TWI240967B - Plasma surface passivation modification treatment method of low dielectric constant film - Google Patents

Plasma surface passivation modification treatment method of low dielectric constant film Download PDF

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TWI240967B
TWI240967B TW92113050A TW92113050A TWI240967B TW I240967 B TWI240967 B TW I240967B TW 92113050 A TW92113050 A TW 92113050A TW 92113050 A TW92113050 A TW 92113050A TW I240967 B TWI240967 B TW I240967B
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plasma
low
film
modification treatment
dielectric constant
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TW200425325A (en
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Sung-De Chen
Jin-Shan Chen
Tsung-Ren Yang
Pi-Yau Li
Tang-Jie Liou
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Univ Feng Chia
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Abstract

A plasma surface passivation modification treatment method of low dielectric constant film is to perform surface passivation modification treatment on a siloxane low dielectric constant (low k) film, which comprises placing the film sample into a reaction chamber; introducing N2/H2 mixture gas which is used to generate the ionized plasma by a radio frequency supplier; using the N2/H2 mixture plasma to perform surface passivation modification treatment on the low k film sample; and thus forming Si-C-N and Si-N mixed bonding passivation layer after the optimized modification treatment. The surface passivation layer can prevent impact damage on the low polarization chemical bonding (methyl, Si-H) and dielectric constant (and insulation property) from the subsequent high oxidation or reduction plasma (such as O2 and H2) processes (and annealing treatment) and thus effectiveness of protecting and reinforcing the low k film can be achieved. The passivation layer can be further used as a diffusion barrier layer to alleviate the thermal diffusion of copper towards the low k film, which can avoid using dielectric material with high dielectric behavior or metal diffusion barrier material with high resistivity as the use of such material can increase the total RC delay time of the interconnect in the semiconductor device and decrease the efficiency of device calculations.

Description

1240967 九、發明說明: 【發明所屬之技術領域】 本發明係關於一種低介電常數薄膜之電漿表面鈍化改質處理方法,特 別是指一種低k薄膜表面之ΝΛ混合電漿表面鈍化改質處理方法;將於表面 塗佈並完成固化之低k薄膜基材放置於真空輝光放電的反應腔體内,並抽氣· 至低於l(T2-l〇-4 Pa後,導入N2/H2的混合氣體(壓力介於1〇2—1(pl 並以 射頻供應器來產生電漿;低k薄膜經此Nz/H2混合電漿處理後,可在薄膜表面 形成Si-C-N與Si-N含氮化物純化層,此鈍化層的存在可防止低k薄膜在其他隹 電漿環境中(如:〇2、H2、N2等)所導致之介電常數及漏電流的衰退,而達 到保護與強化低k薄膜之功效,此外並能提供作為低!^薄膜與銅薄膜間之擴-散阻礙層。 【先前技術】 為了提昇元件的性能,許多新型材料已陸續被導入積體電路晶片元件 製程。但由於材料間的性質差異及製程整合的困難,因此衍生了許多問題, 其中,為了降低内連接導線(加㈣瞻的)之電阻_電容(μ)延遲,籲 金屬間介電材料(Inter-metal Dielectrics)預期將逐漸由Si〇2 (k-4. 2) 轉移至k值低於3之材料;但由於低k材料的熱穩定性、機械強度、鍵結穩定· 性均遜於si〇2,故氧電漿去除光阻、化學機械研磨(CMp)或退火處理往往· 會導致低k材料之芳香族羥基或烷基等低偏極化鍵結的破壞、介電特性的衰 退及熱穩定性之降低,這些退化行為實乃整合低k材料與銅導線大馬士 (Damascene)製程的嚴重障礙,也造成低料無法如預期的被完全整合 至1C製程中。 5 1240967 而目前使用在低k/銅製程之介電性覆蓋層(Capping Layer)材料為 CVD-SiN或CVD—Sic⑻,其k值介於㈤;導電性覆蓋層材料包括化、μ 等’其電阻率通常高於100 μΩ-cm,這些覆蓋層可以提供擴散阻礙、黏著促 進及研磨終止等功能;然而,它們的高k或高電阻率會增加内連接導線的整 體R-C延遲時間,因此也降低了元件的性能,所以,隨著積體電路的特徵尺 寸下降至-百奈米以下,利用電漿表面鈍化低谢料以開發,,現場,,製作超薄 覆盍層的製程是-個非常關鍵性的绿題,近幾年來也因而已被廣泛的研 九’每些研究大多利用單一的反應性氣體(或與純氣混合)產生電製,包 括:脇、N2〇、N2、H2 (He)、〇2以進行表面鈍化處理,或者利用含甲基(CH3) ^^ria(Hexamethyldisilazane^1#HMDS;Trimethyl^ , 簡稱TMCS)對<損偷材料進行回復(ReeQveiT)處理。 然而’使用單-反應性氣體將會出現以下幾個問題: ⑴顧⑷性:由於勵具有雜及毒性,因此在機器維修、人員操作、 廢物排放等方㈣須特別加以考量,故將大幅造成成本支出,及後 保問題; (2)熱預异(lllennal㈣财):齡子具有三個共價鍵結(加* β_), 因此必須施以較高之電襞激發功率或較高之基材處理溫度,意即熱預算較 ⑶材科縣倾細嫩雛⑽錄料—之本細 ===__於某—則物材料,而不適用於 ',,、廣泛運用於各種低k材料,且製程視窗往往也相對的狹 6 1240967 因此’開發可克服以上缺失的表面鈍化之_製輯成為相 積極努力的目標 本發明乃哪纖合性«表面改·化製程,此種溫和性的”環 保友善"«與微電子侧製程有良好搭配性,日前氟氣氣氛為魏基介電 材料最常_乾摘職體,但基於環保之絲以及使崎齡限制、操 作成本的日益增高,此種_氣體目前也逐漸地被其它氣氛所取代,其中, N2、H2、1^/¾均曾被使用過,並以队/jj2最具潛力。[卜幻 有鏗於現有的單-氣氛電漿鈍化會有一項或多項前述之缺失,本案發 明人乃以㈣錄及—乡年之微好__縣之研發驗,積極研 丸異於單-電漿的處理方式(以免除上述之缺失),來解決業界極欲克服 之低k材料性質退化的問題,經不斷的嘗試與試驗後,終發現脇混合電漿 具有制狀表硫質效應,可㈣化齡錢魏絲(Hybrid〇rganic1240967 IX. Description of the invention: [Technical field to which the invention belongs] The present invention relates to a plasma surface passivation modification method for a low dielectric constant film, in particular to a Nk mixed plasma surface passivation modification for a low-k film surface. Treatment method: Place the low-k film substrate coated and cured on the surface in the reaction chamber of vacuum glow discharge, and evacuate to less than l (T2-l0-4 Pa, then introduce N2 / H2 The mixed gas (pressure is between 10—1 (pl and RF plasma generator is used to generate plasma; low-k film is treated with this Nz / H2 mixed plasma to form Si-CN and Si-N on the film surface) Contains a nitride purification layer. The presence of this passivation layer can prevent the dielectric constant and leakage current of low-k films from being reduced in other plasma environments (such as 02, H2, N2, etc.) to achieve protection and Strengthen the function of low-k thin film, and also provide a low-diffusion layer between copper and copper thin film. [Previous technology] In order to improve the performance of components, many new materials have been introduced into the integrated circuit chip component manufacturing process ... but due to the nature difference between materials Difficulties in process integration have led to many problems. Among them, in order to reduce the resistance_capacitance (μ) delay of interconnecting wires (plus), Inter-metal Dielectrics are expected to gradually be changed from Si 〇2 (k-4. 2) Transfer to materials with a k value lower than 3. However, since the thermal stability, mechanical strength, and bond stability of low-k materials are lower than si〇2, the oxygen plasma removes light. Resistance, chemical mechanical polishing (CMp), or annealing treatments often lead to the destruction of low-polarity bonds such as aromatic hydroxyl or alkyl groups of low-k materials, degradation of dielectric properties, and reduction of thermal stability. These degradation behaviors It is a serious obstacle to the integration of low-k materials and copper conductors in the Damascene process, and it also causes low-level materials to not be fully integrated into the 1C process as expected. 5 1240967 The dielectric cover currently used in low-k / copper processes The material of the Capping Layer is CVD-SiN or CVD-Sic⑻, whose k value is between ㈤; the conductive cover layer materials include chemical, μ, etc. 'The resistivity is usually higher than 100 μΩ-cm. These cover layers can provide diffusion Obstruction, adhesion promotion and polishing And other functions; however, their high k or high resistivity will increase the overall RC delay time of the interconnecting wires, thus also reducing the performance of the component. Therefore, as the feature size of integrated circuits drops below -100 nanometers, The use of plasma surface passivation and low passivation materials for the development, on-site, and production of ultra-thin coatings is a very critical green question. In recent years, it has been widely studied. Most of these studies have been used. A single reactive gas (or mixed with pure gas) generates electricity, including: W2, N2O, N2, H2 (He), 02 for surface passivation treatment, or using methyl group (CH3) ^^ ria ( Hexamethyldisilazane ^ 1 # HMDS; Trimethyl ^ (TMCS for short) responds to the damaged material (ReeQveiT). However, 'the use of mono-reactive gas will cause the following problems: ⑴ Guxi: Due to the heterogeneous and toxic nature of the excitation, special consideration must be given to machine maintenance, personnel operation, waste discharge, etc., which will greatly cause Costs and maintenance issues; (2) Thermal pre-differentiation (lllennal): Age has three covalent bonds (plus * β_), so higher electric excitation power or higher base must be applied Material processing temperature, which means that the thermal budget is smaller than that in Caike County. The material is fine === __ 于某 —the material is not suitable for ',', and is widely used in various low-k materials. And the process window is often relatively narrow 6 1240967 Therefore 'development can overcome the above-mentioned lack of surface passivation _ production series has become a goal of active efforts The invention is fibrous «surface modification process, this kind of gentle "Environmental friendliness" has a good compatibility with the microelectronics process. Recently, the fluorine gas atmosphere is the most common of Weiji's dielectric materials. However, it is based on environmental protection and the increasing age limit and increasing operating costs. Species of _ gas Gradually replaced by other atmospheres, among which N2, H2, 1 ^ / ¾ have all been used, and the team / jj2 has the most potential. [卜 幻 There is an item in the existing single-atmosphere plasma passivation. One or more of the aforementioned defects, the inventor of this case is to solve the industry with the record and-the rural year is very good __ county research and development test, actively research pills different from the single-plasma treatment (to avoid the above-mentioned defects) to solve the industry I want to overcome the problem of degradation of low-k material properties. After continuous trials and experiments, I finally found that the mixed plasma has the effect of forming surface sulfur, which can age the hybrid

Siloxane P〇lymer,H0SP)低k薄膜(k = 2·5)之電物特性。 【發明内容】 在詳細說明本發明前,首先先利用三個實例,重點說明三種常見的單馨 氣體(〇2、Η2與Ν2)真空輝光放電(Gl〇w-discharge)電樂:處理對石夕氧烧 基低k薄膜的效應: _ 案例一:氧電漿處理 _ 氧電漿處理會導致矽氧烷基低k薄膜之Si-CH3、Si-Η舆C-Η的斷鍵,形成 Si懸宕鍵結(Dangling Bonds),這些懸宕鍵結極易再與其它的si-〇鍵結 中的氧原子結合成Si-0網狀結構,因此,〇2電漿處理後之梦氧烧基薄膜的籠 狀Si-0減少,網狀Si-〇增加,其Si-CH3、Si-H與C-H低偏極鍵結也大量減少, 1240967 k種、’二過〇2電水處理過之石夕氧燒震膜會因為其特徵鍵結之破帛,而導致低 k特性之喪失及絕緣性、物理特性的大幅衰退。 案例二:氫電漿處理 氫電錢理後之石夕氧燒基低k薄膜中之籠狀Si—〇、& 一弧、C—H鍵結會明 顯地減少,其低k特性、電絕緣性及物理特性的衰退與氧電裝處理類似,這 個、、·〇果顯tfH2電4會如同〇2電聚般的導致Η與c—Η的斷鍵,形成別 懸雜結,這些齡麟極胃再與其它㈣產生麵交鏈(c臓—碰加) 而合成Si-0網狀結構,造成石夕氧燒基低k薄膜之特性的衰退。 _ 案例三:氮電漿處理 氮電漿處理只造成魏燒基低k薄膜之Μ.波峰強度的輕微下降,而 網狀與籠狀Si-G波峰強度幾無變化,此結果暗示·· &賴僅導致少數Si—CH3 的斷鍵,卻不易促成籠狀與網狀Si—〇鍵結間的轉換,但是,這些鍵結改變 仍會負面的影響低k薄膜的電物特性。 有4監於此,本發明則使用有別於上述三個單一氣氛實例之混合性氣體 (N2/H2)所產生的電毅來進行離子氮化(ι〇η表面改質。表· 1為本發明與習用的單-反應性氣體(h2、N2、N2〇與腿)對低k介電材料之 鈍化電漿製程特性比較。其中,目前所習用的單一反應性氣體電漿在製程· 的考量下會分別遭遇不同的製程瓶頸,但本發明所提出的队/112混合性氣體, 電漿的方法卻可有效克服這些製程限制,因此更適用於低料才料的表面鈍化 處理。針對表1所列舉^/¾混合性電漿之優點進一步說明如下: 1·低熱預异一H2的添加能大幅提高队之游離效率,因此,相較於仏鈍化電漿 8 1240967 處理,ΝνΗ2混合性電漿具有較低的熱預算(基於此因,傳統鋼鐵之離子氮 化表面硬化處理不使用沁電漿,而是使用沁/犯混合電漿); 2. 冋安全性一由於冗/H2的無腐蝕、無毒特性,因此較NH3容易處理,應用上 也較為安全; 3. 同衣私整合性一 是取代氟碳蝕刻氣體之最具前膽性的電漿氣氛之 一,且N2/H2氣體源為工業界所常用,故有優良之製程整合性; 4·低操作成本一沁、H2資源不虞匱乏,且物性溫和,沒有後續處理之成本顧 慮’使用成本相對低廉; 5·寬廣製程視窗一沁/出容許分別獨立地控制仏及π,氣體的壓力,故得以控制 產生不同比例之含氮、氫之物種濃度,而可依低k材料的本質特性需求進行 製程最佳化的調整。 表1低k材料鈍化電漿氣氛之相關製程特性比較Siloxane Polymer, HOSP) low-k film (k = 2.5) electrical properties. [Summary of the Invention] Before explaining the present invention in detail, first use three examples to highlight three common single-xin gases (〇2, Η2, and Ν2) vacuum glow discharge (Gl0w-discharge) electric music: treatment of stone Effect of low-k film based on oxygen-fired base: _ Case 1: Oxygen plasma treatment _ Oxygen plasma treatment will cause Si-CH3 and Si-ΗC-Η bond break of siloxane low-k film to form Si Dangling Bonds. These dangling bonds can be easily combined with the oxygen atoms in other si-〇 bonds to form a Si-0 network structure. Therefore, 〇2 plasma treatment of dream oxygen burns The cage-like Si-0 of the base film is reduced, and the network-like Si-〇 is increased. The low-polarity bonding of Si-CH3, Si-H and CH is also greatly reduced. The Shixi oxygen-shocked film will cause the loss of low-k characteristics and the significant degradation of insulation and physical properties due to the breakage of its characteristic bonds. Case 2: Hydrogen plasma treatment of cage-shaped Si—0, & one arc, C—H bond in Shixi oxygen-fired low-k film after hydrogen electricity treatment, its low-k characteristics, electricity The degradation of the insulation and physical properties is similar to the treatment of oxygen equipment. This, ·· 〇 will show that tfH2 electricity 4 will cause the breakage of Η and c- 般 as a result of 〇2 electropolymerization. Linji stomach then cross-links with other gadolinium (c 臓 —push-on) to synthesize the Si-0 network structure, which causes the characteristics of Shixi oxygen-based low-k film to decline. _ Case 3: Nitrogen plasma treatment Nitrogen plasma treatment only caused a slight decrease in the M. peak intensity of the Wei-based low-k film, while the network and cage Si-G peak intensity had little change. This result suggests that & amp Lai only causes a few Si—CH3 bond breaks, but it is not easy to promote the transition between cage-like and network Si—0 bond junctions. However, these bond changes will still negatively affect the electrical properties of low-k films. In view of this, the present invention uses ionization generated by a mixed gas (N2 / H2) that is different from the above three single atmosphere examples to perform ion nitridation (ι〇η surface modification. Table · 1 is The present invention is compared with the conventional single-reactive gas (h2, N2, N20, and legs) passivation plasma process characteristics of low-k dielectric materials. Among them, the currently used single reactive gas plasma is in the process of Under consideration, different process bottlenecks will be encountered, but the team / 112 mixed gas and plasma method proposed in the present invention can effectively overcome these process limitations, so it is more suitable for the surface passivation of low-grade materials. The advantages of the ^ / ¾ mixed plasma listed in 1 are further explained as follows: 1. The addition of low-heat pre-isolated H2 can greatly improve the team's free efficiency. Therefore, compared to the 仏 passivation plasma 8 1240967 treatment, ΝνΗ2 mixed Plasma has a lower thermal budget (for this reason, traditional steel plasma nitriding surface hardening treatment does not use Qin Plasma, but instead uses Qin / Guan mixed plasma); 2. 冋 safety-due to the absence of redundant / H2 Corrosive and non-toxic properties NH3 is easy to handle and safer in application; 3. The same clothing and private integration. One is to replace the fluorocarbon etching gas with one of the most courageous plasma atmospheres, and the N2 / H2 gas source is commonly used in the industry, so Has excellent process integration; 4. Low operating costs, Q2, no shortage of H2 resources, and mild physical properties, no cost concerns about subsequent processing 'The use costs are relatively low; 5. Wide process window Yiqin / output allows independent control仏 and π, the pressure of the gas, so it can control the concentration of species containing nitrogen and hydrogen in different proportions, and the process optimization can be adjusted according to the essential characteristics of low-k materials. Table 1 Low-k materials passivation plasma atmosphere Comparison of related process characteristics

本創作案即發現適當的調節氣體之比例、電聚激發功率及電繁产理 時間能使矽氧烷基低k薄膜產生良好的鈍化效果,以達到強化介電特性之目 1240967 為使貴審查委貞對本發明之方式及特徵能有更深—層的認識與暸解,兹附 以一貫例詳細說明如后。 【實施方式】 將石夕氧燒基低k材料(即H0SP)旋轉塗佈於石夕晶圓基材表面之後,在氮· 氣環境中相繼於15(TC、20(TC與30(TC各烘烤數分鐘,以除去凝膠薄膜中之, 洛Μ而後置於管爐巾(< 4〇〇 C)進行-小時的固化處理,此低k薄膜試 片立即被置入氣氛抽至低於10 3 pa (約τ〇ΓΓ)之真空腔體的基座上,_ 利用13· 56 MHz的射頻供應器連接至腔體内之基座來產生電漿,該電漿氣氛 匕3〇2、Η2、N2單一氣體與各種仏/112混合氣體,並利用質流控制器調整其流 ®大小與比率,所有的電漿處理均在5〇至25〇w的射頻功率下操作丨至加分 鐘,經處理後的HOSP低k薄膜乃利用傅利葉轉換紅外線光譜(FTIR)分析其 主要鐽結波峰的強度改變,尤其是Si-CH3 (127〇cnfl)、網狀Si—〇 (1〇4〇cmIn this creative case, it was found that the proper adjustment of the gas ratio, the excitation power of electropolymerization, and the processing time of electrical propagation can make the siloxy low-k film have a good passivation effect to achieve the purpose of strengthening the dielectric properties. 1240967 Wei Zhen can have a deeper-level understanding and understanding of the methods and features of the present invention, and hereby attach a conventional example to explain it in detail as follows. [Embodiment] After spin-coated low-k material (ie, H0SP) is applied on the surface of the substrate of Shixi wafer, it is successively applied at 15 (TC, 20 (TC and 30 (TC each) in a nitrogen gas atmosphere). Bake for a few minutes to remove the gel film, and then place it in a tube oven towel (< 400C) for a one-hour curing process. This low-k film test piece is immediately placed in the atmosphere and pumped to a low temperature. On the base of a vacuum cavity of 10 3 pa (about τ〇ΓΓ), a 13.56 MHz RF power supply is connected to the base of the cavity to generate a plasma, and the plasma atmosphere is 302 Η, Η2, N2 single gas and various 仏 / 112 mixed gases, and use the mass flow controller to adjust its flow size and ratio. All plasma treatments are operated at RF power of 50 to 25 watts. The processed HOSP low-k films are analyzed by Fourier transform infrared spectroscopy (FTIR) for the intensity changes of the main knot junction peaks, especially Si-CH3 (127〇cnfl), and reticulated Si—〇 (104) cm.

—I V )及籠狀Si-〇 (1130 cm-1)伸縮振盪波,以便鑑定這些電漿處理對薄 膜鍵、、、。的〜f ’ 透過金屬-絕緣—半導體(Me^ai—insuiat〇r—gemic〇n(juct〇r, · MIS)電谷結構元件之電容—電壓(c_v)及電流-電壓(丨—v)量測可以分別 得知電漿處理對低k材料之介電常數及絕緣性所造成的影響;另外,分別以 同乂幸田射光源對HOSP進行X光近緣結構(Near-edge Structure)能譜分析, 汗估電製處理對HOSP薄膜所造成之表面鍵結轉變;二次離子質譜縱深輪廓 (SIMS-depth Profile)則用以分析銅在各種「si/HOSP/Cu」熱處理(300 C、1小時)試片之擴散行為,藉此可評估〇2、H2、仏與仏爪電漿處理後之H〇sp 薄膜對銅的擴散阻礙性質。 1240967 圖-為(a)剛固化與經過(b) Η”(c) 〇2與⑷N2電漿處理後之H〇sp 低k薄膜之FTIR圖譜;這些電襞處理均為1〇〇w/9分鐘,所冑的圖譜均包含網 狀Si-〇與籠狀si-〇以及si-弧三個主要的鍵結波峰,與兩支較微弱之Si_H (2240 cm—1)與c-h (2970 cnfl)波峰;比較圖譜(a)與得知:經 H2電漿處理後之h〇sp低k薄膜的網狀、籠狀Si—〇鍵結的波峰位置與強度均產 生顯著的變化,同時其Si-CH3與Si-H鍵結強度也明顯的降低,這些結果顯示 H0SP低k薄膜會遭受到H3H2電漿相當程度的破壞,⑶與扭電漿處理後之H〇sp 呈現相似的鍵結轉變圖譜,分別如圖一中(b)、(c)所示;這個結果顯肇 示H2電漿具有與〇2電漿類似之破壞效應,可導H的斷鍵,形成 Si懸宕鍵結,這些Si懸宕鍵結會再與其它的^_0形成Si-〇網狀鍵結結構, 因此’ H2電漿處理後之H0SP薄膜的籠狀Si-Ο減少,網狀Si-〇增加;比較圖一 中(a)與(d)得知:N2電漿處理只造成Si-CH3波峰強度的輕微下降,而網 狀與籠狀Si-0波峰的相對強度幾無變化,暗示沁電漿僅能導致少數si-CH3的 斷鍵,卻不易促成籠狀Si-0轉換為網狀Si-0 ;因此,N2電漿對H0SP低k薄膜 之鍵結轉換行為較H2、〇2電漿有明顯之不同。 着 圖二(a)及圖二(b)顯示經過H2、N2與數種比例之N2/H2混合氣氛 (20%N2-8〇m至80跳-20細2)之電漿Si-Ο波峰總強度的比值(Iw)與籠 -狀Si-0對網狀Si-Ο的波峰強度比值(IN/C);實心圓點均是以相同且相當高 - 之能量(100W/9分鐘)的電漿處理後所獲得的結果,其餘的實驗數據點則 是降低電漿功率或能量的結果。圖二乃說明電漿氣氛的改變會衍生截然不 同的鍵結轉變現象,100W/9分鐘之H2電漿處理不但會破壞薄膜之CH3側鏈, 11 1240967—I V) and cage-shaped Si-〇 (1130 cm-1) stretching oscillatory waves in order to identify these plasma treatments for thin-film bonds. ~ F 'through the metal-insulation-semiconductor (Me ^ ai-insuiat〇r-gemic ON (juct〇r, · MIS) capacitance-voltage (c_v) and current-voltage (丨 -v) The measurement can be used to know the influence of plasma treatment on the dielectric constant and insulation of low-k materials. In addition, the X-ray near-edge structure energy spectrum of HOSP was performed by the same source Koda light source. Analysis, Khan estimates the surface bonding transformation caused by electrical processing to HOSP film; the secondary ion mass spectrometry depth profile (SIMS-depth Profile) is used to analyze copper in various "si / HOSP / Cu" heat treatment (300 C, 1 Hours) The diffusion behavior of the test piece can be used to evaluate the diffusive barrier properties of copper to the copper oxide film treated with 〇2, H2, hafnium, and cymbal claw. 1240967 Picture-(a) Just cured ) Η "(c) FTIR spectra of H0sp low-k films after plasma treatment with 〇2 and ⑷N2; these treatments are all 100w / 9 minutes, and all of the pictures include reticulated Si-〇 Three major bond peaks with cage-like si-〇 and si-arc, and two weaker Si_H (2240 cm-1) and ch (2970 cnfl) The comparison of the spectrum (a) with that of the peak position and intensity of the network-shaped and cage-shaped Si—0 bonds of the h0sp low-k film after H2 plasma treatment shows that the Si- The bonding strength of CH3 and Si-H is also significantly reduced. These results show that the H0SP low-k film will suffer considerable damage from the H3H2 plasma, and ⑶ and Hsp with a torsional plasma treatment show similar bond transition patterns. These results are shown in (b) and (c) of Figure 1, respectively. This result shows that the H2 plasma has a similar destructive effect as the 02 plasma, which can lead to the breakage of H to form Si suspension bonds. These Si The dangling bond will form another Si-〇 network structure with other ^ _0, so the cage Si-O of H0SP film after H 2 plasma treatment is reduced, and the network Si-〇 is increased; (A) and (d) It was learned that the N2 plasma treatment only caused a slight decrease in the intensity of the Si-CH3 peak, while the relative intensity of the mesh-like and cage-shaped Si-0 peaks had little change, suggesting that the Qin plasma could only cause a few si-CH3's bond breaking, but it is not easy to promote the conversion of cage Si-0 to network Si-0; therefore, the bonding conversion behavior of N2 plasma to H0SP low-k film is better than that of H2 and 〇. 2 Plasma has obvious differences. Figures 2 (a) and 2 (b) show that after H2, N2 and several ratios of N2 / H2 mixed atmosphere (20% N2-8m to 80 hops -20 fine 2 ) Of plasma Si-O peak intensity ratio (Iw) and cage-shaped Si-0 to the peak intensity ratio of network Si-O (IN / C); solid dots are the same and quite high- Energy (100W / 9 minutes) after plasma treatment results, the remaining experimental data points are the results of reducing plasma power or energy. Figure 2 illustrates that changes in the plasma atmosphere will result in very different bonding transitions. The 100 W / 9 minute H2 plasma treatment will not only destroy the CH3 side chain of the film, 11 1240967

而且也會將大量的籠狀Si - 〇 所示。這些籠狀Si-〇、si-C ,但是逐漸的升高N2添加 而導致Isi-c/si-。衰退達〜25%,如圖二(a)所示,而且 轉變為網狀Si-Ο,使IN/C增加〜50%,如圖二(b)所示 低偏極化鍵結之減弱均不利於H0SP的低k常數特性, 氣體之流纽柯雜地碰Si_⑽破軸_餘綱紐奴轉變,尤 其當N2大於60%時,Si-Ο與Si-C的破壞迅速趨於緩慢Also, a large amount of cage-shaped Si-〇 will be shown. These cage-like Si-O, si-C, but gradually increased N2 addition caused Isi-c / si-. The decline is ~ 25%, as shown in Figure 2 (a), and it is transformed into mesh Si-0, which increases IN / C by ~ 50%. As shown in Figure 2 (b), the weakening of the low-polarization bond is even. It is not conducive to the low-k constant characteristics of H0SP. The flow of gas Nucor mixed with Si_⑽ broken axis _ Yu Gangnuo transition, especially when N2 is greater than 60%, the destruction of Si-O and Si-C quickly becomes slow.

尤其是圆2-2〇%也配合爾/6分鐘電漿處理可以達到最佳化的效果以達到籲 抑制〇2電漿對鍵結的破壞鈍化。(如後敘,此種最佳化電漿處理亦可衍生良In particular, a circle of 2-20% can also be combined with a 6 minute plasma treatment to achieve the optimal effect to achieve the suppression of the passivation of the bond destruction by the 02 plasma. (As described later, this optimized plasma treatment can also be a good idea.

擴散之功能。) 為了說明離子氮化的鈍化效果,創作本發明利用60、80和100%三種高 氮含量之電漿對H0SP低k薄膜進行50W/6分鐘之電漿純化處理,然後再對其 進行強烈之氧電漿(150W/5分鐘)”攻擊”,而後aFTIR分析IsMysi_。與丨㈣比 值的變化,其結果示於圖三,顯然的,剛固化的H〇sp薄膜一旦暴露在氧電讀 漿環境後,其鍵結即遭受嚴重的損傷(與圖一的結果一致);利用1〇〇0/〇N2 或者60%N2-40%H2的電漿處理仍不足以保護h〇SP以對抗氧電漿的攻擊。因-此,這些薄膜仍會遭受氧電漿的破壞,且導致^^。之顯著下降,如圖三(a) 所示,與In/c的上升,如圖三(b)所示;然而,當N2/H2調配至80%-20%的比 例時,經此電漿氮化後之低k薄膜則能抵抗氧電漿的後續攻擊,並維持與剛 固化薄膜相當之ISi-C/Si-。與IΝ/C比值。 12 1240967 表2為顯示H0SP低k薄膜經過〇2(150W/5分鐘)、N2/H2(50W/6分鐘)、 或N2/H2 (50W/6分鐘)立即加上〇2 (150W/5分鐘)、亦或N2/H2 (100W/3分鐘) 立即加上〇2 (150W/5分鐘)電漿處理後之FTIR強度比值(ISi-c/Si_。與ιΝ/〇與介 電常數之數據。N2/%混合氣氛均為最佳化比值:80%-20%。剛固化之H0SP薄 膜之Isi-c/si-o與In/c均量化並定義為1·〇〇,而經C-V量測後所獲得之介電常數為 2.5 ’再經〇2電漿處理後’其ISi-c/SH)僅剩〇·74 (亦即Si-C鍵結大幅衰退); In/c卻大幅上升至2· 03 ;這些結果顯示〇2電漿會產生以下的破壞效應:促成 籠狀Si-Ο轉變為網狀Si-Ο,導致Iswysi-o之大幅上升;破壞Si-CH3之側鏈,造 成Isi-c/si-o之衰退;最終導致H0SP之介電常數由2. 50上升至3. 20,但是,經過 最佳化比率(80%N2-20%¾)、最佳條件(50W/6分鐘)之電漿處理以後,該 試片之Isi-c/SM)與Ιν/c與剛固化之H0SP薄膜試片相當,且其介電常數並未升 高,仍維持在2. 50,而且,此離子氮化試片再經過〇2電漿攻擊以後,亦能維 持穩定的鍵結與良好的低Ji特性(k = 2· 51);然而,若改變電漿功率與處 理時間使之偏離最佳化條件時,縱使經過相同輸入能量(例如:100W/3分 鐘)之離子氮化後,該試片並無法有效地抵抗〇2電漿之侵害,致使ISi-d〇、 In/c與介電常數仍與原始值有甚大差距(如表2所示)。 13 1240967 表2剛固化與各種電漿處理後之H0SP薄膜之FTIR鍵結定量數據 (Isi-C/Si-0、In/C )與介電常數 试片條件 鍵結數據/介電常數 丄 Si - C/Si - 0 In/c k 剛固化 1.00 1.00 2.50 02 (150W/5 分) 0.74 2.03 3.20 N2/H2 (50W/6 分) 0.96 1.17 2.50 N2/H2 (50W/6 分)+〇2 0.99 1.20 2.51 N2/H2 (100W/3 分)+〇2 0.84 1.36 2.70 圖四為為幾種鋼閘(Cu-gate) MIS電容元件之漏電流對應電場強度曲 線,計使用(a)剛固化、(b) 〇2、(c) N2 (50W/6分鐘)再經〇2、⑷ 80跳-20°惠(50W/6分)再經〇2電聚與(e) 8〇m-2〇m (i〇〇w/3分鐘)再經 〇2電漿處理過的H0SP低k薄膜作為介電層,〇2電漿處理均為ι_/5分鐘;曲 線(a)與(b)顯示:〇2電漿處理H0SP介電層之MIS元件的漏電流值較使用 剛固化之H0SP介電層的MIS元件約提高兩個級數,而介電常數亦由2.5〇上升 至3.20 (如表2所示)。這些數據證實&電漿會嚴重地改變H〇sp薄膜之鍵結 而減知其低k與電性絕緣特徵。H2與N2兩種單一氣氛電聚不但均會造成jjQsp 薄膜之鍵結破壞(如表2所示),而且無法對其產生有效的鈍化效果,故漏 電流值提高約一個級數,如圖四中曲線(c)所示。適當的沁/沁電漿處理 (50W/6分鐘)幾乎不會影響到低k薄膜之特徵鍵結,且會產生表面鈍化效 果,使再經過〇2電漿攻擊之H0SP薄膜仍能維持與剛固化者相當大小之低k數 值一其k值仍為2. 5 ’而漏電流則接近於剛固化試片,請比較圖四中曲線(a) 14 1240967 與⑷,然而,若功率/能量輪入不當(例如:1〇〇w/3分鐘),他愚混合 電漿也無法產纽好之舰性,故祕絲攻擊後之此種脇元件也顯現嚴 重的漏電流上升,如圖四中曲線(e)。 以上的FTIR與I-V、介電常數綜合分析言正實··唯有最佳化之離子氮化處 理(ΝΛ = 80%/20%、50W/6分鐘)方可生成有效的鈍化效果。同步輻射χ 光吸收近緣結構分析顯示:這些效果之產生歸因於H〇sp薄膜表面所形成之 氮/碳化物鈍化層。The function of diffusion. ) In order to illustrate the passivation effect of ion nitridation, the invention uses 60, 80, and 100% three high nitrogen content plasmas to perform a plasma purification treatment of H0SP low-k films for 50W / 6 minutes, and then strongly Oxygen plasma (150W / 5min) "attacks" and aFTIR analyzes IsMysi_. The change in the ratio with ㈣ is shown in Figure 3. Obviously, once the newly cured Hosp film is exposed to the oxygen electro-paste environment, its bond will be severely damaged (in accordance with the results in Figure 1). ; Plasma treatment with 10000 / 〇N2 or 60% N2-40% H2 is still not enough to protect HOSP against oxygen plasma attack. Therefore, these films will still be damaged by the oxygen plasma and cause ^^. The significant decrease is shown in Figure 3 (a), and the rise of In / c is shown in Figure 3 (b); however, when N2 / H2 is adjusted to a ratio of 80% -20%, the plasma The low-k film after nitriding can resist the subsequent attack of the oxygen plasma, and maintain the ISi-C / Si- equivalent to the just-cured film. And IN / C ratio. 12 1240967 Table 2 shows the H0SP low-k film immediately after 〇2 (150W / 5 minutes), N2 / H2 (50W / 6 minutes), or N2 / H2 (50W / 6 minutes) plus 〇2 (150W / 5 minutes ), Or N2 / H2 (100W / 3 minutes) Immediately add the FTIR intensity ratio (ISi-c / Si_.) And ιN / 〇 and dielectric constant data after plasma treatment of 〇2 (150W / 5 minutes). N2 /% mixed atmosphere are optimized ratio: 80% -20%. Isi-c / si-o and In / c of newly cured H0SP film are both quantified and defined as 1.0 ×, and measured by CV The obtained dielectric constant is 2.5 'after the plasmon treatment of 02', and its ISi-c / SH) is only 0.74 (that is, the Si-C bond decays sharply); In / c rises sharply to 2.03; These results show that the 02 plasma will have the following destructive effects: promote the transformation of cage-shaped Si-O to reticulated Si-O, leading to a sharp rise in Iswysi-o; destroying the side chain of Si-CH3, causing Isi -c / si-o decline; eventually the dielectric constant of H0SP rises from 2.50 to 3.20, but after the optimization ratio (80% N2-20% ¾), the optimal conditions (50W / 6 Minutes) after plasma treatment, Isi-c / SM) and Ιν / c of the test piece and H0SP just cured The test piece is equivalent, and its dielectric constant has not increased, and remains at 2.50. Moreover, the ion-nitrided test piece can also maintain stable bonding and a good low Ji after a 02 plasma attack. Characteristics (k = 2.51); however, if the plasma power and processing time are changed to deviate from the optimal conditions, even after the ion nitriding of the same input energy (for example: 100W / 3 minutes), the test piece It can't effectively resist the invasion of 02 plasma, so ISi-d0, In / c and dielectric constant are still far from the original value (as shown in Table 2). 13 1240967 Table 2 Quantitative FTIR bonding data (Isi-C / Si-0, In / C) and dielectric constant test condition bonding data / dielectric constant 丄 Si of H0SP film after curing and various plasma treatments -C / Si-0 In / ck Just cured 1.00 1.00 2.50 02 (150W / 5 points) 0.74 2.03 3.20 N2 / H2 (50W / 6 points) 0.96 1.17 2.50 N2 / H2 (50W / 6 points) + 〇2 0.99 1.20 2.51 N2 / H2 (100W / 3 points) + 〇2 0.84 1.36 2.70 Figure 4 is the electric field intensity curve of the leakage current of several types of Cu-gate MIS capacitors. ) 〇2, (c) N2 (50W / 6 minutes) and then go through 〇2, ⑷ 80 jump -20 ° Hui (50W / 6 minutes) and then through 〇2 electropolymerization and (e) 80m-20m ( 〇〇w / 3minutes) H0SP low-k thin film treated with 〇2 plasma as dielectric layer, 〇2 plasma treatment is ι_ / 5 minutes; curves (a) and (b) show: 〇2 The leakage current value of the MIS device treated with the H0SP dielectric layer by plasma treatment is about two stages higher than that of the MIS device using the newly cured H0SP dielectric layer, and the dielectric constant has also increased from 2.50 to 3.20 (as shown in Table 2). ). These data confirm that & Plasma severely alters the bonding of Hosp films and degrades their low-k and electrical insulation characteristics. H2 and N2 electropolymerization in two single atmospheres will not only cause bond damage to the jjQsp film (as shown in Table 2), but also fail to produce an effective passivation effect, so the leakage current value is increased by about one order, as shown in Figure 4. The middle curve (c) is shown. Appropriate Qin / Qin plasma treatment (50W / 6 minutes) will hardly affect the characteristic bonding of low-k films, and will produce a surface passivation effect, so that the H0SP film that has been attacked by 0 2 plasma can still be maintained and rigid. The low-k value of the size of the solidifier-its k value is still 2.5 'and the leakage current is close to that of the solidified test piece. Please compare the curve (a) 14 1240967 and ⑷ in Figure 4. However, if the power / energy wheel If it is improperly inserted (for example: 100w / 3 minutes), the hybrid plasma can not produce good ship performance. Therefore, such threat elements also show a serious leakage current increase after the mystery wire attack, as shown in Figure 4. Curve (e). The above comprehensive analysis of FTIR, I-V, and dielectric constant is true ... Only an optimized ion nitriding treatment (NΛ = 80% / 20%, 50W / 6 minutes) can produce an effective passivation effect. Synchrotron radiation χ light absorption near-structure analysis shows that these effects are attributed to the nitrogen / carbide passivation layer formed on the surface of the Hosp film.

圖五(a)為N之吸收能譜(〜396至414eV);圖五⑻則為C之吸收能 譜(280至310eV);經NVH2電漿處理後之H0SP薄膜會明顯的在〜4〇〇eV附近 產生N的特徵吸收峰(主波峰位於4〇7eV,次波峰位於402. 5eV);但是,N 的特徵吸收峰並不存在於剛固化的H0SP試片;此結果証實:N2/H2混合電漿 表面鈍化改質會使HOSP薄膜形成氮化物表面層;另外,圖五(b)之吸收能 譜顯示:剛固化HOSP試片會因為其本身之Si-CH3側鏈而呈現C-H、Si-C兩個 特徵吸收峰(波峰分別位於288· leV、288· 9eV)。【註:X光吸收能譜分析 言正實熱氧化之Si〇2薄膜並不具有c-Η與Si-C吸收峰但卻具有與HOSP試片相同 的C-C (293· OeV)、C=C (π鍵與σ鍵分別位於284. 8、〜296. 5eV)吸收峰, 故我們判定圖五(b)之C-C、C=C吸收峰主要是真空環境殘留碳素所導致。】 但是經過50W/4分鐘之短時間鈍化處理以後,其〇Η、Si-C逐漸寬化並向高 能量偏移。隨著處理時間進一步的增長,C-Η波峰會更為顯著的減弱、寬化、 並向更高能量偏移,最後經10分鐘之鈍化處理以後,H0SP之C_H、Si-C鐽結 波峰幾乎被新衍生出之C-N鍵結(峰值289. 2eV)所取代。綜合這些高解析X 15 1240967 光吸收能譜分析證實:N2/H2混合電漿表面鈍化改質處理最終可誘發Figure 5 (a) shows the absorption energy spectrum of N (~ 396 to 414eV); Figure 5⑻ shows the absorption energy spectrum of C (280 to 310eV); the H0SP film after NVH2 plasma treatment will obviously be ~ 4. A characteristic absorption peak of N is generated near 〇eV (the main peak is located at 407eV and the secondary peak is at 402.5eV); however, the characteristic absorption peak of N does not exist in the newly cured HOSP test strip; this result confirms: N2 / H2 The passivation and modification of the mixed plasma surface will cause the HOSP film to form a nitride surface layer. In addition, the absorption energy spectrum in Figure 5 (b) shows that the newly cured HOSP test piece will show CH and Si because of its Si-CH3 side chain. -C Two characteristic absorption peaks (peaks at 288 · leV and 288 · 9eV, respectively). [Note: X-ray absorption energy spectrum analysis indicates that the positive thermally oxidized Si0 2 film does not have c- 具有 and Si-C absorption peaks but has the same CC (293 · OeV) and C = C ( The π bond and the σ bond are located at 284.8, ~ 296. 5eV) absorption peaks respectively, so we judge that the absorption peaks of CC and C = C in Fig. 5 (b) are mainly caused by residual carbon in the vacuum environment. ] However, after a short passivation treatment of 50W / 4 minutes, the 〇Η, Si-C gradually widened and shifted to high energy. With the further increase of the processing time, the C- 峰 peak will be more significantly weakened, broadened, and shifted to higher energy. After the 10-minute passivation treatment, the C_H and Si-C 鐽 junction peaks of H0SP are almost Replaced by newly derived CN bond (peak 289.2eV). Comprehensive analysis of these high-resolution X 15 1240967 light absorption spectroscopy analysis confirmed that: N2 / H2 mixed plasma surface passivation and modification treatment can eventually induce

Si-N/Si-C-N鈍化層的生成,這些表面氮化層具有保護H〇Sp薄膜之功能; SIMS氮縱深分佈分析顯示離子氮化後之H〇sp薄膜存在一含氮表面層,視離 子氮化處理之時間長短,其厚度界於10至3〇 nm。 圖六為顯示三種不同的Cu/HOSP/Si試片經300°C,氮氣氣氛退火一小時 以後的二次離子質譜(SIMS)縱深分佈;這些試片分別使用(a)剛固化、 (b) 〇2與(c) 8〇m-2〇m電漿處理後的H0SP低k薄膜,且在SIMS分析前先 以硝酸水溶液去除表層上之銅膜,以增加解析度;試片經過退火處理後,· 銅會顯著的擴散進入剛固化之H0SP低k薄膜中,並累積於H0SP/Si之界面 處’如圖六中曲線(a)所示;如圖六中曲線(b)所示,經過〇2電漿處理以 後的H0SP薄膜會嚴重地喪失阻絕效果,因此,jjosp薄膜内部以及jj〇sp/Si之 界面均會累積最強烈之銅訊號(約為剛沈積H〇sp試片的1〇倍);此外,銅 原子亦會貫穿過H〇SP/Si界面,並深入矽基材内部,這些嚴重的銅擴散乃起 因於〇2電漿對H0SP薄膜所造成之鍵結破壞,並且是導致漏電流大幅上升的主 因;然而,經過離子氮化(8〇m-20%¾電聚)處理後,圖如六中曲線(c) φ 所示,除了近表面區域有銅的存在以外,H〇sp薄膜内層部分具有最低之銅 訊號(幾乎與背景訊號相當),且H0SP/Si界面並沒有銅的累積、Si内部亦 無鋼的存在,亦即N2/H2混合電漿表面鈍化改質製程亦具有抑制銅擴散之附. 加功能。 經由以上的實施例可知,本發明所提出的低k薄膜之私/112混合電浆表面 鈍化改質處理,可以在典型矽氧烷基低k薄膜表面形成Si_c_N/Si_N等含氮 1240967 之鈍化層,達到保護低k薄膜之功效,此鈍化層的存在可防止典型魏烧基 低k薄膜之鍵結破壞、介電常數及_流的嚴重上升,並可兼具阻礙銅原子 擴散的能力。ϋ此,這種製程所”現場”製作之超薄鈍化層將可取代高電阻 之離沈積TaN、TiN”異質”擴散阻礙層與高介電性之Si—c#覆蓋層,可適 用在未來的微電子奈米1C元件。 上列詳細說明係針對本發明之一可行實施例之具體說明,惟該實施例 並非用以_本發明之專繼圍,凡未麟本個技频神所為之等效實 施或變更,均應包含於本案之專利範圍中。 綜上所述,本案在低k薄膜之仏/沁混合電漿表面鈍化改質處理乃屬首先 創作者,不但在技術思想上確屬創新,並能較習用物品增進上述多項功效, 應已充分符合新穎性及進步性之法定發明專利要件,爰依法提出申請,懇 請貴局核准本件發明專利申請案,以勵發明,至感德便。 【參考文獻】 1. T. C. Chang, P. T. Liu, Y. J. Mei, Y. S. Mor, T H. Perng, Y. L.The formation of Si-N / Si-CN passivation layers. These surface nitride layers have the function of protecting HOSp thin films. SIMS nitrogen depth distribution analysis shows that there is a nitrogen-containing surface layer in HOsp thin films after ion nitridation. The length of the nitriding process ranges from 10 to 30 nm. Figure 6 shows the secondary ion mass spectrometry (SIMS) depth distribution of three different Cu / HOSP / Si test specimens after annealing at 300 ° C in a nitrogen atmosphere for one hour; these test specimens were (a) just cured, (b) 〇2 and (c) H0SP low-k film after plasma treatment of 80-200m, and remove the copper film on the surface layer with nitric acid aqueous solution before SIMS analysis to increase the resolution; the test piece is annealed Copper will significantly diffuse into the newly cured H0SP low-k film and accumulate at the H0SP / Si interface 'as shown in curve (a) in Figure 6; as shown in curve (b) in Figure 6, after 〇2 The HOSP film after plasma treatment will seriously lose the barrier effect. Therefore, the strongest copper signal will be accumulated inside the jjosp film and the jj〇sp / Si interface (approximately 1 of the newly deposited HOsp test piece). Times); In addition, copper atoms will also pass through the H0SP / Si interface and penetrate into the silicon substrate. These severe copper diffusions are caused by the bond damage caused by the 02 plasma to the H0SP film, and it is the cause The main reason for the large increase in leakage current; however, after ion nitriding (80m-20% ¾electropolymerization) treatment As shown in the curve (c) φ of the Sixth Middle School, except for the presence of copper in the near surface area, the inner layer of the H0sp film has the lowest copper signal (almost equivalent to the background signal), and there is no copper at the H0SP / Si interface. Accumulation, there is no steel in Si, that is, N2 / H2 mixed plasma surface passivation and modification process also has the function of suppressing copper diffusion. According to the above examples, it can be known that the passivation and modification treatment of the surface of the low-k thin film / 112 mixed plasma of the present invention can form a passivation layer containing nitrogen 1240967, such as Si_c_N / Si_N, on the surface of a typical siloxane low-k film. To achieve the effect of protecting the low-k film, the existence of this passivation layer can prevent the bond damage, the dielectric constant and the current of the typical Wei-based low-k film from rising seriously, and can also have the ability to hinder the diffusion of copper atoms. Therefore, the ultra-thin passivation layer produced on-site by this kind of process will replace the high-resistance ion-deposition TaN and TiN “heterogeneous” diffusion barrier layer and high-dielectric Si—c # cover layer, which can be applied in the future. Microelectronics Nano 1C element. The above detailed description is a specific description of one of the feasible embodiments of the present invention, but this embodiment is not intended to be the exclusive continuation of the present invention. Any equivalent implementation or change made by Wei Lin in this technical frequency should be It is included in the patent scope of this case. To sum up, this case is the first creator to passivate and modify the surface of the low-k thin film 仏 / Qin hybrid plasma. Not only is it technically innovative, but it can also enhance the above-mentioned multiple effects over conventional items. It should be sufficient The statutory invention patent elements that meet the novelty and progressiveness, apply in accordance with the law, and kindly ask your office to approve this invention patent application, in order to stimulate the invention, to the greatest extent. [References] 1. T. C. Chang, P. T. Liu, Y. J. Mei, Y. S. Mor, T H. Perng, Y. L.

Yang, and S. M. Sze, J. Vac. Sci. Technol. B, 17, 2325 (1999). 2. J. J. Kim, Η. H. Park, and S. H. Hyun, Thin Solid Films, 377-378, 525 (2000). 3. J. M. Shi eh, K. C. Tsai, B. T. Dai, S. C. Lee, C. H. Ying, and Y. K. Fang, J. Electrochem. Soc·, 149,G384 (2002)· 4. M. Du. R. L. Opial, V. M. Donnelly, J. Sappjeta, and T. Boone, J.Yang, and SM Sze, J. Vac. Sci. Technol. B, 17, 2325 (1999). 2. JJ Kim, Η. H. Park, and SH Hyun, Thin Solid Films, 377-378, 525 (2000) 3. JM Shi eh, KC Tsai, BT Dai, SC Lee, CH Ying, and YK Fang, J. Electrochem. Soc ·, 149, G384 (2002) · 4. M. Du. RL Opial, VM Donnelly, J . Sappjeta, and T. Boone, J.

Appl· Phys.,85,1496 (1999). 17 1240967 5. S. H. Yang, H. Kim, and J. W. Park, Jpn. J. Appl. Phys., 40, 5990 (2001). 6. S. T. Chen, G. S. Chen, T. J. Yang, T. C. Chang, and W. H. Yang, Electrochem. Solid State-State Lett., 6, F4 (2003).Appl. Phys., 85, 1496 (1999). 17 1240967 5. SH Yang, H. Kim, and JW Park, Jpn. J. Appl. Phys., 40, 5990 (2001). 6. ST Chen, GS Chen , TJ Yang, TC Chang, and WH Yang, Electrochem. Solid State-State Lett., 6, F4 (2003).

18 1240967 【圖式簡單說明】 圖一為(a)剛固化與經過(b) H2電漿、(c) 〇2電漿與(d) N2電漿處 理後之H0SP低k薄膜之傳利葉轉換紅外線光譜儀(FTIR)圖譜; 圖二(a)及圖二(b)為經過不同輸入功率與各種混合比率之沁/出電 漿處理後之H0SP低k薄膜的FTIR圖譜解析結果··(a) IsKysi•。與(b) In/c ;原 始試片之Isi-C/Si-0與In/c皆定義為正常化數值1 ; 圖三(a)及圖三(b)為剛固化與經過各種比率之仏/迅混合氣氛電漿 處理後,再經〇2電漿攻擊之H0SP低k薄膜的(a) 1_卜。與(b) In/c ; 圖四為使用不同的H0SP低k薄膜之MIS電容元件之漏電流對應電場強度 曲線;其中H0SP低k薄膜包含(a)剛固化、(b)〇2電漿、(c)N2電漿(5〇w/6 分鐘)再加上〇2電漿、⑷最佳化n2/H2電裝(50W/6分鐘)再加上〇2電聚與 (e) N2/H2電漿(100W/3分鐘)再加上〇2電衆; 圖五幾種H0SP低k薄膜之(a)氮與⑻碳同步輻射乂光吸收近緣結構 能譜; 圖六為銅膜沈積於數種不同電漿處理之H〇sp薄膜並再經高溫熱處理後 所獲得之二摘離子縱深分佈絲;其帽職㈣膜分別為經⑷剛固 化、(b) 〇2電漿與(c)最佳化仏/沁電漿處理。 【主要元件符號說明】 益 1918 1240967 [Schematic description] Figure 1 shows the passivation leaves of the H0SP low-k film after (a) curing and (b) H2 plasma, (c) 〇2 plasma and (d) N2 plasma treatment. Transformed infrared spectrometer (FTIR) spectrum; Figure 2 (a) and Figure 2 (b) are the FTIR spectrum analysis results of H0SP low-k film after Qin / plasma treatment with different input power and various mixing ratios ... (a ) IsKysi •. And (b) In / c; Isi-C / Si-0 and In / c of the original test strip are both defined as normalized values 1; Figures 3 (a) and 3 (b) are the ratios of just cured and passed through various ratios. (A) 1_b of H0SP low-k film after plasma treatment in a krypton / fast mixed atmosphere, and then attacked by 02 plasma. And (b) In / c; Figure 4 is the electric field intensity curve of the leakage current of MIS capacitors using different H0SP low-k films; where H0SP low-k films include (a) just cured, (b) 〇2 plasma, (C) N2 plasma (50w / 6 minutes) plus 〇2 plasma, ⑷optimized n2 / H2 Denso (50W / 6 minutes) plus 〇2electropolymerization and (e) N2 / H2 plasma (100W / 3 minutes) plus O2 electric mass; Figure 5 (a) Nitrogen and ytterbium carbon synchrotron radiation ray photon absorption structure energy spectrum of several H0SP low-k films; Figure 6 is copper film deposition The two ion-extracting ion depth distribution filaments obtained after several plasma treatments of H0sp films and further high temperature heat treatment; the cap film is hardened, (b) 〇2 plasma and (c ) Optimized 仏 / Qin plasma treatment. [Description of main component symbols] Yi 19

Claims (1)

1240967 - 、 【申請專利範圍】 i. 一種低介電常㈣獻賴表面鈍化改質處理枝,係在對 石夕氧烧低介電常數(k)細進行表面聽改質處理,其方式是將此 薄膜試片置於反應腔體後,導入氣體比率為8〇%仏_2〇%112之仏/112混合氣 體’並利用射頻供應器來產生離子化電漿,以此N2/H2混合電漿對低k 薄膜試片進行電漿表面鈍化改質處理;經以8_2-2娜2配合約50W/6 分鐘最佳化條件之改質處理後,薄膜試片表面可形成&㈢與义N混合鍵 結純化層。1240967-, [Scope of patent application] i. A kind of low dielectric constant relies on surface passivation and modification treatment branch, which is based on surface acoustic modification treatment of low dielectric constant (k) of Shixi oxygen firing. The method is: After placing the thin film test piece in the reaction chamber, a mixed gas of 仏 / 112 with a gas ratio of 80% 仏 2〇% 112 was introduced, and an RF plasma was used to generate an ionized plasma, and the mixture was N2 / H2. Plasma surface passivation and modification treatment of low-k film thin film; after modification treatment with 8_2-2na 2 and about 50W / 6 minutes optimization conditions, the surface of the thin film test piece can be formed & Sense N mixed bond purification layer.
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