4 6ϋ 6 0 a 經濟部中央標準局員工消費合作社印製 Α7 Β7五、發明説明(1 ) ~ ^ ^ 本發明有關一種賤射塗覆法’尤其是一種用以進行,子 化物理性蒸汽沉積(IPVD)以將材料塗覆於基板上乏 J 〜々法及 裝置。 發明背景= I 次微米鬲鏡孔比圖型諸如通孔、溝槽及接觸孔於半導P 製造過程中產生各式各樣之塗覆問題。製造極大划及超大 型積體(VLSI及ULSI)半導體裝置時,該等圖型於底部之接 點經常需塗覆智·料’而該等圖型經常需充塡導電性金屬。 於許多需沉積薄膜之半導體裝置製造過程中,或需或至少 較好使用物理性蒸汽沉積(PVD)法施加塗層。使用物理性 方法於窄幅高鏡孔比圖型(隙孔)底部沉積薄膜時,欲沉積 於該基板上之材料的移動需達到高度方向性。鏡孔比較高 之圖型需要較高之方向性。於位於基板表面上之例如窄幅 高鏡孔比孔之底部塗覆接點時,塗覆材料粒子需於相對於 法線實質上不大於該圖型之角型開口之角度下移動。 於半導體裝置製造過程中,需將例如位於寬度可能介於 0-25至0.3 5微米範園内之高鏡孔比隙孔及溝槽底部之接點 金屬化,而其隨著裝置之持續小型化的趨勢而愈見狹窄。 期望使用物理性沉積方法諸如爽射塗覆法將該接點金屬化 ,因爲P VD法於所得到之膜純度、通量 '及整體成本及處 理設備之簡易性方面在技術上及經濟上皆具有超越代用方 法之優點。例如’化學蒸汽沉積(CVD)法因爲該化學方法 於基板之隙孔或溝槽内表面上形成薄膜之能力,而有時用 於在冰孔及溝槽中沉積薄膜3然而’ 1¾ C V D方法經常需要 -4- 本纸張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) I II (請先閲讀背面之注再填寫本頁) 、-° •IO. 經濟部中央標準局員工消費合作杜印製 * 460602 A7 --------- 一__B7_ 五、發明説明(2 ) 一—~一 "~ 較PVD万法複雜而昴貴之設備。該CVD方法因其化學性 質,故經常涉及環境因素並採用可提供裝置污染來源之化 學先矢,此等系統於非生產時間内一般需要較高頻率之維 修。就許多類型之薄膜而言,pVD方法較cVD方法快速 ,產生較佳通量,因而成本較低。此外’ CVD方法可能不 存在於或可能無法實際應用於許多沉積材料,諸如需要可 能防礙CVD沉積之複雜先質及輸送系統。鈦、氮化鈦及鎢 具有可接受之製造CVD方法。然而,用於鋁、銅' 钽及氮 化钽之CVD方法不是不存在’即若存在,亦不成熟或不具 工業化之可能。此外,於某此方法中,CVD會使在該基板 所邵分形成之裝置長期受熱,而使位於材料邊界之材料移 動及擴散’或使該裝置遭受到其他因熱所致之損傷或超過 所研究之方法的熱極限3 因爲尺寸縮小而圖型之鏡孔比增高,故於特定應用中, 藉著物理性备汽沉積法施加塗層之優勢,增加了在賤射過 程中使該塗覆材料移向基板之方向性増高之需求^除非入 射於基板上之濺射材料粒子路徑可保持高度平行而與該基 板表面之平面垂直’否則嚐試濺射塗覆高鏡孔比圖塑會於 該圖型之較高側面或圖型口部封密處導致過度沉積,此時 該物理性沉積法無法得到令人滿意之結果。 濺射塗覆法一般係將基板及高純度塗覆材料之靶極置於 充填有惰性氣體諸如氬之眞空艙中並於該氣體中產生電浆 而進行3該電装係藉著使該極持續或斷續地保持於負f 位,使該乾極作爲陰極以提供電子,激發該驗中之氣體, -5- 本紙張尺度適用中國國家搮隼(CNS) A4規格(210X297公釐) ---— (請先閎讀背面之注意事項再填寫本頁) ——訂 A7 460602 _______ 87 五、發明説明(3 ) 而於與靶極表面鄰近處形成電漿而產生。該電衆產生通常 係使用磁控管陰極组件增進,其中位於靶極後方之磁體將 此等電子捕集於該靶極表面上,於此處撞擊該過程氣體之 原子’自氣體原子脱出電子’並將彼轉化成正離子。該氣 體離孚被加速衝向負電荷之靶極,於此處撞擊表面,而自 靶極表面噴射出靶極衬料之原子及原子團或粒子及二次電 子。該二次電子於保持電漿中扮演著主要之角色。所喷射 之乾極材料粒子爲電中性,於各個方向傳向該眞空空間, 有些撞擊基板,黏著於該處而形成薄膜。基板上較窄之圖 型及較南鏡孔比之圖型降低該隙孔之可接受角度,遮蔽囷 型之側面,增加被圖型側面及周圍所截取之入射粒子,沉 積於圖型底部之粒子數更少。 已使用各種流程使經傳播之粒子直線垂直移向基板表面 。其中一項研究包括於該靶極與該基板之間使用物理性準 直儀板,以使入射角正常分佈,並藉著以該準直儀截取低 角度粒子而改善入射粒子之方向性,僅使垂直或接近垂直 基板之粒子通過該準直儀。另一項稱爲長程型濺射之研究 係增加該靶極到基板之間隔,使得僅有與基板成垂直或接 近垂直角度之粒子通過該艙長度方向而撞擊該基板,準直 儀提供微粒污染之來源,因爲所截取之粒子沉積於該準直 儀上’於該處積聚,最後剝離,準直沉積及長程式流程兩 者皆藉著消除於低角度下移向基板之材料而達到方向性, 大幅降低入射於基板上之濺射材料百分比,故實質降低沉 積速率°亦增加維修之頻率,降低靶極材枓之利用性,並 -6- 本紙張尺度逋用中國國家標準(CNS ) Α4規格(210Χ297公餐) (請先閲讀背面之注意事項再填寫本頁} 、-=s 經濟部中央標準局員工消費合作杜印製 4606u2 第87丨〇924〇珑專利申請案 屮文說明書修正頁(88年12月) A7 ---------- -R7 _ 五、發明説明(4)\7~^W^~ -- ΐΛ.ν補充, 降低通量。 另種供新的思考之直接漱射材料的方法係為離子化 濺射法,通稱為離子化物理性蒸汽沉積或IPVD。使用IPVD 寺塗覆材料係使用磁控管;賤射或其他習用賤射或蒸發技 ύ自靶極’X射。於濺射塗覆方法中’濺射粒予係於寬幅發 射角下自把極發射叫PVD意圖藉著離予化該粒子而改善 μ方向丨生使其可靜電性地或電性地操縱至與基板垂直之 方向& 於IP VD中,在介於該靶極與該基板間之空間中的氣體中 產生額外電漿’所濺射之粒子路經彼而到達基板。於先前 技蟄中’係藉著各種方法於該空間中產生該額外電裝,諸 如和RF把量電谷性地耦合於位在乾極下游之餘房中,或藉 %子迴捉加速器共振(ECR)或其他微波電漿產生技術於遠 離邊空間處形成電漿,再使之流入該空間中。通過該空間 之粒子撞擊該離子化處理氣體之電子或亞穩中子^該撞擊 使電子脫離經濺射粒子之原予,而使該粒予具有正電荷。 此等經滅射材科之正離子藉由例如於該基板上施加負偏壓 而向著基板電加速。 經濟部中央樣準局負工消費合作社印裝 (請先聞讀背面之注意事項再填寫本頁) 先fl’i技藝之IPVD方法顯示數項妨礙其使用於實際製造 環境之缺點及問題。該等方法例如整體效率低。尤其, 方法之沉積速率一般較低。此外,該先前技藝方法之膜污 染程度高。尤其,使用先前技藝IPVD方法時,當靶極濺射 说力增加時’會損及高鏡孔比圖型之充填。該種損害使鋁 合金之滅射限制於在使用12英吋磁控管靶極時低於3仟瓦 本纸張尺度賴帽邮鮮^74規格⑺D χ 297 4 6 0 6 0 A7 ________B7 五、發明説明(5 ) 於3仟瓦直流電能,而一般使用該種耙極/磁控管组合皆可 達到12至j 0仟瓦。該低濺射能力導致低沉積速率,造成 低產量及通量’而污染增高,例如每個晶圓1 〇至4〇分鐘 之錢射時間,而一般晶圓時間约45秒至1分鐘^此外,已 發現¥非係於該濺射艙中於相當高壓諸如2〇至4〇毫托耳 下操作該裝置,否則經濺射材料之部分離子化程度低。使 用氬處理氣體時,該壓力高於—般低於丨5毫托耳或於低毫 托耳範圍内疋所期望濺射壓力。較高壓力易降低沉積膜性 質I品質並增加膜污染。此外,較高操作壓力降低必需有 較大眞it艙設計之方法的平面場均勻性,而進一步降低離 子化效率。先前技藝IPVD方法所產生之其他問題有電漿 非必要地濺射RF電極或元件、因不期望之沉積而累積之濺 射材料自該RF元件剝離、RF元件因電漿沉積於該元件上 t材料而短路、及電漿及材料與用以將該RF能量耦合於該 毛毁内以使孩賤射材料離子化之電極或元件之其他相互作 用。 經濟部中央標準局員工消費合作社印製 疋故,IPVD裝置及方法具有克服先前技藝之缺點及問 題的需求。尤其’需要—種具有可接受之高整體效率、特 问义沉積速率、高濺射材料離子化效率及低沉積膜污染度 且貴際而有效之IP VD裝置。尤其需要一種製造高均勻度 及南品質之薄膜’而針對該方法提供足以工業化之產能之 裝置ΰ 發明簡i :4 6ϋ 6 0 a Printed by the Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economic Affairs A7 B7 V. Description of the Invention (1) ~ ^ ^ The present invention relates to a low-level coating method, especially a method for carrying out rational vapor deposition of chemical compounds. (IPVD) There are no methods and devices for coating materials on a substrate. Background of the Invention = I-submicron mirror-hole ratio patterns such as through-holes, trenches, and contact holes cause various coating problems during the fabrication of semiconductors. When manufacturing large-scale and ultra-large-scale integrated (VLSI and ULSI) semiconductor devices, the contacts at the bottom of these patterns often need to be coated with smart materials, and these patterns often need to be filled with conductive metal. In many semiconductor device manufacturing processes where thin films need to be deposited, it may be necessary or at least preferred to apply a coating using a physical vapor deposition (PVD) method. When using a physical method to deposit a thin film at the bottom of a narrow, high mirror hole ratio pattern (gap hole), the movement of the material to be deposited on the substrate needs to be highly directional. Patterns with higher mirror holes require higher directivity. When coating a contact on the bottom of a substrate, such as a narrow high mirror hole ratio hole, the coating material particles need to move at an angle that is substantially not larger than the angular opening of the pattern relative to the normal. In the manufacturing process of semiconductor devices, for example, the contacts at the bottom of the high mirror hole ratio gap and the trench, which may be in the range of 0-25 to 0.3 5 micron, need to be metallized, and as the device continues to be miniaturized Trend has become increasingly narrow. It is desirable to metallize the contacts using a physical deposition method, such as a spray coating method, because the PVD method is technically and economically effective in terms of the film purity, flux ', and overall cost and ease of processing equipment obtained. Has the advantage of surpassing alternative methods. For example, 'Chemical Vapor Deposition (CVD) is sometimes used to deposit thin films in ice holes and trenches because of its ability to form thin films on the internal surfaces of gaps or trenches in substrates. However,' 1¾ CVD methods are often Requirement -4- This paper size applies to Chinese National Standard (CNS) A4 specification (210X297 mm) I II (Please read the note on the back before filling out this page),-° • IO. The consumer cooperation of the Central Standards Bureau of the Ministry of Economic Affairs Du printed * 460602 A7 --------- __B7_ V. Description of the invention (2) Ⅰ ~~ 1 " ~ The equipment is more complicated and expensive than PVD. Because of its chemical nature, the CVD method often involves environmental factors and uses a chemical precursor that can provide a source of device pollution. These systems generally require higher-frequency maintenance during non-productive times. For many types of films, the pVD method is faster than the cVD method, produces better throughput, and is therefore less costly. In addition, CVD methods may not exist or may not be practically applicable to many deposition materials, such as requiring complex precursors and delivery systems that may prevent CVD deposition. Titanium, titanium nitride, and tungsten have acceptable CVD manufacturing methods. However, CVD methods for aluminum, copper 'tantalum and tantalum nitride are not non-existent', that is, if they exist, they are not mature or industrially possible. In addition, in a certain method, CVD will cause the device formed on the substrate to be heated for a long period of time, and cause the material located at the material boundary to move and diffuse 'or cause the device to suffer other heat-induced damage or exceed the The thermal limit of the research method 3 Because the size of the pattern is reduced and the mirror aperture ratio is increased, in certain applications, the advantage of applying a coating by physical vapor deposition method has increased the application of the coating during the low shot process. The requirement for high directivity of the material moving to the substrate ^ Unless the path of the sputtered material particles incident on the substrate can be kept highly parallel and perpendicular to the plane of the substrate surface ', attempts to sputter coating with a high mirror hole ratio will result in The high side of the pattern or the sealed portion of the mouth of the pattern causes excessive deposition, and at this time, the physical deposition method cannot obtain satisfactory results. The sputtering coating method is generally performed by placing a target of a substrate and a high-purity coating material in an empty chamber filled with an inert gas such as argon and generating a plasma in the gas. Or intermittently maintain the negative f position, make the dry pole serve as a cathode to provide electrons, and excite the gas in the test. -5- This paper size is applicable to China National Cricket (CNS) A4 specification (210X297 mm)- -— (Please read the precautions on the back before filling out this page) ——Order A7 460602 _______ 87 V. Description of the invention (3) It is generated by the formation of plasma near the target surface. The generation of the electric mass is usually enhanced by using a magnetron cathode assembly, in which a magnet located behind the target traps these electrons on the surface of the target, where the atoms of the process gas are impacted 'from the gas atoms, the electrons are released' And transform it into positive ions. The gas ion is accelerated toward the negatively charged target, where it hits the surface, and the atoms and atomic groups or particles and secondary electrons of the target lining are ejected from the target surface. This secondary electron plays a major role in maintaining the plasma. The sprayed dry electrode material particles are electrically neutral and propagate to the empty space in all directions. Some of them strike the substrate and adhere to them to form a thin film. The narrower pattern on the substrate and the pattern with a ratio of the south mirror hole reduce the acceptable angle of the gap, mask the side of the pattern, increase the incident particles intercepted by the pattern side and the surrounding, and deposit on the bottom of the pattern. Fewer particles. Various processes have been used to move the propagated particles straight and vertically toward the substrate surface. One of the studies includes the use of a physical collimator plate between the target and the substrate so that the incident angle is normally distributed, and the directionality of the incident particles is improved by intercepting low-angle particles with the collimator, only Particles that pass vertically or near a vertical substrate are passed through the collimator. Another study, called long-range sputtering, increases the distance between the target and the substrate, so that only particles that are perpendicular to the substrate or close to a perpendicular angle strike the substrate through the length of the cabin, and the collimator provides particulate pollution The source is because the intercepted particles are deposited on the collimator, accumulate there, and finally peel off. Both the collimation deposition and the long-range process achieve directionality by eliminating the material moving to the substrate at a low angle. The percentage of sputtered material incident on the substrate is greatly reduced, so the deposition rate is substantially reduced, and the frequency of maintenance is also increased, reducing the availability of the target material, and -6- This paper uses the Chinese National Standard (CNS) Α4 Specifications (210x297 meals) (Please read the precautions on the back before filling out this page},-= s Consumer Cooperation Cooperation, Central Standards Bureau, Ministry of Economic Affairs, Du Duan 4606u2 87 丨 〇924〇 Long Patent Application Manuscript Specification Correction Page (December 88) A7 ---------- -R7 _ V. Description of the invention (4) \ 7 ~ ^ W ^ ~-ΐΛ.ν is added to reduce the flux. Another is new The method of thinking about direct gargle material is ionization Shot method, commonly known as ionized rational vapor deposition or IPVD. Use IPVD Temple coating materials using magnetrons; base shot or other conventional base shot or evaporation techniques from the target 'X shot. In the sputtering coating method The 'sputtering particles' are self-emissive PVD at a wide emission angle. The intention is to improve the μ direction by ionizing the particles, which can be electrostatically or electrically manipulated to a direction perpendicular to the substrate. & In IP VD, an extra plasma is generated in the gas in the space between the target and the substrate. The sputtered particles pass through to reach the substrate. In the previous technology, various methods were used. Methods to generate the additional electrical components in the space, such as valley coupling with RF in the remaining room located downstream of the main pole, or by using the% Resonance Accelerator Resonance (ECR) or other microwave plasma generation technology A plasma is formed away from the side space, and then flows into the space. The particles passing through the space impact the electrons or metastable neutrons of the ionized processing gas ^ The impact causes the electrons to escape from the original particles of the sputtered particles, and The particles are given a positive charge. The ions are electrically accelerated toward the substrate by, for example, applying a negative bias voltage to the substrate. Printed by the Consumers' Cooperative of the Central Samples Bureau of the Ministry of Economic Affairs (please read the precautions on the back before filling out this page) The IPVD method shows several shortcomings and problems that prevent its use in the actual manufacturing environment. These methods, for example, have low overall efficiency. In particular, the deposition rate of the method is generally low. In addition, the film contamination of this prior art method is high. Especially, the In the prior art IPVD method, when the sputtering power of the target is increased, it will damage the filling of the high mirror ratio pattern. This damage limits the extinction of the aluminum alloy to the use of the 12-inch magnetron target. Less than 3 仟 Watt paper size 帽 74 specifications ⑺D χ 297 4 6 0 6 0 A7 ________B7 V. Description of the invention (5) For 3 仟 W DC power, and this type of rake pole / magnetron is generally used The tube combinations can reach 12 to j 0 仟 W. This low sputtering capability results in a low deposition rate, resulting in low throughput and throughput, and increased pollution, such as 10 to 40 minutes of money per wafer, and a typical wafer time of about 45 seconds to 1 minute ^ In addition It has been found that ¥ is not due to operating the device in the sputtering chamber at a relatively high pressure such as 20 to 40 millitorr, otherwise the degree of ionization of the sputtered material is low. When using argon treatment gas, the pressure is higher than-generally lower than 5 mTorr or within a range of low mTorr, the desired sputtering pressure. Higher pressures tend to lower the quality of deposited film I and increase film fouling. In addition, a higher operating pressure reduction requires a larger flat field uniformity in the design of the 眞 it cabin, which further reduces the ionization efficiency. Other problems generated by the IPVD method of the prior art include plasma sputtering RF electrodes or components unnecessarily, peeling of sputtered material accumulated due to undesired deposition from the RF component, and RF components being deposited on the component by plasma. Material, and other interactions between the plasma and the material and the electrode or element used to couple the RF energy into the hair to ionize the radioactive material. Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economics For this reason, IPVD devices and methods have the need to overcome the shortcomings and problems of previous techniques. In particular, there is a need for an expensive and effective IP VD device with acceptable high overall efficiency, special deposition rate, high ionization efficiency of sputtering material, and low pollution of deposited film. In particular, there is a need for a device for manufacturing a thin film of high uniformity and southern quality, and a device capable of providing industrialized production capacity for the method.
本發明之主要目的係提供一種方法及裝置,其係於VLSI 本紙張从適準(cns ) ΑϋΤ7^·297公釐 460602 A7 B7 -濟部中夹操準局員工消費合作社印製 五、發明説明(6 及ULSI半導體晶圓中之 窄问釦孔比孔及溝槽底部及某 -程度之側面上沉積薄膜。本發明另—個主要目的係提供 一種用以進㈣子化物理性蒸汽沉積之方法及裝置,並丑 有高整體效率,尤里异认访+话Λ, ' ‘」 、疋於该塗覆材料之高離子化效率下, 於大幅壓力範圍内產生高沪精余 . ϋ躓迷率。本發明另一個目的係 提供一種有效之IPVD方法;5磬笄 ,丄 去及装置,以保持低沉積膜污染 本發明另-個目的係提供—種具有低維修需求之 方法及硬體。 本發明之-特定目的係提供―種IpvD裝置及方法,其 可使該純上之賤射能保持至少適當之程度,而於不需使 該餘保持相當高政射壓力下,於_材料内提供高R]^量 賴合效率。本發明另,的係提供一種方法及裝置:其 中該膽中之電襞與用以將帛RF &量輕纟於該電毁内以使 所濺射(材料離子化之電極或元件之間的負面相互作用保 持極低’尤其是該電極之濺射、被濺射之材料的剥離、或 可能之短路。 根據本發明之原理,提供一種IPVD裝置及方法,其中 於緊鄭該靶極處形成主要電漿,以自該靶極濺射材料,'同 時RF元件將能量耦合於該PVD處理艙中,以於該艙介於 主要電紫與基板間之體積内產生二次電装。該二次電衆係 用以増補一般侷限於該濺射靶極鄰近之主要電漿。該二次 €展通¥充滿遠餘,但主要係佔據介於該把極與該基板間 之空間的至少一部分,以使自靶極移出而處於飛行中之粒 子向著基板電加速,而使該濺射材料於離子協助下沉積於 -9- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X 297公釐) I - !| - I i\1y^r f (請先閲讀背面之注意事項再填寫本頁) T ,-° —1 46(36 02 A7 B7 五、發明説明(7 ) 該基板上= 該離子㈣射材料以藉著施加於基板上之負偏昼以 飛向基板爲佳,其可控制使移動離子具有最佳 f 害晶圓表面。或者或此外:該艙周園環繞有永久礤體:: 磁體,於介於該基板與該乾極間之艘内產生轴向磁場-,二 助琢離子化賤射粒子侷限於與般轴平行而與基板表 之路徑。 且 RG離子化能量耗合元件可^ RF t #,以感應性元件 爲佳,諸如例如一至多條其繞該艙之螺管。如下文所詳述 ,該RF元件或可位於該艙内,以與該艙處理氣體隔離爲佳 ,或位於餘外。 經濟部中央標準局員工消費合作社印繁 較佳裝置亦具有保護結構,包括非導電性及非磁性介電 材料,其保護或隔離該RF元件,使之與艙中之電漿之間不 致產生負面之相互作用,諸如與該主要電漿間之相互作用 ,及與由該RF元件所產生之二次電漿間之相互作用。該保 護結構係使碰撞於彼者之濺射材料(若有)黏著於該結構上 ’不致自該結構剝離而成爲污染來源爲佳。該保護結構之 零件之結構以防止其中或沉積於彼上方之濺射材料層中產 生满流並防止該RF元件之靜電屏蔽爲佳。 於本發明限度内可使用各種RF元件結構及保護結構a例 如,於一具體實例中,RF螺管環繞該艙位於該保護結構後 方之處’其於該處理空間周園形成該艙眞空氣密内牆之— 邵分,該RF螺管覆有外層導電性罩套。或該嫘管係位於該 靶極逢緣外側及下游之處理艙的眞空中,該保護結構防止 -10 本紙張尺度適用中國國家標準(CNS ) AA規格(2丨0X297公釐) 經濟部中央標準局員工消費合作社印製 460602 A7 B7五、發明説明(8 ) 該RF螺管與該電漿相互作用。於另一個具體實例中,提供 一種RF螺管,其覆有保護性絕緣材料或覆有完全覆該螺管 導體之實心絕緣體或覆有具有窄至足以防止該導體附近形 成電漿之狹缝的開缝或區段絕緣體。該RF螺管及保護結構 以圓“型且環繞該處理空間爲佳。 較佳裝置另外包括用以屏蔽該保護結構之屏蔽陣列,使 得保護結構之功能本致因爲上層沉積濺射材料而受到影響 。可採用各種保護結構及屏蔽陣列之具體實例,如以下實 施例所描述。 第一個具體實例 於第一個具體實例中,該RF元件包括自用作保護結構之 大略圓柱型石英小窗後方環繞該艙之螺管。該大略圓柱型 石英小窗可形成該艙之眞空氣密性内牆之一部分,或其可 爲圍繞位於該艙内部之螺管的絕緣體之形式,或爲某些使 該螺管導體與該處理氣體隔離之其他形式。 提供一種實質圓柱型之屏蔽,其環繞該艙與該小窗緊鄰 處,而該窗分隔該螺管與PVD處理艙。該屏蔽之狹缝以處 於與該艙軸平行之方向爲佳。’’緊鄰"意指與小窗之距離短 至足以防止該屏蔽與該小窗之間形成電漿。該狹縫型屏蔽 依循分隔該螺管與該眞空艙及處理氣體之介電小窗之形狀 。該屏蔽防止塗覆材料沉積於該小窗上。當該材料係爲導 電性時,該螺管可短路以防止RF能量傳送至該艙内。該屏 蔽之狹缝以防止該屏蔽本身提供環繞該艙而可能感應周圍 電流之周圍通道爲佳,該電流會消耗來自RF螺管之能量, -11 - (請先閱讀背面之注意事項再填寫本頁) 本紙張尺度逋用中國國家標準(CNS ) A4規格U10X297公釐) 經濟部中央標準局〖只工消費合作社印裝 460602 A7 _________B7 五、發明説明(9 ) 而降低能量糕合於該補充電漿内之效率。該屏蔽可進一步 於軸向延伸至該RF螺管兩端之短轴電場,而使該能量感應 糕合於該電漿中之效率最佳化,並降低該耦合能量之感應 Μ合分量。此外’該屏蔽保持與該小窗緊鄰,以防止該屏 I ' 蔽後方產生電漿’而於該濺射粒子所橫越之空間内更有效 率地產生電漿。該屏蔽與該小窗之間隔不大於該處理氣體 之原子平均自由路程或爲該電漿於該空間内之最小擴散長 度。 琢屏蔽中之狹縫寬至足以於其中形成電漿,以藉著使材 料自該來源經過該狹縫而沉積於該小窗上之任何塗覆材料 再次濺射,而連續移除電漿。 該屏蔽相對於該螺管保護覆層之位置及結構可於該艙空 間内高效率地產生電漿,避免因於該屏蔽與該螺管之間2 成電漿而損失。結果,提供濺射材料之高離子化效率。 此具體實例防止於該艙之無效區域諸如介於該^蔽結構 與該螺管絕緣體或小窗之間之區域產生心 二〜„ ‘ 土弘戒,而避免離子 化效率之損失。 第二個具體f例 於此具體實例中,單獨或結合使用介電小窗或區段絕緣 ,以同時保護RF元件與該電漿及該濺射材料隔離。該屏= 陣列以多個屏蔽區段之形式爲佳’可施加偏壓以控制其= 電漿所致之濺射。該屏蔽陣列具有多個間^ 隊 以主少部分 阻斷該厚蔽區段,防止感應過流消耗能吾π此4, 月匕1而蚪扠能昝梦 該電漿之耦合此外,該個別屏蔽區段以電隔離? &二 12- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事項再填寫本頁) 丁 Jsa 4 4606 02 A7 B7 五、發明説明(10 ) 其可個別施加㈣而使基板上之塗層肖句性及撞向基板之 離子化材料的方向性最佳化。異蔽區段間之間隙有利於該 電漿自孩屏蔽後方擴增至該處理空間内。 第三個具體會钿 .此具體實例中’帛管環繞該艙位於保護結構後方之處。 万、及配置下,忒螺管經保護而不與在該艙内所形成之電漿 接觸&咸艙内提供屏蔽區段陣列,亦環繞介於該靶極與 基板間之空間,以施加偏壓以控制來自電聚之㈣爲佳。 該屏蔽陣列具有多個間隙,卩至少部分使該屏蔽區段絕緣 ,邵分防止感應渦流消耗能量及對抗能量與該電漿之耦合 a構成孩屏蔽區段並定向,且界定該間隙,使該屏蔽區段 遮蔽該保護結構以與靶極隔離,使能量之耦合受螺管及該 二次電漿之形成及位置之影響達到最小。 4異蔽陣列相對於遠保護結構定位,使其不致累積塗屬 ,而於其中支撑渦流或產生該RF螺管之靜電屏蔽。自該保 ?隻結構之任何結構不會看見任何靶極分爲佳,若該保護結 構之任何部分可見到靶極而累積導電性濺射材料之塗層, 則塗覆區域之形狀不支撑渦流或造成明顯之螺管屏蔽。 經濟部中央標準局員工消費合作社印製 於該第三個具體實例之説明實例中,該保護結構包括介 電小窗。該屏蔽陣列係由角狀區段形成,整體阻斷所有介 於該乾極與該小窗之間之通道。該區段亦成—角度,而可 自該螺管看見介於該主要電漿與該基板間之許多空間體積 。如此一來,該小窗可隔絕來自靶極之跨射沉積’而提供 最有效之能量耦合’以形成用以使該濺射材料離子化之二 -13- - i ο—, (請先閏讀背面之注意事項再填寫本頁〕 表紙張尺度適用中國國家標準(CNS ) A4規格(210X297公变) 經濟部中央標準局員工消費合作社印製 460602 A7 ________B7 五、發明説明(11 ) ^人電浆。该属蔽區段以與該小窗間隔爲佳,相鄭區段間具 有使螺管之某些部分可見到該艙用以形成二次電漿之體積 ’故可於緊鄰該小窗處形成電漿,並延伸至將濺射材料離 子化之體積内》 根據此第三個具體實例之—説明例,該屏蔽陣列係由多 個位於該窗内侧而傾斜角度通常與自乾極至小窗之路徑垂 直之轴向間隔截頭圓錐區段。該屏蔽區段可相對於艙軸傾 斜於相同角度’或該區段傾斜於不同角度,例如與該靶極 相距較遠之區段與該軸所成之角度較小。該區段以不遮蔽 該乾極上每一點之相鄰區段爲佳,但最小重疊易減少散射 之政射粒子撞擊該窗。該屏蔽區段之周圍以分段之間隙進 一步分段爲佳,以阻斷電位感應之電流路徑。 根據此第三個具體實例之另一個説明例,該屏蔽陣列係 由多個環繞該窗之餘内侧周園之平面或稍有曲度的軸向延 伸矩型葉片所形成。此等區段與該窗相間隔,各自靶極總 面積與該艙之半徑傾斜於可整體遮蔽該窗之角度,或至少 該窗實質位於螺管範圍内之部分,但使該艙欲形成二次電 褒之體積内可見到部分螺管。如此一來,可於緊鄰該窗處 形成二次電漿,並輕易延伸於濺射粒子欲通過之體積内。 此具體實例之屛蔽區段以於相同角度下與該艙半徑傾斜爲 佳。雖然最小重疊可進一步減少該窗之塗層,但以該區段 自靶極之每一點皆不遮蔽相鄰區段爲佳。該屏蔽區段以周 園彼此相間隔,而與該靶極及該基板之間距等於至少眞空 艙中氣體分子之平均自由路徑爲佳。 -14 - 本纸乐尺度適用中國國家標準(CNS ) A4规格(210X 297公釐) (請先閲讀背面之注意事項再填寫本頁) 訂 460602 A7 B7 五、發明説明(12 ) {請先閱讀背面之注意事賓再填寫本頁) 當二發明料_塗覆线時,可保持高藏射能力,而 保持高沉積速率及高濺射材料離子化速率。可於不產生太 ^問題下達到該等結果,諸如RF螺f短路或增加污染而破 壞沉積膜。結果,使人㈣射材料高度定向於與基板表面 垂直之方向,可藉濺射有效地充填高鏡孔比圖型。消除了 先前技藝降低濺射能力之需求,因爲防止了致密電漿短路 或對產生使濺射材料離子化之電漿之RF電漿耦合元件之 負面影響。防止由RF元件自身所產生之電漿使該元件短路 。濺射氣體壓力可保持低値或正常濺射程度,而防止因散 射而喪失方向性3避免因111:耦合元件之濺射所致之負面影 響。此等優點可於相當於未提供本發明所提供之高品質高 鏡孔比圖型塗層之習用濺射方法的處理時間内達成。 經濟部中央標準局員工消费合作社印製 除改善PVD方法-尤其是用以將塗層沉積於高鏡孔比圖 型之·攻射塗覆方法外,本發明亦於採用蒸發來源或其他蒸 發材料來源而實質上藉物理性技術沉積之PVD方法中提 供優點。藉由或包括材料之化學沉積之反應性方法及物理 性方法亦可於本發明中得到改善。本發明特別可用於沉積 金屬膜,亦於其他材料尤其是氧化物及氮化物之沉積中提 供優勢。 由以下本發明較佳具體實例之詳述可更輕易明瞭本發明 之此等及其他目的及優點。 阐·圖簡述: 圖1係爲本發明具體實例之IPVD濺射裝置正視圖。 -15- 本紙張尺度適用中国國家椟準(CNS )人4^格(2i0x297公釐) A7 五,發明説明(13 放大正視圆。 圆2係為國1之裝置之屏蔽的透視圖。 圆3係為本發明具體實例之IPVD濺射裝置之圖示。 圆4A-4D係為說明圖3之裝置之取代性螺管結構之圖。 囫5係為與圖3所示相反地具有二次電漿rf耦合元件之 取代性結構及保護性結構之IP VD濺射裝置圖示。 圖6係為與圖3及5所示相反地具有二次電漿RF耦合元 件之另一個取代性結構及保護性結構之丨PVD濺射裝置圖 示。 圖7A-7D係為說明取代圖6之具體實例所示之螺管絕緣 保護性結構之形式之圖示。 圖8係為本發明之—具體實例之IPvd濺射裝置之圖示。 圖9係為圖8說明屏蔽陣列之取代性結構之部分的圖。 圖1 0係為圖9屏蔽陣列具體實例沿圖9之3_3線所得之 剖面圖。 左件符號說明_ : ί --- I I I I ^^^1 ^ J J (请先閱讀背面之注意事項再填寫本頁)The main purpose of the present invention is to provide a method and device, which are printed on a VLSI paper from cns ΑϋΤ7 ^ · 297 mm 460602 A7 B7-printed by the Ministry of Economic Affairs of the People's Republic of China. (6 and USI semiconductor wafers are deposited on the narrow pinhole ratio hole and the bottom of the trench and a certain degree of side. Another main purpose of the present invention is to provide a method for the rational vapor deposition of ions. The method and device have high overall efficiency. Yuliyi's interview + words Λ, '' ”, and the high ionization efficiency of the coating material, produces high Shanghai fine surplus in a large pressure range. Ϋ 踬Mistake rate. Another object of the present invention is to provide an effective IPVD method; 5 磬 笄, removing and device to keep the deposition film pollution low. Another object of the present invention is to provide a method and hardware with low maintenance requirements. The specific purpose of the present invention is to provide an IPVD device and method that can maintain the purely low-level radio energy at least to a suitable degree without the need to maintain the remaining high level of political pressure under the _ materials Provide high R] Another aspect of the present invention is to provide a method and device: wherein the galvanic ion in the gallbladder and the electrode used to reduce the RF & amount in the galvanic destruction to make the sputtered (ionized material or electrode) The negative interaction between them is kept extremely low, especially the sputtering of the electrode, the stripping of the sputtered material, or a possible short circuit. According to the principles of the present invention, an IPVD device and method are provided, in which the target is tightly corrected A main plasma is formed at the pole to sputter the material from the target, and at the same time, the RF element couples energy to the PVD processing chamber to generate a secondary electrical assembly in the volume between the main electrode and the substrate. The secondary electrode is used to supplement the main plasma which is generally limited to the sputtering target. The secondary electrode is full of space, but it mainly occupies the space between the electrode and the substrate. At least partly, the particles in flight that are removed from the target are electrically accelerated toward the substrate, and the sputtering material is deposited with the assistance of ions at -9- This paper size applies the Chinese National Standard (CNS) A4 specification (210X 297 Mm) I-! |-I i \ 1y ^ rf (Please read the precautions on the back before filling in this page) T,-° -1 46 (36 02 A7 B7 V. Description of the invention (7) The substrate = the ion emitting material to be applied to the substrate by Negative daylight is better to fly to the substrate, which can control the mobile ions to have the best f harm to the wafer surface. Or or in addition: the perimeter garden is surrounded by a permanent carcass: a magnet between the substrate and the stem An axial magnetic field is generated in the ship between the poles, and the secondary ionizing ionized base radiation particles are limited to the path parallel to the general axis and on the substrate surface. And the RG ionization energy consumption element can be RF t # to an inductive element Preferably, such as, for example, one or more solenoids around the capsule. As detailed below, the RF element may be located in the cabin, preferably isolated from the process gas of the cabin, or located outside. The Better Consumer Printing Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs also has a protective structure, including non-conductive and non-magnetic dielectric materials, which protects or isolates the RF component so that it does not create a negative relationship with the plasma in the cabin. Interactions, such as interactions with the primary plasma, and interactions with secondary plasmas generated by the RF element. The protective structure allows the sputtered material (if any) colliding with the other to adhere to the structure, so as not to be separated from the structure and become a source of pollution. The components of the protective structure are preferably structured to prevent full current in or in the sputtered material layer deposited thereon and to prevent electrostatic shielding of the RF element. Various RF element structures and protective structures can be used within the limits of the present inventiona. For example, in a specific example, an RF solenoid surrounds the cabin at the rear of the protective structure ', which forms the cabin airtightness around the processing space. The inner wall—Shao Fen, the RF solenoid is covered with an outer conductive cover. Or the stern tube is located in the stern of the processing chamber outside and downstream of the target pole, and the protective structure prevents -10. This paper size applies the Chinese National Standard (CNS) AA specification (2 丨 0X297 mm) Central Standard of the Ministry of Economy Printed by the Bureau's Consumer Cooperatives 460602 A7 B7 V. Invention Description (8) The RF solenoid interacts with the plasma. In another specific example, an RF solenoid is provided, which is covered with a protective insulating material or with a solid insulator that completely covers the solenoid conductor or with a slit having a narrow enough to prevent the formation of a plasma near the conductor. Slit or sector insulator. The RF solenoid and the protection structure are preferably round and surround the processing space. The preferred device further includes a shielding array to shield the protection structure, so that the function of the protection structure is affected by the deposition of the sputtering material on the upper layer. Specific examples of various protective structures and shielding arrays can be used, as described in the following examples. The first specific example is in the first specific example, the RF element includes a large cylindrical quartz window that is used as a protective structure to surround the rear The solenoid of the cabin. The roughly cylindrical quartz window may form part of the airtight interior wall of the cabin, or it may be in the form of an insulator surrounding a solenoid located inside the cabin, or some Other forms of solenoid conductor isolation from the process gas. A substantially cylindrical shield is provided that surrounds the cabin and the small window, which separates the solenoid from the PVD processing chamber. The shield's slits are located at The direction parallel to the axis of the cabin is better. "Near by" means that the distance from the small window is short enough to prevent the plasma from forming between the shield and the small window. The slit screen The shield follows the shape of a small dielectric window that separates the solenoid from the plutonium and the processing gas. The shield prevents coating material from depositing on the small window. When the material is conductive, the solenoid can be short-circuited to prevent RF energy is transmitted to the cabin. The shield slit is better to prevent the shield itself from providing a surrounding channel that may surround the cabin and may induce surrounding current, which will consume energy from the RF solenoid, -11-(please first Read the notes on the reverse side and fill in this page) This paper size uses the Chinese National Standard (CNS) A4 specification U10X297 mm) Central Bureau of Standards of the Ministry of Economics 〖Only for consumer cooperatives 460602 A7 _________B7 V. Description of the invention (9) Reducing the efficiency of the energy cake in the supplementary plasma. The shield can further extend in the axial direction to the short-axis electric field at both ends of the RF solenoid, so as to optimize the efficiency of the energy induction cake in the plasma And reduce the induced M component of the coupling energy. In addition, 'the shield is kept close to the small window to prevent the screen from generating plasma' behind the shield and to be more efficient in the space traversed by the sputtering particles A plasma is generated. The distance between the shield and the small window is not greater than the average free path of the atom of the processing gas or the minimum diffusion length of the plasma in the space. The slit in the shield is wide enough to form a plasma in it. In order to continuously remove the plasma by re-sputtering any coating material deposited on the small window from the source through the slit, the position and structure of the shield relative to the solenoid protective coating Plasma can be efficiently generated in the cabin space, avoiding losses due to the formation of plasma between the shield and the solenoid. As a result, high ionization efficiency of the sputtering material is provided. This specific example is prevented in the cabin Ineffective areas, such as the area between the shield structure and the solenoid insulator or small window, create a heart ring to prevent the loss of ionization efficiency. Second Specific Example f In this specific example, a dielectric window or section insulation is used alone or in combination to protect the RF element from the plasma and the sputtering material at the same time. The screen = the array is preferably in the form of multiple shielded sections' which can be biased to control its plasma-induced sputtering. The shielded array has a plurality of blocks to block the thick shielded section with a small number of mains to prevent the induced over-current consumption energy, which can be 4 months, and the fork can dream about the coupling of the plasma. In addition, the individual Shielded sections are electrically isolated? & II 12- This paper size applies Chinese National Standard (CNS) A4 specification (210X297 mm) (Please read the precautions on the back before filling this page) Dsa 4 4606 02 A7 B7 V. Description of the invention (10) The chirp can be applied individually to optimize the syntactic nature of the coating on the substrate and the directionality of the ionized material that hits the substrate. The gap between the shielded sections is conducive to the expansion of the plasma into the processing space from behind the shield. The third specific event is that in this specific example, the 'tube' surrounds the cabin behind the protective structure. In the configuration, the 忒 solenoid is protected from contact with the plasma formed in the cabin & a shielded array of arrays is provided in the cabin, and it also surrounds the space between the target and the substrate to apply It is better to control the bias voltage from the electricity. The shielding array has a plurality of gaps, which at least partially insulates the shielding section, and prevents the induction eddy current from consuming energy and counteracts the coupling of the energy and the plasma. The shielding section is formed and oriented, and the gap is defined so that the The shielding section shields the protection structure from the target, so that the coupling of energy is minimized by the formation and position of the solenoid and the secondary plasma. 4 The alien shielding array is positioned relative to the remote protection structure, so that it does not accumulate coatings, and supports eddy currents or static shielding of the RF solenoid in it. Since any structure of the protection structure does not see any target, it is good. If the target is visible in any part of the protective structure and the coating of conductive sputtering material is accumulated, the shape of the coating area does not support eddy currents. Or cause obvious solenoid shielding. Printed by the Employees' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs In the third specific example, the protective structure includes a small dielectric window. The shielding array is formed by angular sections, which block all the channels between the stem electrode and the small window as a whole. The section is also at an angle, and the volume of space between the main plasma and the substrate can be seen from the solenoid. In this way, the small window can isolate the trans-emission deposition from the target and provide the most effective energy coupling to form the second ionizing material used to ionize the sputtering material. 13--i ο—, (please first Read the notes on the back and fill in this page again.] The paper size of the table is applicable to the Chinese National Standard (CNS) A4 specification (210X297 public change). Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs. 460602 A7 ________B7 V. Description of the invention (11) The shielding section is preferably spaced from the small window. Between the Zhengzheng section and the section, there is a volume that allows some parts of the solenoid to see the compartment to form a secondary plasma. Therefore, it can be next to the small window. Plasma is formed everywhere and extends into the volume where the sputtered material is ionized. According to this third specific example—the illustrative example, the shielding array is composed of multiple located on the inside of the window. The path of the small window is perpendicular to the axially spaced frustoconical section. The shield section can be inclined at the same angle relative to the cabin axis' or the section is inclined at different angles, such as the section farther away from the target and The angle made by this axis is small. It is better to not block adjacent sections at each point on the pole, but the smallest overlap is easy to reduce the impact of the blasting particles. The surrounding area of the shielded section is preferably further divided into sections, so as to Blocks the potential-induced current path. According to another illustrative example of this third specific example, the shielding array is composed of a plurality of flat or slightly curved axially extending rectangular blades surrounding the inner periphery of the window These sections are spaced from the window, the total target area of each target and the radius of the cabin are inclined at an angle that can obscure the window as a whole, or at least the window is substantially within the area of the solenoid, but makes the cabin Part of the solenoid can be seen in the volume to form a secondary electrocathode. In this way, a secondary plasma can be formed immediately adjacent to the window, and it can easily extend into the volume through which the sputtered particles pass. The concealment of this specific example It is better that the sections are inclined at the same angle with the radius of the cabin. Although the minimum overlap can further reduce the coating of the window, it is better that each point of the section from the target does not cover the adjacent section. The shielding Sections with each other in Zhou Yuan It is better that the distance from the target and the substrate is equal to at least the average free path of the gas molecules in the empty capsule. -14-The paper scale is applicable to the Chinese National Standard (CNS) A4 specification (210X 297 mm) ( Please read the notes on the back before filling this page) Order 460602 A7 B7 V. Description of the invention (12) {Please read the notes on the back before filling this page) When the second invention material _ coating line, you can keep high The ability to hide, while maintaining a high deposition rate and high ionization rate of the sputtering material. These results can be achieved without causing too much problems, such as shorting the RF screw f or increasing the pollution and damaging the deposited film. As a result, the human projection material is highly oriented in a direction perpendicular to the surface of the substrate, and a high mirror hole ratio pattern can be efficiently filled by sputtering. Eliminates the need for prior art techniques to reduce sputtering capabilities, as short circuiting of dense plasmas or negative effects on RF plasma coupling elements that generate plasmas that ionize sputtering materials are prevented. Prevent short circuit caused by the plasma generated by the RF component itself. The pressure of the sputtering gas can be kept low, or the normal sputtering degree can be prevented, and the directivity due to scattering can be prevented. 3 Avoid the negative influence caused by the sputtering of 111: coupling element. These advantages can be achieved in a processing time equivalent to the conventional sputtering method which does not provide the high-quality, high-hole-ratio pattern coating provided by the present invention. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs. In addition to improving PVD methods, especially the off-coated coating method used to deposit coatings on high-mirror-hole-ratio patterns, the present invention also uses evaporation sources or other evaporation materials. Sources provide advantages in PVD methods that are essentially deposited by physical techniques. Reactive methods and physical methods by or including chemical deposition of materials can also be improved in the present invention. The invention is particularly useful for depositing metal films and also provides advantages in the deposition of other materials, especially oxides and nitrides. These and other objects and advantages of the present invention will be more easily understood from the following detailed description of the preferred embodiments of the present invention. Explanation · Brief description: Figure 1 is a front view of an IPVD sputtering device according to a specific example of the present invention. -15- This paper size applies to the Chinese National Standards (CNS) person 4 ^ grid (2i0x297 mm) A7 V. Description of the invention (13 Magnification of the circle. Circle 2 is a perspective view of the shield of the country 1. Circle 3 It is a diagram of an IPVD sputtering device according to a specific example of the present invention. The circle 4A-4D is a diagram illustrating the alternative solenoid structure of the device of FIG. 3. Schematic diagram of the IP VD sputtering device with the alternative and protective structure of the plasma rf coupling element. Figure 6 is another alternative structure and protection with a secondary plasma RF coupling element as shown in Figs. 3 and 5. Schematic diagram of the PVD sputtering device. Figures 7A-7D are diagrams illustrating the form of the solenoid insulation protective structure shown in the specific example instead of Figure 6. Figure 8 is the present invention-a specific example Diagram of an IPvd sputtering device. Fig. 9 is a diagram illustrating a part of the alternative structure of the shielding array of Fig. 8. Fig. 10 is a sectional view of the specific example of the shielding array of Fig. 9 taken along line 3-3 of Fig. 9. Left part Explanation of symbols _: ί --- IIII ^^^ 1 ^ JJ (Please read the precautions on the back before filling in this )
-_部中央嗉迭局員工消費合作,ϊιί印I 10 :濺射塗覆裝置 21 表面 10a :濺射塗覆裝置 22 RF濾器 10b :濺射塗覆裝置 23 電漿 11 真空氣密性處理空間 24 RF產生器 12 艙房 25 匹配網 14 基板支架 26 空間 15 晶圓 27 偏壓電路 16 乾極 28 匹配網 17 陰極組件 29 二次電漿 18 乾極支架 -30 螺管組件 19 磁體結構 32 RF產生器 20 動力供應 33 匹S己網 -16 衣紙乐尺度適用中國國家標準 (0^)六4規格(2!〇\ 297公釐) Α7 1.Β7 4赢βι岛申請案 中請皁利範圍修正本(88年3月) 五、發明説明(伽)年s ϋ七:-_Ministry Central Economic and Trade Bureau staff consumer cooperation, I 10: Sputter coating device 21 Surface 10a: Sputter coating device 22 RF filter 10b: Sputter coating device 23 Plasma 11 Vacuum airtight processing space 24 RF generator 12 Cabin 25 Matching grid 14 Substrate bracket 26 Space 15 Wafer 27 Bias circuit 16 Dry pole 28 Matching grid 17 Cathode assembly 29 Secondary plasma 18 Dry pole bracket-30 Solenoid assembly 19 Magnet structure 32 RF generator 20 Power supply 33 horsepower S16. 16 Paper and paper scales Applicable to Chinese national standard (0 ^) Six 4 specifications (2! 〇 \ 297 mm) Α7 1.Β7 4 win βι island application, please soap Revised Margins (March 88) V. Description of Invention (Gamma) Year s
Li_____一一〆 — 39 真空泵 200 屏 蔽陣 列 40 處理氣體 202 屏 蔽區 段 41 流動控制裝置 204 間 隙 50 控制器 206 產 生器 60 窗 207 遽 器匹 配網 61 金屬套罩 208 電 阻器 60a :窗 300 屏 蔽陣 列 6 1 a :金屬套罩 300a :屏蔽陣列 62 模孔 302 屏 蔽區 段 66 絕緣區段 302a :屏蔽區段 80 磁體 303 頂 面 86 遮蔽絕緣層 304 間 隙 86a :實心絕緣體 305 間 隙 86b :分段絕緣體 306 產 生器 86c :絕緣體 307 ί慮 器匹 配網 86d :絕緣體 308 電 阻器 87 間隙 311 轴 向平 面 100 :屏蔽 3 12 軸 103 :狹縫 —^n —^^1 I -·τ - - ^^^1 ^^^1 n^— 1^11 l^i I*. - . I V3r 、-* (請先閱讀背面之注意事項再填踔本頁) 經濟部中央蟑準局員工消費合作杜印製 發明詳述· 圖1係圖示依循本發明原理之濺射塗覆裝置1 〇。裝置i 〇 包括封包於艙房1 2中之真空氣密性處理空間。艙房1 1之— 端裝置有基板支架或托架14,以支撐放置於彼上方之半導 體晶圓1 5。該晶圓1 5裝置於基板支架14上時,與靶極16 平行而面向靶極。該靶極丨6係电欲於晶圓1 5上沉積成薄膜 之藏射塗覆材料所形成。該處理空間11通常係為圓柱型空 間’於處理期間保持超高真空壓力,而充填處理氣體 -16a- 本紐尺度適用中家標準{ CNS—)_ A4規格(210 X 297公爱) ~ — ' A7 B7 經濟部中央標牟局員工消費合作社印製 五、發明説明(14 ) 諸如氮。遠空間1 1係位於驗房12 Φ入 滟居12中介於基板支架14與靶 極1 6之間。 靶極16係爲陰極組件17裝置於艙房丨2中之部分,其— 端與基板支架14相對。該陰極组件丨7包括固定靶極“之 靶極支架18。磁體結構19 一般係位於靶極支架18後方與 基板支架14相反側面。亦於乾極16邊緣環繞黑暗之空間 屏蔽13。該磁體結構19以包括於靶極16表面以上產生密 閉之磁隧道之磁體,如熟習此技藝者所熟知,其於通電至 負電位時,藉陰極组件17捕集射入艙房丨2中之電子。該 磁體結構19可包括熟習此技藝者已知之數種磁控管濺射 组件中任一種之固定或旋轉或其他移動方式之磁體,可爲 永久性或電磁體。 動力供應或電能來源20通常係直流電電源,可連通以保 持固定或可爲脈衝式,係連接於陰極組件17與艙房12牆 之間’該牆通常接地而作爲系統陽極。該陰極组件丨7係與 餘房12之牆,離。動力供應2〇以經甴rf濾器22連接於 陰極組件1 7爲佳。輔助能源諸如RF產生器24亦可選擇性 地經由匹配網2 5連接於該陰極組件爲佳。亦提供偏壓電路 2 7 ’並連接於經由匹配網2 8連接於基板支架14。該偏壓 電路27在裝置於基板支架μ上之晶圓15上施加偏壓。此 時可使甩雙極直流電電源或RF電源》來自穩定或脈衝直流 電電源20及/或RF產生器24之能量於表面21上產生負電 位,使電子自靶極16之表面2 1上發射。所發射之電子由 磁體結構1 9所產生之磁場捕集於表面2 1上,直至其撞擊 -17 {請先閲讀背面之注意事項再填寫本頁) ο. *-口 本紙張尺度適用中國國家標準(CNS ) A4規格(21〇χ297公釐) 4 606 經濟部中央橾车局員工消費合作社印掣 A7 B7 五、發明説明(15) 並使乾極16表面21緊鄰處之處理氣體原子離子化,於該 靶極表面21鄱近形成主要電漿23。該主要電漿23變成氣 體正離子之來源,該離子加速衝向負電荷表面21,於此處 自乾極16射出塗覆材料粒子。 介於把極表面2 I與基板支架14間之空間可視爲兩部分 。—邱分主要係由電漿2 3所佔據,其形狀係於靶極16之 賤射表面2 1上產生所需之沖蝕圖型,而空間i i之第二個 邵分係爲介於電漿2 3與位於基板支架14上之基板15之間 二保留空間26。來自靶極1 6之濺射材料粒子通常係源自 電中性粒子’其僅能藉由衝量穿過空間1 1 ,其中某些_但 非全部-穿透電漿23及體積26而衝撞於基板15上。於習用 歲射裝置中,穿過電漿23之中性濺射粒子未大幅離子化, 因電漿23佔據接近靶極表面2 1之,j、部分體積,於所研究 操作壓力下,該中性濺射粒子與該電漿23粒子間極少發生 撞擊3是故,於習用濺射法中,該中性濺射粒子發射太多 爲中性之電漿23,而於沉積於基板15上成爲薄膜之前保 持中性。 就高鏡孔比孔及其他圖型之底部塗層接點而言,及就藉 著充填濺射之導電性材料以使該孔金屬化而言,於Vlsi 及ULSI半導體裝置製造中極度期望粒子於基板法線之狹 窄角度分佈下撞擊基板表面,使其直接朝著該圖型行進而 到達該圖型低部,而不撞擊或被該圖型側面遮蔽S裝置1 〇 藉著於濺射粒子通過體積26時使之離子化以使該粒子具 有電荷而有利於該粒子垂直撞擊於基板上。該粒子一旦充 -18- 本紙張尺度適用中國國家榡準(CNS ) A4規格(21〇x297公釐) (請先閔讀背面之注意事唷再填寫本頁) 〇 經濟部中央標準局員工消費合作衽印製 4 606 A7 -------- 五、發明説明(16 ) ^"" ~ -- 電,即可靜電性或電性或磁性加速取向於與該艙軸平行而 與該基板15表面垂直之路徑。該過程於技藝界中稱爲離子 化物理性沉積(IP VD)或離子協助性濺射塗覆。 根據本發明較佳具體實0,空間26中之濺射粒子的飛行 中離子化係藉著&供環繞體積2 6而不佔據空間1 I之rf元 件,以使RF能量反應性且較佳係感應性地耦合於體積% 内而進行。雖可使用螺旋以外之螺管結構,但R F元件以螺 官组件30形式爲佳^螺管組件之可能結構3〇a_3〇d之實例 係説明於圖4A-4D中=此外,可於異於前述方式之方式下 將RF能量餵入螺管中,例如,將中心RF塞添加於該螺管 中心,並將其他兩條導線接地或相反。該螺管组件3 〇將能 量感應轉合於體積26中之處理氣體内,以形成二次電設29 ,其通常充填該體積26並異於該主要電紫23。RF產生哭 32 ’於較佳但不限於〇. 1或〇_2仟赫茲至或8〇仟赫茲範 園内操作,經由匹配網3 3連接於螺管組件3〇,以於該螺 管組件3 0上提供能量,而於體積2 6中形成二次電漿2 9。 處理氣體40來源係經由流動控制裝置4 1連接於艙房j j 。就政射方法而言,該供料氣體40 —般係爲惰性氣體諸如 氬。就反應性方法而言,可經由輔助流動控制器導入其他 氣體諸如氮及氧。亦將南眞空系3 9連接於舱房i 2以將驗 房12泵抽至毫托耳或次毫托耳範圍内之眞空度。5至50 笔托耳範園内之壓力較佳。泵39使用5至300標準立方厘 米母秒(seem)範圍内之處理氣體流速保持超高眞空。裝置 亦包括主要控制器50 ’以微處理器爲主之可程式化控制 ___ - 19- 本紙張尺度適用中國國家榡準(CMS ) A4規格(2丨OX 297公釐) (請先閎讀背面之注意事項再填寫本頁} Ό 訂 Λ . 460602 A7 經濟部中央標準局—工消費合作社印製 五、發明説明(17 ) 器爲佳,,用以定序並控制前述組件之操作。該控制器5〇具 有用以k φ彳陰極能源2〇及24之之啓動、基板偏壓能源Μ / ,乂 〇動一'入电漿產生元件螺管组件之RF產生器3 2、 ^ d 4 1泵J 9及裝置.10之其他可控制組件的輸出。 爲】達到離子化濺射粒子之方向性,可使用經由匹配網 28 ^接於基板支架14之偏壓能源27,使該基板Η相對於 一人咕桌王負偏壓,而於基板支架·14前方之電漿鞘中保持 電位梯度,提供使該正離子化賤射粒子加速衝撞基板表面 而沉積於彼上層之力。此時可使用雙極直流電電源或rf 電源。 磁體80可另外或取代性地環繞該艙房12 ’以於艙房12 之軸向產生磁場。磁體80可爲電磁體或由一或多個永久磁 fe所形成。來自磁體80之電場使帶電粒子沿線渦狀旋轉, 而增加其於徑向之定向。存有軸向電場時,帶電粒子可釺 對於軸向而移向基板,使徑向損失減至最少。 於螺管組件30與空間11之間提供保護結構,防止電漿 23及29與該螺管組件接觸而電性相互作用。該結構係爲非 導電性材料,不妨礙環繞該螺管組件3〇之磁場到達體積二 内。其中一個保護結構之較佳形式係爲位於艙房12牆内之 小窗60,由眞空相容性介電材料諸如石英所製造,以該餘 牆裝置成眞空氣密性封條。該窗60可爲單一絕緣或磁性透 明材料,或可於其連接區段中形成,以形成大體上爲圓柱 型之保護結構。螺管组件30係説明於前述具體實例中,捲 繞於餘房1 2周圍,以位於小窗60外爲佳。覆於螺管組件 20- 本紙張尺ϋ用中i國家規格(2丨釐)'^ ------ —I. - I. = - I (I—- - -I - 1 - ·-- I 丁 【 1 ,-卩 (請先閲讀背面之注意事賓再填寫本頁) 460602 A7 、發明説明(18) 者係馬導电性金屬罩套61,其形成密 菘螺管组件3 〇隔魬 ' 、 ]杈孔62 ,與 ,19rih ^ ^離,亦防止電磁能自螺管組件30及自艙 居12内輕射至該艙房12外。模孔62可與餘房n自: 了與外界大氣連通或可充填大氣壓或較低 :啓動螺管组件3。時,模…之氣體不支SL: 維然小窗60本身並非導電性,但其易累積自乾極Μ藏 丁义導電性材料塗層。小窗6〇内或上之導電性支持於艙房 周圍感應電流,降低 '消除或破壞來自螺管组件3〇之能量 RF耦合於體積26中之二次電漿29之效率。小窗6〇上塗層 之導電性’尤其是方位角(周圍)方向,即延伸於艙房12周 圍又方向,產生感應耦合短路可消除所有或許多感應性耦 合於體積26内之能量。 名义防止導電性賤射材料累積於小窗60上,較佳裝置另外 包括屏蔽陣列、各種下文所述之具體實例。 I一個具體實例 經濟部中央標準局員工消費合作社印製 --------------^__rj 一 1-彡 (請先閱讀背面之注意事贫再填荈本頁) 圖1説明一個介於空間,1 1與小窗6 0之間之狹缝圓柱型 屏蔽1 00,緊鄰於小窗60之内表面。該屏蔽1 00遮蔽小窗 6 〇以防止被把極1 6歲射,以阻斷介於乾極16表面2 1任何 點與小窗6 0間之所有直接視線路徑爲佳。根據此具體實例 ’該屏蔽100中具有與艙12軸平行之縱向狹缝103。亦可 使用具有單一或多個用以阻礙周圍電流之狹缝。較佳具體 實例之狹縫1 03實質干擾該屏蔽1 00中環繞該艙1 2之周圍 路徑。防止該屏蔽1 0 0中感應周圍或方位角電流。 -21 - 本紙張尺度適用中國國家標準(CNS ) A4現格(210X297公釐 經濟部中央標準局負工消費合作社印裝 4 6 Ο 6。2 Α7 ~-~~________Β7 五、發明説明(19 ) ^ ^ 屏蔽1 00具有超過螺管纽件3〇軸範圍之軸範圍, :二上達到來自螺管組件30之電場之全部有效韩範圍。結 ,與.導電性屏蔽100有效地抑制於二次電漿29中之電場 7 »軸平行,防止會電容1性遮蔽螺管組件3 〇使之與體積 J :而降低螺管组件30能量對體# 2…之耦合效率之軸 二电場。該屏蔽100以自靶極16表面21平面後方軸向延 土超過小窗60及螺管组件3 〇爲佳。使用此結構,屏蔽 ,有政地使—'欠電漿29中之軸向電場短路,而促進來 組件之能量感應搞合於該二次電漿29中。 本發明較佳具體實例亦因異蔽100與小窗6〇之間隔接近 而^螺管組件30之能量於高效率下耦合於體積%中。此 間保持較佳不大於氣體中原子或分子之平均自由路徑或 該二次電漿29於艙12内之最小擴散長度之距離。此種接 近j屏蔽至小窗間隔與下述之其他具體實例相反,其係於 +窗或螺管保護性非|電性結構鄰近而位#所提供之任何 屏蔽結構後方形成電漿。避免該小窗後方形成電漿具有增 加來自螺管或其他電漿產生電極之能量進入濺射粒子所通 過之體積中之百分比,而增加有效電漿及其所致之濺射材 料離子化效率。於裝置10中,使用介於約5至5〇毫托耳 範圍内之處理氣體壓力。氬氣於該壓力下之爭均自由路徑 各由Π毫不芏1.〇毫米。結果,屏蔽!〇〇與小窗6〇間之較 佳間隔係約1.0至1 5毫米。 另一方面,該狹缝103寬度以太於約1 5毫米爲佳。該狭 縫1 〇3寬度足以容許狹縫丨03中形成二次電装29,以清除 -22- 本紙掁尺度適用中國國家插準(CNS ) AWm ( 210 X 297公釐) _______-____ ^^^^1 th^— ^^^^1 ΛΛ ^^^^1 n (請先閲讀背面之注意事贫再填寫本頁) 訂 460b A7 B7_ 五、發明説明(2〇 ) I ο— (請先閲讀背面之注意事項再填寫本頁) 可能在爽射材料通過狹缝103時沉積於屏蔽1〇〇與狹缝1〇3 相鄰之邊緣上或小窗60上之濺射材料。於狹縫1〇3中形成 之電漿29藉著而次濺射沉積於狹縫! 〇3中之小窗6〇上之 材料而於狹缝103鄰近向#小窗60延伸,並連續移動。 代之小窗60地,該螺管組件30可取代性地包埋於位在 艙房12中之絕緣區段66中,如圖i A所示,其中絕緣區段 66以如同小窗60之方式作用,以隔離螺管組件3〇與位於 餘房11中之該漿及濺射材料。該屏蔽100相對於絕緣體66 之結構係如同其相對於小窗60之結構,如圖1所示。 此第一個具體實例之許多細節皆可用於以下具體實例, 但省略其敘述以求痛化,故具體實例中僅陳述其間之差異。 第二個具體實例 圖3説明屏蔽陣列200,其係圖1之屏蔽ι〇〇之代用物, 但係位於空間丨丨與小窗60之間較不接近小窗6〇内表面處 。該屏蔽陣列200至少部分遮蔽小窗60使之與乾極i6所 錢射之材料隔離’但其間之空隙或間隙2〇4足以使來自螺 管組件3 0之能量耦合於體積26内。 该屏蔽陣列2 0 0以多個個別屏蔽或屏蔽區段2 〇 2爲佳, 經濟部申央標準局負工消費合作社印製 土少遮蔽该小窗6 0 4軸條,而不致使藏射材料塗層形成周 圍導電性路徑。該間隙204之結構係實質阻斷屏蔽陣列2〇〇 中之周圍電流路徑,而延伸至完全或部分橫越該陣列2〇〇 之抽向。該屏蔽202應係由金屬或其他材料構成,選擇於 琢屏蔽區段202上形成塗層時保持位於其上層之浼射材料 塗層。否則該沉積會剝落而使艙房12及欲處理之晶圓15 __ -23- 本紙張尺度適用中國國家標準(CNS ) A4規格(2IOX 297公釐) 4 6 Ο υ 二 Α7 __________Β7 五、發明説明(21 ) 污染。爲了控制沉積材料於屏蔽區段202上之累積以降低 污染之危險,該孱蔽區段202可施加電偏壓。區段2〇2亦 可個別施加偏壓,其偏壓可個別控制以使沉積於基板上之 薄膜分佈最佳化,諸如使基板1 5上之塗層均勻性離子化材 料之方向性最佳化。於該結構中,間隙2〇4使個別施加偏 壓之屏蔽區段2 0 2彼此隔離而絕緣。該偏壓係藉著經由遽 益匹配網2 0 7連接之產生器2 0 6提供,各屏蔽個別經由電 流限制電阻器208連接。該電阻器2〇8可變化或可提供其 他裝置以根據控制器5 0個別控制屏蔽區段2〇2之偏壓。 圖5説明裝置10之取代性具體實例1 〇 a,其中螺管組件 3 0係位於眞空艙12中,艙房12牆内側,而於空間丨丨之外 側。該保護性結構係爲窗60a型,自艙房12牆内側向内延 伸而封包螺管組件3 0。該罩蓋6 i A含有使罩蓋内部淺氣之 通口 62,其中該螺管組件3 0位於餘房1 2之眞空中。該異 ί故陣列2 0 0之位置與前述具體貫例相同,以遮蔽小窗以與 靶極1 6隔離。 經濟部中央標準局員工消費合作社印製 ---ί--1 --- — j - --- (—- n T (請先聞讀背面之注意事項再填寫本頁) 取代小窗60或60a地,圖6之取代性具體實例ί 〇b採用 絕緣塗層8 6形式之保護性結構,以覆蓋螺管組件3 0之導 體。於此具體實例中,該螺管组件3 0係位於該艙房12中 該空間1 1外側,環繞該體積26。該屏蔽陣列200之位置 與前述具體實例相同,遮蔽絕緣層86以與靶極ί 6隔離。 絕緣體86可爲數種形式中之任一種,諸如完全覆蓋螺管组 件30之導體表面之實心絕緣體86a,如圖7A所示,或可 爲多個不連續區段86b之形式,如圖所示。使用分段之 -24- 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 46〇i Α7 Β7 經濟部中央標準局員工消費合作社印製 五、發明説明(22 ) 絕緣體86b,區段間之間隙87有助於螺管组件3 ,而間隙87之窄度以保持不小於艙房12中氣體分子之平 均自由路徑,而不致於使電漿連通於螺管組件3〇、 < / 佳。取代螺管組件30上之絕緣塗層地,絕啖封蚪 +' . 思豕何衬可個別封 包該螺管组件30,諸如圖7€及7D之絕緣體86{:及86d。 此寺圖塑及數種用以隔離螺管組件3 〇斑雷將+甘 一、兒水〜具他取代 性屏蔽及保護性結構可用於其他具體實例中。 第三個具體實例_ 圖8説明介於空間】丨與小窗60之間而與小窗6〇内表面 鄰處之屏蔽陣列300。該屏蔽陣列300遮蔽該小窗以與自 靶極16濺射之材料隔離,以阻斷靶極16表面任何點與+ 窗60間之所有直接視線路徑爲佳。另外,根據本發明^體 實例,屏蔽陣列300中提供空間或間隙3〇5,以實質阻斷 位於小窗60後方之螺管组件3〇與體積%間欲耦合電漿μLi_____ 一一 〆— 39 vacuum pump 200 shielding array 40 processing gas 202 shielding section 41 flow control device 204 gap 50 controller 206 generator 60 window 207 filter matching network 61 metal cover 208 resistor 60a: window 300 shielding array 6 1 a: metal cover 300a: shield array 62 die holes 302 shield section 66 insulation section 302a: shield section 80 magnet 303 top surface 86 shielding insulation layer 304 gap 86a: solid insulator 305 gap 86b: segment insulator 306 Generator 86c: insulator 307, filter matching network 86d: insulator 308, resistor 87, gap 311, axial plane 100: shield 3, 12 axis, 103: slot — ^ n — ^^ 1 I-· τ--^^^ 1 ^^^ 1 n ^ — 1 ^ 11 l ^ i I *.-. I V3r 、-* (Please read the precautions on the back before filling out this page) Employees of the Central Government Procurement Bureau of the Ministry of Economic Affairs, consumer cooperation, Du printed inventions DETAILED DESCRIPTION FIG. 1 illustrates a sputtering coating apparatus 10 according to the principle of the present invention. The device i 〇 includes a vacuum airtight processing space enclosed in the cabin 12. In the cabin 11 1-the end device is provided with a substrate holder or bracket 14 to support the semiconductor wafer 15 placed above it. When the wafer 15 is mounted on the substrate holder 14, it is parallel to the target 16 and faces the target. The target electrode 6 is formed by a thin film coating material deposited on the wafer 15. The processing space 11 is usually a cylindrical space. 'Ultra-high vacuum pressure is maintained during processing, and the processing gas is filled with -16a.-This standard applies the Chinese standard {CNS —) _ A4 specifications (210 X 297 public love) ~ — 'A7 B7 Printed by the Central Consumer Bureau of the Ministry of Economic Affairs, Consumer Cooperatives V. Invention Description (14) Such as nitrogen. The far space 1 1 is located between the inspection room 12 and the living room 12 between the substrate holder 14 and the target 16. The target 16 is a part of the cathode assembly 17 installed in the cabin 2, and its one end is opposite to the substrate support 14. The cathode assembly 7 includes a target holder 18 with a fixed target. The magnet structure 19 is generally located on the opposite side of the target holder 18 from the substrate holder 14. It also shields the dark space 13 around the edge of the dry pole 16. The magnet structure 19 The magnet including a closed magnetic tunnel above the surface of the target 16 is known to those skilled in the art. When it is energized to a negative potential, it uses the cathode assembly 17 to capture the electrons injected into the cabin 2. The magnet structure 19 may include a magnet that is fixed or rotated or otherwise moved by any of several magnetron sputtering assemblies known to those skilled in the art, and may be a permanent or electromagnet. The power supply or power source 20 is usually a direct current The power supply, which can be connected to keep fixed or can be pulsed, is connected between the cathode assembly 17 and the wall of the cabin 12 'the wall is usually grounded as the system anode. The cathode assembly 7 is connected to the wall of the remaining room 12, away from The power supply 20 is preferably connected to the cathode assembly 17 through a rf filter 22. An auxiliary energy source such as an RF generator 24 may also be selectively connected to the cathode assembly via a matching network 25. Also provided The voltage circuit 27 is connected to the substrate holder 14 via the matching network 28. The bias circuit 27 applies a bias voltage to the wafer 15 mounted on the substrate holder μ. At this time, bipolar DC current can be thrown Power source or RF power source> The energy from the stable or pulsed DC power source 20 and / or the RF generator 24 generates a negative potential on the surface 21, causing electrons to be emitted from the surface 21 of the target 16. The emitted electrons are formed by the magnet structure 1 The magnetic field generated by 9 is captured on the surface 2 1 until it hits -17 {Please read the precautions on the back before filling this page) ο. *-The size of the paper is applicable to the Chinese National Standard (CNS) A4 specification (21 〇χ297mm) 4 606 A7 B7 printed by the Consumer Cooperatives of the Central Vehicle Administration Bureau of the Ministry of Economic Affairs 5. Description of the Invention (15) Ionize the processing gas atoms in the immediate vicinity of the surface 21 of the dry pole 16 and place it on the surface of the target 21 极A main plasma 23 is formed near this. The main plasma 23 becomes a source of gas positive ions, which accelerates toward the negatively charged surface 21, where the coating material particles are emitted from the dry electrode 16. Between the electrode surface 2 I and The space between the substrate holders 14 can be regarded as two parts -Qiu Fen is mainly occupied by plasma 23, whose shape is on the base shot surface 21 of target 16 to produce the required erosion pattern, while the second Shao Fen of space ii is between electric There are two reserved spaces 26 between the slurry 23 and the substrate 15 on the substrate holder 14. The particles of the sputtering material from the target 16 are usually derived from electrically neutral particles' which can only pass through the space 1 1 by the impulse, Some _ but not all-penetrated the plasma 23 and the volume 26 and crashed on the substrate 15. In the conventional radiography device, the neutral sputtered particles passing through the plasma 23 were not ionized largely because of the plasma 23 Occupying close to the target surface 21, j, part of the volume, under the operating pressure of the study, there is very little collision 3 between the neutral sputtered particles and the plasma 23 particles. Therefore, in the conventional sputtering method, the The neutral sputtered particles emit too much of the plasma 23, which remains neutral until it is deposited on the substrate 15 to become a thin film. For high-mirror-hole ratio holes and other patterned bottom coating contacts, and for the metallization of the hole by filling with a sputtered conductive material, particles are extremely desired in Vlsi and ULSI semiconductor device manufacturing Strike the substrate surface under a narrow angular distribution of the substrate normal so that it runs directly towards the pattern and reaches the lower part of the pattern without hitting or being obscured by the side of the pattern. S device 1 〇 By sputtering particles Ionization through the volume 26 causes the particles to have a charge, which facilitates the particles to strike the substrate vertically. Once the particles are charged -18- This paper size is applicable to China National Standards (CNS) A4 specifications (21 × 297 mm) (please read the notes on the back first and then fill out this page) 〇 Employees of the Central Standards Bureau of the Ministry of Economic Affairs Co-printed 4 606 A7 -------- V. Description of the Invention (16) ^ " " ~-Electricity, that is, electrostatic or electrical or magnetic acceleration orientation parallel to the axis of the cabin A path perpendicular to the surface of the substrate 15. This process is known in the art as Ionized Rational Deposition (IP VD) or Ion Assisted Sputtering. According to a preferred embodiment of the present invention, the in-flight ionization of the sputtered particles in space 26 is performed by & for an rf element that surrounds volume 2 6 without occupying space 1 I, so that the RF energy is reactive and better. It is inductively coupled within vol%. Although a solenoid structure other than a spiral can be used, the RF component is preferably in the form of a screw official component 30. The possible structure of the solenoid component 30a_30d is illustrated in Figs. 4A-4D = In addition, it can be different from The RF energy is fed into the solenoid in the foregoing manner. For example, a central RF plug is added to the center of the solenoid, and the other two wires are grounded or opposite. The solenoid assembly 30 inductively transfers energy into the processing gas in the volume 26 to form a secondary electrical device 29, which usually fills the volume 26 and is different from the main electrical violet 23. RF generates cry 32 ', which operates in a preferred but not limited to 0.1 or 0_2 Hz to or 80 Hz, and is connected to the solenoid assembly 30 via the matching network 3 3, so that the solenoid assembly 3 0 is supplied with energy, and a secondary plasma 29 is formed in the volume 26. The source of the process gas 40 is connected to the cabin j j via the flow control device 41. In the case of the political firing method, the feed gas 40 is generally an inert gas such as argon. For reactive methods, other gases such as nitrogen and oxygen can be introduced via the auxiliary flow controller. The Nanxuan space system 39 was also connected to cabin i 2 to pump the inspection room 12 to a degree of air in the range of millitorr or sub-mtorr. The pressure in 5 to 50 pen holders is better. Pump 39 maintains a super high vacuum using a process gas flow rate in the range of 5 to 300 standard cubic centimeters (msec). The device also includes the main controller 50 'programmable control based on a microprocessor ___-19- This paper size is applicable to China National Standard (CMS) A4 specification (2 丨 OX 297 mm) (Please read first Note on the back, please fill out this page again} Ό Order Λ. 460602 A7 Printed by the Central Standards Bureau of the Ministry of Economy—Industrial and Consumer Cooperatives V. Invention Description (17) It is better to sequence and control the operation of the aforementioned components. The controller 50 has an RF generator for starting the k φ cathode energy sources 20 and 24, a substrate bias energy source M /, and an RF generator 3, ^ d 4 for moving the plasma generating element solenoid assembly. The output of 1 pump J 9 and other controllable components of device .10. To achieve the directivity of ionized sputtering particles, a bias energy 27 connected to the substrate holder 14 via a matching network 28 can be used to make the substrate Η It is negatively biased relative to one person's table king, and the potential gradient is maintained in the plasma sheath in front of the substrate support · 14, which provides the force to accelerate the positively ionized base shot particles to hit the substrate surface and deposit on the upper layer. Use bipolar DC power or rf power. Magnet 80 can be separately Or instead, surround the cabin 12 'to generate a magnetic field in the axial direction of the cabin 12. The magnet 80 may be an electromagnet or formed by one or more permanent magnets fe. The electric field from the magnet 80 causes the charged particles to vortex along the line. Rotate to increase its radial orientation. When an axial electric field is present, charged particles can move towards the substrate in the axial direction to minimize radial losses. Provide protection between the solenoid assembly 30 and the space 11 The structure prevents the plasma 23 and 29 from contacting with the solenoid assembly and electrically interacting with each other. The structure is a non-conductive material and does not prevent the magnetic field surrounding the solenoid assembly 30 from reaching volume two. One of the protective structures The preferred form is a small window 60 located inside the 12 wall of the cabin, made of a hollow compatible dielectric material such as quartz, and the remaining wall device is used to form a airtight seal. The window 60 may be single insulated or magnetic A transparent material may be formed in its connecting section to form a generally cylindrical protective structure. The solenoid assembly 30 is described in the foregoing specific example, and is wound around the remaining room 12 to be located in the small window 60 Outside is better. Covered with solenoid Item 20- The national paper size (2 丨 centimeter) for this paper size is used. ^ ------ --I.-I. =-I (I—---I-1-·-I Ding [ 1, 卩 (please read the note on the back before filling out this page) 460602 A7, the description of the invention (18) is the horse conductive metal cover 61, which forms the dense solenoid assembly 3 〇 spacer ′ 、 ] Fork hole 62 is separated from 19 rih ^ ^, and also prevents electromagnetic energy from being lightly emitted from the solenoid assembly 30 and from the cabin 12 to the outside of the cabin 12. The mold hole 62 can be connected with the remaining room n from the outside atmosphere Connected or can be filled with atmospheric pressure or lower: start solenoid assembly 3. At this time, the gas of the mold does not support SL: The small window 60 itself is not conductive, but it is easy to accumulate from the coating of conductive material. The conductivity in or on the small window 60 supports the induced current around the cabin, reducing the efficiency of 'eliminating or destroying the energy from the solenoid assembly 30 RF coupling to the secondary plasma 29 in the volume 26. The conductivity of the coating on the small window 60, especially the azimuth (peripheral) direction, which extends in the 12 perimeter and direction of the cabin, and the inductive coupling short circuit can eliminate all or many of the energy inductively coupled into the volume 26. Nominally preventing conductive base material from accumulating on the small window 60, the preferred device additionally includes a shielding array, various specific examples described below. I A specific example Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs -------------- ^ __ rj 1- 彡 (Please read the note on the back before filling out this page) Figure 1 indicates a slot-shaped cylindrical shield 100 between the space 11 and the small window 60, which is close to the inner surface of the small window 60. The shield 100 shields the small window 60 to prevent the pole 16 from being shot, and to block all direct line of sight paths between any point 21 on the surface of the dry pole 16 and the small window 60. According to this specific example, the shield 100 has a longitudinal slit 103 parallel to the axis of the cabin 12. It is also possible to use single or multiple slits to block the surrounding current. The slit 103 of the preferred embodiment substantially interferes with the path surrounding the cabin 12 in the shield 100. Prevent this shield from inducing ambient or azimuth currents. -21-This paper size is applicable to Chinese National Standard (CNS) A4 (210X297 mm printed by the Central Standards Bureau of the Ministry of Economic Affairs and Consumer Cooperatives) 4 6 〇 6.2 2 Α7 ~-~~ ________ B7 V. Description of the invention (19) ^ ^ Shield 100 has an axis range that exceeds the 30 axis range of the solenoid button, and reaches the full effective range of the electric field from the solenoid assembly 30. Second, the conductive shield 100 effectively suppresses the secondary The electric field 7 in the plasma 29 is parallel to the axis, preventing the capacitor assembly from shielding the solenoid assembly 3 with the volume J: and reducing the coupling efficiency of the energy of the solenoid assembly 30 to the body # 2. Shield 100 preferably extends axially beyond the small window 60 and the solenoid assembly 30 from the surface of the target 16 surface 21 plane. Using this structure, the shield can effectively short-circuit the axial electric field in the under-plasma 29 And promote the energy induction of the components in the secondary plasma 29. The preferred embodiment of the present invention is also because the distance between the alienation 100 and the small window 60 is close, and the energy of the solenoid assembly 30 is under high efficiency. Coupling in volume%. Here it is preferably not more than the level of atoms or molecules in the gas. The distance of the free path or the minimum diffusion length of the secondary plasma 29 in the cabin 12. The distance between this close to the shielding and the small window is contrary to other specific examples described below, which are in the + window or solenoid protective non- | Plasma is formed behind any shielding structure provided by the electrical structure adjacent to #. Avoid formation of plasma behind the small window has a percentage increase in the volume of energy passed by the sputtering electrode from the solenoid or other plasma generated electrode , And increase the effective plasma and the ionization efficiency of the sputtered material. In the device 10, the pressure of the processing gas in the range of about 5 to 50 millitorr is used. Argon under this pressure The free paths each have a diameter of no less than 1.0 mm. As a result, the preferred distance between the shield! And the small window 60 is about 1.0 to 15 mm. On the other hand, the width of the slit 103 is more than about 1 5 mm is better. The width of the slit 103 is sufficient to allow the formation of a secondary electrical component 29 in the slit 丨 03 to remove the -22- paper size applicable to China National Standards (CNS) AWm (210 X 297 mm) _______ -____ ^^^^ 1 th ^ — ^^^^ 1 ΛΛ ^^^^ 1 n (Please read first Please note this page before filling in this page) Order 460b A7 B7_ V. Description of the invention (2〇) I ο— (Please read the notes on the back before filling this page) It may be deposited when the spray material passes through the slit 103 Shield 100 sputtering material on the edge adjacent to the slit 103 or the small window 60. Plasma 29 formed in the slit 103 is deposited on the slit by secondary sputtering! 〇3 The material on the middle small window 60 extends adjacent to the slit 103 toward the #small window 60 and continuously moves. Instead of the small window 60, the solenoid assembly 30 can be embedded in the cabin 12 instead. In the insulating section 66 shown in FIG. IA, the insulating section 66 functions like a small window 60 to isolate the solenoid assembly 30 from the slurry and sputtering material in the remaining room 11. The structure of the shield 100 with respect to the insulator 66 is the same as that with respect to the small window 60, as shown in FIG. Many details of this first specific example can be used in the following specific examples, but the description is omitted for pain, so only the differences are stated in the specific examples. Second Specific Example FIG. 3 illustrates a shielding array 200, which is a substitute for the shielding ιOO in FIG. 1, but is located between the space 丨 and the small window 60, which is less close to the inner surface of the small window 60. The shielding array 200 at least partially shields the small window 60 from the material radiated by the dry pole i6, but the gap or gap 204 therebetween is sufficient to couple the energy from the solenoid assembly 30 into the volume 26. The shielding array 200 is preferably a plurality of individual shielding or shielding sections 002. The printed work of the Shenyang Bureau of Standards of the Ministry of Economic Affairs and the Consumer Cooperative Co., Ltd. prints less soil to cover the small window 604 axis, so as not to cause hidden shots. The material coating forms a surrounding conductive path. The structure of the gap 204 substantially blocks the surrounding current path in the shielding array 2000, and extends to fully or partially traverse the drawing direction of the array 2000. The shield 202 should be made of metal or other materials, and the coating of the projection material should be selected to keep the upper layer of the shield section 202 when forming a coating. Otherwise, the deposit will peel off and cause the cabin 12 and the wafer to be processed 15 __ -23- This paper size is applicable to the Chinese National Standard (CNS) A4 specification (2IOX 297 mm) 4 6 Ο υ 2 A7 __________ Β7 5. Description of the invention (21) Pollution. In order to control the accumulation of deposited material on the shield section 202 to reduce the risk of contamination, the shield section 202 may be electrically biased. Section 202 can also be individually biased, and its bias can be individually controlled to optimize the distribution of the thin film deposited on the substrate, such as to optimize the uniformity of the coating on the substrate 15 and the directionality of the ionized material. Into. In this structure, the gap 204 isolates and shields the individual shield sections 202 that are biased. The bias voltage is provided by a generator 206 connected via the beneficial matching network 207, and each shield is individually connected via a current limiting resistor 208. The resistor 208 may be varied or other means may be provided to individually control the bias of the shield section 202 according to the controller 50. Fig. 5 illustrates an alternative specific example 10a of the device 10, in which the solenoid assembly 30 is located in the empty cabin 12, inside the wall of the cabin 12, and outside the space. The protective structure is a window 60a type, which extends inwardly from the inside of the 12th wall of the cabin and encloses the solenoid assembly 30. The cover 6 i A includes a port 62 for shallow air inside the cover, wherein the solenoid assembly 30 is located in the air space of the room 12. The position of the array 200 is the same as that of the previous specific embodiment, so as to shield the small window from the target 16. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs --- ί--1 ----j---- (--- n T (please read the precautions on the back before filling this page) instead of the small window 60 or At 60a, the alternative specific example of FIG. 6 is a protective structure in the form of an insulating coating 86 to cover the conductor of the solenoid assembly 30. In this specific example, the solenoid assembly 30 is located at the The outer space of the space 11 in the cabin 12 surrounds the volume 26. The shielding array 200 is in the same position as the previous specific example, and the shielding insulating layer 86 is isolated from the target electrode 6. The insulator 86 may be in any of several forms Such as a solid insulator 86a that completely covers the conductor surface of the solenoid assembly 30, as shown in Fig. 7A, or may be in the form of a plurality of discontinuous sections 86b, as shown in the figure. Using Segmented-24- This Paper Size Applicable to China National Standard (CNS) A4 specification (210X297 mm) 46〇i Α7 Β7 Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 5. Description of the invention (22) Insulator 86b, gap 87 between sections helps the solenoid Module 3, and the narrowness of the gap 87 to maintain no less than the gas content in the cabin 12 The average free path does not cause the plasma to communicate with the solenoid assembly 30, < / is good. Instead of the insulating coating ground on the solenoid assembly 30, it must be sealed + '. Think of any lining can be individually packaged The solenoid assembly 30, such as the insulator 86 {and 86d of Fig. 7 and 7D. This temple figure and several types are used to isolate the solenoid assembly. 30 斑 雷雷 + 甘 一 、 儿 水 ~ with alternative shielding And the protective structure can be used in other specific examples. The third specific example _ FIG. 8 illustrates the shielding array 300 between the space 60 and the small window 60 and adjacent to the inner surface of the small window 60. The shielding array 300 It is better to shield the small window from the material sputtered from the target 16 to block all direct sight paths between any point on the surface of the target 16 and the window 60. In addition, according to the example of the present invention, the shielding array 300 To provide a space or gap 30 in order to substantially block the to-be-coupled plasma μ between the solenoid assembly 30 and the volume% located behind the small window 60.
之區域,以利於來自螺管组件30及延伸之電漿之能量耦合 於體積26内。 P 該屏蔽陣列300以完全遮蔽小窗6〇使之與靶極丨6上之 每一點隔離之多個屏蔽或屏蔽區段3〇2形式爲佳。此遮蔽 消除於基板60上形成濺射膜累積之大部分可能。是故,既 不產生導電性路徑,易不產生靜電屏蔽。 、於本發明I 一具體實例中,該屏蔽區段3〇2係爲戴頭圓 錐形狀,其内側與平行於靶極16表面21及支架丨4上之基 板15之平面形成角度没。各屏蔽區段3〇2之角度θ可相同 ,但該屏蔽區段302之效率可藉著増加區段3〇2與靶極16 25- (請先閲磧背面之注意事項再填寫本頁)This area allows the energy from the solenoid assembly 30 and the extended plasma to be coupled into the volume 26. P The shield array 300 is preferably in the form of a plurality of shields or shield sections 30 that completely shield the small window 60 from each point on the target electrode 6. This masking eliminates most of the possibility of a sputter film being accumulated on the substrate 60. Therefore, neither conductive path is generated and static shielding is not easily generated. In a specific example of the present invention, the shielding section 302 has a head-shaped cone shape, and an inner side thereof forms an angle with a plane parallel to the surface 21 of the target 16 and the base plate 15 on the bracket 4. The angle θ of each shield section 302 can be the same, but the efficiency of the shield section 302 can be increased by adding section 302 and target 16 25- (please read the precautions on the back of the page before filling this page)
,1T .I n^i ·- I ^—ϋ . 經濟部中央標挛局員工消費合作社印袈 Α7 Β7 一.--------------— — --- 一 五、發明说明(23 ) 問之距離隨之縮小角度Θ而促進或最佳化,使區段302之 頂面303直接面對靶極1 6,針對特定區段面積提供使靶極 16與小窗6 0隔離之最大遮蔽。該屛蔽區段3 〇 2位於空間U 外側及環繞空間11周圍’养此由周園間隙或空間3 0 5軸向 間隔。該間隙3 0 5之最大寬度係完全遮蔽無極1 6表面以使 之與小窗60隔離之最寬間隙S,如線79所示,故小窗60 之周圍帶未曝露於靶極16,以於小窗6 0周圍沉積角狀導 電條。因此,間隙305之最大寬度s於與靶極距離較大處 可較大。該間隙3〇5可較窄’但應不小於在該艙溫度及壓 力下該處理氣體原子之平均自由路徑,且應最佳間隔,於 處理條件下,使RF電漿最有效地擴散於體積26中。相同 理由,區段302各具有鬲度Η,可各區段302皆相同或變 化以使該遮蔽及區段3 02間距最佳化》 該屏蔽區段302之理想數目係根據艙房丨2之幾何形狀而 定。雖可使用單一屏蔽區段302 ’但一般採用兩個至六個 區段302 區段302數目應受限制,而累積之屏蔽區段面 積應最小化以使RF電漿損失減至最少。此外,爲了防止 RF螺管組件30感應形成渦流或其他電流之密閉之周圍路 徑,該區段3 0 2應具有至少一個阻斷彼此之間隙3 〇 4。相 鄰區段302之間隙304可如所示之線狀,或較佳交錯以防 止於橫越小窗60軸向沉積連續膜線。間隙3〇4應寬至足以 防止電弧,其根據處理條件而定,需要约1/4至丨英叶士 寬度。 間隙3 0 4之結構係實質阻斷屏蔽陣列3 0 〇中之電流路巧 -26- 本纸張尺度逋用中國國家標準(CNS )八4規格(2ι〇 χ297公釐) ---I ---1 ---I--j I— I I _ X 〆 1 --5 〔請先閱讀背面之注意事項再填寫本頁) A7 ---------B7 五、發明説明(24 ) ,而完全或部分延伸橫越陣列300之軸向。該屏蔽區段3〇2 可由金屬、眞空相容性介電材科諸如陶覺或石英或某些立 他經選擇以於該異蔽區段302上形成該塗層時保持其上層 之濺射材料塗層之相容性材料製造。否則該沉積剝離以使 碟艙房12及欲處理晶圓15污染。爲了控制沉積材料於屏 蔽陣列300上之累積以降低污染之危險,該屏蔽區段3〇〇 可施加偏壓,並由該情況所使用之金屬製造。該屏蔽區段 302亦個別施加偏壓,以個別控制其偏壓而使欲沉積於基 板上之膜分佈最佳化,諸如使基板】5上之塗層均勻性及離 予化材料之方向性最佳化。於該結構中,間隙3〇4使所個 別施加偏壓之屏蔽區段彼此完全隔離並絕緣。偏壓係由經 由濾器或匹配網307連接之產生器306提供,各屏蔽區段 3 02個別經由電流限制電阻器308連接3該電阻器3〇8可係 爲可變或其他可用以個別針對控制器50控制屏蔽區段302 之偏壓的裝置。 經濟部中夬標準局員工消費合作社印製 I _ ------1 (請先閲讀背面之注意事嗔再填寫本頁) 前述屏蔽陣列300之優點可由具有圖9及10所示之屏蔽 陣列300a之取代性具體實例實現。陣列3〇〇a係由多個平 面或稍具曲度之矩型區段302a形成,其排列環繞小窗60 内部空間1 1周圍之槳片或葉片陣列。該區段3 〇2a邊緣彼 此相隔轴向間隔或狹缝304a,其於區段302a間提供空間 ,以使電漿耦合於體積2 6中,並阻斷環繞該陣列3 0 0 a之 可能周園電流路徑。區段3 02a之取向係使其各界定穿透艎 房12之軸312而與轴向平面311形成之角度φ。介於相鄰 辱蔽區段302a間及介於異蔽區段302a與小窗60間之間隙 -27- 本纸張尺度適用中國國家標準(CNS) Λ4規格(210X297公釐) 46060^ A7 B7 五、發明説明(25 ) W應不小於搶中乳體之平均自由路徑,使電漿可有效地自 小窗60鄰近處延伸至介於區段302a間之間隙304a中之體 積26内。該區段302a軸向長至足以防止小窗6〇位於區段 302a之處形成任何塗層周,部分,該角度φ及間隙w以彼 此相對設定於遮蔽位於小窗6 0上之全部靶極〗6爲佳。 取代小窗60地,前述屏蔽陣列可使用位於該艙内側之介 電窗或位於該艙内之螺管,以絕緣隔離該電漿。 氺伞伞 熟習此技藝者已知本發明可加以變化,而本發明係針對 較佳具體實例描述。是故’可進行加成及改良,各具體實 例之細節可於不偏離本發明原理及意向下相互交换3 I---In----^------—訂 (請先閱讀背面之注意事及再填舄本I) 經濟部中央標準局貝工消費合作社印製 -28 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐), 1T .I n ^ i ·-I ^ —ϋ. Employee Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs 袈 Α7 Β7 Ⅰ .-------------------- 5 、 Explanation of invention (23) The distance is reduced by the angle Θ to promote or optimize, so that the top surface 303 of the segment 302 directly faces the target 16 and provides a target 16 and a small window for a specific segment area. 60 0 maximum shielding. The sheltered section 3 02 is located outside of the space U and around the space 11 ', which is axially spaced by the peripheral space or space 305. The maximum width of the gap 3 0 5 is the widest gap S that completely shields the surface of the electrodeless 16 to isolate it from the small window 60, as shown by line 79. Therefore, the band around the small window 60 is not exposed to the target 16 to An angular conductive strip is deposited around the small window 60. Therefore, the maximum width s of the gap 305 may be larger at a larger distance from the target. The gap 305 may be narrower, but it should not be less than the average free path of the processing gas atoms at the cabin temperature and pressure, and it should be optimally spaced to allow the RF plasma to diffuse most efficiently into the volume under processing conditions. 26 in. For the same reason, each segment 302 has a 鬲 degree, and each segment 302 may be the same or changed to optimize the shielding and the spacing of segments 302. The ideal number of shielding segments 302 is based on the cabin Depending on the geometry. Although a single shielded segment 302 'may be used, generally two to six segments 302 should be used. The number of segments 302 should be limited, and the accumulated shielded segment area should be minimized to minimize RF plasma losses. In addition, in order to prevent the RF solenoid assembly 30 from inductively forming a closed peripheral path of eddy current or other current, the section 302 should have at least one gap 304 that blocks each other. The gaps 304 of adjacent sections 302 may be linear, as shown, or preferably staggered to prevent continuous film lines from being deposited axially across the small window 60. The gap 304 should be wide enough to prevent arcing, which, depending on the processing conditions, requires a width of about 1/4 to a British inch. The structure of the gap 3 0 4 substantially blocks the current in the shielding array 3 0 0. 26- This paper uses the Chinese National Standard (CNS) 8 4 specifications (2ιχχ297 mm) --- I- --1 --- I--j I— II _ X 〆1 --5 [Please read the notes on the back before filling this page) A7 --------- B7 V. Description of the invention (24 ), And extend completely or partially across the axis of the array 300. The shielding section 302 may be selected from metals, hollow compatible dielectric materials such as ceramic or quartz, or some other lithography to be selected to retain the upper layer of the sputtering layer when the coating is formed on the shielded section 302. Made of compatible materials for material coating. Otherwise, the deposition peels off to contaminate the disk compartment 12 and the wafer 15 to be processed. In order to control the accumulation of deposited material on the shielding array 300 to reduce the risk of contamination, the shielding section 300 may be biased and made of the metal used in this case. The shielding section 302 is also individually biased to individually control its bias to optimize the distribution of the film to be deposited on the substrate, such as to uniformize the coating on the substrate and the directionality of the ionizing material. optimize. In this structure, the gap 304 completely isolates and insulates the respective shield sections to which a bias voltage is applied. The bias voltage is provided by a generator 306 connected through a filter or matching network 307. Each shield section 3 02 is individually connected 3 through a current limiting resistor 308. The resistor 3 08 can be variable or other can be used for individual control The device 50 controls the biasing means of the shielding section 302. Printed by the Consumer Affairs Cooperative of the China Standards Bureau of the Ministry of Economic Affairs I _ ------ 1 (Please read the notes on the back before filling this page) The advantages of the aforementioned shielding array 300 can be provided by the shielding shown in Figures 9 and 10. Alternative examples of the array 300a are realized. The array 300a is formed by a plurality of flat or slightly curved rectangular sections 302a arranged in an array of paddles or blades around the inner space 11 of the small window 60. The edges of the section 3 02a are axially spaced or slits 304a from each other, which provides space between the sections 302a, so that the plasma is coupled in the volume 26 and blocks the possible circumference around the array 3 0 0a. Park current path. The orientation of the segments 3 02a is such that each of them defines an angle φ that penetrates the axis 312 of the mortal house 12 and forms with the axial plane 311. The gap between the adjacent degraded section 302a and between the obscured section 302a and the small window 60-27- This paper size applies the Chinese National Standard (CNS) Λ4 specification (210X297 mm) 46060 ^ A7 B7 V. Description of the invention (25) W should not be less than the average free path of the grabbing breast so that the plasma can effectively extend from the vicinity of the small window 60 to the volume 26 in the gap 304a between the sections 302a. This section 302a is axially long enough to prevent the small window 60 from forming any coating perimeter at the section 302a. The angle φ and the gap w are set relative to each other to shield all targets on the small window 60. 〖6 is better. Instead of the small window 60, the aforementioned shielding array may use a dielectric window located inside the cabin or a solenoid located inside the cabin to insulate the plasma. It is known to those skilled in the art that the present invention can be modified, and the present invention is described with reference to preferred specific examples. That's why 'additions and improvements can be made, and the details of each specific example can be exchanged with each other without departing from the principles and intentions of the present invention. Note on the back and re-fill this book I) Printed by the Bayer Consumer Cooperative of the Central Bureau of Standards of the Ministry of Economics -28 This paper size applies to the Chinese National Standard (CNS) A4 specification (210X297 mm)