic manner. First, referring to Fig. 28, the gas introduction member 16 is provided as a gas introduction portion which is disposed opposite to the mounting table 3, for example, and has a long shape in the radial direction of the mounting table 3. The gas introduction member 16 is provided with a nozzle for introducing a gas. For example, a plurality of pores 16a are formed in series below the gas introduction member 16. Fig. 28 shows that the two gas introduction members 16 are linearly arranged such that the length direction thereof overlaps the diameter of the mounting table 3.

S -38- 201215250 另外,氣體導入構件16是配置於離開微波導入單元 27的正下方的位置。氣體導入構件16的長度方向對於在 圓軌道公轉的晶圓W的進行方向(亦即,圓軌道的接線 方向)是正交配置。氣體是從氣體導入構件16的複數個 氣孔16a來朝被載置於載置台3的載置區域SR的晶圓W (未圖示)線狀地噴射。氣體是到達載置台3的上面而分 流於2方向,分別往配設於載置台3的外周部分的下方的 排氣口 11。此形態,排氣口 11是在載置台3的周方向, 設於偏離一對的氣體導入構件16的配設位置大致90°的 位置。如此,從長的氣體導入構件16來線狀地供給氣體 ,在旋轉的載置台3的正上方使分歧成2方向的流動,而 使反應種或反應生成物均等地(旋轉(公轉)的積分値) 分配於各載置區域SR所載置的複數片的晶圓W間,可謀 求晶圓W間的處理均一化、及一片的晶圓W面內的處理 均一化。 氣體導入構件16的配設位置或數量是除了圖28的例 子以外,亦可爲各種的變化。例如,圖29是表示配設3 組(合計6個)在長度方向成對的氣體導入構件之構成例 。亦即,氣體導入構件16A,16A是以該等的長度方向重 疊於載置台3的直徑之方式配置成直線狀。同樣,氣體導 入構件16B,16B、氣體導入構件16C,16C也是分別以 該等的長度方向重疊於載置台3的直徑之方式配置成直線 狀。各氣體導入構件16的構成是與圖28同樣。氣體導入 構件16A,16A與氣體導入構件16B,16B的配設角度、 -39- 201215250 及氣體導入構件16A,16A與氣體導入構件16C,16C的 配設角度分別爲任意。例如可以氣體導入構件1 6A,1 6A 爲基準,將氣體導入構件16B,16B及氣體導入構件16C ,16C分別以錯開45°的角度來配置。藉由如此在處理容 器1的頂壁lc的複數個位置配設氣體導入構件16進行氣 體供給,可使反應種或反應生成物均等地(旋轉(公轉) 的積分値)分配於各載置區域SRK載置的複數片的晶圓 W間,更能謀求晶_ W間的處理均一化、及一片的晶圓 W面內的處理均一化。另外,氣體導入構件16的數量可 比圖29更增加。 並且,在圖29的構成例中,亦可改變例如經由氣體 導入構件16A,16A來導入的氣體種類、及經由氣體導入 構件16B,16B、氣體導入構件16C,16C來導入的氣體 種類。例如,從氣體導入構件16A,16A,與其他的氣體 區別導入產生短壽命的活性種的氣體、或產生一旦長存於 電漿中則對製程造成不良影響的反應種的氣體等。此情況 ,可縮短在處理容器1內的滯留時間,因此可有效率地利 用產生短壽命的活性種的氣體,或抑制一旦長存於電漿中 則對製程造成不良影響的反應種的生成。另外,亦可使從 氣體導入構件16A,16B,16C導入的氣體種類形成不同 的種類。 圖30是表示氣體導入部及排氣部的別的構成例。圖 30的例子是具備彎曲成弓狀的氣體導入構件16D作爲氣 體導入部。又,排氣口 11A亦具有彎曲成弓狀的形狀》S - 38 - 201215250 Further, the gas introduction member 16 is disposed at a position directly below the microwave introduction unit 27 . The longitudinal direction of the gas introduction member 16 is orthogonal to the direction in which the wafer W revolving in the circular orbit (i.e., the wiring direction of the circular track). The gas is ejected linearly from the plurality of pores 16a of the gas introduction member 16 toward the wafer W (not shown) placed on the placement region SR of the mounting table 3. The gas reaches the upper surface of the mounting table 3 and is branched in the two directions, and is disposed to the exhaust port 11 below the outer peripheral portion of the mounting table 3, respectively. In this form, the exhaust port 11 is provided at a position offset from the arrangement position of the pair of gas introduction members 16 by approximately 90 in the circumferential direction of the mounting table 3. In this way, the gas is supplied linearly from the long gas introduction member 16, and the flow is divided into two directions directly above the rotating mounting table 3, and the reaction species or the reaction product are uniformly (rotation (revolution) integration).値) Between the wafers W of the plurality of sheets placed in the respective placement regions SR, the processing between the wafers W can be uniformized, and the processing in the wafer W surface can be uniformized. The arrangement position or number of the gas introduction members 16 may be various changes in addition to the example of Fig. 28. For example, Fig. 29 is a view showing an example of a configuration in which three groups (total of six) of gas introduction members paired in the longitudinal direction are disposed. In other words, the gas introduction members 16A, 16A are arranged linearly so as to overlap the diameter of the mounting table 3 in the longitudinal direction. Similarly, the gas introduction members 16B and 16B and the gas introduction members 16C and 16C are also arranged linearly so as to overlap the diameter of the mounting table 3 in the longitudinal direction. The configuration of each gas introduction member 16 is the same as that of Fig. 28 . The arrangement angles of the gas introduction members 16A, 16A and the gas introduction members 16B, 16B, -39 - 201215250, and the angles of arrangement of the gas introduction members 16A, 16A and the gas introduction members 16C, 16C are arbitrary, respectively. For example, the gas introduction members 16B and 16B and the gas introduction members 16C and 16C may be disposed at an angle of 45° with respect to the gas introduction members 16A and 16A. By arranging the gas introduction member 16 at a plurality of positions on the top wall lc of the processing container 1 to supply the gas, the reaction species or the reaction product can be equally distributed (integral enthalpy of rotation (revolution)) to each of the mounting regions. Further, between the wafers W of the plurality of SRK-mounted wafers, the processing between the wafers W can be uniformized, and the processing in the wafer W surface can be uniformized. In addition, the number of the gas introduction members 16 can be increased more than that of Fig. 29. Further, in the configuration example of Fig. 29, for example, the type of gas introduced through the gas introduction members 16A, 16A and the type of gas introduced through the gas introduction members 16B, 16B and the gas introduction members 16C, 16C can be changed. For example, the gas introduction members 16A and 16A are introduced into a gas which generates a short-lived active species or a gas which generates a reaction species which adversely affects the process once it is stored in the plasma, in addition to other gases. In this case, the residence time in the processing container 1 can be shortened, so that it is possible to efficiently use a gas which generates a short-lived active species, or to suppress the generation of a reaction species which adversely affects the process once it is stored in the plasma. Further, the types of gases introduced from the gas introduction members 16A, 16B, and 16C may be different types. Fig. 30 is a view showing another configuration example of the gas introduction portion and the exhaust portion. The example of Fig. 30 is a gas introduction member 16D having a curved bow shape as a gas introduction portion. Further, the exhaust port 11A also has a shape curved into a bow shape.

S -40- 201215250 此構成例是從設於處理容器1的一側上部的氣體導入構件 16D的位置來往之間夾著載置台3設於斜下方向的處理容 器1的一側下部的排氣口 11A形成大致一方向的氣流。 亦即,從氣體導入構件16D的氣孔16a往下方的載置台3 的一端側噴射的氣體一旦到達載置台3的表面,則如圖 30中箭號所示在與該表面平行的方向改變流向之後,從 載置台3的相反側的端再往下方改變方向而朝向排氣口 11A。其途中,氣體會被均等地分配於在旋轉的載置台3 的載置區域SR所載置的晶圓W的表面,藉此反應種或反 應生成物會均等地(旋轉(公轉)的積分値)分配於各載 置區域SR所載置的複數片的晶圓W間,可謀求晶圓W間 的處理均一化、及一片的晶圓w面內的處理均一化。 並且,若與在頂壁lc的中央附近配置氣體導入部15 的構成(例如圖26)作比較’則因爲圖30的構成是在處 理容器1內的晶圓W的表面附近形成有一方向的氣流, 所以具有對載置於載置區域SR公轉的晶圓W的內側(旋 轉中心側)或晶圓W的外側皆可均等地進行氣體的供給 之優點。另外,在圖30是沿著圓形的處理容器1的內面 (未圖示)來設置氣體導入構件16D及排氣口 11A。 以上,如例示般,電漿處理裝置的氣體導入部及 排氣部的構成可按照處理容器1的大小、微波導入單元 27的配置或透過板28的面積、載置區域SR(或晶圓W) 的片數、載置台3的旋轉速度、處理的內容等(例如氧化 、氮化、成膜、蝕刻等)來適當設定。而且’除了使晶圓 -41 - 201215250 W對複數的微波導入單元27相對移動外,還採用圖25〜 圖30所示那樣的氣體導入部及排氣部的構成,藉此可在 旋轉的載置台3的載置區域SR所載置的晶圓W的表面均 等地分配氣體。並且,藉由與上述氣體導入部及排氣部的 構成組合,以無論在晶圓W上的那個位置,電漿密度的 時間性累計値及/或電漿照射時間的累計値皆形成相同的 方式配置電漿源(透過板),可進行均一的處理。因此, 可謀求複數片的晶0 W間的處理均一化、及一片的晶圓 W面內的處理均一化。 其次,說明有關確認本發明的效果的實驗資料。首先 ,說明有關使用於贸驗的電漿處理裝置的構成。 [實驗1] 如圖31所示,使用一在頂壁lc直線地配設具有直徑 90mm的圆形微波透過區域的透過板28X,28Y,28Z之電 漿處理裝置。亦即’在各透過板28X,28Y,28Z的位置 分別設有微波導入單元。以下,將透過板2 8X記載爲「 第1電漿源28Xj ,將透過板28Y記載爲「第2電漿源 28Y」,將透過板28Z記載爲「第3電漿源28Z」。本實 驗是以第1電漿源28X的中心爲基準(零),分別將至 第2電漿源28Y的中心的距離、及至第3電漿源28Z的 中心的距離設定成175mm。並且,本實驗的目的是評價 處理的均一性,因此假想3 00 mm寬度的一片晶圓w作爲 被處理體來進行評價。S-40-201215250 This configuration example is an exhaust gas disposed at a lower portion of the processing container 1 which is disposed obliquely downward from the position of the gas introduction member 16D provided on the upper portion of the processing container 1 at a position therebetween. The port 11A forms a gas flow in a substantially one direction. In other words, when the gas ejected from the air vent 16a of the gas introduction member 16D to the one end side of the lower stage 3 reaches the surface of the mounting table 3, the flow direction is changed in a direction parallel to the surface as indicated by an arrow in FIG. The direction from the opposite side of the mounting table 3 is further downward and directed toward the exhaust port 11A. In the meantime, the gas is uniformly distributed to the surface of the wafer W placed on the mounting region SR of the rotating mounting table 3, whereby the reaction species or the reaction product are equal (rotation (revolution) integral 値The processing is performed between the wafers W of the plurality of sheets placed in the respective mounting regions SR, and the processing between the wafers W is uniformized, and the processing in the wafer w plane of one wafer is uniformized. Further, when the configuration in which the gas introduction portion 15 is disposed in the vicinity of the center of the top wall lc (for example, FIG. 26) is compared, the configuration of FIG. 30 is such that a flow in one direction is formed in the vicinity of the surface of the wafer W in the processing container 1. Therefore, there is an advantage that gas can be uniformly supplied to the inside (rotation center side) of the wafer W placed on the mounting area SR or the outside of the wafer W. Further, in Fig. 30, the gas introduction member 16D and the exhaust port 11A are provided along the inner surface (not shown) of the circular processing container 1. As described above, the gas introduction unit and the exhaust unit of the plasma processing apparatus can be configured according to the size of the processing container 1, the arrangement of the microwave introduction unit 27, the area of the transmission plate 28, and the placement area SR (or the wafer W). The number of sheets, the rotation speed of the mounting table 3, the contents of the processing, and the like (for example, oxidation, nitridation, film formation, etching, etc.) are appropriately set. Further, in addition to the relative movement of the wafer-41 - 201215250 W to the plurality of microwave introduction units 27, the gas introduction portion and the exhaust portion as shown in Figs. 25 to 30 are used, whereby the rotation can be performed. The surface of the wafer W placed on the mounting area SR of the stage 3 is uniformly distributed with gas. Further, by combining with the configuration of the gas introduction portion and the exhaust portion, the temporal accumulation of the plasma density and/or the accumulation of the plasma irradiation time are the same regardless of the position on the wafer W. The plasma source (transmission plate) is configured in a manner to perform uniform processing. Therefore, it is possible to uniformize the processing between the crystal wafers of the plurality of wafers and to uniformize the processing in the wafer W surface of one wafer. Next, experimental materials for confirming the effects of the present invention will be described. First, the configuration of the plasma processing apparatus used in the trade inspection will be described. [Experiment 1] As shown in Fig. 31, a plasma processing apparatus for transmitting the transmission plates 28X, 28Y, 28Z having a circular microwave transmission region having a diameter of 90 mm was linearly arranged on the top wall lc. That is, a microwave introduction unit is provided at each of the transmission plates 28X, 28Y, and 28Z. Hereinafter, the transmission plate 28X is described as "the first plasma source 28Xj, the transmission plate 28Y is referred to as the "second plasma source 28Y", and the transmission plate 28Z is referred to as the "third plasma source 28Z". This experiment is based on the center of the first plasma source 28X (zero), and the distance to the center of the second plasma source 28Y and the distance to the center of the third plasma source 28Z are set to 175 mm, respectively. Further, the purpose of this experiment was to evaluate the uniformity of the treatment, and therefore, a wafer w of a width of 300 mm was assumed to be evaluated as a processed object.

S -42- 201215250 以下記的條件來使電漿生成,在從頂板1C算起4 9mm 下方的位置測定電漿密度。 <電漿生成條件>S -42 - 201215250 The following conditions were used to generate plasma, and the plasma density was measured at a position below the 49 mm from the top plate 1C. <plasma generation condition>

Ar 氣體流量;l〇〇〇mL/min ( seem) N2 氣體流量;200mL/min ( seem ) 處理壓力;20Pa 載置台的溫度;室溫(2 5 °C ) 各微波功率;Ar gas flow rate; l〇〇〇mL/min (see) N2 gas flow rate; 200mL/min (see) treatment pressure; 20Pa stage temperature; room temperature (25 °C) microwave power;

第1電漿源28X...260W 第2電漿源28Y...260W 第3電漿源28Z...260W 圖32是重疊顯示使第1電漿源28X、第2電漿源 28Y、第3電漿源28Z的各個微波導入單元單獨運轉時的 電漿密度及使全部同時運轉時的電漿密度的圖表。圖32 的縱軸是表示電漿密度、橫軸是表示離成爲基準的第1電 漿源28X的中心的距離。另外,在圖32是以點線來表示 晶圓W的寬度(圖33〜圖35也是同樣)。 由圖32可知,在第1電漿源2 8X、第2電漿源28Y 、或第3電漿源28Z的各微波導入單元的單獨運轉下’電 漿密度是以各透過板的中心附近作爲頂點而呈山形。但’ 在使第1電漿源28X、第2電漿源28Y、第3電漿源28Z 的微波導入單元同時運轉時’可確認在晶圓W的寬度方 向的全域,大致形成一定(約1 xl〇11/cm3 )的電漿密度° -43- 201215250 並且,在圖32中,成爲「合成(計算)」的圖是計算上 合計第1電漿源2 8X、第2電漿源28Y、第3電漿源28Z 的單獨運轉的電漿密度者,與「合成(實測)」的結果幾 乎一致。 [實驗2] 圖33是表示與實驗例1同樣的條件,僅使第1電漿 源28X的微波導入單元的微波功率變化成l〇〇W,260W’ 或5 00W時的結果。圖表中的A’ B,C的符號是分別意 思第1電漿源28X的微波導入單元的微波功率爲100W, 260W,500W。另外,有關第1電漿源28X的微波導入單 元的微波功率爲260W時(B)是實驗例1的再揭示》 如圖33所示,藉由增減3個的其中的中央所配置的 第1電漿源28X的微波導入單元的微波功率,可確認電 漿密度在晶圓W的徑方向形成上凸(C; 500W )或下凸 (A ; 10 0W )變化。藉此,可確認在配設複數個的微波導 入單元時,藉由使各微波導入單元的微波功率變化,可控 制所被合成的電漿密度的強弱分布。 [實驗3] 對晶圓W的矽基板,以下記的條件來進行電賭氮化 處理,測定矽氮化膜的膜厚。另外,從頂板1 c到晶圓W 的距離(間隙)是設爲85mm。The first plasma source 28X...260W, the second plasma source 28Y...260W, the third plasma source 28Z...260W, Fig. 32 shows the first plasma source 28X and the second plasma source 28Y, A graph of the plasma density at the time of operation of each of the microwave introduction units of the third plasma source 28Z and the plasma density at the time of simultaneous operation. The vertical axis of Fig. 32 indicates the plasma density, and the horizontal axis indicates the distance from the center of the first plasma source 28X which serves as a reference. Further, in Fig. 32, the width of the wafer W is indicated by a dotted line (the same applies to Figs. 33 to 35). As can be seen from Fig. 32, in the individual operation of the microwave introduction units of the first plasma source 28X, the second plasma source 28Y, or the third plasma source 28Z, the 'plasma density is taken as the vicinity of the center of each of the transmission plates. The apex is in the shape of a mountain. However, when the microwave introduction unit of the first plasma source 28X, the second plasma source 28Y, and the third plasma source 28Z are simultaneously operated, it is confirmed that the entire area in the width direction of the wafer W is substantially constant (about 1). The plasma density of xl〇11/cm3) is -43-201215250. In Fig. 32, the "synthesis (calculation)" is the calculation of the total of the first plasma source 28X and the second plasma source 28Y. The plasma density of the single plasma source 28Z operating alone is almost identical to the result of "synthesis (measured)". [Experiment 2] Fig. 33 shows the results of the same conditions as in Experimental Example 1, except that the microwave power of the microwave introduction unit of the first plasma source 28X was changed to l 〇〇 W, 260 W' or 500 W. The symbols of A' B and C in the graph are microwave powers of 100 W, 260 W, and 500 W, respectively, of the microwave introduction unit of the first plasma source 28X. In addition, when the microwave power of the microwave introduction unit of the first plasma source 28X is 260 W (B) is a re-disclosure of Experimental Example 1 as shown in FIG. 33, the third portion of the three is added or subtracted. 1 The microwave power of the microwave introduction unit of the plasma source 28X confirms that the plasma density changes in the radial direction of the wafer W by a convex (C; 500 W) or a downward convex (A; 100 W). Thereby, it can be confirmed that when a plurality of microwave introducing units are disposed, the intensity distribution of the plasma density to be synthesized can be controlled by changing the microwave power of each microwave introducing unit. [Experiment 3] The ruthenium substrate of the wafer W was subjected to a gambling nitriding treatment under the following conditions, and the film thickness of the ruthenium nitride film was measured. Further, the distance (gap) from the top plate 1 c to the wafer W was set to 85 mm.

S -44 - 201215250 <電漿氮化處理條件>S -44 - 201215250 <plasma nitriding treatment conditions>

Ar 氣體流量;1000mL/min(sccm) N2 氣體流量;200mL/min ( seem)Ar gas flow rate; 1000 mL/min (sccm) N2 gas flow rate; 200 mL/min (see)

處理壓力;20Pa 載置台的溫度;500 °C 微波功率;僅使第1電漿源28X的微波導入單元的 微波功率變化成l〇〇W,260W,或500W。 各電漿源的功率構成如以下所述般。 A ; 28Y,28X,28Z = 260W > 100W,260W B ; 28Y,28X,28Z = 260W,260W « 260W C ; 28Y , 28X , 28Z=260W , 500W , 260W 處理時間;9 0秒 將結果顯示於圖34。圖34的縱軸是表示矽氮化膜的 光學膜厚(折射率2.0),橫軸是表示離成爲基準的第1 電漿源28X的中心的距離。並且,圖34的圖表中的A, B,C的意思是與圖33同樣。由圖34將3個微波導入單 元的微波功率設定成相同時(B),在晶圓W的徑方向均 等地形成矽氮化膜。並且,藉由增減3個的其中的中央所 配置的第1電漿源28X的微波導入單元的微波功率,可 確認矽氮化膜的面內膜厚在晶圓W的徑方向變化成上凸 (C;500W)或下凸(A;100W)。由圖34可確認,與 圖33大致同樣的傾向。亦即,可確認圖33的電漿密度的 計測結果與圖3 4的矽氮化膜的膜厚的計測結果是對應著 -45- 201215250 並且,面內均一性的指標之Range/2AVE[亦即(氮化 膜厚的最大値-氮化膜厚的最小値)/氮化膜厚的平均値 X 2 ]是圖3 4的A爲4.2 %、B爲1. 3 %、C爲1.9 % »由以上 的結果可確認,在配設複數個的微波導入單元時,藉由使 各微波導入單元的微波功率變化,可在晶圓W的面內控 制矽氮化膜的膜厚。 [實驗4] 除了使各電漿源28X、28Y及28Z的微波導入單元的 微波功率一樣變化以外,其餘則與實驗3同樣,對作爲晶 圓W的矽基板進行電漿氮化處理。 <電漿氮化處理條件> 各電漿源的功率構成如以下所示般。 D ; 28Y,28X,28Z=100W > 100W,100W E ; 28Y > 28X,28Z = 260W,260W,260W F ; 28Y,28X,28Z = 400W,400W,400W 其他的條件則與實驗3同樣。 將結果顯示於圖35。圖35的縱軸是表示矽氮化膜的 光學膜厚(折射率2.0),橫軸是表示離成爲基準的第1 電漿源2 8X的中心的距離。並且,圖35的圖表中的D’ E,F是意指上述電漿氮化條件。由圖35將3個微波導入 單元的微波功率設定成相同時,可確認依功率的大小’晶 圓W的矽氮化膜的面內膜厚的分布是大致平行移動。而Processing pressure; temperature of 20 Pa mounting table; microwave power of 500 ° C; only the microwave power of the microwave introducing unit of the first plasma source 28X is changed to l 〇〇 W, 260 W, or 500 W. The power configuration of each plasma source is as follows. A; 28Y, 28X, 28Z = 260W > 100W, 260W B; 28Y, 28X, 28Z = 260W, 260W « 260W C ; 28Y , 28X , 28Z=260W , 500W , 260W processing time ; Figure 34. The vertical axis of Fig. 34 indicates the optical film thickness (refractive index 2.0) of the tantalum nitride film, and the horizontal axis indicates the distance from the center of the first plasma source 28X which serves as a reference. Further, the meanings of A, B, and C in the graph of Fig. 34 are the same as those of Fig. 33. When the microwave powers of the three microwave introducing units are set to be the same as in Fig. 34 (B), a tantalum nitride film is uniformly formed in the radial direction of the wafer W. In addition, by increasing or decreasing the microwave power of the microwave introduction unit of the first plasma source 28X disposed at the center of the three, it is confirmed that the in-plane thickness of the tantalum nitride film changes in the radial direction of the wafer W. Convex (C; 500W) or convex (A; 100W). As can be seen from Fig. 34, the same tendency as in Fig. 33 was observed. That is, it can be confirmed that the measurement result of the plasma density of FIG. 33 and the measurement result of the film thickness of the tantalum nitride film of FIG. 34 correspond to -45 to 201215250, and Range/2AVE of the index of in-plane uniformity is also That is, (the minimum 氮化 of the nitride film thickness, the minimum 値 of the nitride film thickness) / the average 値X 2 of the nitride film thickness] is 4.2% of A in Fig. 34, 1.3% in B, and 1.9% in C. From the above results, it was confirmed that when a plurality of microwave introducing units are disposed, the film thickness of the tantalum nitride film can be controlled in the plane of the wafer W by changing the microwave power of each microwave introducing unit. [Experiment 4] The ruthenium substrate as the wafer W was subjected to plasma nitriding treatment in the same manner as in Experiment 3 except that the microwave power of the microwave introduction units of the respective plasma sources 28X, 28Y, and 28Z was changed. <plasma nitriding treatment conditions> The power configuration of each plasma source is as follows. D; 28Y, 28X, 28Z=100W > 100W, 100W E; 28Y > 28X, 28Z = 260W, 260W, 260W F; 28Y, 28X, 28Z = 400W, 400W, 400W Other conditions are the same as in Experiment 3. The results are shown in Figure 35. The vertical axis of Fig. 35 indicates the optical film thickness (refractive index 2.0) of the tantalum nitride film, and the horizontal axis indicates the distance from the center of the first plasma source 28X which is the reference. Further, D' E, F in the graph of Fig. 35 means the above-described plasma nitriding conditions. When the microwave powers of the three microwave introduction units were set to be the same as shown in Fig. 35, it was confirmed that the distribution of the in-plane thickness of the tantalum nitride film of the wafer W according to the size of the power was substantially parallel. and

S -46 - 201215250 且,矽氮化膜之晶圓 w的面內均一性的指標之 Range/2AVE[亦即(氮化膜厚的最大値·氮化膜厚的最小値 )/氮化膜厚的平均値x2]是圖35的D爲1.06°/。,E爲 1.2 6 %,F爲0 · 8 5 %,皆爲良好的値。 由以上的實驗結果可確認,藉由以預定的間隔來配置 複數的透過板(微波導入單元)’電漿密度的控制容易, 可使電漿密度均一化。並且,爲了避免在晶圓W的端部 的電漿密度的時間性累計値要比其他部位(例如晶圓W 的中央附近)還下降,而在與晶圓W的相對移動方向正 交的方向等間隔配置複數(例如3個以上)同大小的電漿 源(透過板的微波透過區域),使最外側的2個透過板的 微波透過區域的中心間的距離Μ與晶圓W的直徑D相同 或更廣(Μ 2 D )。藉由此構成,可確認至少在晶圓W的 徑方向可進行均質的處理(例如電漿氮化處理)。該等的 實驗結果是與模擬電漿密度的時間性累計値的重疊的結果 (圖9〜圖14)皆符合。另外,上述實驗結果是假想一片 的晶圓W作爲被處理體時的結果,但可易理解即使令複 數的小基板配置於載置台3旋轉時,照樣可取得同等或更 佳的均一性。 [對ALD法的適用例] 作爲半導體製造製程的成膜手法,例如有被稱爲 ALD ( Atomic Layer Deposition )或 MLD ( Molecular Layer Deposition)等的方法(在此是總稱「aLD法」) -47- 201215250 爲人所知。ALD法是在基板的表面於真空環境下使第1 反應氣體吸附後,將所供給的氣體切換成第2反應氣體, 藉由兩氣體的反應來形成1層或複數層的原子層或分子層 。藉由多次進行此循環,將該等的層予以層疊,而進行往 基板上的成膜。ALD法是可按照循環數來高精度地控制 膜厚,且膜質的面內均一性亦佳,爲可對應於半導體裝置 的薄膜化的有效手法。 圖36是槪念性顯示將本發明的電漿處理裝置適用於 上述ALD法時的構成。成膜裝置200是具備:平面形狀 大槪爲圓形的扁平真空容器201、及設於此真空容器201 內,在該真空容器201的中心具有旋轉中心的載置台202 。載置台202是在中心部固定於圓筒形狀的芯部203,此 芯部203是被固定在延伸於鉛直方向的轉軸(未圖示)。 載置台202及芯部203是可繞著鉛直軸(此例是順時針方 向)旋轉。 在載置台202的表面是沿著旋轉方向(周方向)在複 數處例如5處設有用以載置晶圓W的圓形狀的載置區域 Sr作爲凹部。另外,基於方便起見,在圖36是只在1個 的載置區域SR描繪晶圓W。載置區域SR是其直徑比晶圓 W的直徑稍微大,且其深度是設定成與晶圓W的厚度同 等大小。在載置區域SR的底’用以支撐晶圓W的背面來 使該晶圓W昇降的昇降銷(未圖示)是配備於貫通孔內 〇 真空容器201的內部是被區分成第1區域Rl、第2S -46 - 201215250 Also, Range/2AVE of the in-plane uniformity of the wafer w of the tantalum nitride film [that is, the minimum 氮化 of the nitride film thickness and the minimum thickness of the nitride film) / nitride film The thick average 値x2] is D of Fig. 35 being 1.06°/. , E is 1.2 6 %, F is 0 · 8 5 %, all are good defects. From the above experimental results, it was confirmed that it is easy to control the plasma density by arranging a plurality of transparent plates (microwave introduction means) at predetermined intervals, and the plasma density can be made uniform. Further, in order to prevent the temporal accumulation of the plasma density at the end portion of the wafer W from being lower than the other portions (for example, near the center of the wafer W), the direction orthogonal to the relative movement direction of the wafer W is orthogonal. A plurality of (for example, three or more) plasma sources of the same size (the microwave transmission region of the transmission plate) are disposed at equal intervals, so that the distance 中心 between the centers of the microwave transmission regions of the outermost two transmission plates is the diameter D of the wafer W. Same or wider (Μ 2 D ). With this configuration, it is confirmed that a homogeneous process (e.g., plasma nitridation treatment) can be performed at least in the radial direction of the wafer W. The results of these experiments are consistent with the results of the overlap of the temporal accumulations of simulated plasma densities (Figs. 9 to 14). Further, as a result of the above experiment, the wafer W of a virtual one is a result of the object to be processed. However, it can be easily understood that even when a plurality of small substrates are placed on the mounting table 3 for rotation, the same or better uniformity can be obtained. [Application to the ALD method] As a film formation method for a semiconductor manufacturing process, for example, a method called ALD (Atomic Layer Deposition) or MLD (Molecular Layer Deposition) (herein, collectively referred to as "aLD method") -47 - 201215250 is known. In the ALD method, after the first reaction gas is adsorbed on the surface of the substrate in a vacuum environment, the supplied gas is switched to the second reaction gas, and the atomic layer or the molecular layer of one or more layers is formed by the reaction of the two gases. . By repeating this cycle a plurality of times, the layers are laminated to form a film on the substrate. In the ALD method, the film thickness can be controlled with high precision in accordance with the number of cycles, and the in-plane uniformity of the film quality is also excellent, which is an effective method for thinning the semiconductor device. Fig. 36 is a view showing a configuration in which the plasma processing apparatus of the present invention is applied to the above ALD method. The film forming apparatus 200 is a flat vacuum container 201 having a flat shape and a large circular shape, and a mounting table 202 provided in the vacuum container 201 and having a center of rotation at the center of the vacuum container 201. The mounting table 202 is fixed to the cylindrical core portion 203 at the center portion, and the core portion 203 is fixed to a rotating shaft (not shown) extending in the vertical direction. The stage 202 and the core 203 are rotatable about a vertical axis (in this case, a clockwise direction). On the surface of the mounting table 202, a circular mounting region Sr for placing the wafer W is provided as a concave portion at a plurality of, for example, five locations along the rotation direction (circumferential direction). Further, for the sake of convenience, in Fig. 36, the wafer W is drawn in only one of the mounting regions SR. The mounting area SR has a diameter slightly larger than the diameter of the wafer W, and its depth is set to be equal to the thickness of the wafer W. A lift pin (not shown) for supporting the back surface of the wafer W to support the wafer W at the bottom of the mounting region SR is provided in the through hole. The inside of the vacuum container 201 is divided into the first region. Rl, 2nd

S -48- 201215250 區域R2、第3區域R3及第4區域R4。第1〜第4區 R1〜R4是從載置台202的旋轉方向的上游側往下游側 第1區域R1、第2區域R2、第3區域R3、第4區域 的順序配置。在圖36是以線(符號BR)來表示各區域 境界部分,但各區域的境界亦可具有一定的寬度(面積 來形成。該等第1〜第4區域R1〜R4是以境界部分Br 分離,而使能夠一邊令載置台202旋轉,一邊實質地遮 各區域的環境。作爲分別分離第1〜第4區域R1〜R4 手段,雖詳細省略,但例如可組合採用以氣簾的原理來 第1〜第4區域R1〜R4的各區域的境界部分BR導入分 氣體,或狹隘地形成真空容器201的頂面(未圖示)與 置台202的上面之間隔等的構成。並且,亦可在第1〜 4區域R1〜R4分別設置連接至真空泵的排氣口。 圖36所示的成膜裝置200是在第1區域R1中,在 載置台202的載置區域SR的通過區域對向的位置設有 1反應氣體噴嘴205A。第1反應氣體噴嘴205A是被連 至第1反應氣體的DCS (二氯矽烷)氣體的氣體供給源 未圖示)。 在第3區域R3是配備有複數(例如4個)的微波 入單元。在圖36是依透過板28的位置來顯示微波導入 元的位置。並且’在第3區域R3中’在與載置台202 載置區域Sr的通過區域對向的位置設有第2反應氣體 嘴20 5B。第2反應氣體噴嘴205B是被連接至第2反應 體的NH3氣體的氣體供給源(未圖示)° 域 依 R4 的 ) 來 斷 的 對 離 載 第 與 第 接 導 單 的 噴 氣 -49- 201215250 在第1反應氣體噴嘴205A及第2反應氣體噴嘴205B 中,分別用以朝下方側吐出反應氣體的氣體吐出孔206會 在噴嘴的長度方向取間隔配列。第1區域R1是用以使 DCS氣體吸附於晶圓W的處理區域,第3區域R3是用以 使被活化的NH3氣體吸附於晶圓W的處理區域。該等第 1反應氣體噴嘴205 A及第2反應氣體噴嘴205B是例如安 裝於真空容器201的側周壁》 並且,在第2區域R2及第4區域R4分別配備有例 如導入N2氣體等的淨化氣體之淨化氣體噴嘴207 A,20 7B 。該等的淨化氣體噴嘴207A,207B是分別被連接至N2 氣體供給源(未圖示)。淨化氣體噴嘴207A,207B是例 如安裝於真空容器201的側周壁。 圖示雖省略,但實際在真空容器201的底壁設有複數 的排氣口,各排氣口是經由排氣管來連接至真空泵等的排 氣裝置。並且,在載置台202與真空容器201的底壁之間 設有未圖示的加熱器等加熱手段,可經由載置台202來將 晶圓W加熱至預定的溫度。 更在真空容器201的側壁形成有搬送口 208,其係用 以在未圖示的搬送裝置與載置台202之間進行基板亦即晶 圓W的交接,此搬送口 208可藉由未圖示的閘閥來開閉 。載置台202的載置區域SR是在面對此搬送口 208的位 置在與未圖示的搬送裝置之間進行晶圓W的交接。 在成膜裝置200是如以下那樣進行矽氮化膜的形成。 首先,打開未圖示的閘閥,藉由未圖示的外部搬送裝置經S -48- 201215250 Zone R2, Zone 3 R3 and Zone 4 R4. The first to fourth regions R1 to R4 are arranged in order from the upstream side to the downstream side in the rotation direction of the mounting table 202 in the first region R1, the second region R2, the third region R3, and the fourth region. In Fig. 36, the boundary portion of each region is indicated by a line (symbol BR), but the boundary of each region may also have a certain width (area formed). The first to fourth regions R1 to R4 are separated by the boundary portion Br. In addition, it is possible to substantially obstruct the environment of each area while rotating the mounting table 202. The means for separating the first to fourth regions R1 to R4, respectively, are omitted in detail, but for example, the first principle can be used in combination with the principle of an air curtain. The boundary portion BR of each of the fourth regions R1 to R4 is introduced into the gas, or the gap between the top surface (not shown) of the vacuum container 201 and the upper surface of the table 202 is formed in a narrow manner. Each of the 1 to 4 regions R1 to R4 is provided with an exhaust port connected to the vacuum pump. The film forming apparatus 200 shown in Fig. 36 is a position facing the passing region of the mounting region SR of the mounting table 202 in the first region R1. A reaction gas nozzle 205A is provided. The first reaction gas nozzle 205A is a gas supply source of DCS (chlorinated gas) gas connected to the first reaction gas (not shown). In the third region R3, a plurality of (for example, four) microwave input units are provided. In Fig. 36, the position of the microwave introducing element is displayed in accordance with the position of the transmitting plate 28. Further, in the third region R3, the second reaction gas nozzle 20 5B is provided at a position opposed to the passage region of the mounting table 202 in the mounting region Sr. The second reaction gas nozzle 205B is a gas supply source (not shown) connected to the NH3 gas of the second reaction body, and the gas flow source (not shown) is disconnected from the first and the first guide. -49-201215250 In the first reaction gas nozzle 205A and the second reaction gas nozzle 205B, the gas discharge holes 206 for discharging the reaction gas toward the lower side are arranged in the longitudinal direction of the nozzle. The first region R1 is a processing region for adsorbing DCS gas on the wafer W, and the third region R3 is a processing region for adsorbing the activated NH 3 gas on the wafer W. For example, the first reaction gas nozzle 205 A and the second reaction gas nozzle 205B are attached to the side wall of the vacuum container 201, and the second region R2 and the fourth region R4 are respectively provided with a purge gas such as N 2 gas. The purge gas nozzles 207 A, 20 7B. The purge gas nozzles 207A, 207B are respectively connected to an N2 gas supply source (not shown). The purge gas nozzles 207A, 207B are, for example, side peripheral walls mounted to the vacuum vessel 201. Although not shown in the drawings, a plurality of exhaust ports are actually provided in the bottom wall of the vacuum container 201, and each of the exhaust ports is connected to an exhaust device such as a vacuum pump via an exhaust pipe. Further, a heating means such as a heater (not shown) is provided between the mounting table 202 and the bottom wall of the vacuum container 201, and the wafer W can be heated to a predetermined temperature via the mounting table 202. Further, a transfer port 208 is formed in the side wall of the vacuum container 201 for transferring the wafer W, which is a substrate between the transfer device (not shown) and the mounting table 202. The transfer port 208 can be omitted from the drawing. The gate valve is opened and closed. The mounting area SR of the mounting table 202 is to transfer the wafer W between the transfer port 208 and the transfer device (not shown). In the film forming apparatus 200, the formation of a tantalum nitride film is performed as follows. First, a gate valve (not shown) is opened, and an external transfer device (not shown) is used.

S -50- 201215250 由搬送口 208來將晶圓W交接至例如被加熱至200〜 400°C的載置台202的載置區域SR內。此交接是在載置區 域SR停止於面對搬送口 208的位置時藉由未圖示的昇降 銷來進行,該昇降銷是經由載置區域SR的底面的貫通孔 來從真空容器201的底部側昇降。使載置台202間歇性地 旋轉來進行如此的晶圓W的交接,在載置台2 02的5個 載置區域SR內分別載置晶圓W。接著關閉閘閥,藉由未 圖示的排氣裝置來將真空容器201內抽真空至預定的壓力 ’且一邊使載置台202順時針旋轉,一邊藉由未圖示的加 熱器單元來加熱晶圓W。然後,從第1反應氣體噴嘴205 及第2反應氣體噴嘴205B來分別使DCS氣體及NH3氣體 吐出,且從淨化氣體噴嘴207A,207B吐出淨化氣體的N2 氣體。 晶圓W是藉由載置台202的旋轉,交替通過設有第1 反應氣體噴嘴205A的第1區域R1及電漿生成部的第3 區域R3 ’因此DCS氣體會吸附,其次活化後NH3氣體會 吸附’該等的氣體分子會反應而形成1層或複數層氮化矽 的分子層。如此一來’氮化矽的分子層會被依序層疊而形 成預定膜厚的矽氮化膜(SiN膜)。第1區域R1的DCs 氣體、第3區域R3的NH3氣體是由設於各個區域的排氣 口(未圖示)來排氣。並且,藉由載置台202的旋轉,在 第2區域R2’可對從第1區域R1送出的晶圓w進行淨 化’在第4區域R4,可對從第3區域R3送出的晶圓W 進行淨化。另外’亦可將第2區域R2及第4區域R4作 -51 - 201215250 爲用以分離第1區域R1與第3區域R3的分離區域利用 ,此情況,亦可由具有複數個氣孔的長噴嘴來線狀地放出 N2氣體。藉此,第1區域R1的環境與第3區域R3的環 境會被完全地分離,可進行DCS氣體與NH3氣體不會互 相混合的處理。 本實施形態的成膜裝置200是以上那樣在載置台202 的旋轉方向配置複數的晶圓W,使載置台2 02旋轉,依序 通過第1區域R1及第3區域R3,進行所謂的ALD (或 MLD)。在第3區域R3因爲配置複數的電漿源Γ透過板 28 )來使產生NH3氣體的電漿,所以可進行均一的處理 ,使無論在晶圓W上的那個位置,電漿密度的時間性累 計値及/或電漿照射時間的累計値皆形成相同。因此可謀 求複數片的晶圓W間的處理均一化、及一片的晶圓W面 內的處理均一化。 ALD法是適於使例如利用於閘絕緣膜的高介電質膜 ,例如矽氮化膜(SiN膜)或矽氧化膜(Si02膜)等在低 溫下形成極薄膜的目的。以上的說明是舉矽氮化膜的成膜 例爲例,但例如可使用DCS氣體作爲第1反應氣體’使 用氧氣體或臭氧氣體作爲第2反應氣體,藉此進行矽氧化 膜的成膜。 又,其他的適用例,例如亦可使用TiCl4氣體作爲第 1反應氣體,使用NH3氣體作爲第2反應氣體’在低溫下 極薄地形成TiN膜。並且,成膜裝置200的區域的區分並 非限於4個。例如,亦可在第1區域形成Si膜’在第3S - 50 - 201215250 The wafer W is transferred from the transfer port 208 to, for example, the mounting area SR of the mounting table 202 heated to 200 to 400 °C. This transfer is performed by a lift pin (not shown) when the placement area SR is stopped at the position facing the transfer port 208, and the lift pin is passed from the bottom of the vacuum container 201 through the through hole of the bottom surface of the mounting area SR. Side lift. The wafers W are placed in the five mounting regions SR of the mounting table 208 by intermittently rotating the mounting table 202 to carry out the transfer of the wafers W. Then, the gate valve is closed, and the vacuum chamber 201 is evacuated to a predetermined pressure by an exhaust device (not shown), and while the mounting table 202 is rotated clockwise, the wafer is heated by a heater unit (not shown). W. Then, the DCS gas and the NH3 gas are discharged from the first reaction gas nozzle 205 and the second reaction gas nozzle 205B, respectively, and the N2 gas of the purge gas is discharged from the purge gas nozzles 207A and 207B. The wafer W is alternately passed through the first region R1 in which the first reaction gas nozzle 205A and the third region R3 of the plasma generating portion are provided by the rotation of the mounting table 202. Therefore, the DCS gas is adsorbed, and the NH3 gas is activated after the second activation. The adsorbed 'the gas molecules react to form a molecular layer of one or more layers of tantalum nitride. As a result, the molecular layer of tantalum nitride is sequentially laminated to form a tantalum nitride film (SiN film) having a predetermined film thickness. The DCs gas in the first region R1 and the NH3 gas in the third region R3 are exhausted by an exhaust port (not shown) provided in each region. Further, the wafer w sent from the first region R1 can be cleaned in the second region R2' by the rotation of the mounting table 202. In the fourth region R4, the wafer W sent from the third region R3 can be processed. Purification. Further, the second region R2 and the fourth region R4 may be -51 - 201215250, which are used for separating the separation regions of the first region R1 and the third region R3. In this case, the long nozzles having a plurality of pores may be used. N2 gas is released linearly. Thereby, the environment of the first region R1 and the environment of the third region R3 are completely separated, and the process in which the DCS gas and the NH3 gas are not mixed with each other can be performed. In the film forming apparatus 200 of the present embodiment, a plurality of wafers W are arranged in the rotation direction of the mounting table 202, and the mounting table 222 is rotated to sequentially pass the first region R1 and the third region R3 to perform so-called ALD ( Or MLD). In the third region R3, since a plurality of plasma sources are disposed through the plate 28) to generate plasma of NH3 gas, uniform processing can be performed to make the plasma density temporal in any position on the wafer W. The cumulative enthalpy of cumulative enthalpy and/or plasma irradiation time is the same. Therefore, it is possible to uniformize the processing between the wafers W of a plurality of sheets and to uniformize the processing in the wafer W in one sheet. The ALD method is suitable for forming a thin film at a low temperature, for example, a high dielectric film used for a gate insulating film, for example, a tantalum nitride film (SiN film) or a tantalum oxide film (SiO 2 film). In the above description, a film formation example of the nitride film is exemplified. For example, a DCS gas can be used as the first reaction gas, and an oxygen gas or an ozone gas can be used as the second reaction gas to form a film of the tantalum oxide film. Further, as another application example, for example, TiCl4 gas may be used as the first reaction gas, and NH3 gas may be used as the second reaction gas. The TiN film may be formed extremely thin at a low temperature. Further, the distinction between the regions of the film forming apparatus 200 is not limited to four. For example, a Si film may be formed in the first region.

S -52- 201215250 區域進行氧化(氮化)處理,更在第5區域對矽氧化膜( 矽氮化膜)進行電漿改質處理。此情況,可在第3區域及 第5區域的其中任一方或雙方配置複數的電漿源(透過板 28 )來進行處理。 以上敘述本發明的實施形態,但本發明並非限於上述 實施形態,亦可爲各種的變形。例如,本發明的電漿處理 裝置是除了電漿氮化處理裝置以外,還可適用於例如電漿 氧化處理裝置或電漿CVD處理裝置、電漿蝕刻處理裝置 、電漿灰化處理裝置等。而且,本發明的電漿處理裝置 100並非限於作爲被處理體的基板爲半導體晶圓時,亦可 適用於例如以太陽電池面板的基板或平板顯示器用基板作 爲被處理體的電漿處理裝置。 並且,在上述實施形態是由複數的微波產生裝置來個 別地往複數的微波導入單元供給微波的構成,但亦可構成 從單一的微波產生裝置,利用分岐的導波管來往2個以上 的微波導入單元供給微波。而且,在上述實施形態是利用 微波電漿處理裝置,但亦可適用於使用高頻作爲電磁波的 電漿處理裝置。而且,亦可例如使用ICP電漿方式、ECR 電漿方式、表面波電漿方式、磁控管電漿方式等的其他方 式作爲電漿的生成方式之電漿處理裝置。又,非限於真空 處理,亦可利用大氣壓電漿。 本國際申請案是根據2010年3月31日申請的日本國 專利申請案20 1 0-8 1 987號來主張優先權者,將申請案的 全內容援用於此》 -53- 201215250 【圖式簡單說明】 圖1是表示本發明之一實施形態的電漿處理裝置的構 成例的槪略剖面圖。 圖2A是表示載置台的外觀構成的立體圖。 圖2B是表示別例的載置台的外觀構成的立體圖。 圖3是微波供給部的槪略構成圖。 圖4A是平面天線之一例的平面圖。 圖4B是平面天線的別例的平面圖。 圖4C是平面天線的另外別例的平面圖。 圖5是表示微波導入單元的配設例的頂壁的底面圖。 圖6是說明微波導入單元與載置台的載置區域的位置 關係的圖面。 圖7是表示控制部的構成例的圖面。 圖8A是說明本發明之一實施形態的電漿處理裝置的 電漿處理的原理的圖面。 圖8B是說明本發明之一實施形態的電漿處理裝置的 電漿處理的原理的圖面。 圖9是表示微波導入單元的配置與電子密度的關係的 模擬結果的圖表。 圖10是表示微波導入單元的配置與電子密度的關係 的模擬結果的圖表* 圖11是表示微波導入單元的配置與電子密度的關係 的模擬結果的圖表。 圖12是表示微波導入單元的配置與電子密度的關係The S-52-201215250 area is subjected to oxidation (nitridation) treatment, and the ruthenium oxide film (矽 nitride film) is subjected to plasma modification treatment in the fifth region. In this case, a plurality of plasma sources (transmission plates 28) may be disposed in either or both of the third region and the fifth region for processing. The embodiment of the present invention has been described above, but the present invention is not limited to the above embodiment, and various modifications are possible. For example, the plasma processing apparatus of the present invention can be applied to, for example, a plasma oxidation treatment apparatus or a plasma CVD treatment apparatus, a plasma etching treatment apparatus, a plasma ashing treatment apparatus, and the like in addition to the plasma nitriding treatment apparatus. Further, the plasma processing apparatus 100 of the present invention is not limited to the case where the substrate to be processed is a semiconductor wafer, and may be applied to, for example, a substrate for a solar cell panel or a substrate for a flat panel display as a workpiece to be processed. Further, in the above-described embodiment, the microwave introducing means for individually reciprocating the plurality of microwave generating means supplies microwaves. However, it is also possible to configure two or more microwaves from the single microwave generating means by using the branched waveguide. The introduction unit supplies microwaves. Further, in the above embodiment, the microwave plasma processing apparatus is used, but it is also applicable to a plasma processing apparatus using high frequency as electromagnetic waves. Further, for example, a plasma processing apparatus in which a plasma is produced may be used in another manner such as an ICP plasma method, an ECR plasma method, a surface wave plasma method, or a magnetron plasma method. Further, it is not limited to vacuum processing, and atmospheric piezoelectric slurry can also be used. This international application is based on the Japanese Patent Application No. 20 1 0-8 1 987 filed on March 31, 2010. The full content of the application is used for this. -53- 201215250 Brief Description of the Drawings Fig. 1 is a schematic cross-sectional view showing a configuration example of a plasma processing apparatus according to an embodiment of the present invention. Fig. 2A is a perspective view showing an external configuration of a mounting table. 2B is a perspective view showing an external configuration of a mounting table of another example. Fig. 3 is a schematic block diagram of a microwave supply unit. 4A is a plan view showing an example of a planar antenna. 4B is a plan view of another example of a planar antenna. 4C is a plan view of another alternative of the planar antenna. Fig. 5 is a bottom plan view showing a top wall of an example of arrangement of the microwave introduction unit. Fig. 6 is a view for explaining the positional relationship between the microwave introduction unit and the mounting area of the mounting table. FIG. 7 is a view showing a configuration example of a control unit. Fig. 8A is a view showing the principle of plasma treatment of a plasma processing apparatus according to an embodiment of the present invention. Fig. 8B is a view for explaining the principle of plasma treatment of the plasma processing apparatus according to the embodiment of the present invention. Fig. 9 is a graph showing simulation results of the relationship between the arrangement of the microwave introduction unit and the electron density. Fig. 10 is a graph showing simulation results of the relationship between the arrangement of the microwave introduction unit and the electron density. Fig. 11 is a graph showing the results of simulation of the relationship between the arrangement of the microwave introduction unit and the electron density. Figure 12 is a diagram showing the relationship between the arrangement of the microwave introduction unit and the electron density.

S -54- 201215250 的模擬結果的圖表。 圖13是表示微波導入單元的配置與電子密度的關谭 的模擬結果的圖表。 圖14是表示微波導入單元的配置與電子密度的關係 的模擬結果的圖表。 圖15是說明微波導入單元的配設例的圖面。 圖16是說明微波導入單元的別的配設例的圖面。 圖17是說明微波導入單元的別的配設例的圖面。 圖18是說明微波導入單元的別的配設例的圖面。 圖19是說明微波導入單元的別的配設例的圖面。 圖20是說明微波導入單元的別的配設例的圖面。 圖21是說明微波導入單元的別的配設例的圖面。 圖22是說明微波導入單元的別的配設例的圖面。 圖23是說明微波導入單元的別的配設例的圖面。 圖24是說明微波導入單元的別的配設例的圖面。 圖25是說明處理容器內的氣流的圖面。 圖26是表示氣體導入部的配設例的圖面。 圖27是表示氣體導入部的別的配設例的圖面。 圖28是表示氣體導入部的另外別的配設例及處理容 器內的氣流的圖面。 圖29是表示氣體導入部的另外別的配設例的圖面。 圖30是表示氣體導入部的另外別的配設例及處理容 器內的氣流的圖面。 圖31是說明使用於實驗的電漿處理裝置的透過板( -55- 201215250 微波導入單元)的配置的圖面。 .圖32是表示實驗1的電漿密度的測定結果的圖表. 圖33是表示實驗2的電漿密度的測定結果的圖表。 圖34是表示實驗3的矽氮化膜的膜厚的測定結果的 圖表。 圖35是表示實驗4的矽氮化膜的膜厚的測定結果的 圖表。 圖36是說明可適用本發明的ALD成膜裝置的槪要圖 面。 【主要元件符號說明】 1 :處理容器 2 :支撐裝置 3 :載置台 4 :支撐部 1 1 :排氣口 15 :氣體導入部 1 8 :氣體供給裝置 24 :排氣裝置 27 :微波導入單元 2 8 :透過板 3 7 :導波管 39 :微波產生裝置 5 〇 :控制部A graph of the simulation results for S-54- 201215250. Fig. 13 is a graph showing the results of simulation of the arrangement of the microwave introduction unit and the electron density. Fig. 14 is a graph showing simulation results of the relationship between the arrangement of the microwave introduction unit and the electron density. Fig. 15 is a view for explaining an example of arrangement of a microwave introducing unit. Fig. 16 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 17 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 18 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 19 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 20 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 21 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 22 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 23 is a view for explaining another example of arrangement of the microwave introducing unit. Fig. 24 is a view for explaining another example of arrangement of the microwave introducing unit. Figure 25 is a diagram illustrating the flow of air in the processing vessel. FIG. 26 is a view showing an arrangement example of the gas introduction portion. Fig. 27 is a view showing another example of arrangement of the gas introduction portion. Fig. 28 is a view showing another arrangement example of the gas introduction portion and an air flow in the processing container. Fig. 29 is a view showing another example of arrangement of the gas introduction portion. Fig. 30 is a view showing another arrangement example of the gas introduction portion and an air flow in the processing container. Fig. 31 is a view for explaining the arrangement of a transmission plate (-55-201215250 microwave introduction unit) used in the experimental plasma processing apparatus. Fig. 32 is a graph showing the measurement results of the plasma density in Experiment 1. Fig. 33 is a graph showing the measurement results of the plasma density in Experiment 2. Fig. 34 is a graph showing the measurement results of the film thickness of the tantalum nitride film of Experiment 3. Fig. 35 is a graph showing the measurement results of the film thickness of the tantalum nitride film of Experiment 4. Figure 36 is a schematic view showing an ALD film forming apparatus to which the present invention is applicable. [Description of main component symbols] 1 : Processing container 2 : Support device 3 : Mounting table 4 : Support portion 1 1 : Exhaust port 15 : Gas introduction portion 1 8 : Gas supply device 24 : Exhaust device 27 : Microwave introduction unit 2 8: Transmitting plate 3 7 : Waveguide 39: Microwave generating device 5 〇: Control unit

S -56- 201215250 100 :電漿處理裝置 W:半導體晶圓(基板) S R :載置區域 -57S -56- 201215250 100 : Plasma processing unit W: Semiconductor wafer (substrate) S R : Mounting area -57

Claims (1)

201215250 七、申請專利範圍: 1. 一種電漿處理裝置,係臭備: 可抽真空的處理容器,其係形成處理被處理體的處理 空間; 支撐裝置’其係於上述處理容器內支撐被處理體; 電磁波產生裝置’其係產生電磁波,該電磁波係用以 使電漿生成於上述處理容器內; 複數的電磁波導入單元,其係將在上述電磁波產生裝 置產生的電磁波導入至上述處理容器內;及 驅動裝置,其係以上述支撐裝置的中央作爲旋轉中心 ,使被該支撐裝置支撐的複數的被處理體及/或上述複數 的電磁波導入單元旋轉,而使環繞運動, 上述電磁波導入單元係具有電磁波導入窗,該電磁波 導入窗係面對上述處理空間而設置,使電磁波透過而導入 至上述處理容器內, 上述支撐裝置係具有載置複數的被處理體之載置台, 被載置於上述載置台的複數的被處理體係對上述電磁 波導入窗相對移動,以各個的被處理體至少通過一個上述 電磁波導入窗的電磁波透過區域的對向位置之方式構成。 2. 如申請專利範圍第1項之電漿處理裝置,其中,在 上述相對移動之間,以一個的被處理體對於2個以上的上 述電磁波導入窗至少部分地依序通過對向的位置之方式構 成。 3. 如申請專利範圍第1項之電漿處理裝置,其中,在 S -58- 201215250 上述相對移動之間,以一個的被處理體同時對於2個以上 的上述電磁波導入窗至少部分地通過對向的位置之方式構 成。 4. 如申請專利範圍第2或3項之電漿處理裝置,其中 ,上述複數的電磁波導入窗係以藉由從各電磁波導入窗所 導入的電磁波來生成的電漿之電漿密度的時間性累計値及 /或電漿照射時間的累計値無論在一個被處理體的哪個位 置皆形成相同之方式配置》 5. 如申請專利範圍第1項之電漿處理裝置,其中,更 具備輔助性的電磁波導入單元,其係對於上述相對移動的 被處理體的軌道,具有設於偏離對向的位置之位置的電磁 波導入窗。 6. 如申請專利範圍第1項之電漿處理裝置,其中,具 備複數的電磁波導入單元,其係上述電磁波導入窗的面積 相異。 7. 如申請專利範圍第1項之電漿處理裝置,其中,上 述電磁波產生裝置係對應於上述電磁波導入單元來個別地 設置。 8. 如申請專利範圍第1項之電漿處理裝置,其中,供 給至上述複數的電磁波導入單元的電磁波的功率可個別地 設定》 9. 如申請專利範圍第1項之電漿處理裝置,其中,從 處於接近上述旋轉中心的位置之內側的電磁波導入窗所導 入的電磁波的功率與從比該內側的電磁波導入窗更位於環 -59- 201215250 繞半徑的外側之外側的電磁波導入窗所導入的電磁波的功 率相異。 10.—種電漿處理方法,係使用電漿處理裝置,經由 上述複數的電磁波導入窗來將電磁波導入至上述處理容器 內而使電漿生成,且在上述處理容器之中以被處理體至少 通過一個上述電磁波導入窗的電磁波透過區域的對向位置 之方式,一邊使被處理體對於上述電磁波導入窗相對移動 ,一邊以無論在被處理體上的那個位置,電漿密度的時間 性累計値及/或電漿照射時間的累計値皆形成相同的方式 進行電漿處理, 該電漿處理裝置係具備: 可抽真空的處理容器,其係形成處理被處理體的處理 空間; 支撐裝置,其係於上述處理容器內支撐被處理體; 電磁波產生裝置,其係產生電磁波,該電磁波係用以 使電漿生成於上述處理容器內; 複數的電磁波導入單元,其係將在上述電磁波產生裝 置產生的電磁波導入至上述處理容器內;及 驅動裝置,其係以上述支撐裝置的中央作爲旋轉中心 ,使被該支撐裝置支撐的複數的被處理體及/或上述複數 的電磁波導入單元旋轉,而使環繞運動, 上述電磁波導入單元係具有電磁波導入窗,該電磁波 導入窗係面對上述處理空間而設置,使電磁波透過而導入 至上述處理容器內, S -60- 201215250 上述支撐裝置係具有載置複數的被處理體之載置台。 C: -61 -201215250 VII. Patent application scope: 1. A plasma processing device, which is a smear preparation: a vacuum-processable processing container, which forms a processing space for processing a processed object; the support device is attached to the processing container to be processed An electromagnetic wave generating device that generates electromagnetic waves for generating plasma in the processing container, and a plurality of electromagnetic wave introducing units that introduce electromagnetic waves generated by the electromagnetic wave generating device into the processing container; And a driving device that rotates a plurality of objects to be processed supported by the supporting device and/or the plurality of electromagnetic wave introducing units supported by the center of the supporting device to cause a wraparound motion, and the electromagnetic wave introducing unit has The electromagnetic wave introduction window is provided to face the processing space, and electromagnetic waves are transmitted and introduced into the processing container, and the supporting device has a mounting table on which a plurality of objects to be processed are placed, and is placed on the loading table. Placing a plurality of processed systems for the above electromagnetic waveguide Window movement relative to the respective object to be processed by the at least one of said electromagnetic wave introduced through the window area of positions constituting the embodiment. 2. The plasma processing apparatus according to claim 1, wherein between the relative movements, one of the objects to be processed passes through the opposing positions at least partially in sequence with respect to the two or more electromagnetic wave introduction windows. Way composition. 3. The plasma processing apparatus according to claim 1, wherein, between the relative movements of S-58-201215250, at least one of the objects to be processed simultaneously passes at least partially on the electromagnetic wave introduction window of the two or more electromagnetic waves. The way to the position. 4. The plasma processing apparatus according to claim 2, wherein the plurality of electromagnetic wave introduction windows have temporal properties of plasma density of plasma generated by electromagnetic waves introduced from respective electromagnetic wave introduction windows. The cumulative enthalpy and/or the cumulative time of the plasma irradiation time are configured in the same manner regardless of the position of a treated object. 5. The plasma processing apparatus of claim 1 is more auxiliary. The electromagnetic wave introduction unit has an electromagnetic wave introduction window provided at a position deviated from the opposite position with respect to the track of the object to be moved that moves relatively. 6. The plasma processing apparatus according to claim 1, wherein the plurality of electromagnetic wave introducing units have different areas of the electromagnetic wave introducing windows. 7. The plasma processing apparatus according to claim 1, wherein the electromagnetic wave generating device is individually provided corresponding to the electromagnetic wave introducing unit. 8. The plasma processing apparatus according to claim 1, wherein the power of the electromagnetic waves supplied to the plurality of electromagnetic wave introducing units can be individually set. 9. The plasma processing apparatus according to claim 1, wherein The power of the electromagnetic wave introduced from the electromagnetic wave introduction window located inside the position close to the rotation center is introduced from the electromagnetic wave introduction window on the outer side of the radius of the ring-59-201215250 from the electromagnetic wave introduction window on the inner side. The power of electromagnetic waves is different. 10. A plasma processing method, wherein a plasma processing apparatus is used to introduce electromagnetic waves into the processing container through the plurality of electromagnetic wave introduction windows to generate plasma, and at least a processed object in the processing container When the object to be processed moves relative to the electromagnetic wave introduction window by the relative position of the electromagnetic wave introduction window of the electromagnetic wave introduction window, the plasma density is accumulated at any position on the object to be processed. And/or the cumulative enthalpy of the plasma irradiation time is performed in the same manner for plasma treatment, the plasma processing apparatus comprising: a vacuumable processing container that forms a processing space for processing the object to be processed; and a support device The electromagnetic wave generating device is configured to generate electromagnetic waves for generating plasma in the processing container, and a plurality of electromagnetic wave introducing units to be generated in the electromagnetic wave generating device. Electromagnetic waves are introduced into the processing container; and the driving device is above The center of the supporting device serves as a center of rotation, and a plurality of objects to be processed supported by the supporting device and/or the plurality of electromagnetic wave introducing units are rotated to cause a wraparound motion. The electromagnetic wave introducing unit has an electromagnetic wave introducing window, and the electromagnetic wave introducing window The apparatus is provided to face the processing space, and electromagnetic waves are transmitted and introduced into the processing container. S-60-201215250 The supporting device has a mounting table on which a plurality of objects to be processed are placed. C: -61 -
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