TW200410332A - Method and device for plasma treatment - Google Patents
Method and device for plasma treatment Download PDFInfo
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- TW200410332A TW200410332A TW092123978A TW92123978A TW200410332A TW 200410332 A TW200410332 A TW 200410332A TW 092123978 A TW092123978 A TW 092123978A TW 92123978 A TW92123978 A TW 92123978A TW 200410332 A TW200410332 A TW 200410332A
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- semiconductor wafer
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/32431—Constructional details of the reactor
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P50/00—Etching of wafers, substrates or parts of devices
- H10P50/20—Dry etching; Plasma etching; Reactive-ion etching
- H10P50/24—Dry etching; Plasma etching; Reactive-ion etching of semiconductor materials
- H10P50/242—Dry etching; Plasma etching; Reactive-ion etching of semiconductor materials of Group IV materials
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2237/00—Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
- H01J2237/004—Charge control of objects or beams
- H01J2237/0041—Neutralising arrangements
- H01J2237/0044—Neutralising arrangements of objects being observed or treated
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- Plasma & Fusion (AREA)
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- Container, Conveyance, Adherence, Positioning, Of Wafer (AREA)
- Drying Of Semiconductors (AREA)
Abstract
Description
200410332 (1) 玖、發明說明 【發明所屬之技術領域】 本發明係關於電獎處理方法及電漿處理裝置,特別是 有關於對半導體晶圓或LCD用基板等之被處理基板施以 電漿蝕刻處理等之電漿處理方法及電漿處理裝置。 【先前技術】 以往,電漿多用於進行半導體晶圓或L C D用基板等 被處理基板之電漿處理方法。例如,在半導體裝置之製造 工程中,用以在被處理基板,例如半導體晶圓,形成微細 之電氣電路之技術方面,多採用將被形成於半導體晶圓上 之薄膜等用電漿蝕刻除去之電漿蝕刻處理。 進行該電漿蝕刻處理之蝕刻裝置方面,例如,在內部 被構成可氣密閉鎖之處理室(蝕刻室)內製作成產生電漿 之方式。接著,在設置於該蝕刻室內之基座(suscepter) 上載置半導體晶圓,進行蝕刻。 此外,就使產生上述電漿之手段方面已知有種種之型 態。其中,對被設成上下相對方向之方式之一對平行平板 電極供給高頻電力以產生電漿之型態之裝置方面,平行平 板電極之中的一方,例如下部電極則兼作基座。接著,在 該下部電極上配置半導體晶圓,對平行平板電極間施加高 頻電壓產生電漿,且進行触刻。 然而,該型態之蝕刻裝置方面,在蝕刻中’於半導體 晶圓之表面,會產生閃電之異常放電之所謂表面弧光現 -5 - (2) (2)200410332 象。 上述表面弧光,大多例如在導體層之上形成絕緣體 層,且在蝕刻之場合下產生該絕緣體層之情況。例如,在 蝕刻由矽氧化膜形成之絕緣體層,並在下層之由金屬層形 成之導體層形成貫通之接觸孔之場合等,大多會產生破壞 藉由蝕刻讓膜厚減少之矽氧化膜之情況。 接著,如該異常放電產生,因爲半導體晶圓中之矽氧 化膜的大部分會遭到破壞,故而造成該半導體晶圓之大部 分元件之不良。此外,同時在蝕刻室內產生金屬污染,常 此下來便無法進行蝕刻處理,導致必須進行蝕刻室內之淸 理。因此,造成生產性顯著降低之問題。 【發明內容】 於是,本發明之目的在於提供一種能夠防止被處理基 板所產生之表面弧光之發生,且相較於以往能謀求生產性 之提升之電漿處理方法及電漿處理裝置。 本發明之電漿處理方法之特徵係:在使電漿作用於被 處理基板進行電漿處理之際,在進行前述電漿處理之前, 以弱於使用在電漿處理之電漿作用於前述被處理基板’使 該被處理基板之電荷狀態成爲一定之狀態,之後’進行前 述電漿處理。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,使前述弱的電漿以指定時間作用於前述被處 理基板,之後,對靜電夾盤施加用以吸著保持前述被處理 -6- (3) (3)200410332 基板之直流電壓。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,在前述弱的電漿消失前,開始對前述靜電夾 fe施加直流電壓。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,前述弱的電漿是由 Ar、02、CF4、或者N2 所形成之電漿。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,前述弱的電漿係由0.15〜1.0 w/ cm2之高頻 電力所形成。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,前述弱的電漿係作用於前述被處理基板時間 長達5〜2 0秒。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,在前述電漿處理開始時,在開始施加用以產 生電漿之高頻電力後,開始對前述靜電夾盤施加直流電 壓,且在前述電漿處理終了時,在停止對前述靜電夾盤施 加直流電壓後,停止施加前述高頻電力。 此外,本發明之電漿處理方法之特徵係:於上述電漿 處理方法中,在利用在前述靜電夾盤之上方藉導體接地之 支撐棒以支撐前述被處理基板之狀態下,開始對前述靜電 夾盤施加直流電壓,之後,使前述被處理基板下降並載置 於前述靜電夾盤上。 此外,本發明之電漿處理方法之特徵係:於上述電漿 200410332200410332 (1) 发明 Description of the invention [Technical field to which the invention belongs] The present invention relates to an electromagnet processing method and a plasma processing apparatus, and more particularly, to applying plasma to a substrate to be processed such as a semiconductor wafer or an LCD substrate. Plasma processing method and plasma processing apparatus such as etching process. [Prior art] In the past, plasma was mostly used for plasma processing methods for substrates such as semiconductor wafers and substrates for LCDs. For example, in the manufacturing process of semiconductor devices, the technology used to form fine electrical circuits on a substrate to be processed, such as a semiconductor wafer, often uses plasma etching to remove films and the like formed on the semiconductor wafer. Plasma etching. In the etching apparatus for performing the plasma etching process, for example, a plasma-generating method is formed in a processing chamber (etching chamber) which can be hermetically sealed inside. Next, a semiconductor wafer is placed on a suscepter provided in the etching chamber, and etching is performed. In addition, various types of means for generating the above-mentioned plasma are known. Among them, in a device that supplies high-frequency power to a parallel plate electrode in a manner of facing up and down to generate a plasma type, one of the parallel plate electrodes, for example, the lower electrode also serves as a base. Next, a semiconductor wafer is placed on the lower electrode, a high-frequency voltage is applied between the parallel flat electrodes to generate a plasma, and the etching is performed. However, in terms of this type of etching device, the so-called surface arcing of the abnormal discharge of lightning on the surface of the semiconductor wafer during the etching process appears to be -5-(2) (2) 200410332. The above-mentioned surface arc light is often formed, for example, by forming an insulator layer on a conductor layer and generating the insulator layer during etching. For example, when an insulator layer formed by a silicon oxide film is etched, and a through contact hole is formed by a conductive layer formed by a metal layer on the lower layer, the silicon oxide film that causes the film thickness to be reduced by etching is often caused. . Then, if the abnormal discharge occurs, most of the silicon oxide film in the semiconductor wafer will be damaged, which causes the failure of most of the components of the semiconductor wafer. In addition, at the same time, metal contamination is generated in the etching chamber, and the etching process is often unable to be performed, resulting in the necessity of performing the treatment in the etching chamber. Therefore, there is a problem that productivity is significantly reduced. SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a plasma processing method and a plasma processing apparatus capable of preventing the occurrence of surface arc light generated from a substrate to be processed and improving productivity as compared with the past. The plasma processing method of the present invention is characterized in that when plasma is applied to a substrate to be processed for plasma processing, before the aforementioned plasma processing is performed, the plasma is weaker than the plasma used in the plasma processing to act on the substrate. The processing substrate 'makes the state of charge of the substrate to be processed constant, and then performs the aforementioned plasma processing. In addition, the plasma processing method of the present invention is characterized in that: in the above plasma processing method, the weak plasma is applied to the substrate to be processed for a specified time, and thereafter, an electrostatic chuck is applied to hold the foregoing by suction. DC voltage to be processed -6- (3) (3) 200410332 substrate. In addition, the plasma processing method of the present invention is characterized in that, in the above-mentioned plasma processing method, before the weak plasma disappears, a DC voltage is applied to the electrostatic clamp fe. In addition, the plasma processing method of the present invention is characterized in that: in the above plasma processing method, the aforementioned weak plasma is a plasma formed of Ar, 02, CF4, or N2. In addition, the plasma treatment method of the present invention is characterized in that: in the above plasma treatment method, the aforementioned weak plasma is formed by a high-frequency power of 0.15 to 1.0 w / cm2. In addition, the plasma processing method of the present invention is characterized in that in the above plasma processing method, the aforementioned weak plasma system acts on the substrate to be processed for a period of 5 to 20 seconds. In addition, the plasma processing method of the present invention is characterized in that: in the above plasma processing method, at the beginning of the aforementioned plasma processing, after the application of high-frequency power for generating plasma is started, the electrostatic chuck is started to be applied. DC voltage, and when the plasma processing is completed, after the DC voltage is stopped from being applied to the electrostatic chuck, the high frequency power is stopped from being applied. In addition, the feature of the plasma processing method of the present invention is that in the above plasma processing method, the static electricity is started in a state where a support rod grounded by a conductor above the electrostatic chuck is used to support the substrate to be processed. After applying a DC voltage to the chuck, the substrate to be processed is lowered and placed on the electrostatic chuck. In addition, the plasma treatment method of the present invention is characterized in that the above-mentioned plasma 200410332
處理方法中,前述電漿處理係蝕刻處理,在進行該蝕刻處 理之處理室內,使前述弱的電紫作用於前述被處理基板。 此外,本發明之電漿處理裝置,係具備對被處理基板 施以電漿處理之電漿處理機構,其特徵爲:具備控制前述 電漿處理機構,且進行上述電漿處理方法之控制部。 【實施方式】In the processing method, the plasma treatment is an etching process, and the weak electric violet is applied to the substrate to be processed in a processing chamber in which the etching process is performed. In addition, the plasma processing apparatus of the present invention includes a plasma processing mechanism for performing a plasma processing on a substrate to be processed, and is characterized in that it includes a control unit that controls the aforementioned plasma processing mechanism and performs the above-mentioned plasma processing method. [Embodiment]
以下’就本發明之實施型態方面,參照圖面並加以說 明。 第1圖係顯示本發明之實施型態所使用之電漿處理裝 置(蝕刻裝置)全體之槪略構成的模式圖。同圖中,圖號 1係表示,材質由例如鋁等所形成,內部被構成可氣密閉 鎖,且構成處理室之圓筒狀的真空室。In the following, aspects of the embodiments of the present invention will be described with reference to the drawings. Fig. 1 is a schematic diagram showing a schematic configuration of the entire plasma processing apparatus (etching apparatus) used in the embodiment of the present invention. In the figure, the drawing number 1 indicates that the material is made of, for example, aluminum, etc., and the inside is configured as a hermetically sealed vacuum chamber and constitutes a cylindrical vacuum chamber of a processing chamber.
上述真空室1係被接續至接地電位。於真空室1內 部’由導電性材料例如鋁等製作成區塊狀,且設置兼作下 部電極之載置台2。 該載置台2係中介著陶瓷等絕緣板3而被支撐於真空 室1內。於載置台2之半導體晶圓W載置面設置靜電夾 盤4。該靜電夾盤4係被製作成使靜電夾盤用電極4a中 介於由絕緣性材料形成之絕緣膜4 b中,且於靜電夾盤用 電極4 a接續直流電源5。靜電夾盤用電極4 a係由例如銅 等所構成,絕緣膜4 b則由聚醯胺等所構成。 此外,於載置台2內部設置:用以使控制溫度用之熱 媒體進行絕緣性流體循環之熱媒體流路6,與用以將氦等 -8- (5) 200410332 控制溫度用氣體供給至半導體晶圓 W之背面之氣體流路 7。 於是,形成藉由在熱媒體流路6內使被控制成指定溫 度之絕緣性流體循環,能將載置台2控制成指定溫度,而 且,對該載置台2與半導體晶圓W之背面之間透過氣體 流路7供給控制溫度用之氣體促進其間之熱交換,並精確 度良好地且有效率地控制半導體晶圓W於指定溫度。The vacuum chamber 1 is connected to a ground potential. Inside the vacuum chamber 1 ', a block 2 made of a conductive material such as aluminum is provided, and a mounting table 2 serving as a lower electrode is provided. The mounting table 2 is supported in the vacuum chamber 1 via an insulating plate 3 such as ceramics. An electrostatic chuck 4 is provided on the mounting surface of the semiconductor wafer W on the mounting table 2. The electrostatic chuck 4 is formed so that the electrostatic chuck electrode 4a is interposed in an insulating film 4b formed of an insulating material, and the electrostatic chuck electrode 4a is connected to a DC power source 5. The electrostatic chuck electrode 4a is made of, for example, copper, and the insulating film 4b is made of polyamine. In addition, inside the mounting table 2, a heat medium flow path 6 for insulating fluid circulation of a heat medium for temperature control, and a helium gas etc. are supplied to the semiconductor. Gas flow path 7 on the back of wafer W. Thus, by forming an insulating fluid that is controlled to a predetermined temperature in the heat medium flow path 6, it is possible to control the mounting table 2 to a predetermined temperature, and between the mounting table 2 and the back surface of the semiconductor wafer W. Supplying a temperature-controlling gas through the gas flow path 7 promotes heat exchange therebetween, and controls the semiconductor wafer W to a predetermined temperature with good accuracy and efficiency.
此外,於載置台2上方之外周設置以導電性材料或者 絕緣性材料形成之聚焦環8,再者,於載置台2之大致中 央接續著用以供給高頻電力之給電線9。製作成在該給電 線9透過整合器1 0接續高頻電源(RF電源)1 1,且由高 頻電源1 1供給指定頻率之高頻電力之型態。Further, a focusing ring 8 made of a conductive material or an insulating material is provided on the outer periphery above the mounting table 2, and a power supply wire 9 for supplying high-frequency power is connected to a substantially center of the mounting table 2. The power supply line 9 is connected to a high-frequency power supply (RF power supply) 11 through an integrator 10, and a high-frequency power supply of a specified frequency is supplied from the high-frequency power supply 11.
此外,在上述之聚焦環8外側被製作成環狀,且設置 形成多數排氣孔之排氣環〗2,透過該排氣環1 2,利用被 接續至排氣通道1 3之排氣系1 4之真空泵浦等,進行真空 室1內之處理空間之真空排氣。 另一方面,於載置台2上方之真空室1之頂部,蓮蓬 頭(shower head) 15被設置成與載置台2平行地相對 向,而該蓮蓬頭1 5被接地。因此,該蓮蓬頭1 5與載置台 2之功能便構成一對電極(上部電極與下部電極)。 上述蓮蓬頭1 5,在其下面設置多數個氣體吐出孔 1 6,而且在其上部具有氣體導入部1 7。然後,在蓮蓬頭 1 5內部形成氣體擴散用空隙1 8。於氣體導入部1 7接續氣 體供給管1 9,於該氣體供給管1 9之另一端則接續氣體供 -9- (6) (6)200410332 給系2 0。該氣體供給系2 0係由用以控制氣體流量之氣體 流量控制器(MFC ) 2 1,與用以供給例如蝕刻用之處理氣 體等之處理氣體供給源22,以及用以供給Ar之Ar供給 源2 3等所構成。 一方面,在真空室1外側周圍,以與真空室1同心狀 地配置環狀之磁場形成機構(環狀磁石)2 4,製作成在載 置台2與蓮蓬頭1 5間之處理空間形成磁場。該磁場形成 機構24係利用旋轉機構25,讓其全體能以指定之旋轉速 度繞行真空室1 一週。 此外,用以對半導體晶圓W施以電漿處理之上述直 流電源5、高頻電源1 1、氣體供給系2 0等之電漿處理機 構係被構成由控制部40所控制的型態。 其次,就依照如上述方式構成之蝕刻裝置依其蝕刻處 理順序加以說明。 (第1實施例) 首先,開放被設於真空室1之未圖示之閘閥(gate valve ),透過被配置於鄰接該閘閥之載入閉鎖真空室 (load-lock chamber)(未圖示),利用搬送機構(未圖 示)將半導體晶圓W搬入真空室1內,載置於載置台2 上。接著,在使搬送機構向真空室1外退避後,關閉閘 閥。又,該時點,並未由直流電源5對靜電夾盤4之靜電 夾盤用電極4a施加直流電壓(HV)。 之後’首先,一面利用排氣系1 4之真空泵浦通過排 -10- (7) (7)200410332 氣通道將真空室1內排氣成指定之真空度,一面從A r供 給源2 3將Ar供給至真空室1內。接著,在該狀態下,如 第2圖所不,先由问頻电源1】對作爲下部電極之載置台 2供給例如300 W _電力較低之高頻電力〔頻率例如 1 3 .56MH^ ),產生弱的電漿,使該弱的電漿作用於半導 體晶圓W ° 如此’使弱的電獎作用於半導體晶圓W,係根據如下 之理由。 亦即’進fr處理之41導體晶圓w方面,係根據前工 程(例如CVD等之成膜工程)中之處理的狀態等,該狀 態並非相同’例如’有在半導體晶圓w之內部蓄積電荷 之場合。於是,在如此於半導體晶圓w內部蓄積電荷之 狀態下,若使強的電獎作用’因爲產生表面弧光等之可能 性高,所以在使該強的電漿作用之前,使弱的電漿作用, 以使被蓄積於半導體晶圓w內部之電荷狀態等調整成相 同(初期化)° 接著,在調整如此被蓄積於半導體晶圓 w內部之電 荷狀態時,由於半導體晶圓W內部電荷易於移動,所以 在未進行對靜電夾盤4之靜電夾盤用電極4a施加直流電 壓(HV)之狀態下,利用該弱的電紫進行半導體晶圓之 調整(初期化)。 又,用以產生該弱的電漿之高頻施加電力係大約 0.15W / cm2 〜1.0 W/cm2,例如 100 〜500W 左右,使弱 的電漿作用於半導體晶圓W之時間則例如5〜2 0秒左 -11 - (8) (8)200410332 右。 此外,上述中,係就採用A r,使A r之電漿作用之場 合加以說明,然氣體種類並不侷限於此,亦能使用例如 02、CF4、N2等氣體。但是,針對該氣體種類之選擇方 面,必須選擇使產生之電漿,對於半導體晶圓W,以及對 於真空室1之內壁,引起蝕刻等非期待之作用之程度小的 氣體,而且必須選擇讓電漿易於點火之氣體。再者,進行 處理之半導體晶圓W’亦根據在前工程是否被施以何種處 理,而有最適之氣體種類改變之場合,最好是考慮該場合 後適當選擇。 接著,在如上述使弱的電漿作用於半導體晶圓 W 後,如第2圖所示,進行對靜電夾盤用電極4a施加來自 直流電源5之直流電壓(HV )。之後,由處理氣體供給 源22對真空室1內供給指定之處理氣體(鈾刻氣體), 由高頻電源 11對作爲下部電極之載置台 2供給例如 2 0 00W等通常處理用之電力之高的高頻電力(頻率例如 13.56MHz ),產生強的電漿,進行通常之電漿處理(蝕 刻處理)。又,第2圖中,橫軸表示時間,縱軸表示在靜 電夾盤HV之場合爲電壓値,在RF輸出之場合爲電力 値。 此時,藉由對下部電極之載置台2施加高頻電力’於 上部電極之蓮蓬頭1 5與下部電極之載置台2間的處理空 間形成高頻電場,而且依照磁場形成機構24形成磁場’ 在該狀態下由電漿進行蝕刻。 -12 - (9) 200410332 接著,一旦實行指定之蝕刻處理,便藉由停止由高頻 電源11供給高頻電力以停止蝕刻處理,且以與上述順序 相反之順序,將半導體晶圓w搬出至真空室1外。In addition, the above-mentioned focusing ring 8 is formed in a ring shape, and an exhaust ring 2 is formed to form a large number of exhaust holes. Through the exhaust ring 12, an exhaust system connected to the exhaust passage 13 is used. A vacuum pump such as 14 performs vacuum exhaust of the processing space in the vacuum chamber 1. On the other hand, on the top of the vacuum chamber 1 above the mounting table 2, a shower head 15 is provided so as to face the mounting table 2 in parallel, and the shower head 15 is grounded. Therefore, the functions of the shower head 15 and the mounting table 2 constitute a pair of electrodes (upper electrode and lower electrode). The shower head 15 is provided with a plurality of gas discharge holes 16 under the shower head, and has a gas introduction part 17 at an upper portion thereof. Then, a gas diffusion space 18 is formed inside the shower head 15. A gas supply pipe 19 is connected to the gas introduction part 17 and a gas supply is connected to the other end of the gas supply pipe 19-(6) (6) 200410332 to the system 20. The gas supply system 20 is composed of a gas flow controller (MFC) 21 for controlling the gas flow rate, a processing gas supply source 22 for supplying, for example, a processing gas for etching, and an Ar supply for supplying Ar. Source 2 3 and so on. On the other hand, a ring-shaped magnetic field forming mechanism (ring magnet) 2 4 is arranged concentrically with the vacuum chamber 1 around the outside of the vacuum chamber 1 to produce a magnetic field in a processing space between the stage 2 and the shower head 15. The magnetic field forming mechanism 24 uses a rotating mechanism 25 to allow the entire magnetic field forming mechanism 24 to orbit the vacuum chamber 1 at a specified rotation speed. In addition, the plasma processing mechanism system such as the above-mentioned DC power supply 5, high-frequency power supply 11, gas supply system 20, and the like for plasma processing the semiconductor wafer W is configured to be controlled by the control unit 40. Next, the etching apparatus constructed as described above will be described in accordance with its etching processing order. (First Embodiment) First, a gate valve (not shown) provided in the vacuum chamber 1 is opened, and a load-lock chamber (not shown) disposed adjacent to the gate valve is opened. The semiconductor wafer W is transferred into the vacuum chamber 1 by a transfer mechanism (not shown) and placed on the mounting table 2. Next, after the transfer mechanism is retracted outside the vacuum chamber 1, the gate valve is closed. At this time, a DC voltage (HV) was not applied to the electrostatic chuck electrode 4a of the electrostatic chuck 4 by the DC power source 5. After 'First, while exhausting the vacuum pump of the exhaust system 1 4 through the exhaust passage -10- (7) (7) 200410332, the inside of the vacuum chamber 1 is exhausted to a specified degree of vacuum, and from the supply source 2 3 will be Ar is supplied into the vacuum chamber 1. Then, in this state, as shown in FIG. 2, first, the frequency power source 1] supplies the mounting table 2 as the lower electrode with, for example, 300 W _ low-frequency high-frequency power [frequency such as 1 3.56MH ^) A weak plasma is generated, and the weak plasma is applied to the semiconductor wafer W. Thus, the weak plasma is applied to the semiconductor wafer W, for the following reasons. In other words, the 41-conductor wafer w processed into fr is based on the processing status in the previous process (such as a film-forming process such as CVD), and the state is not the same. For example, there is accumulation in the semiconductor wafer w Occasion of charge. Therefore, in the state where the electric charge is accumulated in the semiconductor wafer w, if a strong electro-optical effect is generated, there is a high possibility that surface arcing or the like will occur. Therefore, before the strong plasma is applied, a weak plasma is caused. Function to adjust the state of charge and the like accumulated in the semiconductor wafer w to be the same (initialization) °. Then, when the state of charge thus accumulated in the semiconductor wafer w is adjusted, the internal charge of the semiconductor wafer W is easy to adjust. Since the movement is performed, the semiconductor wafer is adjusted (initialized) using the weak electric violet without applying a DC voltage (HV) to the electrostatic chuck electrode 4a of the electrostatic chuck 4. In addition, the high-frequency applied power used to generate the weak plasma is about 0.15W / cm2 to 1.0 W / cm2, for example, about 100 to 500W, and the time for the weak plasma to act on the semiconductor wafer W is, for example, 5 to 20 seconds left-11-(8) (8) 200410332 right. In addition, in the above, the field where Ar is used to cause the plasma action of Ar is described, but the type of gas is not limited to this, and gases such as 02, CF4, and N2 can also be used. However, with regard to the selection of the gas type, it is necessary to select a gas that generates plasma, which has a small degree of causing unexpected effects such as etching to the semiconductor wafer W and the inner wall of the vacuum chamber 1, and it is necessary to select Plasma easily ignites gas. Moreover, the semiconductor wafer W 'to be processed is also selected based on whether or not the previous process has been applied, and when the most suitable gas type is changed. Next, after a weak plasma is applied to the semiconductor wafer W as described above, as shown in FIG. 2, a DC voltage (HV) from the DC power source 5 is applied to the electrostatic chuck electrode 4a. Thereafter, a specified processing gas (uranium-etched gas) is supplied into the vacuum chamber 1 from the processing gas supply source 22, and a high-frequency power source 11 is supplied to the mounting table 2 serving as the lower electrode at a high level, such as 2000 W. The high-frequency power (frequency, for example, 13.56 MHz) generates a strong plasma, and is subjected to a usual plasma treatment (etching treatment). In Fig. 2, the horizontal axis represents time, and the vertical axis represents voltage 値 in the case of the electrostatic chuck HV, and power 电力 in the case of the RF output. At this time, a high-frequency electric field is formed in the processing space between the shower head 15 of the upper electrode and the mounting table 2 of the lower electrode by applying high-frequency power to the mounting table 2 of the lower electrode, and a magnetic field is formed in accordance with the magnetic field forming mechanism 24. In this state, etching is performed by plasma. -12-(9) 200410332 Then, once the specified etching process is performed, the high frequency power from the high frequency power supply 11 is stopped to stop the etching process, and the semiconductor wafer w is carried out in the reverse order of the above order. Outside the vacuum chamber 1.
如上述方式,首先,使弱的電漿作用於半導體品圓, 之後,進行半導體晶圓 w之蝕刻處理,便能使半導體晶 圓W所產生表面弧光之比例成爲接近零(I %以下),不 因生產批次而有所不同。另一方面,在未使如上述之弱的 電漿發揮作用便開始處理之場合,半導體晶圓W所產生 表面弧光之比例則隨著批次不同而有成爲8 0 %左右之場 合。原因是在比蝕刻更前面的工程中造成半導體晶圓 W 帶電,該種表面弧光,特別是在前工程藉由 CVD形成所 謂Low— K膜之工程的場合下,發生之機率高。 因而能確認:在開始通常之處理前,藉由如上述使弱 的電漿作用於半導體晶圓W,便能大幅地降低半導體晶圓 W所產生表面弧光之比例。As described above, first, a weak plasma is applied to the semiconductor circle, and then the semiconductor wafer w is etched to make the proportion of surface arc light generated by the semiconductor wafer W close to zero (I% or less). Does not vary by production batch. On the other hand, when the processing is started without the weak plasma as described above, the proportion of surface arc light generated by the semiconductor wafer W may be about 80% depending on the lot. The reason is that the semiconductor wafer W is electrified in a process earlier than etching, and this kind of surface arcing, especially in the case of the former process in which the so-called Low-K film is formed by CVD, has a high probability. Therefore, it can be confirmed that the ratio of surface arc generated by the semiconductor wafer W can be greatly reduced by applying a weak plasma to the semiconductor wafer W as described above before starting the normal processing.
可是,上述實施型態方面,如第1圖所示,係就使用 僅對下部電極之載置台2施加高頻電力之構成之裝置的場 合加以說明,但亦能適用於例如第3圖所示之,被構成亦 對作爲上部電極之蓮蓬頭1 5透過整合器由高頻電源3 1施 加高頻電力之方式之所謂上下部施加型的電漿處理裝置。 該場合,例如第4圖所示,首先,對下部電極之載置 台2開始施加低電力之高頻電力,之後對上部電極之蓮蓬 頭1 5開始施加低電力之高頻電力,在此,暫時停止對下 部電極之載置台2施加高頻電力。接著,在該狀態下以指 -13- (10) 200410332 定期間使弱的電漿作用於半導體晶圓w之後’亦停止對 上部電極之蓮蓬頭1 5施加高頻電力’且暫時讓電漿消 失。However, as shown in FIG. 1, the above-mentioned embodiment is described in the case of using a device configured to apply high-frequency power only to the mounting table 2 of the lower electrode, but it can also be applied to, for example, FIG. 3 In other words, the so-called upper and lower application type plasma processing device is configured so that high-frequency power is applied from the high-frequency power source 31 to the shower head 15 as the upper electrode through the integrator. In this case, for example, as shown in FIG. 4, first, low-frequency high-frequency power is applied to the lower electrode mounting table 2, and then low-frequency high-frequency power is applied to the shower head 15 of the upper electrode. Here, temporarily stop. High-frequency power is applied to the lower electrode mounting table 2. Then, in this state, after a period of -13- (10) 200410332, a weak plasma was applied to the semiconductor wafer w to 'stop applying high-frequency power to the shower head 15 of the upper electrode' and let the plasma disappear temporarily. .
然後,依序開始:對靜電夾盤4之靜電夾盤用電極 4 a施加直流電壓(Η V ),對下部電極之載置台2施加處 理用之通常之高頻電力(高電力之高頻電力)’對上部電 極之蓮蓬頭1 5施加處理用之通常之高頻電力(高電力之 高頻電力),開始半導體晶圓W之通常之處理。 如此一來,即使是上下部施加型之電漿處理裝置’本 發明亦能適用。 又,最好是除了如上述使弱的電漿發揮作用’或者, 單獨地,在開始處理之前,使例如離子化機作用於半導體 晶圓W,以減低其內部之電荷。藉由該離子化機之作用, 可抑制表面弧光之發生。該離子化機可以設置於真空室 內,或者亦能設置於真空室外之其他場所。Then, start sequentially: apply a DC voltage (Η V) to the electrostatic chuck electrode 4 a of the electrostatic chuck 4, and apply normal high-frequency power (high-frequency high-frequency power) for processing to the lower electrode mounting table 2. ) 'Normal high-frequency power (high-frequency high-frequency power) for processing is applied to the shower head 15 of the upper electrode, and normal processing of the semiconductor wafer W is started. In this way, the present invention can be applied to a plasma processing apparatus of an upper and lower application type. In addition, it is preferable to use a weak plasma as described above 'or separately, before starting the process, for example, an ionizer is applied to the semiconductor wafer W to reduce its internal charge. By the action of the ionizer, the occurrence of surface arc light can be suppressed. The ionizer can be installed in a vacuum chamber, or it can be installed in other places outside the vacuum chamber.
可是,第2圖所示之電漿處理方法方面,係在對下部 電極之載置台2施加弱的高頻電力並在使弱的電漿發揮作 用後不施加高頻電力之狀態下’開始對靜電夾盤4之靜電 夾盤用電極4 a施加直流電壓(Η V )。如此,在施加弱的 高頻電力並在使弱的電漿發揮作用後不施加高頻電力之狀 態下,開始對靜電夾盤用電極4 a施加直流電壓(Η V ), 則在開始施加直流電壓(Η V )之際,就可能產生閃電狀 放電且對基板造成損傷。該種場合如第5圖所示,在對載 置台2施加高頻電力之狀態(使弱的電漿發生之狀態) -14- (11) 200410332 下,便開始對靜電夾盤用電極4 a施加直流電壓(Η V ) ’ 就能抑制放電的發生。 以上,對於第1實施例’係就:在蝕刻等電漿處理前 用 A r使弱的電漿發揮作用之方法,以及此時之對靜電夾 盤用電極4 a施加直流電壓之時機加以說明。 (第2實施例)However, in the plasma processing method shown in FIG. 2, the low-frequency power is applied to the lower electrode mounting table 2 and the high-frequency power is not applied after the weak plasma is activated. The electrostatic chuck electrode 4 a of the electrostatic chuck 4 applies a DC voltage (Η V). In this way, when a weak high-frequency power is applied and a weak plasma is not applied after the high-frequency power is applied, a DC voltage (ΗV) is applied to the electrostatic chuck electrode 4a, and then DC is applied. When the voltage (Η V), a lightning discharge may occur and damage the substrate. In this case, as shown in FIG. 5, in a state where high-frequency power is applied to the mounting table 2 (a state where a weak plasma is generated) -14- (11) 200410332, the electrode for electrostatic chucks 4 a is started. By applying a DC voltage (Η V) ', the occurrence of discharge can be suppressed. The foregoing description of the first embodiment is a method of using weak plasma with Ar before plasma treatment such as etching, and the timing of applying a DC voltage to the electrostatic chuck electrode 4a at this time. . (Second Embodiment)
其次,針對進行鈾刻處理等之電漿處理之際施加高頻 電力之時機與對靜電夾盤用電極4 a施加直流電壓之時機 之關係,以適當例子予以說明。Next, the relationship between the timing of applying high-frequency power during the plasma processing such as uranium etching and the timing of applying a DC voltage to the electrostatic chuck electrode 4a will be explained with a suitable example.
又,在上述靜電夾盤4有雙極型與單極型,另外這些 型態方面亦分別有庫侖(coul〇mb)型與 Johnson- Lav eik 型。其中,使用單極型且庫侖型之靜電夾盤4之場合,最 好是按照如下之程序進行吸著半導體晶圓W。於第6圖表 示該程序。橫軸表示時間,縱軸方面虛線表示施加高頻電 力値(W )、實線則表示施加直流電壓値(V )。 亦即,在將半導體晶圓W載置於載置台2 (靜電夾盤 4 )上之後,開始朝真空室1內導入氣體。接著,之後如 第6圖以虛線所示,首先,開始朝載置台2施加高頻電力 產生電漿,之後,如同圖以實線所示,進行對靜電夾盤用 電極4a施加直流電壓(HV)。 又,因爲在開始對靜電夾盤用電極4a施加直流電壓 (HV)前,半導體晶圓 W並未被吸著於靜電夾盤4,所 以溫度控制並未充分進fj。因此’在最初產生電榮之際對 -15- (12) (12)200410332 載置台2所施加之高頻電力,該電力會設定成低於進行處 理時所施加之局頻電力(例如5 0 0 W左右)’且最好是形 成藉由電漿之作用,讓半導體晶圓 W之溫度不會上昇之The electrostatic chuck 4 includes a bipolar type and a unipolar type. In addition, these types also include a coulomb type and a Johnson-Lav eik type. Among them, when a unipolar and Coulomb-type electrostatic chuck 4 is used, it is preferable to perform the adsorption of the semiconductor wafer W according to the following procedure. The procedure is shown in Figure 6. The horizontal axis indicates time, the vertical axis indicates the application of high-frequency power 値 (W), and the solid line indicates the application of DC voltage 値 (V). That is, after the semiconductor wafer W is placed on the mounting table 2 (electrostatic chuck 4), introduction of gas into the vacuum chamber 1 is started. Next, as shown by a dotted line in FIG. 6, first, high-frequency power is applied to the stage 2 to generate plasma, and then, as shown by a solid line in FIG. 6, a DC voltage (HV) is applied to the electrostatic chuck electrode 4 a. ). In addition, because the semiconductor wafer W was not attracted to the electrostatic chuck 4 before the application of the DC voltage (HV) to the electrostatic chuck electrode 4a, the temperature control was not sufficiently advanced. Therefore, the high-frequency power applied to -15- (12) (12) 200410332 on the stage 2 when the electric power was first generated is set to be lower than the local-frequency power applied during processing (for example, 5 0 0 W or so) and it is best to form the semiconductor wafer W without increasing its temperature
方式C 接著,在將半導體晶圓W從靜電夾盤4取下之際, 亦如同圖所示,於電漿處理結束之後,首先,將施加高頻 電力値降低至低於進行處理時所施加之高頻電力之電力値 (並非0W )。之後,停止對靜電夾盤用電極4a施加直流 電壓(HV ),然後,停止施加高頻電力讓電漿消失。 又,在停止對靜電夾盤用電極4a施加直流電壓(HV )之 際,暫時對靜電夾盤用電極4a施加,極性與吸著時之極 性相反之電壓(例如負2 0 0 0 V左右),以除去電荷,且 易於取下半導體晶圓W。施加該種極性相反之電壓方面須 因應需要而進行,至於不進行施加極性相反之電壓亦能將 半導體晶圓W從靜電夾盤4輕易地取下之場合,便不進 行極性相反之電壓之施加。 第7圖顯示,如上述由靜電夾盤4吸著半導體晶圓W 之程序進行時,靜電夾盤(ESC)之銅製電極部(Cu)及 聚醯胺製絕緣膜部(PI ),與多層半導體晶圓(Multi Layer Wafer )之背面氧化膜部(B.S. Ox )及矽基板部(Si sub )及氧化膜部(0x ),與真空室內之處理空間部 (Space )及上部電極部(Wall )等各部的電位變化。 如同圖所示,首先,使被設於載置台2之晶圓支撐用 之栓下降以將半導體晶圓W載置於載置台2上,如圖中 -16- (13) 200410332 ①所示,各部之電位爲零的狀態,之後,對真空室 始導入氣體時亦如圖中②所示,各部之電位爲零的 之後,當開始施加高頻電力產生電漿,如圖 示’半導體晶圓W之電位成爲決定於電漿之狀 100V左右之電位。 接著,於該狀態下,當開始對靜電夾盤用電極 加直流電壓(Η V ),如圖中④所示,靜電夾盤用1 之電位成爲施加之直流電壓(HV )之電位(例如 左右),且於絕緣膜部(ΡI )產生電位差而進行吸 體晶圓W。 如此,若依照上述由靜電夾盤4吸著半導體( 之程序,因爲在半導體晶圓 W表面不會伴隨對靜 用電極4a施加直流電壓(HV )而施加高的電壓, 止在半導體晶圓W表面產生非期待之異常放電。 又,第2實施例說明至此,就施加高頻電力後 流電壓之程序方面,具有如以下所說明之效果。 第9圖所示之程序,亦即若進行在電漿處理開 靜電夾盤用電極4 a施加直流電壓後朝下部電極( 部電極)施加高頻電力’及在電漿處理結束後,高 OFF後之直流電壓OFF,則在使半導體晶圓W吸 離脫時,如第1 〇圖所不’會對半導體晶圓w施加 壓。因此,在半導體晶圓w可能發生損傷,具體 能發生直徑數十a m左右的缺陷’該缺陷發生場所 刻中引起弧光,造成製品不良。此外’缺陷會形成 1內開 狀態。 中③所 態之負 4a施 t極 4a 1 .5KV 著半導 晶圓 w 電夾盤 故能防 施加直 始時朝 或者上 頻電力 著或者 大的電 而言可 會在蝕 田5 业丄 賴丰ϋ , -17- (14) (14)200410332 也會造成附著於半導體晶圓W之情況。 但是,本實施例說明至此,所謂在處理開始時RF ON— HV ON,在處理結束時 HV OFF— RF OFF之 程序之場合,因爲不會對半導體晶圓施加高電壓’所以不 會對半導體晶圓W造成損傷,而且能防止半導體晶圓w 表面弧光。 此外,依第9圖之程序,即使在半導體晶圓W表面 不會造成損傷之場合,因爲隨著對靜電夾盤用電極4 a施 加直流電壓導致半導體晶圓 W帶電,故可能造成該靜電 力所導致在處理室內通常浮遊之帶電顆粒會附著於半導體 晶圓w。 但是,所謂在處理開始時RF ON— HV ON,在處 理結束時HV OFF— RF OFF之程序之場合,因爲在對 靜電夾盤施加直流電壓前會持續高頻放電,所以浮遊之帶 電顆粒會被捕捉至離子層中,結果能使附著於半導體晶圓 W之顆粒減少。亦有該種效果。 以下,顯示檢證離子層之捕捉效果。 第1 1圖顯示根據用以吸著半導體晶圓W之靜電夾盤 之直流施加電壓的大小不同所導致附著顆粒數不同之調查 結果。 亦即顯示,首先,使成爲顆粒發生源之CF系之反應 物附著(護套處理(sheathing))於電漿處理裝置之處理 室內,之後,將半導體晶圓 W搬入處理室內載置於靜電 夾盤上並使處理氣體流通一定時間,然後,進行半導體晶 -18- (15) (15)200410332 圓w之除電後搬出處理室內,將附著於半導體晶圓W之 顆粒數,依顆粒大小分成3種類,計算該3種大小顆粒之 顆粒數,將靜電夾盤之直流電壓設定成〇 V、1 . 5 k V、 2.0 k V、2.5 k V ,就種種場合調查後之結果。 如同圖所示可知,若提高靜電夾盤之直流施加電壓, 則附著於半導體晶圓 W之顆粒數會增加。亦即可知,朝 靜電夾盤施加之直流電壓會對半導體晶圓w之顆粒的附 著造成影響。 又,上述護套處理工程之處理條件爲··壓力: 6.65Pa、高頻電力:3500W、使用氣體:C4F8/Ar/ CH2F2=13/600/5sccm、晶圓背面壓力(中央/周 緣):1 3 3 0 / 3 9 9 0 P a、溫度(頂部/側壁/底部):6 〇 / 6 0 / 6 0 °C、高頻施加時間:3分鐘。 此外,將半導體晶圓W配置於靜電夾盤上使氣體流^ 通之際的壓力、使用氣體、晶圓背面壓力、溫度的條丨牛I系 與上述相同,而局頻電力=〇、氣體流通時間爲6 〇秒、。 再者,上述除電工程方面,係於壓力:26.6 Pa、施_ 電壓:一1 .5kV、電壓施加時間:1秒、以及壓力. 5 3 · 2 P a、N 2 : 1 0 0 0 s c c m、時間:1 5秒之條件下進行半導 體晶圓W之除電,並於施加電壓:一 2 · Ok V、電壓施加日$ 間:1秒之條件下進行靜電夾盤之除電。又,因爲以該$ 式進行除電係在製程結束後之搬送半導體W之際^ _ 體晶圓W跳脫則有招致無益之顆粒再附著之虞,$ ^ 之,藉由除電,使不發生該種半導體晶圓W彈起之_ -19- (16) (16)200410332 形。 此外,第1 2圖係顯示:在上述護套處理工程之後, 將半導體晶圓W配置於處理室內,在該狀態下進行0 2乾 式淸洗後使護套處理工程中附著之反應物發生多數之顆 粒,針對所謂在處理開始時RF ON-> HV ON、在處理 結束時HV OFF— RF OFF之程序之場合,與所謂在處 理開始時 HV ON— RF ON、在處理結束時 RF OFF -> Η V 〇 F F之程序之場合,測定附著於半導體晶圓W之 顆粒數之結果。又,關於測定方面,護套處理工程及除電 工程係與前述之場合相同,而02乾式淸洗工程之處理條 件爲:壓力:13.3Pa、高頻電力:1 000W、使用氣體: 〇2=l〇〇〇sccm、晶圓背面壓力(中央/周緣):1330/ 3 9 9 0 P a、溫度(頂部/側壁/底部):6 0 / 6 0 / 6 0 °C、高 頻施加時間:3 0秒。 如同圖所示,藉由採用所謂在處理開始時RF ON — HV ON、在處理結束時HV OFF— RF OFF之程序, 能使附著之顆粒數大幅減少。 又,如第8圖所示之程序,在將半導體晶圓以被設於 載置台2之晶圓支撐用之栓(支撐棒)支撐之狀態(①) 下開始對靜電夾盤用電極 4a施加直流電壓(HV ) (②),之後,使晶圓支撐用之栓下降以將半導體晶圓w 載置於載置台2上(③、④),即使在吸著半導體晶圓W 之場合,亦不會使半導體晶圓W之表面成爲施加之直流 電壓(HV )之電位。因此,即使藉由該方式之吸著程 -20- (17) 200410332 序,亦能防止在半導體晶圓 W之表面產生非預期之異常 放電。但是,該方式之程序方面’晶圓支撐用之栓爲導電 性,而非得形成從該栓供給電荷至半導體晶圓 W之構成 才能進行。 此外,上述方式之利用靜電夾盤吸著之際所產生之異 常放電方面,同樣地,即使是庫侖型之靜電夾盤,如使用 雙極型之靜電夾盤,亦能防止異常放電。Method C Next, when the semiconductor wafer W is removed from the electrostatic chuck 4, as shown in the figure, after the plasma processing is completed, first, the high-frequency power 値 is reduced to less than that applied during processing. The power of high-frequency power (not 0W). After that, the application of the DC voltage (HV) to the electrostatic chuck electrode 4a is stopped, and then the application of high-frequency power is stopped so that the plasma disappears. In addition, when the application of a DC voltage (HV) to the electrostatic chuck electrode 4a is stopped, a voltage having a polarity opposite to that at the time of adsorption is temporarily applied to the electrostatic chuck electrode 4a (for example, about 2 0 0 0 V). To remove the charge and to easily remove the semiconductor wafer W. The application of the voltage of the opposite polarity must be carried out as required. As long as the semiconductor wafer W can be easily removed from the electrostatic chuck 4 without the application of the voltage of the opposite polarity, the application of the voltage of the opposite polarity is not performed. . FIG. 7 shows that when the semiconductor wafer W is attracted by the electrostatic chuck 4 as described above, the copper electrode portion (Cu) of the electrostatic chuck (ESC) and the polyimide insulation film portion (PI), and the multilayer Backside oxide film portion (BS Ox) and silicon substrate portion (Si sub) and oxide film portion (0x) of the semiconductor wafer (Multi Layer Wafer), and processing space portion (Space) and upper electrode portion (Wall) in the vacuum chamber Wait for the potential of each part to change. As shown in the figure, first, the wafer supporting pins provided on the mounting table 2 are lowered to place the semiconductor wafer W on the mounting table 2, as shown in -16- (13) 200410332 ①, The state of the potential of each part is zero. After that, when the gas is introduced into the vacuum chamber, it is also shown as ② in the figure. After the potential of each part is zero, the high-frequency power is applied to generate plasma, as shown in the figure. The potential of W becomes a potential that is about 100 V depending on the state of the plasma. Then, in this state, when a DC voltage (Η V) is applied to the electrode for the electrostatic chuck, as shown by (4) in the figure, the potential of the electrostatic chuck 1 becomes the potential of the applied DC voltage (HV) (for example, left and right). ), And a potential difference is generated in the insulating film portion (PI) to perform the getter wafer W. In this way, if the semiconductor is sucked by the electrostatic chuck 4 in accordance with the above-mentioned procedure, because a high voltage is not applied to the surface of the semiconductor wafer W along with the application of a DC voltage (HV) to the static electrode 4a, the semiconductor wafer W is stopped. Unexpected abnormal discharge occurs on the surface. The second embodiment has been described so far, and the procedure of applying a high-frequency power after-flow voltage has the following effects. The procedure shown in FIG. Plasma treatment opens the electrostatic chuck electrode 4 a. After applying a DC voltage, high-frequency power is applied to the lower electrode (part electrode) and after the plasma treatment is completed, the DC voltage after the high OFF is turned off. At the time of suction and release, the pressure on the semiconductor wafer w is not applied as shown in Fig. 10. Therefore, the semiconductor wafer w may be damaged, and a defect having a diameter of about several tens of am may be generated. Causes arc light, resulting in defective products. In addition, 'defects will form an internal open state. The negative 4a and t pole 4a 1 .5KV in the state ③ are on the semiconducting wafer w electric chuck, so it can prevent the application from facing up or up. frequency In the case of electric power or large electricity, it may occur in the etch field 5 and Lai Fengye, -17- (14) (14) 200410332 may also cause the situation of attaching to the semiconductor wafer W. However, this embodiment has been described so far. In the process of RF ON—HV ON at the start of processing and HV OFF—RF OFF at the end of processing, the semiconductor wafer W will not be damaged because high voltage is not applied to the semiconductor wafer, and it can prevent Arc on the surface of the semiconductor wafer w. In addition, according to the procedure of FIG. 9, even if the surface of the semiconductor wafer W does not cause damage, the semiconductor wafer W is charged with a DC voltage applied to the electrostatic chuck electrode 4 a. Therefore, the electrostatic force may cause the charged particles normally floating in the processing chamber to attach to the semiconductor wafer w. However, the so-called RF ON- HV ON at the beginning of processing and the HV OFF- RF OFF procedure at the end of processing In this case, because a high-frequency discharge continues until a DC voltage is applied to the electrostatic chuck, floating charged particles are trapped in the ion layer, and as a result, particles attached to the semiconductor wafer W can be caused. This effect is also shown below. The capture effect of the verification ion layer is shown below. Figure 11 shows the number of particles attached due to the difference in the applied DC voltage of the electrostatic chuck used to attract the semiconductor wafer W. That is, it was shown that, first, a CF-based reactant, which is a source of particle generation, was attached (sheathing) in a processing chamber of a plasma processing apparatus, and then the semiconductor wafer W was carried into the processing chamber to load Place it on an electrostatic chuck and let the process gas circulate for a certain period of time. Then, remove the semiconductor wafer-18- (15) (15) 200410332 round w and remove it from the processing chamber. The number of particles attached to the semiconductor wafer W is determined by The particle size is divided into 3 types, and the number of particles of the 3 types of particles is calculated. The DC voltage of the electrostatic chuck is set to 0V, 1.5kV, 2.0kV, and 2.5kV, and the results are investigated on various occasions. As shown in the figure, if the DC applied voltage of the electrostatic chuck is increased, the number of particles attached to the semiconductor wafer W will increase. In other words, it is known that the DC voltage applied to the electrostatic chuck will affect the attachment of particles on the semiconductor wafer w. In addition, the processing conditions of the sheath processing project are: pressure: 6.65Pa, high-frequency power: 3500W, gas used: C4F8 / Ar / CH2F2 = 13/600 / 5sccm, pressure on the backside of the wafer (central / peripheral): 1 3 3 0/3 9 9 0 Pa, temperature (top / side wall / bottom): 6 0/60/60 ° C, high frequency application time: 3 minutes. In addition, the semiconductor wafer W is arranged on an electrostatic chuck to make the gas flow ^ the pressure, the gas used, the pressure on the back of the wafer, and the temperature are the same as above, and the local frequency power = 0, the gas The circulation time is 60 seconds. Moreover, the above static elimination engineering aspects are based on pressure: 26.6 Pa, applied voltage: -1.5kV, voltage application time: 1 second, and pressure. 5 3 · 2 P a, N 2: 1 0 0 0 sccm, Time: 15 seconds to perform the static elimination of the semiconductor wafer W, and to perform electrostatic elimination of the electrostatic chuck under the conditions of applied voltage:-2 · Ok V, voltage application date: 1 second. In addition, because the $ type static elimination is performed when the semiconductor W is transported after the end of the process ^ _ bulk wafer W is off, which may cause unwanted re-attachment of particles. In the case of $ ^, by eliminating electricity, it does not occur. This type of semiconductor wafer W pops up in the shape of -19- (16) (16) 200410332. In addition, Fig. 12 shows that after the above-mentioned sheath processing process, the semiconductor wafer W is arranged in a processing chamber, and in this state, the dry reacting is performed to cause a large number of reactants attached to the sheath processing process. The particles are for the program called RF ON- > HV ON at the start of processing, HV OFF- RF OFF at the end of processing, and HV ON- RF ON at the start of processing, and RF OFF at the end of processing- > In the case of the ΗV FF program, the number of particles attached to the semiconductor wafer W was measured. In terms of measurement, the sheath treatment process and the static elimination process are the same as those described above, and the processing conditions of the 02 dry cleaning process are: pressure: 13.3Pa, high-frequency power: 1,000W, and gas: 〇2 = 1 〇〇〇sccm, wafer back pressure (central / peripheral): 1330/3 9 9 0 P a, temperature (top / side wall / bottom): 6 0/6 0/60 ° C, high frequency application time: 3 0 seconds. As shown in the figure, by adopting a program called RF ON—HV ON at the beginning of processing and HV OFF—RF OFF at the end of processing, the number of attached particles can be greatly reduced. Further, as shown in the procedure shown in FIG. 8, the application of the electrostatic chuck electrode 4 a is started in a state (①) in which a semiconductor wafer is supported by a wafer support pin (support rod) provided on the mounting table 2. After the DC voltage (HV) (②), the wafer support pins are lowered to place the semiconductor wafer w on the mounting table 2 (③, ④), even when the semiconductor wafer W is being held. The surface of the semiconductor wafer W does not become a potential of the applied DC voltage (HV). Therefore, even by the sorption process of this method -20- (17) 200410332, it is possible to prevent the occurrence of an unexpected abnormal discharge on the surface of the semiconductor wafer W. However, in this method, the pin for wafer support is conductive, and it is not necessary to form a structure in which a charge is supplied to the semiconductor wafer W from the pin. In addition, with regard to the abnormal discharge generated when the electrostatic chuck is used in the above manner, even a Coulomb-type electrostatic chuck, such as a bipolar electrostatic chuck, can prevent abnormal discharge.
又,以上之例中,針對使用平行平板型蝕刻裝置之蝕 刻處理的實施型態加以說明,然本發明並不侷限於該實施 型態,而當然可以使用於所謂的電漿處理。此外,上述實 施型態中,針對在進行蝕刻處理之蝕刻裝置之真空室內使 弱的電漿發揮作用之場合加以說明,然亦能在進行處理之 裝置之其他場所使弱的電漿發揮作用,並初期化半導體晶 圓W。In the above example, an embodiment of the etching process using a parallel plate type etching apparatus is described. However, the present invention is not limited to this embodiment, but it can be applied to a so-called plasma process. In addition, in the above-mentioned embodiment, the case where a weak plasma is made to function in the vacuum chamber of the etching device that performs the etching process is described, but the weak plasma can also be made to function in other places of the processing device. And the semiconductor wafer W is initialized.
如以上δ羊細說明’根據本發明,能防止被處理基板所 產生之表面弧光之發生,且相較於以往能謀求生產性之提 升。 產業上之利用可能性 關於本發明之電漿處理方法及電漿處理裝置係能使用 於進行半導體裝置之製造之半導體製造產業等。所以,具 有產業上之利用可能性。 【圖式簡單說明】 -21 - (18) 200410332 第1圖係使用於本發明之一實施型態之裝置之槪略構 成的模式圖。 第2圖係用以說明關於本發明之一實施型態之電漿處 理方法之圖。 第3圖係使用於本發明之其他實施型態之裝置之槪略 構成的模式圖。As described in the above [delta], according to the present invention, the occurrence of surface arcs on the substrate to be processed can be prevented, and the productivity can be improved compared with the past. Industrial Applicability The plasma processing method and the plasma processing apparatus of the present invention are applicable to the semiconductor manufacturing industry for manufacturing semiconductor devices. Therefore, there are industrial possibilities. [Brief description of the drawings] -21-(18) 200410332 The first diagram is a schematic diagram of the general structure of a device used in one embodiment of the present invention. Fig. 2 is a diagram for explaining a plasma processing method according to an embodiment of the present invention. Fig. 3 is a schematic diagram of a schematic configuration of a device used in another embodiment of the present invention.
第4圖係用以說明關於本發明之其他實施型態之電漿 處理方法之圖。 第5圖係用以說明關於第2圖所示之實施型態之變形 例之電漿處理方法之圖。 第6圖係用以說明依照靜電夾盤之夾盤方法之圖。 第7圖係用以說明第6圖之夾盤方法之各部的電位變 化之圖。 第8圖係用以說明其他之夾盤方法之各部的電位變化 之圖。Fig. 4 is a diagram for explaining a plasma processing method according to another embodiment of the present invention. Fig. 5 is a diagram for explaining a plasma processing method according to a modified example of the embodiment shown in Fig. 2; FIG. 6 is a diagram for explaining a chuck method according to an electrostatic chuck. Fig. 7 is a diagram for explaining changes in potential of each part of the chuck method of Fig. 6; Fig. 8 is a diagram for explaining potential changes in each part of other chuck methods.
第9圖係用以說明依照靜電夾盤之夾盤方法之比較例 之圖。 第1 〇圖係用以說明第9圖之夾盤方法之各部的電位 變化之圖。 第Π圖係顯示靜電夾盤之施加電壓與顆粒數之關係 圖。 第1 2圖係顯示程序不同造成顆粒數不同之圖。 圖號說明 -22- (19)200410332 w 半 導 體 晶圓 1 真 空 室 2 載 置 台 η j 絕 緣 板 4 靜 電 夾 盤 5 直 流 電 源 6 埶 媒 體 流路 7 氣 體 流 路 8 聚 隹 環 9 給 電 線 10 整 合 器 11 局 頻 電 源 -23-Fig. 9 is a diagram for explaining a comparative example of the chuck method according to the electrostatic chuck. Fig. 10 is a diagram for explaining potential changes in each part of the chuck method of Fig. 9. Figure Π shows the relationship between the voltage applied to the electrostatic chuck and the number of particles. Figure 12 shows the number of particles caused by different procedures. Figure number description-22- (19) 200410332 w Semiconductor wafer 1 Vacuum chamber 2 Mounting stage η j Insulation plate 4 Electrostatic chuck 5 DC power supply 6 Media flow path 7 Gas flow path 8 Polycondensation ring 9 Feeder wire 10 Integrator 11 Office Frequency Power
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| JP2002256096A JP4322484B2 (en) | 2002-08-30 | 2002-08-30 | Plasma processing method and plasma processing apparatus |
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| TWI324361B TWI324361B (en) | 2010-05-01 |
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| TW092123978A TW200410332A (en) | 2002-08-30 | 2003-08-29 | Method and device for plasma treatment |
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| JP (1) | JP4322484B2 (en) |
| KR (1) | KR100782621B1 (en) |
| CN (1) | CN100414672C (en) |
| AU (1) | AU2003261790A1 (en) |
| TW (1) | TW200410332A (en) |
| WO (1) | WO2004021427A1 (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI424792B (en) * | 2005-03-31 | 2014-01-21 | Tokyo Electron Ltd | Plasma processing device and plasma processing method |
| TWI463597B (en) * | 2010-12-16 | 2014-12-01 | 應用材料股份有限公司 | High efficiency electrostatic chuck assembly for semiconductor wafer processing |
| TWI595557B (en) * | 2014-02-28 | 2017-08-11 | 愛發科股份有限公司 | Plasma etching method, plasma etching device, plasma processing method, and plasma processing device |
| TWI697940B (en) * | 2016-02-26 | 2020-07-01 | 美商得昇科技股份有限公司 | Implanted photoresist stripping process by layers using inductively coupled plasma strippers |
| TWI698928B (en) * | 2015-01-06 | 2020-07-11 | 日商東京威力科創股份有限公司 | Plasma processing method |
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| US7205250B2 (en) * | 2003-03-18 | 2007-04-17 | Matsushita Electric Industrial Co., Ltd. | Plasma processing method and apparatus |
| US7316785B2 (en) * | 2004-06-30 | 2008-01-08 | Lam Research Corporation | Methods and apparatus for the optimization of etch resistance in a plasma processing system |
| CN100416758C (en) * | 2005-12-09 | 2008-09-03 | 北京北方微电子基地设备工艺研究中心有限责任公司 | A method for completely releasing static electricity from electrostatic chucks in wafer etching equipment |
| CN101740340B (en) * | 2008-11-25 | 2011-12-21 | 北京北方微电子基地设备工艺研究中心有限责任公司 | Reaction chamber and semiconductor processing device |
| JP2010199310A (en) * | 2009-02-25 | 2010-09-09 | Sharp Corp | Plasma etching method |
| JP5835985B2 (en) * | 2010-09-16 | 2015-12-24 | 東京エレクトロン株式会社 | Plasma processing apparatus and plasma processing method |
| WO2014049915A1 (en) * | 2012-09-26 | 2014-04-03 | シャープ株式会社 | Substrate treatment device, substrate treatment method, and production method for semiconductor device |
| JP6595334B2 (en) * | 2015-12-28 | 2019-10-23 | 株式会社日立ハイテクノロジーズ | Plasma processing apparatus and plasma processing method |
| US10535505B2 (en) * | 2016-11-11 | 2020-01-14 | Lam Research Corporation | Plasma light up suppression |
| US20190119815A1 (en) * | 2017-10-24 | 2019-04-25 | Applied Materials, Inc. | Systems and processes for plasma filtering |
| SG11202105295TA (en) * | 2018-12-13 | 2021-06-29 | Applied Materials Inc | Methods for depositing phosphorus-doped silicon nitride films |
| WO2020214607A1 (en) | 2019-04-15 | 2020-10-22 | Applied Materials, Inc. | Electrostatic chucking process |
| JP7482657B2 (en) * | 2020-03-17 | 2024-05-14 | 東京エレクトロン株式会社 | CLEANING METHOD AND SEMICONDUCTOR DEVICE MANUFACTURING METHOD |
| CN113154610A (en) * | 2021-05-31 | 2021-07-23 | 北京十三和科技发展有限公司 | Air purifier with temperature adjusting function |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06318552A (en) * | 1993-05-10 | 1994-11-15 | Nissin Electric Co Ltd | Plasma processing and its apparatus |
| JPH1027780A (en) * | 1996-07-10 | 1998-01-27 | Nec Corp | Plasma treating method |
| JP3907256B2 (en) * | 1997-01-10 | 2007-04-18 | 芝浦メカトロニクス株式会社 | Electrostatic chuck device for vacuum processing equipment |
| KR100635975B1 (en) * | 2000-02-14 | 2006-10-20 | 동경 엘렉트론 주식회사 | Apparatus and method for plasma treatment |
-
2002
- 2002-08-30 JP JP2002256096A patent/JP4322484B2/en not_active Expired - Fee Related
-
2003
- 2003-08-28 AU AU2003261790A patent/AU2003261790A1/en not_active Abandoned
- 2003-08-28 KR KR1020057003051A patent/KR100782621B1/en not_active Expired - Fee Related
- 2003-08-28 WO PCT/JP2003/010937 patent/WO2004021427A1/en not_active Ceased
- 2003-08-28 CN CNB038206455A patent/CN100414672C/en not_active Expired - Lifetime
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI424792B (en) * | 2005-03-31 | 2014-01-21 | Tokyo Electron Ltd | Plasma processing device and plasma processing method |
| TWI463597B (en) * | 2010-12-16 | 2014-12-01 | 應用材料股份有限公司 | High efficiency electrostatic chuck assembly for semiconductor wafer processing |
| TWI595557B (en) * | 2014-02-28 | 2017-08-11 | 愛發科股份有限公司 | Plasma etching method, plasma etching device, plasma processing method, and plasma processing device |
| TWI698928B (en) * | 2015-01-06 | 2020-07-11 | 日商東京威力科創股份有限公司 | Plasma processing method |
| TWI697940B (en) * | 2016-02-26 | 2020-07-01 | 美商得昇科技股份有限公司 | Implanted photoresist stripping process by layers using inductively coupled plasma strippers |
Also Published As
| Publication number | Publication date |
|---|---|
| CN1679148A (en) | 2005-10-05 |
| TWI324361B (en) | 2010-05-01 |
| KR100782621B1 (en) | 2007-12-06 |
| CN100414672C (en) | 2008-08-27 |
| AU2003261790A1 (en) | 2004-03-19 |
| JP4322484B2 (en) | 2009-09-02 |
| JP2004095909A (en) | 2004-03-25 |
| WO2004021427A1 (en) | 2004-03-11 |
| KR20050058464A (en) | 2005-06-16 |
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