TW200948219A - Plasma processing apparatus and method - Google Patents

Plasma processing apparatus and method Download PDF

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Publication number
TW200948219A
TW200948219A TW098112045A TW98112045A TW200948219A TW 200948219 A TW200948219 A TW 200948219A TW 098112045 A TW098112045 A TW 098112045A TW 98112045 A TW98112045 A TW 98112045A TW 200948219 A TW200948219 A TW 200948219A
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Taiwan
Prior art keywords
gas
processing chamber
chamber
locations
plasma
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TW098112045A
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Chinese (zh)
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TWI563882B (en
Inventor
Gaku Furuta
Young-Jin Choi
Soo-Young Choi
Beom-Soo Park
John M White
Suhail Anwar
Robin L Tiner
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Applied Materials Inc
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Priority claimed from US12/271,616 external-priority patent/US20090255798A1/en
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Publication of TW200948219A publication Critical patent/TW200948219A/en
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Publication of TWI563882B publication Critical patent/TWI563882B/en

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    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/50Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges
    • C23C16/505Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges using radio frequency discharges
    • C23C16/509Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges using radio frequency discharges using internal electrodes
    • C23C16/5096Flat-bed apparatus
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/4401Means for minimising impurities, e.g. dust, moisture or residual gas, in the reaction chamber
    • C23C16/4405Cleaning of reactor or parts inside the reactor by using reactive gases
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45561Gas plumbing upstream of the reaction chamber
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45563Gas nozzles
    • C23C16/45565Shower nozzles
    • 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
    • H01J37/32357Generation remote from the workpiece, e.g. down-stream
    • 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
    • H01J37/3244Gas supply means
    • H01J37/32449Gas control, e.g. control of the gas flow
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • General Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Plasma & Fusion (AREA)
  • Analytical Chemistry (AREA)
  • Manufacturing & Machinery (AREA)
  • Electromagnetism (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Chemical Vapour Deposition (AREA)
  • Plasma Technology (AREA)

Abstract

The present invention generally includes a plasma enhanced chemical vapor deposition (PECVD) processing chamber having an RF power source coupled to the backing plate at a location separate from the gas source. By feeding the gas into the processing chamber at a location separate from the RF power, parasitic plasma formation in the gas tubes leading to the processing chamber may be reduced. The gas may be fed to the chamber at a plurality of locations. At each location, the gas may be fed to the processing chamber from the gas source by passing through a remote plasma source as well as an RF choke or RF resistor.

Description

200948219 六、發明說明: 【發明所屬之技術領域】 本發明實施例大致係關於處理腔室,其之功率供應在 與氣體供應分隔位置處耦接至處理腔室。 【先前技術】 隨著較大平板顯示器與太陽能面板的需求持續增加, φ 因此基材與處理腔室的尺寸必然得提高。隨著處理腔室 尺寸提高,有時需要較高的RF電流以補償RF電流的消 散(隨著RF電流移動離開RF源而發生)。一種沉積材料 於平板顯示器或太陽能面板之基材上的方法係電漿增強 化學氣相沉積(PECVD)。電漿增強化學氣相沉積中,可 透過喷頭將處理氣體導入處理腔室並藉由施加至喷頭之 RF電流點燃成電漿。隨著基材尺寸提高,施加至喷頭之 RF電流亦對應地增加。隨著RF電流的增加,氣體經過 V 喷頭之前的氣體過早分解以及喷頭上方寄生電漿形成的 可能性提高。 因此,技藝中需要允許傳送足夠RF電流同時減少寄生 •電漿形成的設備。 【發明内容】 本發明大致包括PECVD處理腔室,其具有在與氣源分 隔位置處耦接至背板之RF功率源。藉由在與RF功率分 4 200948219 隔位置處供給氣體進入處理腔室,可減少通到處理腔室 之氣體管中形成寄生電漿。可在複數個位置供給氣趙至 腔室。各個位置上,氣源可藉由經過遠端電漿源以及RF 扼流器或RF電阻器而供給氣體至處理腔室。200948219 VI. Description of the Invention: [Technical Field of the Invention] Embodiments of the present invention generally relate to a processing chamber to which a power supply is coupled to a processing chamber at a gas supply separation location. [Prior Art] As the demand for larger flat panel displays and solar panels continues to increase, φ is therefore inevitably increased in size of the substrate and the processing chamber. As the processing chamber size increases, higher RF currents are sometimes required to compensate for the dissipation of RF current (which occurs as the RF current moves away from the RF source). One method of depositing material on a substrate of a flat panel display or solar panel is plasma enhanced chemical vapor deposition (PECVD). In plasma enhanced chemical vapor deposition, a process gas can be introduced into the processing chamber through a showerhead and ignited into a plasma by an RF current applied to the showerhead. As the substrate size increases, the RF current applied to the showerhead also increases correspondingly. As the RF current increases, the premature decomposition of the gas before passing the V nozzle and the possibility of parasitic plasma formation above the nozzle increase. Therefore, there is a need in the art for equipment that allows for the transfer of sufficient RF current while reducing parasitic plasma formation. SUMMARY OF THE INVENTION The present invention generally includes a PECVD processing chamber having an RF power source coupled to a backplane at a location spaced from a source of gas. By supplying gas into the processing chamber at a location spaced from RF power 4 200948219, parasitic plasma can be reduced in the gas tubes that pass into the processing chamber. The gas can be supplied to the chamber at a plurality of locations. At various locations, the gas source can supply gas to the processing chamber by passing through a remote plasma source and an RF choke or RF resistor.

一實施例中’揭露電漿處理設備。設備包括處理腔室, 其具有氣體分配板與大致矩形背板;一或更多功率源, 在一或更多第一位置處耦接至背板;及一或更多氣源, 在三個其他位置處耦接至背板,三個其他位置各自與一 或更多第一位置有所分隔》三個位置之第一個係置於背 板之兩個平行側邊之間實質相等距離處。 另一實施例中,揭露電漿增強化學氣相沉積設備。設 備包括處理腔室,其具有穿過至少一壁之狹縫閥開口; 及氣體分配喷頭,置於處理腔室中並與基材支撐件有所 間隔。設備亦包括置於氣體分配喷頭後並與其有所間隔In one embodiment, the plasma processing apparatus is disclosed. The apparatus includes a processing chamber having a gas distribution plate and a generally rectangular backing plate; one or more power sources coupled to the backing plate at one or more first locations; and one or more gas sources, in three The other locations are coupled to the backplane, and the three other locations are each separated from the one or more first locations. The first of the three locations is placed at substantially equal distances between the two parallel sides of the backplane. . In another embodiment, a plasma enhanced chemical vapor deposition apparatus is disclosed. The apparatus includes a processing chamber having a slit valve opening through at least one of the walls; and a gas distribution showerhead disposed in the processing chamber and spaced from the substrate support. The equipment also includes and is spaced behind the gas distribution nozzle

之背板。背板可具有在三個 將三個位置的第一位置比其 口而配置。設備亦可包括一 耦接至背板;及RF功率源, 置處耦接至背板。 位置穿過其之三個開口。可 他兩個位置更遠於狹縫閥開 或更多氣源,在三個位置處. 在與二個位置有所間隔之位 另一實施例中,揭露一方法。方法包括透過第一位置 將處理氣體導入腔室、點燃處理氣體成電聚、並沉積材 料於基材上。方法亦包括將清潔氣體導入一或更多遠端 電漿源、在一或更多遠端電槳湃φ 漿源中點燃清潔氣體成電Back plate. The backing plate can have a configuration in which three first positions of three positions are compared to the other. The device can also include a coupling to the backplane; and an RF power source coupled to the backplane. Position through its three openings. The two positions may be further away from the slit valve opening or more air sources, at three locations. In a position spaced from the two positions, in another embodiment, a method is disclosed. The method includes introducing a process gas into the chamber through the first location, igniting the process gas to electropolymerize, and depositing the material on the substrate. The method also includes introducing a cleaning gas into one or more remote plasma sources, igniting the cleaning gas into electricity in one or more remote electrospray 湃 φ pulp sources

漿、並透過第一位置與至少一盘笛 .._ N 與第一位置分隔之其他位 200948219 置由遠端點燃之清潔氣體電漿將自由基流入腔室 【實施方式】 本發明大致包括PECVD4理腔室,其具有在與氣源分 隔位置處耦接至背板之以功率源。藉由在與rf功率分 隔位置處供給氣體進人處理腔室,可❹㈣處理腔室 之,體管中形成寄生電漿。可在複數個位置供給氣體至 腔至。各個位置上,氣源可藉由通過遠端電衆源以及rf 扼流器或RF電阻器而供給氣體至處理腔室。 參照處理大面積基材之化學氣相沉積系統例示性地描 述本發明於下,例如得自AppHed Matedals,inc⑺⑽匕Pulp, and through the first position and at least one flute.._N separated from the first position 200948219, the remotely ignited cleaning gas plasma flows free radicals into the chamber [Embodiment] The present invention generally includes PECVD4 A chamber having a power source coupled to the backing plate at a location spaced from the source. By supplying gas into the processing chamber at the rf power separation location, the chamber can be processed (4) to form parasitic plasma in the body tube. Gas can be supplied to the chamber at a plurality of locations. At various locations, the gas source can supply gas to the processing chamber by passing through a remote source and an rf choke or RF resistor. The invention is exemplarily described with reference to a chemical vapor deposition system for processing large-area substrates, such as from AppHed Matedals, inc(7)(10).

Clara,California)之分公司 AKT America,Inc.的 PECVD 系統。然而,應當理解設備與方法可用於其他系統結構 中,包括那些設以處理圓形基材之系統。 第1圖係根據本發明一實施例耦接至處理腔室丨〇〇之 功率源102與氣源104的概要圖示。如第1圖中所示, 功率源102在位置1 〇6耦接至處理腔室1 〇〇,位置1 〇6 不同於氣源104轉接至處理腔室1〇〇之位置1〇8A、1〇8B。 需理解雖然已經顯示兩個位置1〇8Α、i〇8B耦接氣源 104至處理腔室100,但位置i〇8A、i〇8b的數目並不限 於兩個。可應用單一位置108A、108B »或者,可應用超 過兩個位置108A、108B。當複數個位置i08A、l〇8B用 來耦接氣源104至處理腔室1〇〇時’可流至處理腔室1〇〇 200948219 複數個位置108A、108B之氣體係來自相同氣源1 〇4。一 實施例中,氣體流至處理腔室1〇〇之各個位置1〇8Α、1〇8B 可具有其本身專屬氣源104。 亦應理解雖然顯示單一位置1 〇6來耦接功率源1 〇2至 處理腔室100,但可在複數個位置丨〇6耦接功率源ioz 至處理腔室100。一實施例中,功率源102可包括RF功 率源。此外’雖然顯示功率源1 〇2在對應於處理腔室1 〇〇 之實質中心的位置106處耦接至處理腔室1〇〇,但功率 源102可在非對應於處理腔室ι〇〇之實質中心的位置ι〇6 處耦接至處理腔室100。 雖然顯示氣源104在位置l〇8A、108B(置於實質離開 處理腔室之中心)處耦接至處理腔室1〇〇,但位置1〇8Α、 108B並不如此受限。位置ι〇8Α、ι〇8Β可比位置1〇6(功 率源102耦接至處理腔室1〇〇之處)更接近處理腔室1〇〇 之中心。 第2A圖係根據本發明一實施例之處理腔室2〇〇的概要 剖面圖。處理腔室200係PECVD腔室。處理腔室200 具有腔室主體208。腔室主體中,可配置基座204坐落 於氣體分配喷頭210對面。基材206可置於基座204上。 基材206可透過狹缝閥開口 222進入處理腔室200。可 藉由基座204提高與降低基材206以處理、移除與/或插 入基材206。 喷頭210可具有複數個氣體通道212,由上游側218 通過喷頭21 0至下游側22〇。喷頭210的下游側220係 200948219 處理過程中噴頭面對基材206的那側β 喷頭210係自基材206橫跨處理空間216而置於處理 腔室2〇〇中。喷頭21〇後方存在有氣室214。氣室'Μ 係介於噴頭210與背板202之間。 可藉由功率源224提供功率給喷頭21〇,功率源224 係透過供給線226耦接至背板202。_實施例中,功率 源224可包括RF功率源。顯示之實施例中,供給線226 在對應於背板202之實質中心的位置耦接至背板2〇2。 可理解功率源224也可在其他位置處耦接至背板2〇2。 可由氣源234傳送處理氣體通過背板202至處理腔室 2〇〇。來自氣源234之氣體在到達處理腔室2〇〇之前可移 動通過遠端電衆源2 2 8。一實施例中,經過遠端電漿源 228之處理氣體係用於沉積,因此不在遠端電漿源228 中點燃成電漿。另一實施例中,來自氣源234之氣體可 在遠端電漿源228中被點燃成電漿並接著送至處理腔室 〇 2〇〇°來自遠端電漿源228之電漿可清潔處理腔室200及 其中暴露部件。此外’電漿會清潔氣體在遠端電漿源228 之後經過之冷卻塊230與扼流器或電阻器232。 在遠端電漿源228中點燃電漿時,遠端電漿源228會 變得非常熱。因此’可將冷卻塊230置於扼流器或電阻 器232與遠端電漿源228之間,以確保扼流器或電阻器 232不因遠端電漿源228的高溫而斷裂。 可理解雖然已經顯示兩個分隔的氣源234,但遠端電 聚源228可共有相同的氣源234。此外,雖然顯示遠端 8 200948219 電漿源228耦接於各個氣源234與背板之間,但處理腔 室200可具有更多或更少遠端電漿源228與其耦接。 第2B圖係第2A圖之處理腔室200的概要剖面圖,其 顯示RF電流路徑。RF電流具有「集膚效應(skin effect)」’藉此RF電流在導電體之外表面上移動並僅穿 透物體i某一深度。因此,對足夠厚的物體而言,物體内 部可具有零可偵測R F電流,同時外表面具有流於其上之 RF電流並被視為RF「熱」^ 箭頭「A」顯示RF電流由功率源224至喷頭2^0採取 之路徑。RF電流由功率源224沿著供給線226移動β位 置236上,RF電流碰見背板202並沿著背板202之背面 流動並向下至喷頭210的下游面220。 氣體在位置238處穿過背板202進入處理腔室2〇〇。 箭頭「Β」顯示位置238(氣體進入處理腔室2〇〇處)與位 置236(RF電流碰到背板202處)之間的距離。隨著RF電 流移動’其會傾向消散。換句話說,相對於更向下游線 路之功率水平而言,離開功率源224之RF電流具有較高 的功率水平。第2B圖顯示之實施例中,相對於沿著背= 2〇2流動通過位置238(氣體進入處理腔室2〇〇處)之 電流而言,位置236的RF電流具有較高的功率水平。由 於位置238的功率量低於位置236,可減少在包含進入 處理腔室2GG之氣體的管24G中點燃氣體的可能性。因 為管240中處理氣體點燃的可能性減少,可降低管238、 扼流器或電阻器232、冷卻塊23〇、遠端電漿源228以及 9 200948219 喷頭210後之氣室214中的寄生電漿形成。一實施例中, 管240可包括陶瓷材料。 第3圖係根據本發明一實施例之處理腔室3〇〇的背板 302的概要等角圖。可藉由在位置324處耦接RF功率源 304至背板302而供應RF功率至腔室300。雖然已經顯 示位置324對應背板302的實質中心,但可理解位置324 可位於责板324上許多其他點。此外,可同時應用超過 一個位置324 〇 相同氣源308可供應氣體至處理腔室3〇〇β可理每雖 然顯示單一氣源308,但可應用多個氣源308。可透過氣 體管310將來自氣源308之氣體供應至遠端電漿源3 〇6。 可理解雖然顯示四個遠端電漿源3〇6,但可應用更多更 少的遠端電漿源306。此外,雖然顯示遠端電漿源3〇6 置於背板302上’但可將遠端電漿源3〇6置於鄰接背板 302 處。 φ 來自氣源308之氣體經過氣體管310至遠端電漿源 306。若處理腔室300運作於清潔模式中,可將遠端電漿 源306中之氣體點燃成電漿並供給通過冷卻塊314與扼 流器或電阻器322至處理腔室300。然而,若處理腔室 運作於沉積模式中’氣體將通過遠端電漿源3 〇6而不點 燃成電敷。未點燃電漿的情況下,清潔氣體以非-電漿狀 態進入處理腔室並造成無效率的清潔。 若一遠端電漿源306失效或不有效運轉,則可關閉遠 端電漿源306。若其他遠端電漿源3〇6如所欲般運作, 200948219 則流過無運行之遠端電漿源306進入處理腔室300的清 潔氣體在進入處理腔室300之前不會點燃。上述態樣 中,處理腔室300無法有效地進行清潔。Branch of Clara, California AKT America, Inc.'s PECVD system. However, it should be understood that the apparatus and method can be used in other system configurations, including those designed to handle circular substrates. 1 is a schematic illustration of a power source 102 and a gas source 104 coupled to a processing chamber, in accordance with an embodiment of the present invention. As shown in FIG. 1, the power source 102 is coupled to the processing chamber 1 at position 1 〇6, and the position 1 〇6 is different from the position where the gas source 104 is transferred to the processing chamber 1〇〇1〇8A, 1〇8B. It is to be understood that although the two positions 1 〇 8 Α, i 〇 8B have been coupled to the gas source 104 to the processing chamber 100, the number of positions i 〇 8A, i 〇 8b is not limited to two. A single location 108A, 108B can be applied » or more than two locations 108A, 108B can be applied. When a plurality of positions i08A, l8B are used to couple the gas source 104 to the processing chamber 1〇〇, 'flow to the processing chamber 1〇〇200948219. The gas systems of the plurality of positions 108A, 108B are from the same gas source 1 〇 4. In one embodiment, the gas flows to various locations 1 〇 8 Α, 1 〇 8B of the processing chamber 1 可 may have its own exclusive gas source 104. It should also be understood that although a single location 1 〇 6 is shown to couple the power source 1 〇 2 to the processing chamber 100, the power source ioz can be coupled to the processing chamber 100 at a plurality of locations 丨〇6. In one embodiment, power source 102 can include an RF power source. Furthermore, although the display power source 1 〇 2 is coupled to the processing chamber 1 at a location 106 corresponding to the substantial center of the processing chamber 1 , the power source 102 may not correspond to the processing chamber ι The position of the substantial center is π6 coupled to the processing chamber 100. Although the air source 104 is shown coupled to the processing chamber 1 at positions l 8A, 108B (placed substantially away from the center of the processing chamber), the positions 1 〇 8 Α, 108 B are not so limited. The position ι〇8Α, ι〇8Β comparable position 1〇6 (where the power source 102 is coupled to the processing chamber 1〇〇) is closer to the center of the processing chamber 1〇〇. Fig. 2A is a schematic cross-sectional view showing a processing chamber 2A according to an embodiment of the present invention. The processing chamber 200 is a PECVD chamber. Processing chamber 200 has a chamber body 208. In the chamber body, the configurable base 204 is located opposite the gas distribution showerhead 210. Substrate 206 can be placed on susceptor 204. Substrate 206 can enter processing chamber 200 through slit valve opening 222. The substrate 206 can be raised and lowered by the susceptor 204 to handle, remove, and/or insert the substrate 206. The showerhead 210 can have a plurality of gas passages 212 that pass from the upstream side 218 through the showerhead 210 to the downstream side 22〇. The downstream side 220 of the showerhead 210 is the one of the side nozzles 210 that the nozzle faces the substrate 206 during processing, and is placed in the processing chamber 2 from the substrate 206 across the processing space 216. There is a gas chamber 214 behind the nozzle 21 . The plenum is between the showerhead 210 and the backing plate 202. The power source 224 can be powered by the power source 224 to the showerhead 21, and the power source 224 is coupled to the backplane 202 via the supply line 226. In an embodiment, power source 224 can include an RF power source. In the illustrated embodiment, the supply line 226 is coupled to the backing plate 2〇2 at a location corresponding to the substantial center of the backing plate 202. It is understood that the power source 224 can also be coupled to the backplane 2〇2 at other locations. Process gas may be delivered by gas source 234 through backing plate 202 to processing chamber 2''. Gas from gas source 234 can be moved through remote source 2 2 8 before reaching processing chamber 2〇〇. In one embodiment, the process gas system passing through the remote plasma source 228 is used for deposition and is therefore not ignited into a plasma in the remote plasma source 228. In another embodiment, the gas from the gas source 234 can be ignited into a plasma in the remote plasma source 228 and then sent to the processing chamber. The plasma from the remote plasma source 228 can be cleaned. The chamber 200 and its exposed components are processed. In addition, the plasma will clean the gas passing through the cooling block 230 and the choke or resistor 232 after the remote plasma source 228. When the plasma is ignited in the remote plasma source 228, the remote plasma source 228 can become very hot. Thus, the cooling block 230 can be placed between the choke or resistor 232 and the remote plasma source 228 to ensure that the choke or resistor 232 does not break due to the high temperature of the remote plasma source 228. It will be appreciated that although two separate gas sources 234 have been shown, the remote electrical energy sources 228 may share the same gas source 234. In addition, although the remote end 8 200948219 plasma source 228 is shown coupled between each of the gas sources 234 and the backing plate, the processing chamber 200 can have more or fewer distal plasma sources 228 coupled thereto. Figure 2B is a schematic cross-sectional view of the processing chamber 200 of Figure 2A showing the RF current path. The RF current has a "skin effect" whereby the RF current moves on the outer surface of the conductor and penetrates only a certain depth of the object i. Therefore, for a sufficiently thick object, the inside of the object can have zero detectable RF current, while the outer surface has RF current flowing on it and is regarded as RF "hot" ^ arrow "A" shows RF current by power Source 224 to the path taken by the nozzle 2^0. The RF current is moved by power source 224 along supply line 226 at beta position 236, which encounters backplane 202 and flows along the back side of backplane 202 and down to downstream face 220 of showerhead 210. The gas enters the processing chamber 2〇〇 through the backing plate 202 at a location 238. The arrow "Β" shows the distance between position 238 (where the gas enters the processing chamber 2〇〇) and position 236 (where the RF current hits the backing plate 202). As the RF current moves, it tends to dissipate. In other words, the RF current exiting power source 224 has a higher power level relative to the power level to the downstream line. In the embodiment shown in Fig. 2B, the RF current at position 236 has a higher power level relative to the current flowing along the back = 2〇2 through position 238 (the gas enters the processing chamber 2〇〇). Since the amount of power at position 238 is lower than position 236, the likelihood of igniting gas in tube 24G containing gas entering processing chamber 2GG can be reduced. Because of the reduced likelihood of process gas igniting in tube 240, parasitic flow in chamber 238, choke or resistor 232, cooling block 23, remote plasma source 228, and chamber 214 after nozzle 112 210 can be reduced. Plasma formation. In one embodiment, tube 240 can comprise a ceramic material. Figure 3 is a schematic isometric view of a backing plate 302 of a processing chamber 3 in accordance with an embodiment of the present invention. RF power can be supplied to the chamber 300 by coupling the RF power source 304 to the backplane 302 at location 324. While position 324 has been shown to correspond to the substantial center of backplane 302, it will be appreciated that location 324 can be located at many other points on board 324. In addition, more than one location 324 同时 can be applied simultaneously. The same gas source 308 can supply gas to the processing chamber 3 〇〇β. Although a single gas source 308 is shown, a plurality of gas sources 308 can be applied. The gas from the gas source 308 can be supplied to the remote plasma source 3 〇6 through the gas tube 310. It will be appreciated that although four remote plasma sources 3 〇 6 are shown, more and fewer remote plasma sources 306 can be applied. In addition, although the remote plasma source 3〇6 is shown placed on the backing plate 302, the remote plasma source 3〇6 can be placed adjacent to the backing plate 302. The gas from gas source 308 passes through gas tube 310 to remote plasma source 306. If the processing chamber 300 is operating in a clean mode, the gas in the remote plasma source 306 can be ignited into a plasma and supplied through the cooling block 314 and the choke or resistor 322 to the processing chamber 300. However, if the processing chamber is operating in a deposition mode, the gas will pass through the remote plasma source 3 〇 6 without burning the electricity. In the absence of ignited plasma, the cleaning gas enters the processing chamber in a non-plasma state and causes inefficient cleaning. If a remote plasma source 306 fails or does not operate effectively, the remote plasma source 306 can be turned off. If other remote plasma sources 3〇6 operate as desired, then 200948219, the clean gas flowing into the processing chamber 300 through the non-operating remote plasma source 306 will not ignite prior to entering the processing chamber 300. In the above aspect, the processing chamber 300 cannot be effectively cleaned.

表I NF3流 率 (slm) 運作的 RPS 單元 無運作 的RPS 單元 清潔時 間(秒) 24 所有 無 24.2 36 所有 無 29.5 48 所有 無 38 48 3 1 87.3 48 3 1 92.2 48 2 2 248.3 48 2 2 84.4 48 2 2 118.9Table I NF3 flow rate (slm) Operating RPS unit Non-operating RPS unit Cleaning time (seconds) 24 All without 24.2 36 All without 29.5 48 All without 38 48 3 1 87.3 48 3 1 92.2 48 2 2 248.3 48 2 2 84.4 48 2 2 118.9

表I顯示當一或更多遠端電漿源不運作時清潔腔室的 作用。在SiN沉積之後清潔腔室。表I所示之資料中, 當RPS不運作時,氣體持續流過RPS單元至腔室。如表 I所示,當一或更多RPS單元停止運作時,但是卻讓清 © 潔氣體持續流過,清潔時間便提高。然而,當RPS單元 失效時,但是有關閉流至失效RPS單元之氣體,則清潔 時間不會提高。Table I shows the effect of cleaning the chamber when one or more remote plasma sources are not operating. The chamber is cleaned after SiN deposition. In the data shown in Table I, when the RPS is not operating, gas continues to flow through the RPS unit to the chamber. As shown in Table I, when one or more RPS units are stopped, but the purge gas continues to flow, the cleaning time increases. However, when the RPS unit fails, but the gas flowing to the failed RPS unit is turned off, the cleaning time does not increase.

表II nf3 流率 (slm) 1RPS 單元 (SiN) 3/4 RPS 單元 (SiN) 4 RPS 單元 (SiN) 1RPS 單元 (a-Si) 3/4 RPS 單元 (a-Si) 4 RPS 單元 (a-Si) 20 50.4 38.9 36.4 24.8 27.9 23.2 24 45.4 34.9 32.3 21.4 27 43.0 32.6 30.6 19.9 22.6 19.0 36 29.7 26.1 11 200948219 | 48 22.8 22.5 16.8 11.4 如表π中所示,藉由關閉流至失效RPS單元之氣體, 便可實質維持清潔速率。因此’關閉氣體管線310中之 閥312有利於避免清潔氣體流過非運作遠端電漿源306 並在沒有於遠端電漿源306中點燃成電漿的情況下進入 處理腔室300。因此,藉由關閉閥312,可將氣流轉離非 運作遠端電漿源306。因此,可利用比耦接至背板302 〇 之遠端電漿源少的遠端電漿源3 06清潔處理腔室300。 一實施例中,閥312可位於遠端電漿源306後方。 在經過遠端電漿源306之後’氣體可經過冷卻塊3 14 » 冷卻塊314可透過冷卻管318耦接至將冷卻流體流至冷 卻塊3 14之冷卻源3 16。冷卻流體可流動離開冷卻塊3 14 並透過冷卻管320返回冷卻流體源3 16。冷卻塊3 14提 供遠端電漿源306與扼流器或電阻器322之間的接合, ^ 以致減少扼流器或電阻器322的斷裂。 在經過冷卻塊3 14之後,氣體經過扼流器或電阻器 322。一實施例中,扼流器或電阻器322可包括電絕緣材 料’例如陶瓷。電絕緣材料可避免RF功率沿著氣體流動 路徑移動。氣體可穿過位置326處的背板302進入處理 腔室3 00。可理解雖然顯示四個位置326,但可應用更多 或更少的位置326將氣體導至處理腔室300。此外’位 置326不需位於背板3〇2角落附近。例如,位置326可 位於接近背板302中心處。 12 200948219 此外,位置324(RF功率耦接至背板3〇2)與位置326(氣 體進入處理腔室300)不限於顯示之位置。位置324可位 於接近背板302邊緣處而一或更多氣體供給位置326可 位於對應背板302中心之區域。 第4圖係根據本發明一實施例之遠端電漿源與處理腔 室之間輕合的概要圖。扼流器或電阻器4〇〇可執合於冷 卻塊402與連接塊404之間。第4圖中顯示一電阻器 ❹ 400,但可理解可應用扼流器取代之。爲了產生扼流器, 金屬線圈(例如,銅線圈)纏繞於電阻器4〇〇外側。連接 塊404可搞接至管406 ’其可讓流過扼流器或電阻器4〇〇 之氣髏流入背板。一實施例中,管4〇6可包含陶瓷。此 外,一實施例中,連接塊404可包含陶瓷。另一實施例 中,連接塊404可包含不鏽鋼。另一實施例中,連接塊 404可包含鋁。當連接塊4〇4包含金屬時,連接扼流器 或電阻器400之管412與管406至腔室的管可應用電絕 ❹ 緣材料。冷卻塊402可包含金屬。 扼流器或電阻器400可包括内管412,氣體經由此内 管412流過以到達腔室。—實施例中,内管412可包括 電絕緣材料。另一實施例中,内管412可包含陶瓷。内 管412可位於套管414中。一實施例中,套管414可包 括電絕緣材料。另一實施例中,套管414可包含陶瓷。 電絕緣材料允許處理氣體流於管内而不暴露氣體至RF 電流。 套管414與管412可在一端41〇連接至連接塊4〇4並 13 200948219 在另一端408連接至冷卻塊402。雖然未顯示,但在某 些實施例中導電材料可纏繞套管414周圍。若有需要的 話,導電材料可用來提供額外尺|?電流接地路徑。 第5圖係根據顯示三個氣體供給位置之一實施例的處 理腔室500之背板5〇2的概要等角圖。三個位置係實質 位於基材上假定分成三個實質相等區域之中心。虛線劃 分三個實質相等區域。可藉由在位置524處耦接RF功率 源504至背板502而提供RF功率至腔室5〇〇。雖然已經 顯示位置524對應背板502的實質中心,但可理解位置 524可位於背板524上的許多其他位置。此外可同時 應用超過一個位置524。 相同氣源508可供應氣體至處理腔室5〇〇。可理解雖 然顯示單一氣源508,但可應用多個氣源5〇8。可透過氣 體管510將離開氣源.5〇8之氣體供應至遠端電漿源 506 。雖然顯示遠端電漿源5〇6位於背板5〇2上但遠 端電漿源506可置於鄰接背板5 02處。 來自氣源508之氣體經過氣體管51〇至遠端電漿源 506。若處理腔室500運作於清潔模式中可將遠端電漿 源506中之氣體點燃成電漿並接著供給自由基通過冷卻 塊514與扼流器或電阻器522至處理腔室5〇〇。然而, 若處理腔室運作於沉積模式中,氣體將經過遠端電漿源 506而不被點燃成電漿。未點燃電漿的情況下,清潔氣 體以非-電漿狀態進入處理腔室並造成無效率的清潔。 關閉氣體管線5H)中之閥512有利㈣免清潔氣體流 14 200948219 過非運作遠端電漿源506並在沒有於遠端電漿源506中 點燃成電漿的情況下進入處理腔室500。因此,藉由關 閉閥5 12,可將氣流轉離非運作遠端電漿源506。因此, 可利用比耦接至背板502之遠端電漿源少的遠端電漿源 506清潔處理腔室500 » —實施例中’閥512可位於遠端 電漿源506後方 經過遠端電漿源506之後’氣艘可經過冷卻塊5 14 » 冷卻塊514可透過冷卻管518耦接至將冷卻流艎流至冷 w 卻塊5 14之冷卻源5 16。冷卻流體可流動離開冷卻塊5 14 並透過冷卻管520返回冷卻流體源516。冷卻塊514提 供遠端電漿源506與扼流器或電阻器522之間的接合, 以致減少扼流器或電阻器522的斷裂。 經過冷卻塊5 14之後’氣體經過扼流器或電阻器522。 一實施例中,扼流器或電阻器522可包括電絕緣材料, 例如陶瓷。電絕緣材料可避免RF功率沿著氣髏流動路徑 _ 移動。氣體.可在位置526穿.過背板5 02進入處理腔室5〇〇。 此外’位置524(RF功率耦接至背板502)與位置526(氣 體進入處理腔室500)不限於顯示之位置。位置524可位 於接近背板502邊緣處而一或更多氣體供給位置526可 位於對應背板502中心之區域。 第6圖係顯示對應氣體導入通道位置之基座的概要 圖。如圖所示,已經將基座分成三個實質相等區域,其 中長度(L1-L3)與寬度(W1-W3)係實質相同。各個區域^ 中心602對應於上方氣體導入通道穿過背板之位置。中 15 200948219 心602與氣體導入通道係經配置以致假設三角形(以虛線 顯示)具有兩個實質相同角度(α)與一其他角度(β),角度 (β)可與其他角度(α)相同或不同。角度(β)是否相同於角 度(α)將取決於基座的設計。 雖然描述的係基座,但該配置可同樣地應用在基材, 以致氣體通道係位於置於基座上之基材的三個實質相等 區域之中心上。另一實施例中,配置可同樣地應用在背 0 板本身,以致氣體通道係位於中心地穿過背板之三個實 質相等區域。此外,配置可同樣地應用在喷頭或電極, 以致氣體通道係在噴頭或電極之三個實質相等區域的中 心上。 第7圖係根據另一實施例之設備700的概要俯視圖。 設備700可為PECVD設備。設備700包括背板7〇2。氣 源704不僅提供處理氣體至處理腔室,也提供清潔氣體 至處理腔室。雖然顯示單一氣源704,但可理解可應用 ® 多個氣源。 沉積過程中’自氣源704供給處理氣體至處理腔室。 處理氣體在開口 724、726、728 (以虛線顯示)處穿過背 板702進入處理腔室之前,移動經過遠端電漿源7〇6、 708、710、冷卻塊712、714、716與氣體供給塊718、 720、722。冷卻塊712、714、716係用來提供遠端電漿 源706、708、710與氣體供給塊718、72〇、722之間的 連接。遠端電漿源706、708、710可因為電漿達成如此 高溫,使得氣體供給塊718、72〇、722與遠端電漿源7〇6、 16 200948219 708、710之間的溫度梯度會造成任一者失效。冷卻塊 71 2、714、7 1 6可減少系統失敗的可能性。 自功率源73〇提供RF功率至處理腔室,功率源730 係透過匹配網路732耦接至背板702。如圖所示,RF功 率係在背板702之實質中心734處麴接至背板702。可 以理解功率源730亦可在背板702之中心734以外或替 代的其他位置處耦接至背板702。此外,可以約10 ΜΗζ 與約100 MHz之間的頻率傳送rf功率。傳送rf功率之 ® 位置與傳送氣體之位置有所間隔。 如第7圖中所示,氣體經由開口 724、726、728穿過 背板702進入處理腔室,開口 724、726、728係與背板 702之中心734有所間隔,以致氣體進入處理腔室之位 置與功率源730耦接至背板702之位置分隔。第7圖顯 示之實施例中’開口 724、726、728各自與背板702之 中心734有實質相等間隔。因此’開口 724、726、728 ❹ 可以相等半徑748、75〇、752與中心734分隔(以虛線740 所示)。一實施例中’開口 724、726、728可與背板7〇2 之中心7 3 4相隔約2 5與約3 0英时之間。 藉由間隔開口 724、726、728與RF供給位置,可減少 處理腔室外之氣體供給塊718、72〇、722或冷卻塊712、 714、716附近或之中寄生電漿點燃的可能性。腔室中rf 電位差異最大的位置係RF進入腔室處,因為RF電流沿 著壁返回時RF返回路徑就在旁邊。藉由在與供給氣體進 入腔至位置分隔處具有將RF#率耦合至腔室之位置,開 17 200948219 口 724、726、728係位於RF電位差異減小之位置。因此, 減小寄生電漿形成的可能性。 此外,可以預定角度α間隔開口 724、726、728。一 實施例中,角度α係12〇度。顯示出三個開口 724、726、 728之第一開口 724係與背板702之兩側754、756具有 實質相等間隔(如箭頭C、D所示)。第一開口 724與中心 734有所間隔,因此並不位於側邊736與738之間的中 心。其他兩個開口 726、724並不位於任一侧邊736、738、Table II nf3 flow rate (slm) 1RPS unit (SiN) 3/4 RPS unit (SiN) 4 RPS unit (SiN) 1RPS unit (a-Si) 3/4 RPS unit (a-Si) 4 RPS unit (a- Si) 20 50.4 38.9 36.4 24.8 27.9 23.2 24 45.4 34.9 32.3 21.4 27 43.0 32.6 30.6 19.9 22.6 19.0 36 29.7 26.1 11 200948219 | 48 22.8 22.5 16.8 11.4 As shown in Table π, by closing the gas flowing to the failed RPS unit, The cleaning rate can be substantially maintained. Thus, closing valve 312 in gas line 310 facilitates preventing cleaning gas from flowing through non-operating distal plasma source 306 and entering processing chamber 300 without being ignited into plasma in remote plasma source 306. Thus, by closing valve 312, the airflow can be diverted away from non-operating remote plasma source 306. Thus, the processing chamber 300 can be cleaned with a remote plasma source 306 that is less than the remote plasma source coupled to the backing plate 302. In one embodiment, the valve 312 can be located behind the distal plasma source 306. After passing through the remote plasma source 306, the gas can pass through the cooling block 3 14 . The cooling block 314 can be coupled through a cooling tube 318 to a cooling source 3 16 that flows cooling fluid to the cooling block 314. The cooling fluid can flow away from the cooling block 3 14 and back through the cooling tube 320 to the cooling fluid source 3 16 . Cooling block 314 provides a bond between remote plasma source 306 and choke or resistor 322, thereby reducing breakage of choke or resistor 322. After passing through the cooling block 314, the gas passes through a choke or resistor 322. In one embodiment, the choke or resistor 322 can comprise an electrically insulating material such as ceramic. Electrically insulating materials prevent RF power from moving along the gas flow path. Gas can enter the processing chamber 300 through the backing plate 302 at location 326. It will be appreciated that although four locations 326 are shown, more or fewer locations 326 may be applied to direct gas to the processing chamber 300. In addition, the position 326 does not need to be located near the corner of the back panel 3〇2. For example, location 326 can be located proximate to the center of backplane 302. 12 200948219 Additionally, location 324 (RF power coupled to backplane 3〇2) and location 326 (gas entering processing chamber 300) are not limited to the displayed position. Position 324 can be located near the edge of backing plate 302 and one or more gas supply locations 326 can be located in the area corresponding to the center of backing plate 302. Figure 4 is a schematic illustration of the light coupling between a remote plasma source and a processing chamber in accordance with an embodiment of the present invention. A choke or resistor 4 can be engaged between the cooling block 402 and the connection block 404. A resistor ❹ 400 is shown in Figure 4, but it is understood that a choke can be used instead. To create a choke, a metal coil (eg, a copper coil) is wound around the outside of the resistor 4〇〇. The connection block 404 can be coupled to the tube 406' which allows gas flowing through the choke or resistor 4 to flow into the backing plate. In one embodiment, the tube 4〇6 may comprise ceramic. Additionally, in one embodiment, the connection block 404 can comprise ceramic. In another embodiment, the connection block 404 can comprise stainless steel. In another embodiment, the connection block 404 can comprise aluminum. When the connection block 4〇4 contains metal, the tube 412 connecting the choke or resistor 400 and the tube 406 to the chamber may be electrically insulated. Cooling block 402 can comprise a metal. The choke or resistor 400 can include an inner tube 412 through which gas flows to reach the chamber. - In an embodiment, the inner tube 412 can comprise an electrically insulating material. In another embodiment, the inner tube 412 can comprise ceramic. Inner tube 412 can be located in sleeve 414. In one embodiment, the sleeve 414 can comprise an electrically insulating material. In another embodiment, the sleeve 414 can comprise a ceramic. The electrically insulating material allows the process gas to flow into the tube without exposing the gas to the RF current. The sleeve 414 and the tube 412 can be connected to the connection block 4〇4 at one end 41〇 and 13 200948219 to the cooling block 402 at the other end 408. Although not shown, in some embodiments a conductive material can be wrapped around the sleeve 414. Conductive materials can be used to provide additional ground current paths if needed. Figure 5 is a schematic isometric view of the backing plate 5〇2 of the processing chamber 500 in accordance with one embodiment showing three gas supply locations. The three locations are essentially located on the substrate and are assumed to be centered into three substantially equal regions. The dotted line is divided into three substantially equal areas. RF power can be provided to the chamber 5 by coupling the RF power source 504 to the backplane 502 at location 524. While position 524 has been shown to correspond to the substantial center of backing plate 502, it will be appreciated that position 524 can be located at many other locations on backing plate 524. In addition, more than one location 524 can be applied simultaneously. The same gas source 508 can supply gas to the processing chamber 5〇〇. It will be appreciated that although a single source 508 is shown, a plurality of sources 5 〇 8 may be employed. Gas leaving the gas source .5〇8 can be supplied to the remote plasma source 506 through the gas tube 510. Although the remote plasma source 5〇6 is shown on the backing plate 5〇2, the remote plasma source 506 can be placed adjacent to the backing plate 502. Gas from gas source 508 is passed through gas line 51 to remote plasma source 506. If the processing chamber 500 is operating in a clean mode, the gas in the remote plasma source 506 can be ignited into a plasma and then the free radicals can be supplied through the cooling block 514 and the choke or resistor 522 to the processing chamber 5A. However, if the processing chamber is operating in a deposition mode, the gas will pass through the remote plasma source 506 without being ignited into a plasma. In the absence of ignited plasma, the cleaning gas enters the processing chamber in a non-plasma state and causes inefficient cleaning. Closing the valve 512 in the gas line 5H) advantageously (iv) the purge-free gas stream 14 200948219 passes through the non-operating remote plasma source 506 and enters the processing chamber 500 without being ignited into a plasma in the remote plasma source 506. Thus, by closing valve 51, the airflow can be diverted away from non-operating distal plasma source 506. Thus, the processing chamber 500 can be cleaned with a remote plasma source 506 that is less than the remote plasma source coupled to the backing plate 502. - In the embodiment, the valve 512 can be located behind the distal plasma source 506 through the distal end. After the plasma source 506, the 'aircraft can pass through the cooling block 5 14 » The cooling block 514 can be coupled through a cooling tube 518 to a cooling source 5 16 that flows the cooling stream to the cold block 514. The cooling fluid can flow away from the cooling block 514 and back through the cooling tube 520 to the cooling fluid source 516. Cooling block 514 provides engagement between remote plasma source 506 and choke or resistor 522 to reduce breakage of choke or resistor 522. After passing through the cooling block 5 14 'gas' passes through a choke or resistor 522. In one embodiment, the choke or resistor 522 can comprise an electrically insulating material, such as ceramic. Electrically insulating material prevents RF power from moving along the airflow path _. The gas can be passed through position 526 through the backing plate 052 into the processing chamber 5〇〇. Further, the 'position 524 (RF power coupled to the backing plate 502) and the position 526 (the gas entering the processing chamber 500) are not limited to the displayed position. Position 524 can be located proximate the edge of backing plate 502 and one or more gas supply locations 526 can be located in the region corresponding to the center of backing plate 502. Fig. 6 is a schematic view showing a susceptor corresponding to the position of the gas introduction passage. As shown, the pedestal has been divided into three substantially equal regions, wherein the length (L1-L3) is substantially the same as the width (W1-W3). Each zone ^ center 602 corresponds to the position of the upper gas introduction passage through the backing plate.中 15 200948219 The heart 602 and the gas introduction channel are configured such that the hypothetical triangle (shown in dashed lines) has two substantially identical angles (α) and one other angle (β), the angle (β) may be the same as the other angles (α) or different. Whether the angle (β) is the same as the angle (α) will depend on the design of the pedestal. Although a pedestal is described, this configuration can equally be applied to the substrate such that the gas channel is centered on three substantially equal regions of the substrate disposed on the susceptor. In another embodiment, the configuration can be applied equally to the backplate itself such that the gas passageway is centrally located through the three substantially equal regions of the backing plate. In addition, the configuration can be equally applied to the showerhead or electrode such that the gas passage is centered on three substantially equal regions of the showerhead or electrode. Figure 7 is a schematic top plan view of an apparatus 700 in accordance with another embodiment. Device 700 can be a PECVD device. Apparatus 700 includes a backing plate 7〇2. The gas source 704 provides not only process gas to the processing chamber but also cleaning gas to the processing chamber. Although a single gas source 704 is shown, it is understood that more than one gas source can be applied. The process gas is supplied from the gas source 704 to the processing chamber during deposition. The process gas moves past the remote plasma source 7〇6, 708, 710, the cooling blocks 712, 714, 716 and the gas before passing through the backing plate 702 into the processing chamber at openings 724, 726, 728 (shown in phantom). Blocks 718, 720, 722 are supplied. Cooling blocks 712, 714, 716 are used to provide a connection between remote plasma sources 706, 708, 710 and gas supply blocks 718, 72, 722. The remote plasma sources 706, 708, 710 may cause such a high temperature as the plasma, such that a temperature gradient between the gas supply blocks 718, 72A, 722 and the remote plasma source 7〇6, 16 200948219 708, 710 may cause Either one is invalid. Cooling blocks 71 2, 714, 7 1 6 reduce the likelihood of system failure. The power source 73 is supplied from the power source 73 to the processing chamber, and the power source 730 is coupled to the backplane 702 through the matching network 732. As shown, the RF power is coupled to the backing plate 702 at a substantial center 734 of the backing plate 702. It can be appreciated that power source 730 can also be coupled to backplane 702 at a location other than center 734 of backplane 702 or alternatively. In addition, the rf power can be transmitted at a frequency between about 10 ΜΗζ and about 100 MHz. The position of the transfer rf power ® is spaced from the position of the transfer gas. As shown in FIG. 7, gas passes through the openings 724, 726, 728 through the backing plate 702 into the processing chamber, and the openings 724, 726, 728 are spaced from the center 734 of the backing plate 702 such that gas enters the processing chamber. The location is separated from the location at which power source 730 is coupled to backplane 702. In the embodiment shown in Fig. 7, the openings 724, 726, 728 are each substantially equally spaced from the center 734 of the backing plate 702. Thus, the openings 724, 726, 728 ❹ can be separated from the center 734 by equal radii 748, 75 〇, 752 (shown by dashed line 740). In one embodiment, the openings 724, 726, 728 may be spaced between about 25 and about 30 inches from the center 7 3 4 of the backing plate 7〇2. By spacing the openings 724, 726, 728 and the RF supply location, the likelihood of parasitic plasma ignition near or within the gas supply blocks 718, 72, 722 or cooling blocks 712, 714, 716 outside the processing chamber can be reduced. The location where the difference in rf potential is greatest in the chamber is where RF enters the chamber, as the RF return path is next to it as the RF current returns along the wall. By having a position where the RF# rate is coupled to the chamber at the point of separation from the supply gas into the chamber, the opening 17 200948219 port 724, 726, 728 is located at a position where the RF potential difference is reduced. Therefore, the possibility of parasitic plasma formation is reduced. Further, the openings 724, 726, 728 may be spaced apart by a predetermined angle a. In one embodiment, the angle α is 12 degrees. The first opening 724 showing the three openings 724, 726, 728 is substantially equally spaced from the sides 754, 756 of the backing plate 702 (as indicated by arrows C, D). The first opening 724 is spaced from the center 734 and is therefore not centered between the sides 736 and 738. The other two openings 726, 724 are not located on either side 736, 738,

A ^ 754、756之間的中心。 因為有三個開口 724、726、728,有可能可調節移動 穿過背板702進入處理腔室之處理氣體與/或清潔氣體自 由基。例如,可選擇性打開與關閉閥742、744、746而 以預定方式讓處理氣體與/或清潔氣體自由基經過開口 724、726、728進入處理腔室。例如,可選擇性透過一 開口 724、726、728輸送處理氣體與/或清潔氣體而不透 _ 過其他開口 724、726、728輸送。實際上,爲了攪動處 理腔室中之處理氣體與/或清潔氣體自由基,可持續轉換 開口 724、726、728(氣體經由此進入腔室)。對處理氣體 而言,可藉由上述步驟攪動腔室中點燃之電漿。同樣地, 可攪動自遠端電漿源706、708、710輸送之自由基。 設備700將具有進入處理腔室之狹縫閥開口,以允許 基材進入與離開處理腔室。第7圖顯示之實施例中,設 備之側邊736具有狹縫閥開口。因此,開口 724比開口 726、728置於更遠離狹縫閥開口處。 18 200948219 腔室中的狹缝閥開口會影響腔室中的電漿分佈。因為 具有狹缝闕開Π之壁不同於其他三個壁,所以狹缝闕開 口會影響電漿分佈。施加至背板702之RF電流試圖返回 丨功率源730。如此返回中,RF電流沿著腔室壁移動回 工力率源703。因為壁RF電位相對電漿rf電位之差異, 沿著腔室壁移動回功率源73〇之RF電流會影響電漿。因 為具有狹縫閥開π之壁不同於其他壁,所以狹缝間開口 ❹ 目為1^電位差異而影響電漿分佈。不均勻電漿分佈會造 成基材上的不均勻沉積。 流入腔室之處理氣體亦影響電漿分佈。電漿濃度越高, 材料沉積越夕。已經出乎意外地發現當透過所有三個開 口 724 726、728輸送處理氣體至處理腔室時,出現在 基材中心區域上的沉積量係高於其他區域。因此,沉積 材料將係「中心高^然而,當僅透過一開口 724供給處 理氣體進入處理腔室且避免透過其他開口 726、728流動 ® 時,基材上的沉積係更均勻》因此,僅透過一開口 724 而不透過開口 726、728供給處理氣體可減少「中心高」 效應。 透過開口 724而非開口 726或開口 728供給係有利 的,因為開口 724在「Υ」方向中位於侧邊754、7%之 間的實質中心,而「X」方向中則無。另一方面,開口 726、728沒有在「X」或「Υ」方向任一者中位於中心。 因為開口 724係位於側邊754與側邊756之間的中心, 預期「γ」方向中的氣體分配係實質均勻。因為開口 724 19 200948219 不在「X」方向的中心734,「x」方向中的氣體分配可能 不均勻。因此相對於開口 726、728,開口 724提供至少 一可控制方向。沉積過程中,可關閉閥742、746以確保 僅透過開口 724輸送處理氣體。 另一方面,腔室清潔過程中,自遠端電漿源7〇6、7〇8、 710中產生之電漿輸送之自由基可進入穿過所有三個開 口 724、726、728以有效地清潔處理腔室。 ❻ 一實施例中,設備7〇〇可如下般運作。可關閉閥742 與746以避免處理氣體穿過開口 726、728進入處理腔 室。因此’處理氣體不經過遠端電漿源7〇8、710、冷卻 塊714、716或氣體供給塊722、724。閥744將打開而 處理氣趙將移動通過遠端電漿源7〇6、冷卻塊712、氣體 供給塊718並通過開口 724進入處理腔室。處理氣體將 移動通過遠端電漿源7〇6而不被點燃成電漿。藉由僅透 過一開口 724供給氣體進入處理腔室,可控制處理氣體 ® 量並減少中心高沉積的可能性。若透過所有三個開口 724、726、728供給氣體,那麼沉積可能會不均勻且發 生中心尚沉積。 自功率源730將RF電流提供至處理腔室,透過匹配網 路732在與開口 724、726、728有所間隔之位置輸送至 背板702。RF電流可點燃處理氣體成電漿以沉積材料於 基材上。處理之後,可移除基材並排空處理氣體。之後, 可清潔處理腔室。打開閥742與746並自氣源7〇4輸送 清潔氣體至遠端電漿源7〇6、7〇8、71〇(其被點燃成電 20 200948219 漿)來自遠端電漿源706、γ〇8、710之自由基接著可經 過冷部塊712、714、716、氣體供給塊718、720、722 並通過開口 724、726、728進入處理腔室。清潔氣體接 著蝕刻或自處理腔室之暴露表面移除污染物。 清潔過程中,清潔氣體量並非重要考量。事實上,越 多越好,以確保適當地清潔腔室。因此,可透過所有三 個開口 724、726、728供給清潔氣體。如同沉積一樣, 0 清潔中亦樂見均勻性,但在清潔時,腔室表面對清潔氣 體自由基呈現相對惰性,以致主要地移除沉積在腔室表 面上之材料。非常少(若有的話)的腔室被移除。因此, 越多的清潔氣體自由基越好。爲了確保存在盡可能多的 清潔自由基’應用所有三個開口 724、726、728。根據 剛剛討論之實施例’清潔過程中’可改變氣體進入腔室 的供給位置以及位置數目。清潔之後,可排空處理腔室 而處理腔室再度準備好用於沉積。 ® 第8圖係根據另一實施例之設備800的概要俯視圖。 設備800可為PECVD設備。設備800包括背板8〇2。氣 源804不僅提供處理氣體至處理腔室,並提供清潔氣體 至處理腔室。雖然顯示單一氣源804,但可理解可應用 多個氣源。 沉積過程中’自氣源804供給處理氣體至處理腔室。 處理氣體在開口 824、826、828 (以虛線顯示)處穿過背 板802進入處理腔室之前’移動經過遠端電漿源806、 808、810、冷卻塊812、814、816與氣體供給塊818、 21 200948219 820、822。冷卻塊812、814、816係用來提供遠端電漿 源806、808、810與氣體供給塊818、820、822之間的 連接?遠端電漿源806、8〇8、810可因為電漿達成如此 高溫,使得氣體供給塊818、820、822與遠端電漿源806、 808、810之間的温度梯度會造成任一者失效。冷卻塊 8 12、8 14、8 1 6可減少系統失敗的可能性。 自複數個功率源830、832、860、862提供RF功率至 處理腔室’複數個功率源830、832、860、862係透過匹 配網路麵接至背板8〇2。如圖所示,rf功率源mo、832、 860、862係在與背板802之實質中心834處有所間隔之 位置搞接至背板。可以理解功率源830、832、860、862 亦可在其他位置(包括背板8〇2之中心834)處耦接至背板 802。此外,可以約1〇 MHz與約1〇〇 MHz之間的頻率傳 送RF功率。傳送RF功率之位置與傳送氣體之位置有所 間隔。此外,不同功率源830、832、860、862輸送之功 率的位相可不同。 如第8圖中所示,氣體經由開口 gw、826、828穿過 背板802進入處理腔室,開口 824、826、828係與背板 802之中心834有所間隔’以致氣體進入處理腔室之位 置與功率源830、832、860、862耦接至背板802之位置 分隔。第8圖顯示之實施例中,開口 824、826、828各 自與背板802之中心834有實質相等間隔。因此,開口 824、826、828可以相等半徑848、85〇、852與中心834 分隔(以虛線840所示)。一實施例中,開口 824、826、 22 200948219 828可與背板802之中心834相隔約25與約30英对之 間。 藉由間隔開口 824、826、828與RF供給位置,可減少 位於處理腔室外之氣體供給塊818、820、822或冷卻塊 812、814、816附近或之中寄生電漿點燃的可能性。腔 室中RF電位差異最大的位置係RF進入腔室處,因為 RF電流沿著壁返回時RF返回路徑就在旁邊。藉由在與 供給氣體進入腔室位置分隔處具有將RF功率叙合至腔 室之位置,開口 824、826、828係位於RF電位差異減小 之位置。因此,減小寄生電漿形成的可能性。 此外’可以預定角度α間隔開口 824、826、828。一 實施例中,角度α係120度。顯示出三個開口 824、826、 828之第一開口 824係與背板802之兩側854、856具有 實質相等間隔(如箭頭E、F所示)。第一開口 824與中心 834有所間隔,因此並不位於側邊836與838之間的中 心。其他兩個開口 826、824並不位於任一侧邊836、838、 854、856之間的中心。 因為有三個開口 824、826、828,有可能可調節移動 穿過背板802進入處理腔室之處理氣體與/或清潔氣體自 由基。例如,可選擇性打開與關閉閥842、844、846而 以預定方式讓處理氣體與/或清潔氣體自由基經過開口 824、826、828進入處理腔室。例如’可選擇性透過一 開口 824、826、828輸送處理氣體與/或清潔氣體而不透 過其他開口 824、826、828輸送。實際上,爲了攪動處 23 200948219 理腔室中之處理氣體與/或清潔氣體自由基,可持續轉換 開口 824、826、828(氣體經由此進入腔室)。對處理氣體 而言,可藉由上述步驟攪動腔室中點燃之電衆。同樣地, 可攪動自遠端電漿源806、808、810輸送之自由基。 設備800將具有進入處理腔室之狹縫閥開口,以允許 基材進入與離開處理腔室。第8圖顯示之實施例中,設 備之側邊836具有狹缝閥開口。因此,開口 824比開口 826、828置於更遠離狹縫閥開口處。 ❹ 腔室中的狹縫閥開口會影響腔室中的電聚分佈。因為Center between A ^ 754, 756. Because there are three openings 724, 726, 728, it is possible to adjust the process gas and/or cleaning gas free radicals that move through the backing plate 702 into the processing chamber. For example, valves 742, 744, 746 can be selectively opened and closed to allow process gas and/or cleaning gas radicals to enter the processing chamber through openings 724, 726, 728 in a predetermined manner. For example, the process gas and/or cleaning gas may be selectively delivered through an opening 724, 726, 728 without being conveyed through other openings 724, 726, 728. In effect, openings 724, 726, 728 (through which the gas enters the chamber) can be continuously switched in order to agitate the process gas and/or cleaning gas radicals in the process chamber. For the process gas, the plasma ignited in the chamber can be agitated by the above steps. Likewise, free radicals delivered from the distal plasma source 706, 708, 710 can be agitated. Apparatus 700 will have a slit valve opening into the processing chamber to allow the substrate to enter and exit the processing chamber. In the embodiment shown in Fig. 7, the side 736 of the device has a slit valve opening. Thus, opening 724 is placed further away from the slit valve opening than openings 726,728. 18 200948219 The slit valve opening in the chamber affects the plasma distribution in the chamber. Since the wall with the slit opening is different from the other three walls, the slit opening affects the plasma distribution. The RF current applied to the backplane 702 attempts to return to the helium power source 730. In this return, the RF current is moved back to the power rate source 703 along the chamber wall. Because of the difference in wall RF potential versus plasma rf potential, the RF current moving back to the power source 73 along the chamber wall affects the plasma. Since the wall having the slit valve opening π is different from the other walls, the opening between the slits is a difference in potential and affects the plasma distribution. Uneven plasma distribution can cause uneven deposition on the substrate. The process gas flowing into the chamber also affects the plasma distribution. The higher the plasma concentration, the more the material is deposited. It has been surprisingly found that when processing gas is delivered to the processing chamber through all three openings 724 726, 728, the amount of deposition that occurs on the central region of the substrate is higher than in other regions. Therefore, the deposited material will be "center high". However, when the process gas is supplied through only one opening 724 into the processing chamber and from flowing through the other openings 726, 728, the deposition on the substrate is more uniform. Supplying the process gas through an opening 724 without passing through the openings 726, 728 reduces the "center height" effect. The supply through the opening 724 instead of the opening 726 or the opening 728 is advantageous because the opening 724 is located at the substantial center between the sides 754 and 7% in the "Υ" direction, but not in the "X" direction. On the other hand, the openings 726, 728 are not centered in either the "X" or "Υ" direction. Since the opening 724 is centered between the side 754 and the side 756, the gas distribution in the "gamma" direction is expected to be substantially uniform. Since the opening 724 19 200948219 is not at the center 734 in the "X" direction, the gas distribution in the "x" direction may be uneven. Thus, opening 724 provides at least one controllable direction relative to openings 726, 728. During deposition, valves 742, 746 can be closed to ensure that process gas is only delivered through opening 724. On the other hand, during the chamber cleaning process, the free radicals transported from the plasma generated in the remote plasma source 7〇6, 7〇8, 710 can enter through all three openings 724, 726, 728 to effectively Clean the processing chamber. In one embodiment, the device 7 can operate as follows. Valves 742 and 746 can be closed to prevent process gases from entering the processing chamber through openings 726, 728. Thus, the process gas does not pass through the remote plasma source 7〇8, 710, the cooling blocks 714, 716, or the gas supply blocks 722, 724. Valve 744 will open and the process gas will move through remote plasma source 7〇6, cooling block 712, gas supply block 718 and through opening 724 into the processing chamber. The process gas will move through the remote plasma source 7〇6 without being ignited into a plasma. By supplying gas through only one opening 724 into the processing chamber, the amount of process gas ® can be controlled and the likelihood of high center deposition can be reduced. If gas is supplied through all three openings 724, 726, 728, the deposition may be uneven and the center may still deposit. The self-power source 730 provides RF current to the processing chamber and is delivered to the backplane 702 through the matching network 732 at a location spaced from the openings 724, 726, 728. The RF current ignites the process gas into a plasma to deposit material onto the substrate. After processing, the substrate can be removed and the process gas vented. After that, the processing chamber can be cleaned. Valves 742 and 746 are opened and the cleaning gas is delivered from gas source 7〇4 to remote plasma source 7〇6, 7〇8, 71〇 (which is ignited into electricity 20 200948219 slurry) from remote plasma source 706, γ The free radicals of 〇 8, 710 can then enter the processing chamber through cold blocks 712, 714, 716, gas supply blocks 718, 720, 722 and through openings 724, 726, 728. The cleaning gas is then etched or removed from the exposed surface of the processing chamber. The amount of clean gas is not an important consideration during the cleaning process. In fact, the more the better, to ensure that the chamber is properly cleaned. Therefore, the cleaning gas can be supplied through all three openings 724, 726, 728. As with deposition, homogeneity is also seen in the cleaning of the 0, but when cleaned, the surface of the chamber is relatively inert to the free radicals of the cleaning gas, so that the material deposited on the surface of the chamber is primarily removed. Very few (if any) chambers were removed. Therefore, the more cleaning gas radicals are, the better. In order to ensure that as many cleaning radicals as possible are present, all three openings 724, 726, 728 are applied. The supply position of the gas entering the chamber and the number of positions can be varied according to the embodiment just discussed 'during the cleaning process'. After cleaning, the processing chamber can be evacuated and the processing chamber ready for deposition. ® Figure 8 is a schematic top plan view of an apparatus 800 in accordance with another embodiment. Device 800 can be a PECVD device. Apparatus 800 includes a backing plate 8〇2. Gas source 804 provides not only process gas to the processing chamber but also clean gas to the processing chamber. Although a single gas source 804 is shown, it is understood that multiple gas sources can be applied. The process gas is supplied from the gas source 804 to the processing chamber during deposition. The process gas moves through the remote plasma source 806, 808, 810, cooling blocks 812, 814, 816 and the gas supply block before the openings 824, 826, 828 (shown in phantom) pass through the backing plate 802 into the processing chamber. 818, 21 200948219 820, 822. Cooling blocks 812, 814, 816 are used to provide a connection between remote plasma sources 806, 808, 810 and gas supply blocks 818, 820, 822. The remote plasma sources 806, 8〇8, 810 may be such that the plasma reaches such a high temperature that the temperature gradient between the gas supply blocks 818, 820, 822 and the remote plasma sources 806, 808, 810 may cause either Invalid. Cooling blocks 8 12, 8 14 and 8 1 6 reduce the possibility of system failure. The plurality of power sources 830, 832, 860, 862 provide RF power to the processing chamber. A plurality of power sources 830, 832, 860, 862 are connected to the backplane 8A through the matching network. As shown, the rf power sources mo, 832, 860, 862 are attached to the backplane at a location spaced from the substantial center 834 of the backplane 802. It will be appreciated that power sources 830, 832, 860, 862 may also be coupled to backplane 802 at other locations, including center 834 of backplane 8〇2. In addition, RF power can be transmitted at a frequency between about 1 〇 MHz and about 1 〇〇 MHz. The position at which the RF power is transmitted is spaced from the position at which the gas is delivered. Moreover, the phase of power delivered by different power sources 830, 832, 860, 862 can be different. As shown in Figure 8, gas passes through the openings gw, 826, 828 through the backing plate 802 into the processing chamber, and the openings 824, 826, 828 are spaced from the center 834 of the backing plate 802 'to allow gas to enter the processing chamber The location is separated from the location at which the power sources 830, 832, 860, 862 are coupled to the backplane 802. In the embodiment shown in Fig. 8, the openings 824, 826, 828 are each substantially equally spaced from the center 834 of the backing plate 802. Thus, the openings 824, 826, 828 can be separated from the center 834 by equal radii 848, 85, 852 (shown by dashed line 840). In one embodiment, the openings 824, 826, 22 200948219 828 can be spaced apart from the center 834 of the backing plate 802 by between about 25 and about 30 inches. By spacing the openings 824, 826, 828 and the RF supply location, the likelihood of parasitic plasma ignition near or within the gas supply blocks 818, 820, 822 or cooling blocks 812, 814, 816 outside the processing chamber can be reduced. The location where the RF potential difference is greatest in the chamber is where RF enters the chamber because the RF return path is next to it as the RF current returns along the wall. The openings 824, 826, 828 are located at a position where the RF potential difference is reduced by having a position at which the RF power is summed to the chamber at a location separated from the supply gas entering the chamber. Therefore, the possibility of parasitic plasma formation is reduced. Further, the openings 824, 826, 828 can be spaced apart by a predetermined angle α. In one embodiment, the angle a is 120 degrees. The first opening 824 showing the three openings 824, 826, 828 is substantially equally spaced from the sides 854, 856 of the backing plate 802 (as indicated by arrows E, F). The first opening 824 is spaced from the center 834 and therefore is not centered between the sides 836 and 838. The other two openings 826, 824 are not centered between either of the sides 836, 838, 854, 856. Because there are three openings 824, 826, 828, it is possible to adjust the process gas and/or cleaning gas free radicals that move through the backing plate 802 into the processing chamber. For example, valves 842, 844, 846 can be selectively opened and closed to allow process gas and/or cleaning gas radicals to enter the processing chamber through openings 824, 826, 828 in a predetermined manner. For example, the process gas and/or cleaning gas may be selectively delivered through an opening 824, 826, 828 without being transported through other openings 824, 826, 828. In effect, openings 824, 826, 828 (through which the gas enters the chamber) can be continuously switched in order to agitate the process gas and/or cleaning gas radicals in the chamber. For the process gas, the electricity ignited in the chamber can be agitated by the above steps. Likewise, free radicals transported from the remote plasma sources 806, 808, 810 can be agitated. Apparatus 800 will have a slit valve opening into the processing chamber to allow substrate entry and exit from the processing chamber. In the embodiment shown in Fig. 8, the side 836 of the device has a slit valve opening. Thus, opening 824 is placed further away from the slit valve opening than openings 826,828. The slit valve opening in the chamber affects the distribution of electropolymerization in the chamber. because

具有狹縫閥開口之壁不同於其他三個壁,所以狹縫闕開 口會影響電漿分佈。施加至背板802之RF電流試圖返回 其功率源830、832、860、862。如此返回中,rf電流沿 著腔室壁移動回功率源830、832、860、862 »因為壁RF 電位相對電漿RF電位之差異,沿著壁移動回功率源 83 0、83 2、860、862之RF電流會影響電漿。因為具有 φ 狹縫閥開口之壁不同於其他壁,所以狹縫閥開口因為RF 電位差異而影響電漿分佈。不均勻電漿分佈會造成基材 上的不均勻沉積。 流入腔室之處理氣體亦影響電漿分佈。電漿濃度越高, 材料沉積越多。已經出乎意外地發現當透過所有三個開 口 824、8%、輸送處理氣體至處理腔室時,出現在 基材中心區域上的沉積量係高於其他區域。因此,沉積 材料將係「中心高」。然而,當僅透過一開口 824供給處 理氣體進入處理腔室且避免透過其他開口 826、828流動 24 200948219 時’基材上的沉積係更均勻。 _ . J J囚此,僅透過一開口 824 而不透過開口 826、828供絡* 友 供給處理氣體可減少「中心高」 效應。 透過開口 8 2 4而非關口 8,士 n n 叩非開口 820或開口 828供給係有利 的,因為開口 824扁「ν η,- > , 」方向中位於側邊854、856之 間的實質中心,而「X 方向中刖& 八」乃同甲則無。另一方面,開口 826、828 沒有在「χ^「γ , 八」及 γ」方向任一者中位於中心。 ❹因為開口 824係位於側邊854與側邊856之間的中心, 預期「γ」方向中的氣體分配係實質均勻。因為開口 824 不在「X」方向的中心834,Γχ」方向中的氣體分配可能 不均勻。因此相對於開口 826、828,開口 824提供至少 一可控制方向。沉積過程中,可關閉閥842、846以確保 僅透過開口 824輸送處理氣體。 另一方面,腔室清潔過程中,自遠端電槳源806、808、 810中產生之電漿輸送之自由基可進入穿過所有三個開 ❿ 口 824、826、828以有效地清潔處理腔室。 一實施例中’設備800可如下般運作。可關閉閥842 與846以避免處理氣體穿過開口 826、828進入處理腔 室。因此,處理氣體不經過遠端電漿源808、810、冷卻 塊814、816或氣體供給塊822、824。閥844將打開而 處理氣體將移動通過遠端電漿源806、冷卻塊812、氣體 供給塊81 8並通過開口 824進入處理腔室。處理氣體將 移動通過遠端電漿源806而不被點燃成電漿。藉由僅透 過一開口 824供給氣體進入處理腔室,可控制處理氣體 25 200948219 量並減少中心高沉積的可能性。若透過所有三個開口 824、826、828供給氣體,那麼沉積可能會不均勻且發 生中心高沉積。The wall with the slit valve opening is different from the other three walls, so the slit opening affects the plasma distribution. The RF current applied to the backplane 802 attempts to return to its power source 830, 832, 860, 862. In this return, the rf current moves back along the chamber wall to the power source 830, 832, 860, 862 » because the wall RF potential is different from the plasma RF potential, moving back along the wall to the power source 83 0, 83 2, 860, The RF current of 862 affects the plasma. Since the wall with the φ slit valve opening is different from the other walls, the slit valve opening affects the plasma distribution due to the difference in RF potential. Uneven plasma distribution can cause uneven deposition on the substrate. The process gas flowing into the chamber also affects the plasma distribution. The higher the plasma concentration, the more material is deposited. It has been surprisingly found that when all three openings 824, 8% are delivered to the processing chamber, the amount of deposition that occurs on the central region of the substrate is higher than in other regions. Therefore, the deposited material will be "center high." However, when only the treatment gas is supplied through an opening 824 into the processing chamber and from flowing through the other openings 826, 828 24 200948219, the deposition on the substrate is more uniform. _ . J J prisoner, only through an opening 824 and not through the openings 826, 828 supply * processing gas can reduce the "center height" effect. It is advantageous to supply the non-opening 820 or the opening 828 through the opening 8 2 4 instead of the opening 8, since the opening 824 is flat "ν η, - > ," in the direction of the substantial center between the sides 854, 856 And "X-direction & 8" in the X direction is the same as A. On the other hand, the openings 826, 828 are not centered in any of the "χ^"γ, 八" and γ" directions. Because the opening 824 is centered between the side 854 and the side 856, the gas distribution in the "gamma" direction is expected to be substantially uniform. Since the opening 824 is not in the center 834 of the "X" direction, the gas distribution in the "Γχ" direction may be uneven. Thus, opening 824 provides at least one controllable direction relative to openings 826, 828. During deposition, valves 842, 846 can be closed to ensure that process gas is only delivered through opening 824. On the other hand, during chamber cleaning, the free radicals transported from the remote propeller sources 806, 808, 810 can pass through all three openings 824, 826, 828 for effective cleaning. Chamber. In one embodiment, device 800 can operate as follows. Valves 842 and 846 can be closed to prevent process gases from entering the processing chamber through openings 826, 828. Therefore, the process gas does not pass through the remote plasma source 808, 810, the cooling blocks 814, 816, or the gas supply blocks 822, 824. Valve 844 will open and process gas will move through remote plasma source 806, cooling block 812, gas supply block 81 8 and through opening 824 into the processing chamber. The process gas will move through the remote plasma source 806 without being ignited into a plasma. By supplying gas through only one opening 824 into the processing chamber, the amount of process gas 25 200948219 can be controlled and the likelihood of high center deposition can be reduced. If gas is supplied through all three openings 824, 826, 828, the deposition may be uneven and a high center deposit may occur.

自功率源830、832、860、862將RF電流提供至處理 腔室,透過匹配網路在與開口 824、826、828有所間隔 之位置輸送至背板802。RF電流可點燃處理氣體成電裝 以沉積材料於基材上。處理之後,可移除基材並排空處 理氣體。之後’可清潔處理腔室。打開閥842與846並 自氣源804輸送清潔氣體至遠端電漿源8〇6、8〇8、81〇(其 被點燃成電漿)。來自遠端電漿源8〇6、808、810之自由 基接著可經過冷卻塊812、814、816、氣體供給塊818、 820、822並通過開口 824、826、828進入處理腔室。清 潔氣體接著蝕刻或自處理腔室之暴露表面移除污染物。 清潔過程中,清潔氣體量並非重要考量。事實上,越 多越好,以確保適當地清潔腔室。因此,可透過所有三 個開口 824、826、828供給清潔氣體。如同沉積一樣, 清潔中亦樂見均勻性’但在清潔時,腔室表面對清潔氣 自由基呈現相對惰性,以致主要地移除沉積在腔室表 面上之材料。非常少(若有的話)的腔室被移除。因此, 越多的♦潔乳體自由基越好。爲了媒保存在盡可能多的 清潔自由基’應用所有三個開口 824、826、828。根據 剛剛討論之實施例,清脅h 』π潔過程中,可改變氣體進入腔室 的供給位置以及位置數目。 罝數目清潔之後’可排空處理腔室 而處理腔室再度準備好用於沉積。 26 200948219 第9圖係根據另一實施例之設備900的概要俯視圖。 設備900可為PECVD設備。設備9〇〇包括背板9〇2。氣 源904不僅提供處理氣體至處理腔室,並提供清潔氣體 至處理腔室。雖然顯不單一乳源9〇4,但可理解可應用 多個氣源。 沉積過程中,自氣源904供給處理氣體至處理腔室。 處理氣體在開口 924、926、928 (以虛線顯示)處穿過背 板902進入處理腔室之前,移動經過遠端電漿源9〇6、 參 908、910、冷卻塊912、914、916與氣體供給塊918、 920、922。冷卻塊912、914、916係用來提供遠端電漿 源906、908、910與氣體供給塊918、920、922之間的 連接。遠端電漿源906、908、910可因為電漿達成如此 高溫’使得氣體供給塊918、920、922與遠端電漿源9〇6、 9〇8、910之間的溫度梯度會造成任一者失效。冷卻塊 912、914、916可減少系統失敗的可能性❶ φ 自功率源930提供RF功率至處理腔室,功率源93〇 係透過匹配網路在多個位置處耦接至背板902。如圖所 示,RF功率源930係在與背板902之實質中心934有所 間隔位置處耦接至背板902。可以理解功率源93〇亦可 在其他位置(包括背板902之中心934)處耦接至背板 902。此外,可以约〗〇 MHz與約1 〇〇 之間的頻率傳 送RF功率。傳送RF功率之位置與傳送氣體之位置有所 間隔。 如第9圖中所示’氣體經由開口 924、926、928穿過 27 200948219 背板902進入處理腔室,開口 924、926、928係與背板 902之中心934有所間隔,以致氣體進入處理腔室之位 置與功率源930耦接至背板902之位置分隔。第9圖顯 承之實施例中,開口 924、926、928各自與背板902之 中心934有實質相等間隔。因此,開口 924、926、928 <以相等半徑948、950、952與中心934分隔(以虛線940 所承)。一實施例中,開口 924、926、928可與背板902 之中心934相隔約25與約30英吋之間。 ^ 藉由間隔開口 924、926、928與RF供給位置,可減少 位於處理腔室外之氣體供給塊918、920、922或冷卻塊 912、914、916附近或之中寄生電漿點燃的可能性。腔 室中RF電位差異最大的位置係RF進入腔室處,因為 RF電流沿著壁返回時RF返回路徑就在旁邊。藉由在與 供給氣體進入腔室位置分隔處具有將RF功率耦合至腔 爹之位置,開口 924、926、928係位於RF電位差異減小 之位置。因此,減小寄生電漿形成的可能性。 Φ 此外,可以預定角度α間隔開口 924、926、928。一 實施例中,角度α係12〇度。顯示出三個開口 924、926、 928之第一開口 924係與背板902之兩側954、956具有 實質相等間隔(如箭頭G、Η所示)。第一開口 924與中心 934有所間隔,因此並不位於側邊936與938之間的中 心。其他兩個開口 926、924並不位於任一側邊936、938、 954、956之間的中心。 因為有三個開口 924、926、928,有可能可調節移動 28 200948219 穿過背板902進入處理腔室之處理氣體與/或清潔氣體自 由基。例如,可選擇性打開與關閉閥942、944、946而The RF sources 830, 832, 860, 862 provide RF current to the processing chamber and are delivered to the backplane 802 at a location spaced from the openings 824, 826, 828 through the matching network. The RF current ignites the process gas into an electrical device to deposit material onto the substrate. After processing, the substrate can be removed and the process gas vented. The chamber can then be cleaned. Valves 842 and 846 are opened and purge gas is supplied from gas source 804 to remote plasma sources 8〇6, 8〇8, 81〇 (which are ignited into plasma). Free radicals from remote plasma sources 8〇, 808, 810 can then enter the processing chamber through cooling blocks 812, 814, 816, gas supply blocks 818, 820, 822 and through openings 824, 826, 828. The cleaning gas then etches or removes contaminants from the exposed surface of the processing chamber. The amount of clean gas is not an important consideration during the cleaning process. In fact, the more the better, to ensure that the chamber is properly cleaned. Therefore, the cleaning gas can be supplied through all three openings 824, 826, 828. As with deposition, uniformity is also seen in cleaning' but when cleaned, the chamber surface is relatively inert to the cleansing gas radicals, so that the material deposited on the surface of the chamber is primarily removed. Very few (if any) chambers were removed. Therefore, the more ♦ the milk free radicals, the better. All three openings 824, 826, 828 are applied for the medium to save as many clean radicals as possible. According to the embodiment just discussed, the supply position and the number of positions of the gas entering the chamber can be changed during the mitigation process. After the number of defects is cleaned, the processing chamber can be evacuated and the processing chamber is again ready for deposition. 26 200948219 Figure 9 is a schematic top plan view of a device 900 in accordance with another embodiment. Device 900 can be a PECVD device. The device 9A includes a backing plate 9〇2. Gas source 904 provides not only process gas to the processing chamber but also clean gas to the processing chamber. Although it is not a single source of milk 9 〇 4, it can be understood that multiple gas sources can be applied. During the deposition process, process gas is supplied from gas source 904 to the processing chamber. The process gas moves past the remote plasma source 9〇6, the reference 908, 910, the cooling blocks 912, 914, 916 and before the openings 924, 926, 928 (shown in phantom) pass through the backing plate 902 into the processing chamber. Gas supply blocks 918, 920, 922. Cooling blocks 912, 914, 916 are used to provide a connection between remote plasma sources 906, 908, 910 and gas supply blocks 918, 920, 922. The remote plasma source 906, 908, 910 can achieve such a high temperature because of the plasma 'the temperature gradient between the gas supply blocks 918, 920, 922 and the remote plasma source 9 〇 6, 9 〇 8, 910 One is invalid. Cooling blocks 912, 914, 916 may reduce the likelihood of system failure ❶ φ from power source 930 providing RF power to the processing chamber, and power source 93 is coupled to backplane 902 at a plurality of locations through the matching network. As shown, the RF power source 930 is coupled to the backplane 902 at a spaced apart location from the substantial center 934 of the backplane 902. It will be appreciated that power source 93A can also be coupled to backplane 902 at other locations, including center 934 of backplane 902. In addition, the RF power can be transmitted at a frequency between about 〇 MHz and about 1 。. The position at which the RF power is transmitted is spaced from the position at which the gas is delivered. As shown in Figure 9, 'gas passes through the openings 924, 926, 928 through the 27 200948219 backing plate 902 into the processing chamber, and the openings 924, 926, 928 are spaced from the center 934 of the backing plate 902 such that gas enters the process. The position of the chamber is separated from the position at which the power source 930 is coupled to the backing plate 902. In the embodiment of Fig. 9, the openings 924, 926, 928 are each substantially equally spaced from the center 934 of the backing plate 902. Thus, openings 924, 926, 928 are separated from center 934 by equal radii 948, 950, 952 (indicated by dashed line 940). In one embodiment, the openings 924, 926, 928 can be spaced apart from the center 934 of the backing plate 902 by between about 25 and about 30 inches. By spacing the openings 924, 926, 928 and the RF supply location, the likelihood of parasitic plasma ignition near or within the gas supply blocks 918, 920, 922 or cooling blocks 912, 914, 916 outside the processing chamber can be reduced. The location where the RF potential difference is greatest in the chamber is where RF enters the chamber because the RF return path is next to it as the RF current returns along the wall. The openings 924, 926, 928 are located at a position where the RF potential difference is reduced by having a position to couple RF power to the cavity at a location spaced from the supply gas entering the chamber. Therefore, the possibility of parasitic plasma formation is reduced. Φ In addition, the openings 924, 926, 928 may be spaced apart by a predetermined angle α. In one embodiment, the angle α is 12 degrees. The first opening 924 showing the three openings 924, 926, 928 is substantially equally spaced from the sides 954, 956 of the backing plate 902 (as indicated by arrows G, Η). The first opening 924 is spaced from the center 934 and is therefore not centered between the sides 936 and 938. The other two openings 926, 924 are not centered between either of the sides 936, 938, 954, 956. Because there are three openings 924, 926, 928, it is possible to adjust the movement 28 200948219 through the backing plate 902 into the process chamber processing gas and / or cleaning gas free radicals. For example, valves 942, 944, 946 can be selectively opened and closed.

以預定方式讓處理氣體與/或清潔氣體自由基經過開口 924、926、928進入處理腔室。例如,可選擇性透過一 開口 924、926、928輸送處理氣體與/或清潔氣體而不透 過其他開口 924、926、928輸送。實際上,爲了挽動處 理腔至中之處理氣體與/或清潔氣體自由基,可持續轉換 開口 924、926、928(氣體經由此進入腔室)。對處理氣體 而言,可藉由上述步驟攪動腔室中點燃之電聚。同樣地, 可攪動自遠端電漿源906、908、910輸送之自由基。 設備900將具有進入處理腔室之狹缝閥開口,以允許 基材進入與離開處理腔室。第9圖顯示之實施例中,設 備之側邊936具有狹缝閥開口。因此’開〇 924比開口 926、928置於更遠離狹縫閥開口處。 腔室中的狹缝閥開口會影響腔室中的電漿分佈。因為 具有狹縫閥開口之壁不同於其他三個壁,所以狹縫閥開 口會影響電漿分佈。施加至背板9〇咖電流試圖返回 其功率源930。如此返回中,RF電流沿著腔室壁移動回 功率源930。因為壁RF電位相對電漿rf電位之差異, =壁移動回功率源93。之灯電流會影響電漿。因為具 有狹縫閥開口之壁不同於装 、 、、壁,所以狹.縫閥開口因為· RF電位差異而影響電 ㈣電漿刀佈。不均句電漿分佈會造成基 材上的不均勻沉積。 流入腔室之處理氣體亦影 響電漿分佈。電浆 >辰度越向, 29 200948219 材料沉積越多。已經出乎意外地發現當透過所有三個開 口 924、926、928輸送處理氣體至處理腔室時,出現在 基材中心區域上的沉積量係高於其他區域。因此,沉積 材料將係「中心高」。然而,當僅透過一開口 924供給處 理氣體進入處理腔室且避免透過其他開口 92 6、928流動 時’基材上的沉積係更均勻。因此,僅透過一開口 924 而不透過開口 926、928供給處理氣體可減少「中心高」 效應》 ❻、、 透過開口 924而非開口 926或開口 928供給係有利 的’因為開口 924在「Y」方向中位於側邊954、956之 間的實質中心,而「X」方向中則無。另一方面,開口 926、928沒有在「X」或「γ」方向任一者中位於中心。 因為開口 924係位於側邊954與侧邊956之間的中心, 預期「Y」方向中的氣體分配係實質均勻。因為開口 924 不在「X」方向的中心934,「X」方向中的氣體分配可能 • 不均勻。因此相對於開口 926、928,開口 924提供至少 一可控制方向。沉積過程中,可關閉閥942、946以確保 僅透過開口 924輸送處理氣體。 另一方面,腔室清潔過程中,自遠端電漿源9〇6、9〇8、 910中產生之電漿輸送之自由基可進入穿過所有三個開 口 924、926 ' 928以有效地清潔處理腔室。 一實施例中’設備900可如下般運作。可關閉閥942 與946以避免處理氣體穿過開口 926、928進入處理腔 至。因此,處理氣體不經過遠端電漿源9〇8、冷卻 30 200948219 塊914、916或氣體供給塊922、924。閥944將打開而 處理氣體將移動通過遠端電聚源906、冷卻塊912、氣體 供給塊918並通過開口 924進入處理腔室。處理氣體將 移動通過遠端電漿源906而不被點燃成電漿。藉由僅透 過一開口 924供給氣體進入處理腔室,可控制處理氣體 量並減少中心高沉積的可能性。若透過所有三個開口 924、926、928供給氣體,那麼沉積可能會不均勻且發 生中心高沉積。 自功率源930將RF電流提供至處理腔室,透過匹配網 路在與開口 924、926、928有所間隔之位置輸送至背板 902。RF電流可點燃處理氣體成電漿以沉積材料於基材 上。處理之後,可移除基材並排空處理氣體。之後,可 清潔處理腔室。打開閥942與946並自氣源904輸送清 潔氣體至遠端電漿源906、908、910(其被點燃成電漿)。 來自遠端電漿源906、908、910之自由基接著可經過冷 φ 卻塊912、914 ' 916、氣體供給塊918、920、922並通 過開口 924、926、928進入處理腔室。清潔氣體接著蝕 刻或自處理腔室之暴露表面移除污染物。 清潔過程中,清潔氣鱧量並非重要考量。事實上,越 多越好,以確保適當地清潔腔室。因此,可透過所有三 個開口 924、926、928供給清潔氣體。如同沉積一樣, 清潔中亦樂見均勻性,钽在清潔時,腔室表面對清潔氣 體自由基呈現相對惰性,以致主要地移除沉積在腔室表 面上之材料。非常少(若有的話)的腔室被移除。因此, 31 200948219 越多的清潔氣體自由基越好。爲了確保存在盡可能多的 清潔自由基,應用所有三個開口 924、926、928 »根據 剛剛討論之實施例’清潔過程中,可改變氣體進入腔室 的供給位置以及位置數目。清潔之後,可排空處理腔室 而處理腔室再度準備好用於沉積。 藉由分隔RF電流耦合背板之位置以及處理氣體耗合 至背板之位置,可減少通到處理腔室之氣體供給中寄生 電漿的形成。: 雖然上述係關於本發明之實施例,但可設計出本發明 其他與進一步實施例而不捧離其之基本範圍,其之範圍 係由隨後之申請專利範圍所確定。 【圖式簡單說明】 為了更詳細地了解本發明之上述特徵,可參照實施例 (某些描繪於附圖中)來理解本發明簡短概述於上之特定 描述。然而,需注意附圖僅描螬本發明之典型實施例而 因此不被視為其之範圍的限制因素,因為本發明可允許 其他等效實施例。 第1圖係根據本發明一實施例耦合至處理腔室100之 功率源102與氣源104的概要圖示。 第2A圖係根據本發明一實施例之處理腔室200的概要 剖面圖。 第2B圖係顯示RF電流路徑之第2A圖處理腔室200 32 200948219 的概要剖面圖。 第3圖係根據本發明一實施例之處理腔室3〇〇的背板 302之概要等角圖。 第4圖係根據本發明一實施例之遠端電漿源與處理腔 室之間耦合的概要圖示。 第5圖係根據一實施例之處理腔室500的背板502之 概要等角圖。 第6圖係根據一實施例顯示氣體導入通道對應位置之 基材支撐件的概要俯視圖。 第7圖係根據另一實施例之設備700的概要俯視圖。 第8圖係根據另一實施例之設備8〇〇的概要俯視圖。 第9圖係根據另一實施例之設備900的概要俯視圖。 爲了助於理解,已經盡可能應用相同元件符號來代表 圖不中共有的相同元件。可思及一實施例揭露之元件可 有利地用於其他實施例而不必特別註明。 【主要元件符號說明】 100、200、300、500 處理腔室 102、224、730、830、832、860、862、930 功率源 104、234、308、508、704、804、904 氣源、 106、108A、108B、23 6、238、324、326、524、526 位 置 202 ' 302、502、702 ' 802、902 背板 33 200948219 204 基座 206 基材 208 腔室主體 210 喷頭 212 氣體通道 214 氣室 216 處理空間 218 上游側 220 下游側 222 狹縫閥開口 226 供給線 228、306、506、706、708、710、806' 808、810' 906、 908、910 遠端電漿源Process gas and/or cleaning gas radicals are passed through openings 924, 926, 928 into the processing chamber in a predetermined manner. For example, the process gas and/or cleaning gas may be selectively delivered through an opening 924, 926, 928 without being conveyed through other openings 924, 926, 928. In effect, openings 924, 926, 928 (through which the gas enters the chamber) can be continuously transitioned in order to move the processing gas to the process gas and/or cleaning gas radicals. For the process gas, the electrocoagulation ignited in the chamber can be agitated by the above steps. Likewise, free radicals transported from the distal plasma source 906, 908, 910 can be agitated. Apparatus 900 will have a slit valve opening into the processing chamber to allow substrate entry and exit from the processing chamber. In the embodiment shown in Fig. 9, the side 936 of the device has a slit valve opening. Therefore, the opening 924 is placed farther away from the slit valve opening than the openings 926, 928. The slit valve opening in the chamber affects the plasma distribution in the chamber. Since the wall with the slit valve opening is different from the other three walls, the slit valve opening affects the plasma distribution. The current applied to the backplane 9 attempts to return to its power source 930. In this return, the RF current moves back to the power source 930 along the chamber wall. Because of the difference in wall RF potential versus plasma rf potential, the =wall moves back to power source 93. The lamp current affects the plasma. Since the wall with the slit valve opening is different from the mounting, wall, and wall, the slit valve opening affects the electric (4) plasma knife cloth due to the difference in RF potential. Inhomogeneous plasma distribution can cause uneven deposition on the substrate. The process gas flowing into the chamber also affects the plasma distribution. Plasma > Chen Yue, 29 200948219 The more material deposits. It has been surprisingly found that when the process gas is delivered to the processing chamber through all three openings 924, 926, 928, the amount of deposition that occurs on the central region of the substrate is higher than in other regions. Therefore, the deposited material will be "center high." However, when the process gas is supplied through only one opening 924 into the processing chamber and from flowing through the other openings 92, 928, the deposition on the substrate is more uniform. Therefore, the supply of the process gas through only one opening 924 without passing through the openings 926, 928 can reduce the "center height" effect, and the supply through the opening 924 instead of the opening 926 or the opening 928 is advantageous because the opening 924 is at "Y". The direction is located at the substantial center between the sides 954, 956, but not in the "X" direction. On the other hand, the openings 926, 928 are not centered in either the "X" or "γ" directions. Since the opening 924 is centered between the side 954 and the side 956, the gas distribution in the "Y" direction is expected to be substantially uniform. Since the opening 924 is not in the center 934 of the "X" direction, the gas distribution in the "X" direction may be uneven. Thus, the opening 924 provides at least one controllable direction relative to the openings 926, 928. During deposition, valves 942, 946 can be closed to ensure that process gas is only delivered through opening 924. On the other hand, during the chamber cleaning process, the free radicals transported from the plasma generated in the remote plasma source 9〇6, 9〇8, 910 can enter through all three openings 924, 926 '928 to effectively Clean the processing chamber. In one embodiment, device 900 can operate as follows. Valves 942 and 946 can be closed to prevent process gases from entering the processing chamber through openings 926, 928. Therefore, the process gas does not pass through the remote plasma source 9〇8, cooling 30 200948219 blocks 914, 916 or gas supply blocks 922, 924. Valve 944 will open and process gas will move through remote electropolymer source 906, cooling block 912, gas supply block 918 and through opening 924 into the processing chamber. The process gas will move through the remote plasma source 906 without being ignited into a plasma. By feeding gas into the processing chamber through only one opening 924, the amount of process gas can be controlled and the likelihood of high center deposition can be reduced. If gas is supplied through all three openings 924, 926, 928, the deposition may be uneven and a high center deposit may occur. The self-power source 930 provides RF current to the processing chamber and is delivered to the backplane 902 at a location spaced from the openings 924, 926, 928 through the matching network. The RF current ignites the process gas into a plasma to deposit material onto the substrate. After processing, the substrate can be removed and the process gas vented. The processing chamber can then be cleaned. Valves 942 and 946 are opened and a purge gas is delivered from gas source 904 to remote plasma sources 906, 908, 910 (which are ignited into plasma). The radicals from the remote plasma source 906, 908, 910 can then pass through the cold φ block 912, 914 ' 916, gas supply blocks 918, 920, 922 and through the openings 924, 926, 928 into the processing chamber. The cleaning gas then etches or removes contaminants from the exposed surface of the processing chamber. Cleaning the amount of air is not an important consideration during the cleaning process. In fact, the more the better, to ensure that the chamber is properly cleaned. Therefore, the cleaning gas can be supplied through all three openings 924, 926, 928. As with deposition, uniformity is also observed during cleaning. When cleaning, the surface of the chamber is relatively inert to the free radicals of the cleaning gas, so that the material deposited on the surface of the chamber is primarily removed. Very few (if any) chambers were removed. Therefore, 31 200948219 The more cleaning gas free radicals, the better. To ensure that as many cleaning radicals as possible are present, all three openings 924, 926, 928 are applied. » According to the embodiment just discussed, during the cleaning process, the supply position of the gas into the chamber and the number of positions can be varied. After cleaning, the processing chamber can be evacuated and the processing chamber ready for deposition. By separating the position of the RF current coupling backplane and the location of the process gas to the backing plate, the formation of parasitic plasma in the gas supply to the processing chamber can be reduced. While the foregoing is a description of the embodiments of the present invention, it is intended to BRIEF DESCRIPTION OF THE DRAWINGS For a more detailed understanding of the above described features of the present invention, reference should be made It is to be understood, however, that the invention is not limited by the 1 is a schematic illustration of a power source 102 and a gas source 104 coupled to a processing chamber 100 in accordance with an embodiment of the present invention. Figure 2A is a schematic cross-sectional view of a processing chamber 200 in accordance with an embodiment of the present invention. Figure 2B is a schematic cross-sectional view showing the processing chamber 200 32 200948219 of Figure 2A of the RF current path. Figure 3 is a schematic isometric view of a backing plate 302 of a processing chamber 3 in accordance with an embodiment of the present invention. Figure 4 is a schematic illustration of the coupling between a remote plasma source and a processing chamber in accordance with an embodiment of the present invention. Figure 5 is a schematic isometric view of the backing plate 502 of the processing chamber 500 in accordance with an embodiment. Fig. 6 is a schematic plan view showing a substrate support member corresponding to a position of a gas introduction passage, according to an embodiment. Figure 7 is a schematic top plan view of an apparatus 700 in accordance with another embodiment. Figure 8 is a schematic top plan view of a device 8A according to another embodiment. Figure 9 is a schematic top plan view of an apparatus 900 in accordance with another embodiment. To facilitate understanding, the same component symbols have been used as much as possible to represent the same components that are common to the drawings. It is contemplated that elements disclosed in one embodiment may be used in other embodiments without particular limitation. [Main component symbol description] 100, 200, 300, 500 processing chambers 102, 224, 730, 830, 832, 860, 862, 930 power source 104, 234, 308, 508, 704, 804, 904 gas source, 106 108A, 108B, 23 6, 238, 324, 326, 524, 526 Position 202 ' 302, 502, 702 ' 802, 902 Backplane 33 200948219 204 Base 206 Substrate 208 Chamber Body 210 Head 212 Gas Channel 214 Air chamber 216 processing space 218 upstream side 220 downstream side 222 slit valve opening 226 supply line 228, 306, 506, 706, 708, 710, 806' 808, 810' 906, 908, 910 distal plasma source

230、314、402、514、712、714、716、812、814、816、 912 ' 914 > 916 冷卻塊 232、322、400、522 扼流器或電阻器 240 ' 406 管 304、504 RF功率源 310、510 氣體管 312、512、742、744、746、842、844、846、942 ' 944、 946 閥 316 ' 516 冷卻源 318 > 320 ' 518 ' 520 404 連接塊 412 内管 602 、 734 ' 834 、 934 冷卻管 408 、 410 端 414 套管 中心 700 ' 800 ' 900 設備 718、720 ' 722、818 ' 820、822、918 ' 920、922 氣 體供給塊 724、726、728、824、826、828、924、926、928 開 34 200948219230, 314, 402, 514, 712, 714, 716, 812, 814, 816, 912 '914 > 916 cooling block 232, 322, 400, 522 choke or resistor 240 ' 406 tube 304, 504 RF power Source 310, 510 gas tubes 312, 512, 742, 744, 746, 842, 844, 846, 942 '944, 946 valve 316 ' 516 cooling source 318 > 320 ' 518 ' 520 404 connecting block 412 inner tubes 602 , 734 '834, 934 cooling tube 408, 410 end 414 casing center 700 '800 '900 equipment 718, 720 '722, 818 '820, 822, 918 '920, 922 gas supply blocks 724, 726, 728, 824, 826, 828, 924, 926, 928 Open 34 200948219

732 匹配網路 736、73 8' 754、756、836、838、854、856' 936、938 ' 954、95 6 侧邊 740、840 ' 940 虛線 748、750、752、848、850、852、948、950、952 半 35732 matching network 736, 73 8' 754, 756, 836, 838, 854, 856' 936, 938 '954, 95 6 side 740, 840 '940 dashed line 748, 750, 752, 848, 850, 852, 948 , 950, 952 half 35

Claims (1)

200948219 七、申請專利範圍: 1. 一種電漿處理設備,其至少包括: 處理腔至’具有一氣體分配喷頭與一大致矩形背 板; -或更多功率源,在—或更多第—位置_接至該背 板;及 一或更多氣源,在三個其他位置耦接至該背板,該三 φ 個其他位置各自與該一或更多第-位置分隔’其中該三 個位置之一係置於一第二位置,該第二位置與該背板之 兩個平行側邊之間有實質相等距離。 2. 如申請專利範圍第1項所述之設備,其中該設備係一 電漿增強化學氣相沉積設備。 3. 如申請專利範圍第1項所述之設備,其中該一或更多 ® 功率源包括複數個各自在分隔位置耦接至該背板之功率 4. 如申請專利範圍第1項所述之設備,其中該三個位置 係以一實質相等距離與該第一位置間隔並以約12〇度相 互間隔。 5. 如申請專利範圍第1項所述之設備,更包括一或更多 36 200948219 遠端電漿源,耦接至該至少一氣源。 6. 如申請專利範圍第5項所述之設備,其中該一或更多 遠端電漿源包括三個遠端電浆源。 7. 如申請專利範圍第1項 迷之5又備’更包括一狹縫閥 開口穿過該處理腔室之一第一壁。 © 8.如申請專利範圍第7項所沭夕机锯甘丄从祕 項所述之3又備,其中該第二位置 係配置比該一或更多第一伤番音 ^ ^ 位置更退離該狹縫閥開口。 9. 一種電漿增強化學氣相沉積設備,其至少包括: 一處理腔室,具有一狹縫閥開口穿過至少一壁; 一氣體分配噴頭,置於該處理腔室中並與一基材支撐 件有所間隔; 一背板’置於該氣體分配喷頭後並與該氣體分配喷頭 有所間隔,該背板具有在三個位置穿過其之三個開口, 其中該二個位置之一位置係配置比該其他兩個位置更 遠離該狹縫閥開口; 一或更多氣源’在該三個位置耦接至該背板;及 一或更多RF功率源,在與該三個位置間隔之位置耦 接至該背板。 10. 如申請專利範圍第9項所述之設備,其中該一或更多 37 200948219 RF功率源包括一在該背板之一實質中心耦接至該背板 之RF功率源。 11. 如申請專利範圍第10項所述之設備,其中該三個位 置係各自配置與該背板之中心相隔一實質相等徑向距 離。 12. 如申請專利範圍第u項所述之設備,其中該三個位 置係相互間隔約120度。 13. 如申請專利範圍第9項所述之設備,更包括一遠端電 漿源’在各個該三個位置耦接至該背板。 14. 一種方法,依序包括: 透過一第一位置將處理氣體導入一腔室; 點燃該處理氣體成一電漿; 沉積材料於一基材上; 將清潔氣體導入一或更多遠端電漿源; 在該一或更多遠端電漿源中點燃該清潔氣體成一電 漿;及 透過該第一位置與至少一與該第—位置分隔之第二 位置自該遠端點燃之清潔氣體電漿流動自由基進入該 腔室。 38 200948219 15_如申請專利範圍第14項所述之方法,其中該腔室具 有一狹縫閥開口穿過該腔室之一第一壁,而該自由基流 過之第二位置比該第一位置更接近該狹缝閥開口。 16. 如申請專利範圍第μ項所述之方法,其中該方法係 一電漿増強化學氣相沉積方法。 17. 如申請專利範圍第16項所述之方法,其中該腔室具 有一背板’該點燃之清潔氣體自由基與該處理氣體係經 由該背板導入,且其中該第一位置係與該背板之一實質 中心有所間隔。 18. 如申請專利範圍第17項所述之方法,其辛該至少一 其他位置包括兩個位置,且其中該兩個位置與該第一位 置係與該背板之實質中心有實質相等間隔。 19. 如申請專利範圍第is項所述之方法,其中該兩個位 置與該第一位置係相互間隔約120度。 20. 如申請專利範圍第14項所述之方法,更包括在一與 該第一位置間隔之位置施加一 RF電偏壓至該腔室中之 一電極。 39200948219 VII. Patent application scope: 1. A plasma processing equipment, comprising at least: a processing chamber to 'having a gas distribution nozzle and a substantially rectangular back plate; - or more power sources, at - or more - Position_connected to the backplane; and one or more air sources coupled to the backplane at three other locations, the three φ other locations being separated from the one or more first-positions, wherein the three One of the positions is placed in a second position that is substantially equidistant from the two parallel sides of the backing plate. 2. The apparatus of claim 1, wherein the apparatus is a plasma enhanced chemical vapor deposition apparatus. 3. The device of claim 1, wherein the one or more power sources comprise a plurality of powers each coupled to the backplane at a separation location. 4. As described in claim 1 Apparatus wherein the three locations are spaced from the first location by a substantially equal distance and are spaced apart from each other by about 12 degrees. 5. The apparatus of claim 1, further comprising one or more 36 200948219 remote plasma sources coupled to the at least one gas source. 6. The device of claim 5, wherein the one or more remote plasma sources comprise three remote plasma sources. 7. As claimed in the first paragraph of the patent application, the invention further includes a slit valve opening through the first wall of one of the processing chambers. © 8. For example, in the seventh paragraph of the patent application scope, the saw blade is prepared from the 3 item described in the above, wherein the second position configuration is more backward than the one or more first injury sounds ^ ^ position Open the slit valve. 9. A plasma enhanced chemical vapor deposition apparatus, comprising: at least: a processing chamber having a slit valve opening through at least one wall; a gas distribution showerhead disposed in the processing chamber and associated with a substrate The support members are spaced apart; a backing plate is disposed behind the gas distribution showerhead and spaced apart from the gas distribution showerhead, the backing plate having three openings therethrough at three locations, wherein the two locations One of the positional configurations is further from the slit valve opening than the other two locations; one or more gas sources 'coupled to the backing plate at the three locations; and one or more RF power sources, The position of the three position intervals is coupled to the backplane. 10. The device of claim 9, wherein the one or more of the 37 200948219 RF power sources comprise an RF power source coupled to the backplane substantially at a center of the backplane. 11. The apparatus of claim 10, wherein the three locations are each configured to be substantially equidistant from the center of the backing plate. 12. The device of claim 5, wherein the three locations are spaced apart from each other by about 120 degrees. 13. The apparatus of claim 9 further comprising a remote plasma source coupled to the backplane at each of the three locations. 14. A method comprising: introducing a process gas into a chamber through a first position; igniting the process gas into a plasma; depositing material on a substrate; and introducing the cleaning gas into one or more remote plasmas Source: igniting the cleaning gas into a plasma in the one or more remote plasma sources; and cleaning gas from the distal end through the first position and at least one second position separated from the first position The slurry flows free radicals into the chamber. 38. The method of claim 14, wherein the chamber has a slit valve opening through a first wall of the chamber, and the free radical flows through the second position A position is closer to the slit valve opening. 16. The method of claim 5, wherein the method is a plasma-based chemical vapor deposition method. 17. The method of claim 16, wherein the chamber has a backing plate 'the ignited cleaning gas radicals and the processing gas system are introduced via the backing plate, and wherein the first location is associated with the One of the back plates is separated by a substantial center. 18. The method of claim 17, wherein the at least one other location comprises two locations, and wherein the two locations and the first location are substantially equally spaced from a substantial center of the backplane. 19. The method of claim 1, wherein the two locations are spaced apart from the first location by about 120 degrees. 20. The method of claim 14, further comprising applying an RF electrical bias to an electrode in the chamber at a location spaced from the first location. 39
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