TWI317539B - End point detection in time division multiplexed etch process - Google Patents

End point detection in time division multiplexed etch process Download PDF

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TWI317539B
TWI317539B TW93102381A TW93102381A TWI317539B TW I317539 B TWI317539 B TW I317539B TW 93102381 A TW93102381 A TW 93102381A TW 93102381 A TW93102381 A TW 93102381A TW I317539 B TWI317539 B TW I317539B
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plasma
monitoring
frequency
etching
steps
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TW93102381A
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TW200416875A (en
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David J Johnson
Russell Westerman
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Unaxis Usa Inc
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1317539 玖、發明說明: 【發明所屬之技術領域】 本發明係概括關於半導體製造之領域。更為特別而言 ,本發明係針對偵測一個分時多 夕 division _1 tiplexed)蝕刻及沉積製程的終點之一種改良方法。 相關申請案之交互參照 此申請案係關於西元2003年2月U s路植山 丁匕月日所提出之共同 擁有的美國臨時專利申請案序號6〇/447, 594且主 權,標題為:分時多工的蝕刻製程中 良 衣狂γ &終點偵測,此件臨 時專利申請案係以參照方式而納入本文。 【先前技術】 於諸多的_s裝置之生產期間’需要蝕刻—層的材料 以完成停止於下方之層(例如:絕緣體上石夕晶片(s〇i si 1 iC〇n-〇n-insulator),即:清除其停止於一下面的二氧 化石夕層之KSi)層)。允許敍刻製程為進行超過當第一層 已經移除之時間係將造成下面的停止層之減小的厚度、或 -特徵輪廓(profUe)降級(針_ s〇I應用係於此技藝所習 稱為“切口(notching)”)。 普遍運用以偵測電毁製程終止時間之一種方法係光學 〇ptical emission spectrometry) 〇 0ES係分析由一電渡源所放射的光,以引出其關於電毁製 程的化學與物理狀態之影響。於半導體處理中,此技術係 普遍運用以積測於電激餘刻製程期間之材料介面。一 之專題論Π於電漿處理之光學精技術,,係提出—優 !317539 越的評論於電漿放射光譜技術之原理與應用。 OES技術係涉及監視由電漿所放射的輻射,通常為於 光譜之uv/m⑽⑽至11GGnm)部分。第1圖係顯示 -種典型的GES架構之示意圖。電襞之組成(且尤指存在反 應蝕刻物種或蝕刻副產物)係由所放射的輻射之光譜(即:強 度對波長)所決定。於一蝕刻製程之進行期間(且特別是於 一材料轉變(transition)),電襞之組成係改變,且造成於 放射光譜之一變化。藉著連續監視電漿放射,一 〇es終點 系統係可能偵測於放射光譜之一變化,且運用其以決定該 薄膜為何時已經完全清除。實行上,關於終點之大部分的 資訊係通常為含有於少許的波長之内,該些波長係對應於 餘刻期間所消耗的反應物或是所產生的蝕刻副產物。 欲發展一 OES終點策略之一種常用的方法係收集於終 點前及終點後的條件期間内之電漿放射的多個光譜。此等 光議係可運用以辨識針對該製程之候選的波長區域。候選 區域係含有其隨著製程達到於二個有關材料之間的轉變而 顯示顯著的強度變化之波長。終點波長候選區域係可運用 多種方法而決定。用於終點偵測之光譜區域係可透過統計 方法而選取,諸如:因數分析或主要分量分析(參閱:授與 Angell等人之美國專利苐5,658,423號)。欲決定終點候 選者之另一種策略係透過介於終點前(主要蚀刻)與終點後( 過度蝕刻)的光譜之間的一差異繪圖之構成。—旦諸個候 選區域為已經選定,類似的化學物種之指定係可針對諸個 候選區域而作成(即:來自游離的氣體前導者之反應物的物 1317539 種、或姓刻產物)。句杯7 盘Pe瓶等人的的“光譜線之圖表” '、 寻的刀子光譜之辨識,,之多個參考文獻、關 連於製程化學物的知識係 馱關 之類似的物種辨識者。針斜 产 ^Uine; ^ 子於一個八虱化硫(SF6)電漿之一 石夕(Si)姓刻製程的類似終 687…〇3nm之氟(F:選者之—個實例係將為於 及於440 nm之氟化矽(SiF) 放射帶(band)。一旦此等區域 次為已,決疋,後續部分者係 可運用相同的OES策略而處理。 儘管此等OES方式係相當適用於單步祿之製程或是具 -有限數目之離散的蝕刻步驟(諸如:隨後為一主要蝕刻 的一蝕刻起始)之製程,錄庙 μ用OES至具有快速及週期性的 電漿擾動之電毅製程係困難。該等製程之實例係分時多工 的製程’如由〇kudaira等人於美國專利第4,985,114號以 及Ue贿等人於美國專利第5 5〇1 893號所揭示者。此 %•作者係揭示一種TDM制is ,ra .. 裡I私,運用一交替組的蝕刻與沉積 步驟以姓刻高長寬比的特徵至Si。 第2a-e圖係顯示TDM蝕刻製程之示意代表圖。τ⑽蝕 刻製程係典型為實施於一反應器,其構成具有典型為一感 應搞合電敷(ICP,Inductively Coupled Plasma)之一高密 度電聚源’且關連於—射頻⑽,radio freQuency)偏慶的 基板電極。針對Si的,#刻製程所運用之最為普遍的製 程氣體係六敦化硫(Sf6)與八氟化四碳(认)。%係典型運 用為姓刻氣體,而c4f8係典型運用為沉積氣體。於姓刻步 驟期間’ SF6係有助於梦之自發與各向同性的㈣(第咖 1317539 圖);於沉積步驟中,c,8係有助於保護性的聚合物沉積於 姓刻結構之側壁以及底部(第2(c)圖)。製程係 = 替於姓刻與沉積製程步驟之間,使得高的長寬比的 ^ 能夠界定於-遮罩後的石夕基板。於高能量及方向性 轟擊(其為存在於蝕刻步驟)’由先前的沉積步驟所 蝕刻結構的底部之聚合物薄膜係將為移除以露出1、 面,以供進-步的㈣(第2⑷圖)。於側壁的聚:物= =保持’因為其未受到直接的離子義擊,以禁止側向的 運用TDM理論係允許高長寬比的特徵為以高^ 速率而界定㈣基板。f 2(e)圖係顯示其運用—咖製= 所蝕刻之一矽結構的一個橫 W電子顯微鏡(SEM, scannlng electr〇n micr〇sc〇pe)影像。 =與沉積步驟之電衆放射光譜係顯著為不同,歸因 存在於沉積與勉刻步驟之不同的電衆條件(參閱第3 :ε =體型式、壓力、RF功率、等等)。應;= 期性(第4圖)。洲石夕餘刻f程係造成一終點軌跡,其為週 含於之I所預期的是’大多數的敍刻終點資訊係包 3於1 之蝕刻分段(segment)。 取-=:广(美國專利第^^ =二™製程之電漿放射的終點資訊之方法。一系 至==二在供應的觸發(其典型為自-㈣程步驟 , 史而檢視僅為於蝕刻步驟期間之於電f之 二-=(針對〜而典型為氟或二^^ 者運用一觸發且闕連於-個取樣及保持電路,於後 1317539 續的蝕刻步驟中所觀察之放射強度係可結合在一起,以得 到其本質為非週期性之-放射訊號。針對於各個蝕刻步驟 w 放射強度值係於後繼的沉積步驟期間而保持在 最後的已知值。以此方式,週期性的放射訊號係轉換為其 類似於—步進函數之—曲線,其可運用於製程終點決定。、 此理論的限制係需要—個外在供應㈣,此外,需要於觸 發與得到各個餘刻步驟期間的放射資料之間的一使用者輸 入延遲。 :erde等人(美國專利第4,491,499號)於提高〇ES方 法靈敏度之努力係揭示:測量放射光譜之一窄帶而且同時 測量其中心為繞於該窄帶之一較寬的背景帶之強度。以此 方式月万、訊號係可為自終點訊號而減去,以造成該窄帶 訊號之一更為準確的值。 多個團體係已經注意電漿放射光譜之頻率分量。Buck 等人(美國專利帛6,1〇4, 487幻係描述運用諸如快速傅立 葉變換(FFT,Fast Fourier Transform)之數位訊號處理技 術以求取電漿放射光譜之頻率分量。Buck係揭示的是,此 等分置係提供關於電漿條件的變化之資訊且可運用以偵測 於基板材料的轉變,而允許蝕刻終點偵測。Buck係揭示其 降至1 0 Hz之音頻外的頻率。Buck係考慮的是,監視的頻 率係將對於不同的製程而改變;然而,其僅為考慮穩態(單 步驟)製程,而運用關連於其為週期性及反覆性的分時多 工(TDM)製程之FFT光學放射係未揭示。1317539 发明, DESCRIPTION OF THE INVENTION: TECHNICAL FIELD OF THE INVENTION The present invention relates generally to the field of semiconductor manufacturing. More particularly, the present invention is directed to an improved method of detecting the end of an etch and deposition process for a time-sharing division _1 tiplexed). Cross-reference to the relevant application This application is related to the US-issued US Provisional Patent Application No. 6〇/447, 594 proposed by Us Lu Zhishan Dingyue in February 2003 and sovereignty, titled: Time-sharing In the multiplexed etching process, the zebra gamma & endpoint detection, this provisional patent application is incorporated herein by reference. [Prior Art] During the production of many _s devices, the material of the etch-layer is required to complete the layer that stops at the bottom (for example, the insulator on the silicon chip (s〇i si 1 iC〇n-〇n-insulator) That is, it removes the KSi) layer which stops at the lower layer of the dioxide layer. Allowing the engraving process to proceed beyond the time when the first layer has been removed will result in a reduction in the thickness of the underlying stop layer, or a degradation of the characteristic profile (profUe) (needle_s〇I application is based on this technique) Called "notching"). One method commonly used to detect the end of electrical destruction process is optical specptical emission spectrometry. 〇 0ES analyzes the light emitted by an electrical source to induce its effects on the chemical and physical states of the electrical destruction process. In semiconductor processing, this technique is commonly used to integrate the material interface during the electro-acoustic process. One of the themes discussed in the optical precision technology of plasma processing, is proposed - excellent! 317539 Yue commented on the principle and application of plasma emission spectroscopy technology. The OES technology involves monitoring the radiation emitted by the plasma, typically in the uv/m(10)(10) to 11 GGnm portion of the spectrum. Figure 1 shows a schematic diagram of a typical GES architecture. The composition of the electrode (and especially the presence of reactive etching species or etching by-products) is determined by the spectrum of the radiation emitted (i.e., intensity versus wavelength). During the course of an etching process (and especially for a material transition), the composition of the electrode changes and causes a change in one of the radiation spectra. By continuously monitoring plasma emissions, a 终点es endpoint system may detect a change in one of the emission spectra and use it to determine when the film has been completely removed. In practice, most of the information about the endpoint is typically contained within a few wavelengths that correspond to the reactants consumed during the remainder or the resulting by-products of the etch. One common method for developing an OES endpoint strategy is to collect multiple spectra of plasma radiation during the conditions before and after the endpoint. These light schemes can be used to identify wavelength regions for candidates for the process. The candidate region contains wavelengths that exhibit significant intensity changes as the process reaches a transition between two related materials. The endpoint wavelength candidate region can be determined using a variety of methods. Spectral regions for endpoint detection can be selected by statistical methods, such as factor analysis or principal component analysis (see U.S. Patent No. 5,658,423 to Angell et al.). Another strategy for determining the candidate for the endpoint is to construct a difference between the spectra before the end (primary etch) and after the end point (over etched). Once the candidate regions have been selected, the designation of similar chemical species can be made for the candidate regions (i.e., 1317539 species, or surname products) from the reactants of the free gas leader. The seven-plate Pe bottle and other people's "spectral line graph" ', the identification of the knife spectrum, the multiple references, the knowledge related to the process chemicals are similar to the species identifier. Needle oblique production ^Uine; ^ in one of the eight bismuth sulphur (SF6) plasma, Shi Xi (Si) surname engraving process similar to the end of 687 ... 〇 3nm of fluorine (F: choose one of the examples will be The cesium fluoride (SiF) band at 440 nm. Once these areas are secondary, the subsequent parts can be processed using the same OES strategy. Although these OES methods are quite suitable for single use. The process of stepping is either a process with a finite number of discrete etching steps (such as an etch start followed by a major etch), recording the OES to a fast and periodic plasma disturbance. The process is difficult. The examples of such processes are those that are time-multiplexed, as disclosed in U.S. Patent No. 4,985,114, issued to U.S. Pat. This %• author reveals a TDM system is, ra.. I private, using an alternating set of etching and deposition steps to name the high aspect ratio to Si. The 2a-e diagram shows the schematic representation of the TDM etching process Figure τ (10) etching process is typically implemented in a reactor, the composition of which is typically One is to apply one of the high-density electro-convergence sources of ICP (Inductively Coupled Plasma) and is related to the substrate electrode of RF (10), radio freQuency. For Si, the most common process gas system used in the engraving process is Stan (Sf6) and octafluoride (carbon). The typical use of % is the gas of the surname, while the c4f8 is typically used as the deposition gas. During the engraving step, the SF6 system contributes to the spontaneous and isotropic nature of the dream (4) (Fig. 1317539); in the deposition step, the c, 8 system contributes to the deposition of protective polymers in the structure of the surname. Side wall and bottom (Fig. 2(c)). The process system = between the surname and the deposition process step, so that a high aspect ratio of ^ can be defined in the - behind the mask. In high energy and directional bombardment (which is present in the etching step) 'the polymer film system at the bottom of the structure etched by the previous deposition step will be removed to expose the 1 surface for the step-by-step (4) 2 (4) Figure). The poly-materials on the sidewalls = = hold 'because they are not subjected to direct ion bombardment to prohibit lateral use. The TDM theory allows high aspect ratios to be characterized by a high rate of (iv) substrate. The f 2(e) diagram shows a transverse W electron microscope (SEM, scannlng electr〇n micr〇sc〇pe) image of the 矽 structure. = Significantly different from the electron emission spectrum of the deposition step, due to the different battery conditions in the deposition and engraving steps (see 3: ε = body type, pressure, RF power, etc.). Should; = period (figure 4). The Zhou Shixi re-environment creates a trajectory of the end point, which is what Zhou expects to be the etch segment of the majority of the information. Take -=: wide (the method of the end point information of the plasma radiation of the US patent ^^ = two TM process. One line to == two in the supply trigger (which is typically the self-(four) step, history only view During the etching step, the second of the electric f-= (for the ~ and typically the fluorine or the two, using a trigger and connected to a sample and hold circuit, the radiation observed in the subsequent etching step of 1317539) The strengths can be combined to obtain a non-periodic-radio signal. The radiation intensity values are maintained at the last known value during the subsequent deposition step for each etching step. The sexual radio signal is converted to a curve similar to the step function, which can be applied to the process end point decision. The limitation of this theory is the need for an external supply (4). In addition, it is necessary to trigger and obtain each moment. A user input delay between the radiological data during the step. : erde et al. (U.S. Patent No. 4,491,499), the effort to improve the sensitivity of the 〇ES method reveals that measuring one of the narrow bands of the radio spectrum and simultaneously measuring its center The strength of the wider background band around one of the narrow bands. In this way, the signal can be subtracted from the end signal to cause a more accurate value of the narrowband signal. The frequency component of the plasma emission spectrum. Buck et al. (U.S. Patent No. 6,1,4, 487, the illusion describes the use of digital signal processing techniques such as Fast Fourier Transform (FFT) to obtain plasma emission spectra. Frequency components. Buck reveals that these separations provide information about changes in plasma conditions and can be used to detect changes in substrate material while allowing etch endpoint detection. Buck reveals that it drops to 10 The frequency outside the Hz audio. Buck considers that the frequency of the monitoring will change for different processes; however, it only considers the steady-state (single-step) process, and the application is related to its periodicity and repetitiveness. The FFT optical radiation system of the time division multiplexing (TDM) process is not disclosed.

Kornblit等人(美國專利第6,〇21,215號)亦描述其關 1317539 連於先學放射光譜的傅 π ± 得立葉變換之運用。Kornblit係揭示 同時監視所有的頻率八θ 光學放射m之運用…但是未揭示針對-窗製程的 D:Vld〇W等人(美國專利第6,455,437號)亦描述其產 生來自電漿放射的頻率公县a J頭羊刀量以及監視隨著時間經過之訊 的振幅。儘管Davidow俜田万田认&亡,夕 ° 係心及用於蝕刻多層堆疊之多步驟 的製程,針對TDM贺鞀夕Β月.* ^王之關連於FFT的光學放射之運用係 未揭不。甚者,—係藉著注意哪些頻率為出現於製 程進行期間以描述該雷想愈 " 电漿1耘,而非檢視由TDM製 環性質所加諸於製程的特徵頻率之大小。 二〇’NeUl等人(美國專利第5, 308, 414號)係描述其運用Kornblit et al. (U.S. Patent No. 6, 〇 21, 215) also describes the use of the Fu π ± Deli transform coupled to the first-class radioactivity spectrum of 1317539. The Kornblit system reveals the simultaneous use of all frequency eight θ optical radiation m. However, D: Vld〇W et al. (U.S. Patent No. 6,455,437), which is not disclosed for the windowing process, also describes the frequency of the county that produces plasma radiation. a J head sheep knife and monitor the amplitude of the signal as time passes. Although Davidow 俜田万田 recognizes & 死, 夕 ° center and the multi-step process used to etch multilayer stacks, for TDM He Xi Xi Yueyue. * ^ Wang Zhiguan connected to the FFT optical radiation system is not revealed . In other words, by paying attention to which frequencies appear during the process to describe the Raytheon, instead of examining the characteristic frequencies imposed by the TDM loop properties on the process. 〇'NeUl et al. (US Patent No. 5, 308, 414) describes its application

訊號解調變之一種光學放射备 n, M 元予放射糸統。〇NeUl係監視其關聯 ' '物之一乍的光譜區域以及其將運用作為一背景 修正之-較寬的光譜帶。〇’Nei i i亦揭示其透過運用一鎖 入式(lock-ιη)放大器之訊號的頻率解調變。鎖入式放大器 係需要一外部的同步化訊號。〇,NeUi係未考慮 = 或TDM製程。 &The signal demodulation becomes an optical radiation preparation n, M element to the radiation system. The 〇NeUl system monitors the spectral region of one of its associated ''objects' and it will be used as a background correction - a wider spectral band. 〇'Nei i i also revealed that it is demodulated by the frequency of the signal using a lock-type amplifier. Lock-in amplifiers require an external synchronization signal. Hey, NeUi does not consider the = or TDM process. &

Sawm等人(美國專利第5,450,205號)係描述其運用 關連於FFT之光學放射干涉技術(〇EI . pilcal emission mterferometry)以決定製程終點之一種系統。相對於其分 析電漿放射之光學放射光譜技術(0ES),放射干涉技術係2 像由晶圓表面所反射的電漿放射以決定於晶圓上的薄膜厚 度。不同於OES,0EI技術係需要成像偵測器為具认曰 圓表面之一清楚的視線。〇Ε I技術係不適用於彭程, 11 1317539 “有反覆性的沉積與蝕刻步驟,歸因於隨著蝕 一鈍化薄膜的循環性加入及移除。 仃之 疋以’存在用於TDM電漿製程的一種終點策略之 牛驟::要一個外在觸發以使得電漿放射資;程 步驟為同步化。 ,、我枉 【發明内容】 本發明之一個較佳實施例係針對一種用以建立於— 異性電㈣刻製程期間的-個終點之方法 之二=用一電聚且透過一㈣光罩而提供於該基板 之側向界疋的凹部結構。根據該種方法 :一個崎驟中馳刻,藉著接觸於-反應丄面: :除自違基板之表面的材料且提供暴露的表面而達成。 吕玄=之表面係於-個沉積步驟中純化,俾使其為暴露於 先前的㈣步驟之水平與垂直表面係均為由-純化 PasS1Vatlon)層所覆蓋。該钱刻步驟與純化步驟係交替重 複。電毀放射係監視於一特定的波長或波長區域且為於一 特徵頻率’其Λ TD"程之交替的本質所施加。特定波長 區域係較佳為基於製程期間所運用的一材料之一放射光譜 :決定。於另一個實施例中,電激放射係於二或多個心 區域中被監視’且第一波長區域與第二或多個波長區域之 大小的比值(或其他的數學運算)係被計算出。於該實施例 中,—或多個波長區域係可選擇以代表背景訊號。施加的 特徵製程頻率係基於姓刻步驟的持續期間與純化步驟的持 續期間之總和而決定。針對一典型的TDM製程,製程之特 12 1317539 徵頻率係小於 之一時間。Sawm et al. (U.S. Patent No. 5,450,205) describes a system for determining the end of a process using an optical radiation interference technique (〇 . . pilcal emission mterferometry) associated with FFT. Relative to its optical emission spectroscopy (0ES), which analyzes plasma radiation, the radiation interference technique 2 is based on the plasma radiation reflected from the surface of the wafer to determine the film thickness on the wafer. Unlike OES, the 0EI technology department requires an imaging detector to have a clear line of sight on one of the recognizable circular surfaces. 〇Ε I Technology Department does not apply to Peng Cheng, 11 1317539 “There are repetitive deposition and etching steps due to the cyclic addition and removal of a passivation film with etch. 仃之疋' exists for TDM One of the end-point strategies of the pulping process: an external trigger to make the plasma radiology; the process steps are synchronized., I am [invention] A preferred embodiment of the present invention is directed to The second method of establishing an end point during the process of the anisotropic electric (four) engraving process is to use a concavity structure provided on the lateral boundary of the substrate by a photopolymer and through a (four) photomask. According to the method: a subsequent In the middle of the process, by contact with the reaction surface: : In addition to the material that violates the surface of the substrate and provides an exposed surface. The surface of Lu Xuan = is purified in a deposition step, which is exposed to The horizontal and vertical surface systems of the previous (four) steps are covered by a layer of purified PasS1Vatlon. The steps of the engraving and the purification steps are alternately repeated. The electrical destruction radiology is monitored in a specific wavelength or wavelength region and is a feature. Frequency 'its The nature of the TD" alternation is applied. The specific wavelength region is preferably based on one of the materials used during the process: the emission spectrum is determined. In another embodiment, the electrical stimulation is applied to two or more regions of the heart. The ratio (or other mathematical operation) of the size of the first wavelength region to the second or more wavelength regions is calculated. In this embodiment, - or a plurality of wavelength regions are selectable to represent Background signal. The applied characteristic process frequency is determined based on the sum of the duration of the surname step and the duration of the purification step. For a typical TDM process, the frequency of the process 12 1317539 is less than one time.

Hz。該製程係中斷於其為取決 於監視步驟Hz. The process is interrupted because it depends on the monitoring step

發月之另—個實施命H 程的一t > 喱俏測用於—TDM t 個一占之方法。根據該種方 展 射光譜的一第一喻旦拓丄… x表転之—電漿放 λ長區域係辨識。由該了⑽fj# 一特徵製程頻率仫·^ 4 M I耘所施加之 羊係亦為辨識,且該電漿放射 長區域係被監視於此胜 D日的第一波 M h 此特徵製程頻率。該特徵^ 於其存在於續匍和山, 取^土项手係基 ' I転中的蝕刻與沉積步驟總和之一# 續期間。辨識的波县+/ 决疋的持 ❹小係於此製程期間被監視, :/1¾之終點。該放射光譜的一第二、 區域係亦被監視。哕TDM _ " 波長 之-數⑴ ㈣終點係基於諸個波長區域 千、Q ^如:加法、減法或除法)而決定。一快速傅 兮電=:或一對應的數位訊號處理技術係運用以解析 口系電,灵放射光譜之箱座八旦 . 刀里。5亥I程之終點係典型為基於 /、發生於姓刻樂I兹直日p q + ,, p 』B之一材料轉變。於該種情形,玆朵 譜之辨識的波長區域你美 Μ 堞係基於TDM製程所運用之一材料的一 已知光譜特性。 本發明之又一個實施例係針對一種偵測於一個τ跗製 鲛的不同材料之間的轉變之方法。根據此方法,該製程之 —特徵頻率係被辨辨識。該製程之特徵頻率係基於其執行 為TDM製程的部分者之—個钱刻步驟與—個沉積步驟的持 續期間之總和。該製程之—光譜放射的—區域係被監視於 特徵頻率以決定於不同材料之間的轉變。轉變係發生在其 執行為TDM製私的部分者之一連争的钮刻步驟之一個終點 13 !317539 取決於TDM製程 。於特徵頻率所監視之光譜放射的區域係 所運用之—材料的-已知光譜特性。 【實施方式】 本發明之一個較佳實施例係 多工(T D Μ)製避的τ r對種偵測於-個分時 ,藉著分料之間的轉變之方式 者刀析對應於TDM製程之 電磁放射的至少-個波長分量。 料之收集 ::: 製程之週期性與重複的本質,該 猎:广而具有關聯於其之多個特徵頻率。作為一個實例 之 個二步驟™石夕敍刻製程’其為隨後為重複多-欠 二-個四秒的韻刻步驟與一個六秒的沉積 2 閱如下之表1)。 |、颂Λ參 表1 sf6 流4 —- seem 沉積 0.5 Ί虫刻 Too~~ A、;奋县 ~~~ ~~--- seem —70 05 m -h —---- seem 40 40 — /7 RF ---- mtorr 22 23 ~~~~~ AVI Jyj 举 TPP r.-h Φ ------ 瓦"~~ 1 12 1000 1000 步驟時"^ ~~- ———- ____ 1 * h秒 ____ 4 6 ~~ -----^The other month of the month is a method of implementing the life cycle of T> According to this kind of spectrum, a first meta-analysis of the spectrum is obtained... x 転 転 - plasma discharge λ long area identification. The sheep system applied by the (10)fj#-characteristic process frequency 仫·^ 4 M I耘 is also identified, and the plasma radiation long region is monitored for the first wave M h of the characteristic D process frequency. This feature is found in the continuation of the sum of the etching and deposition steps in the continuation of the 匍 匍 and the mountain. The identified Boxian+/ 疋 ❹ 系 is monitored during this process, : / 13⁄4 end. A second, regional system of the emission spectrum is also monitored.哕TDM _ " The number of wavelengths (1) (4) The end point is determined based on the wavelength regions of thousands, Q ^ such as: addition, subtraction or division. A fast 兮 兮 = = or a corresponding digital signal processing technology is used to resolve the oral system, the spectrum of the radio spectrum is eight denier. The end point of the 5 Hai I process is typically based on /, which occurs in the name of the music, I am a day, p q + ,, p 』B one material transformation. In this case, the wavelength region identified by the spectrum is based on a known spectral property of a material used in the TDM process. Yet another embodiment of the present invention is directed to a method of detecting a transition between different materials of a τ 跗 。. According to this method, the characteristic frequency of the process is recognized. The characteristic frequency of the process is based on the sum of the duration of the process of performing a part of the TDM process and the duration of the deposition process. The process-spectral radiation-area is monitored by the characteristic frequency to determine the transition between different materials. The transition occurs at one of the end points of the buttoning step in which one of the parties performing the TDM system is contending 13 !317539 depending on the TDM process. The area of the spectral emission monitored by the characteristic frequency is the known spectral characteristic of the material. [Embodiment] A preferred embodiment of the present invention is a multiplexed (TD Μ) avoidance τ r pair detection in a time division, by the transformation between the materials, the knife corresponding to the TDM At least one wavelength component of the electromagnetic radiation of the process. Collection of materials ::: The nature of the periodicity and repetition of the process, which is broad and has multiple characteristic frequencies associated with it. As an example, a two-step TM stone etch process is followed by a repeating multi-under two-four-second rhyme step and a six-second deposition 2 as shown in Table 1 below. |颂Λ颂Λ表1 sf6流4—- seem deposition 0.5 Ί Inscribed Too~~ A,; Fen County~~~~~--- seem —70 05 m -h —---- seem 40 40 — /7 RF ---- mtorr 22 23 ~~~~~ AVI Jyj Lift TPP r.-h Φ ------ 瓦"~~ 1 12 1000 1000 Steps "^ ~~- ——— - ____ 1 * h seconds ____ 4 6 ~~ -----^

主思,>儿積步驟與蝕刻步驟之化學作用、RF偏壓功率 =I力係不同,而造成顯著不同的放射光譜。歸因於tdm 製耘之,複性質以及沉積步驟與蝕刻步驟之持續時間,於 表1之只例的製程係具有i。秒之一循環重複時間且因此為 14 1317539 二:預期的特徵頻率。該光譜之取樣速率係必須為 决,以準確捕捉電漿放射之 (ai iQo; x 〜w别注為而無混〉有現象The main idea is that the chemistry of the entanglement step is different from the chemistry of the etch step, the RF bias power = I force, resulting in a significantly different emission spectrum. Due to the tdm system, the complex nature and the duration of the deposition and etching steps, the process of the example of Table 1 has i. One of the cycles repeats the time and is therefore 14 1317539 II: the expected feature frequency. The sampling rate of the spectrum must be determined to accurately capture the plasma radiation (ai iQo; x ~ w don't be a no-mix)

Uliasmg)。因此,取樣頻 頻率,B 糸須為阿於奈氏(Nyquist) 且較佳為預期的特徵頻率之1〇倍。 對用:第示本發明之-個實^ ^ TD 、 良的〇ES技術。於步驟500,一 之^係構成具有至少__個特徵頻率,其為取決於該製 :的持續期間。TDM製程之特徵頻率係典型為小於5 L1:程的”放射光譜之至少一個波長區域(針對電 d為於200-1 1 00 nm)係辨識以供製程終點谓測 。於步驟502,光譜區域係被監視於钮刻製程之進行 』間。由於用於叫固TDM製程之放射訊號係週期性且反覆 放射訊號係可解析成為頻率分量。於步驟5〇4,至少 二:頻率分量係於製程特徵頻率且為求取。求取諸個頻率 为置之一種方法係透過快速傅立葉變換(FFT)之運用,雖然 其他的數位訊號處理(DSP)技術亦可運用。若於步驟5〇6 = 偵測一材料轉變,該種方法係進行至步驟5〇8,其中,該 種方法係進行至下一個製程步驟或TDM序列。若於步驟 5〇6係未偵測一材料轉變,該種方法係返回至步驟,其 中,至少一個光譜區域之電漿強度係被監視而直到一材^ 轉變為偵測。相對於其運用藉著FFT之OES的先前揭示者 ,監視於一 TDM製程特徵頻率(典型而非恆為小於5 Η?)之 放射訊號的大小係提供一種可靠的方法,以供侦測於一 TDM蝕刻製程期間之層間的轉變。 15 1317539 本發明之另—個實施例係運用其出自放射資 多^皮長分量,以改善終㈣測之靈敏度。至少—個2 /刀置係TDM製程之一特徵波長。其他波長分量係 景訊號。二或客彻八曰 八衣月 法)係揭供於京L刀置之數學組合(諸如:加法、減法或除 、八;’、1應用之較大的靈敏度。 J主意,本發明之理論係不限於一種二步驟的循環製程 。貫際上,普遍為進而再分割該製程 : ^ ,製 進一步的分割為多個子步驟係僅造成額 外之製程施加的特徵頻率。 亦為重要以指出的是’於—個蝕刻步驟與—個 驟之各個反覆性的製程迴 L積步 %參數係無須為維持宗 =同循環。舉例而言,之TM#刻期間,普遍= I程之進行而逐漸改變沉積或姓刻步驟之效率,以維 持輪廓控制(於此技藝而f稱為製程形態(⑽ 一形態製程中,小的參數變 g))於 驟之間的製程參數。此# # Μ ;㈤_或沉積步 /数此4係包括而不限於··Uliasmg). Therefore, the sampling frequency, B, is not required to be Nyquist and is preferably 1 times the expected characteristic frequency. For the purpose of: the first embodiment of the present invention ^ TD, good 〇 ES technology. In step 500, a system has at least __ characteristic frequencies, which are dependent on the duration of the system. The characteristic frequency system of the TDM process is typically less than 5 L1: the "at least one wavelength region of the emission spectrum (for electrical d is 200-1 1 00 nm) is identified for process endpoint prediction. In step 502, the spectral region The system is monitored during the process of the button engraving process. Since the radio signal used for the fixed TDM process is periodic and the repeated radio signal is resolved into a frequency component. In step 5〇4, at least two: the frequency component is in the process. The characteristic frequency is obtained. The method of obtaining the frequencies is based on the application of Fast Fourier Transform (FFT), although other digital signal processing (DSP) techniques can be used. If in step 5〇6 = Detect To determine a material transition, the method proceeds to step 5:8, wherein the method proceeds to the next process step or TDM sequence. If a material transition is not detected in step 5〇6, the method is Returning to the step wherein the plasma intensity of at least one of the spectral regions is monitored until a material is converted to detection. Relative to the prior disclosure of the OES by the FFT, monitoring the characteristic frequency of a TDM process The size of the radio signal, rather than being constant less than 5 Η?), provides a reliable method for detecting interlayer transitions during a TDM etch process. 15 1317539 Another embodiment of the present invention uses From the radioactive material, the long component of the material is used to improve the sensitivity of the final (four) measurement. At least one of the 2 / knife sets is one of the characteristic wavelengths of the TDM process. The other wavelength components are the signal. The second or the guest is the eight-eighth-eight-month method. It is a mathematical combination of the L-knife set (such as: addition, subtraction or division, eight; ', 1 application of greater sensitivity. J idea, the theory of the invention is not limited to a two-step cycle process. In general, the process is generally further divided: ^, further division into multiple sub-steps only results in additional characteristic frequencies applied by the process. It is also important to point out that 'in an etching step and a step Each repetitive process back to the L-step % parameter system does not need to be a maintenance = same cycle. For example, during the TM# engraving, the general = I process progresses and gradually changes the efficiency of the deposition or surname step to maintain the contour control (This technique is called process pattern ((10) in a morphological process, small parameters are changed to g)) process parameters between the steps. This # # Μ ; (5) _ or deposition step / number of 4 series including Limited to ··

偏壓功率、製程壓力、减 八机’、、RF ^ 戍應源功率(ICP’ inducti source P〇wer、等等。此等變化亦可包括: 循&quot;内之諸個製程步驟的持續期間。若於製程之進行: 的猶環時間變化係大於變換之頻率解析度,演^間 以監視相鄰的頻率分量之總和, 糸正 移位。 爾所施加的製程頻率 儘管本發明之一個較佳實施例係 sf6/c4f8的製程之深度Si 個基於 本發明之較佳實 16 1317539 』系可利用*無關於化學物,假設一個分時多Ji (TDM)製 程係運用。該等較佳的方法亦為特別有用以供㈣於其他 材料之材料轉變,諸如:介電材料與金屬,其中,一個反 覆性的分時多工(TDM)製程係運用。 欲論證本發明之一個實施例的可利用性,一 TDM方案 係運用以蝕刻-絕緣體上矽晶片⑽)之晶圓。該方案係列 表於如下之表2。以下的實例係應用本發明之一個實施例 至一種3步驟的TDM矽触刻製程。 表2 沉積 姓刻A 如刻B 处6流率 seem 1 50 100 〇^8流率 seem 70 1 1 Ar流率 seem 40 40 40 壓力 毫托耳 22 23 23 RF偏壓功率 瓦 1 12 12 ICP功率 步驟時間 瓦 1500 1500 1500 秒 6 3 7 s亥等貫驗係執行於一商用Unaxis Shuttlelock系列之 永度石夕蚀刻(DSE,Deep Si 1 icon Etch)工具。放射光譜係 運用一商用Unaxis Spectraworks放射光譜儀以1 Hz之頻 率所收集。 欲決定有關的波長區域,一測試晶圓係蝕刻且於沉積 步驟與蝕刻步驟之電漿放射光譜係在矽層為已經清除(製 私終點)之前以及之後而分析。第6圖係顯示針對測試晶 圓的電漿放射光譜之強度對波長的繪圖。在該製程的終點 17 1317539 之前的沉積光譜600、製程的終點之後的沉積光言普602、製 程的終點之前的㈣㈣_、與製程的終點之後的飯刻 光譜606係顯示於第6 M貞測器飽和6()8係由該圖形的 頂部之直線所代表。由於少量的㈣係預期於製程之沉積 仏匕段’第7圖係針對來自㈣步驟在碎層為已經清除之前 及之後的放射光譜700與7〇2。注意,接近45〇⑽之於蝕 刻光譜的些微差異704。為了決定終點候選者,一種點對 點(point-by-p〇int)的差異光譜係建立。 /合成光譜8GG係顯示於第8 ®。針對終則貞測之候選 者係發生於440 nm與686 nm。440 nm峰值係可指定至氟 化石夕(SiF)放射(姓刻產物—隨著Si為清除而減少),而咖 ⑽峰值係可指定至氟(F)放射(反應物_隨著si為清除而增 加)。 一種終點策略係基於440 nm放射峰值而建立。第9圖 係顯示終點之前的蝕刻放射光譜9〇〇與終點之後的蝕刻放 射光譜9G2之放大圖’藉以更為接近檢視44() nm峰值。為 了降低相關聯的雜訊,二個光譜區域9〇4肖9〇6係被監視 以供背景修正’即:-個窄@ 440 rnn峰值(SlF放射)與其 中心為繞於445 nm之一個較寬的光譜區域。 ^第10圖係描繪對時間之該二個區域的值。儘管存在隨 著蝕刻進行之於振盪訊號的峰對峰值之一稍微減小,欲決 定一製程終點係困難。帛11圖係顯示於總I虫刻時間之3〇〇 至4 0 0秒的範圍之第1 〇圖的 J ^ ^ /工思,汛观〈440 η 1100與背景(445 nm) 1102區域係於較高強度的沉積步 18 1317539 〇4而彼此為適當追蹤,但是接近蝕刻步驟11 μ之結束 而發散建立440 nm訊號與445 nm背景之比值係造成第 12圖’其中’於钮刻與沉積步驟之間的大放射變化係已經 消除’且造成的訊號係更為代表其進㈣刻之程度。注意 ’如於第12圖所示的比值訊號12〇〇之週期性與反覆性的 本質。 第13 係顯示於姓刻《進行的比值訊號(44〇⑽ 8趟5 nm背景)13〇〇β注意,如於第i3圖所示之於接 近600秒的連續峰值高度之減小。於第13圖所示之軌跡的 特徵頻率係G.G6Hz。此係方案施加頻率,對應於“秒, 其為於表2之循環製程的個別製程步驟之時間的總和。 〃運用—快速傅立葉變換(FFT)以自時域至頻域而轉換於 第13圖之訊號係造成於第Μ圖所示之功率頻譜。FFT計 算係基於128元素陣列,其附加以隨著製程進行而形成 OES訊號之-展開窗。由點狀方塊所強調的頻率係歸因於 TDM製程方案之週期性與反覆的本質而所預期者。第η圖 係顯示於製程中的二個點之FFT功率頻譜的振幅。注意, 0.06 Hz分量係具有在終點之前的一大振幅,且在&amp;層為 已經清除後而減小為接近於零。繪製於時間之〇 Hz八 量的大小係造成第16圖所示之製程終點軌跡。由此曲線 而決定實際的終點時間係可藉由種種的方式而作成,包括 而不限於:簡單的臨限谓測或差動㈣”亥等技術係對於 熟悉此技藝之人士為眾所週知。 以上論述的實施例係允許一個TDM製程之終點為準確 19 1317539 j :著以裝私之—特徵頻率而監視該沉積步驟與蚀 之放射光譜。準確決定該製程的一終點之能力係使 =過 期望特徵之可能性為最小或消❺,且因此減小 ” 層之厗度。此外,於此技藝所習稱為“切口 二1寺:輪廓降級亦為最小化。再者,本發明係相當適用 ::”、肖速及週期性的電漿擾動之任何電漿製程。因此 本發明係於先前技藝之一實質改良。 本揭示内容係包括於隨附的申請專利範圍所含有之部 刀者、以及前述說明者。雖然本發明係 個程度的特定性之其較佳形式,應瞭解M,較佳形= 2示内容係僅為舉例而作成’且於構成的細節與零件的 、,且S及配置之諸多變4卜糸 與範B壽。 K匕係均了採取而未偏離本發明之精神 【圖式簡單說明】 第1圖係一種典型的OES架構之示意圖; 第2(a)至2(e)圖係顯示一種TDM蝕刻製程之代表圖. 第3圖係針對一個範例的削製程之沉積與兹刻電聚 放射光譜圖; 第4圖係針對一個範例的™製程之終點線跡; 第5圖係顯示本發明的一個實施例之概觀,針 TDM製程之一種改良的OES技術; ; 第6圖係顯示強度對波長之繪圖,針對其為運用以確 認本發明的一個實施例之一測試晶圓;、 第7圖係顯示一個削製程的終點之前與之後的蝕刻 20 1317539 光譜圖; 第8圖係顯示針對 闽. 乐7圖的蝕刻光譜之標稱化的差異 光譜圖; ’冬點之前與之後的蝕刻放射光譜放大 弟9圖係顯示在 圖;Bias power, process pressure, minus eight ',, RF ^ 戍 source power (ICP' inducti source P〇wer, etc. These changes may also include: the duration of the various process steps within If the process is carried out: the time variation of the heliosphere is greater than the frequency resolution of the transformation, and the sum of the adjacent frequency components is monitored to correct the displacement. The process frequency applied by the processor is not a The preferred embodiment is the depth of the process of sf6/c4f8. Si is based on the preferred embodiment of the present invention. 16 1317539 can be utilized * regardless of the chemical, assuming a time-sharing multiple Ji (TDM) process is used. The method is also particularly useful for (iv) material conversion of other materials, such as: dielectric materials and metals, wherein a repetitive time division multiplexing (TDM) process system is utilized. To demonstrate one embodiment of the present invention Utilities, a TDM scheme utilizes wafers that are etched-on-insulator wafers (10). The program series is shown in Table 2 below. The following examples apply one embodiment of the present invention to a 3-step TDM crucible etch process. Table 2 Deposition of the surname A as engraved B at 6 flow rate seem 1 50 100 〇 ^ 8 flow rate seek 70 1 1 Ar flow rate seek 40 40 40 pressure millitorn 22 23 23 RF bias power watt 1 12 12 ICP power Step time watts 1500 1500 1500 seconds 6 3 7 shai and other inspection systems are executed in a commercial Unaxis Shuttlelock series of DSE (Deep Si 1 icon Etch) tools. The emission spectroscopy was collected at a frequency of 1 Hz using a commercial Unaxis Spectraworks radioactivity spectrometer. To determine the relevant wavelength region, a test wafer is etched and the plasma emission spectra in the deposition and etching steps are analyzed before and after the germanium layer has been removed (custom end point). Figure 6 is a graph showing the intensity versus wavelength of the plasma emission spectrum for the test wafer. The deposition spectrum 600 before the end point of the process, the deposition spectrum 600 after the end of the process, the deposition light 602 after the end of the process, the (four) (four) _ before the end of the process, and the rice-cut spectrum 606 after the end of the process are shown in the 6th M detector. The saturated 6() 8 is represented by the line at the top of the graph. Since a small amount of (4) is expected to be deposited in the process, the 7th figure is directed to the emission spectra 700 and 7〇2 before and after the fragmentation has been removed from the (4) step. Note that some 45 〇 (10) is close to the slight difference 704 of the etched spectrum. To determine the endpoint candidate, a point-by-p〇int differential spectroscopy is established. /Synthetic spectroscopy 8GG is shown in Section 8®. Candidates for the final speculation occurred at 440 nm and 686 nm. The 440 nm peak can be assigned to the fluorite (SiF) radiation (the surname product - reduced with Si removal), while the coffee (10) peak can be assigned to fluorine (F) radiation (reactant _ with si for removal) And increase). An endpoint strategy was established based on a 440 nm emission peak. Fig. 9 shows an enlarged view of the etched emission spectrum 9G2 before the end point and the etched emission spectrum 9G2 after the end point, which is closer to the 44 () nm peak. In order to reduce the associated noise, the two spectral regions 9〇4 〇9〇6 are monitored for background correction 'ie: a narrow @ 440 rnn peak (SlF radiation) compared to one centered around 445 nm Wide spectral area. ^ Figure 10 depicts the values for the two regions of time. Although there is a slight decrease in peak-to-peak value of the oscillation signal as the etching progresses, it is difficult to determine a process end point. The 帛11 image is displayed in the first 〇 of the total I insect time in the range of 3〇〇 to 400 seconds. J ^ ^ / 思思, 汛 〈 <440 η 1100 and background (445 nm) 1102 regional system In the higher-strength deposition step 18 1317539 〇 4 and properly tracked each other, but close to the end of the 11 μ μ etching step and divergence to establish the ratio of the 440 nm signal to the 445 nm background, resulting in Figure 12 'where' in the button and deposition The large radiological changes between the steps have been eliminated and the resulting signal system is more representative of its progress. Note the nature of the periodicity and repetitiveness of the ratio signal 12〇〇 as shown in Figure 12. The thirteenth line is shown in the last name "The ratio signal (44 〇 (10) 8 趟 5 nm background) 13 〇〇 β Note, as shown in Figure i3, the decrease in the continuous peak height of nearly 600 seconds. The characteristic frequency of the trajectory shown in Fig. 13 is G.G6Hz. This scheme applies a frequency corresponding to "seconds, which is the sum of the time of the individual process steps of the cyclic process of Table 2. 〃Using - Fast Fourier Transform (FFT) to convert from time domain to frequency domain to Figure 13 The signal is caused by the power spectrum shown in the figure. The FFT calculation is based on a 128-element array, which is added to form an OES signal-expanding window as the process progresses. The frequency emphasized by the dot-shaped block is attributed to The periodicity and repetitive nature of the TDM process scheme is expected. The nth graph shows the amplitude of the FFT power spectrum at two points in the process. Note that the 0.06 Hz component has a large amplitude before the end point, and After the &amp; layer has been cleared, it is reduced to close to zero. The size of 八 八 eight times plotted in time is the end point trajectory of the process shown in Figure 16. The actual end time is determined by the curve. It is made in a variety of ways, including, but not limited to, simple thresholding or differential (4). The technology is well known to those skilled in the art. The embodiments discussed above allow the end of a TDM process to be accurate. 19 1317539 j: The depositional step and the emission spectrum of the etch are monitored at the privileged-characteristic frequency. The ability to accurately determine an end point of the process is such that the likelihood of = over-desired features is minimized or eliminated, and thus the "thickness of the layer" is reduced. Further, this technique is known as "cutting two temples: contours Downgrades are also minimized. Furthermore, the present invention is quite applicable to any plasma process of ":", "short-speed" and periodic plasma disturbances. The present invention is therefore a substantial improvement over the prior art. The present disclosure is included in the accompanying patent application. The knives included in the scope, as well as the above-mentioned instructors. Although the present invention is a preferred form of the degree of specificity, it should be understood that M, the preferred form = 2 shows that the content is merely for example and is constructed Details and parts, and S and configuration of many changes 4 Di and Fan Bshou. K匕 is taken without departing from the spirit of the present invention [Simple description] Figure 1 is a typical OES architecture Schematic; Figures 2(a) through 2(e) show a representative diagram of a TDM etch process. Figure 3 is a plot of deposition and etched emission spectra for an example of a dicing process; Figure 4 is for a An end point trace of an exemplary TM process; Figure 5 is an overview of one embodiment of the present invention, a modified OES technique for a needle TDM process; and Figure 6 shows a plot of intensity versus wavelength for which Confirming an embodiment of the present invention A test wafer; Figure 7 shows the etched 20 1317539 spectrum before and after the end of a cutting process; Figure 8 shows the difference spectrum of the etched spectrum for the 7. The etched emission spectrum before and after the winter point is shown in the figure;

第1 0圖係顯示於第Q y圖所辨識的二個光譜區域内 譜強度值對時間的繪圖; 尤 秒範圍之第 第11圖係顯示於蛐名λ六丨士 ~餘刻時間的300至400 10圖的放大圖; 第12圖係於第11圖所 nm訊 Μ所不的440 nm訊號與443 號之比值的圖; 圖; 第13圖係於帛12圖所示的比值訊號之於钱刻 期間的 .第14圖係於第13 ®的訊號之於頻域的圖; 第15圖係第14圖的頻域訊號在製程的終點之前與 後的振幅繪圖;及 &amp; 〃之 量之頻率的繪 第16圖係於第15圖所示的〇 〇 6 Ηζ分 圖。 【主要元件符號說明】 6〇〇 製程終點之前的沉積光譜 602製程終點之後的沉積光譜 604 製程終點之前的蝕刻光譜 606 製程終點之後的蝕刻光譜 508 積測器飽和 1317539 700 終點之前的蝕刻放射光譜 702 終點之後的蝕刻放射光譜 704 蝕刻光譜的差異 800 合成光譜Figure 10 shows the plot of the spectral intensity values versus time in the two spectral regions identified by the Q y diagram; the eleventh graph of the sec-second range is shown in the 蛐6 丨 six gentlemen~ 300 times of the time Figure 4 is a magnified view of the figure; Figure 12 is a plot of the ratio of the 440 nm signal to the number 443 in Figure 11; Figure 13; Figure 13 is the ratio signal shown in Figure 12 In the period of money engraving, Figure 14 is a diagram of the signal from the 13th to the frequency domain; Figure 15 is a plot of the frequency domain signal of Figure 14 before and after the end of the process; and &amp; Figure 16 of the frequency of the quantity is based on the 〇〇6 Ηζ part of the figure shown in Figure 15. [Main component symbol description] 6〇〇Precipitation spectrum before the end of the process 602 Deposition spectrum after the end of the process 604 Etched spectrum before the end of the process 606 Etched spectrum after the end of the process 508 Accumulator saturation 1317539 700 Etched emission spectrum before the end point 702 Etched emission spectrum after the end point 704 Difference in etching spectrum 800 Synthetic spectrum

900 終點之前的蝕刻放射光譜 902 終點之後的蝕刻放射光譜 904 窄的光譜區域(於440 nm) 906 較寬的光譜區域(於445 nm) 1100 訊號(440 nm) 1102 背景(445 nm) 1104 沉積步驟 1106 蝕刻步驟 1 200 ' 1 300 比值訊號(440 nm SiF/445 nm 背景)900 Etched emission spectrum before endpoint 902 Etched emission spectrum after endpoint 904 Narrow spectral region (at 440 nm) 906 Wide spectral region (at 445 nm) 1100 Signal (440 nm) 1102 Background (445 nm) 1104 Deposition step 1106 Etch Step 1 200 ' 1 300 Ratio Signal (440 nm SiF/445 nm Background)

22twenty two

Claims (1)

1317539 拾、申請專利範固: 該方 1.-種用於建立電漿蝕刻製程中料點 法係包含下列步驟: 4法 置放一基板於一真空室之中; 藉由一電漿而蝕刻自該基板而來之一材料,· 藉由一電漿而沉積一鈍化層於該基板;’ 執行重複該蝕刻步驟與沉積步驟之一製程迴 ^以—對應於製程迴路步驟之蝕刻步驟或沉脚沾舌 设率之特徵頻率而監視於一電漿放射強度中之變化·、 基於該監視步驟而中斷該製程迴路步驟;及 自該真空室而移除該基板。 2·如申請專利_ &quot;員之方法,其中,該特徵頻率 係基於該製程迴路步驟之蝕刻步驟及沉積步驟的持續期間 之總和而決定。 3·如申請專利範圍帛1項之方法,其中,該製程施加 頻率係小於約5 Hz。 4. 如申請專利範圍第丨項之方法,其中,該製程迴路 更包含:每個製程迴路之多個蝕刻步驟。 5. 如申請專利範圍第1項之方法,其中,該製程迴路 更包含:每個製程迴路之多個沉積步驟。 6 如申請專利範圍第1項之方法’其中’該監視步驟 更包含:監視於複數個波長區域之電漿放射強度。 7.如申請專利範圍第6項之方法,其中,該監視複數 個波長區域之步驟更包含:執行數學運算,以求取複數個 23 1317539 頻率刀S而知·至丨j至少—個特徵頻率。 該數學運算 該等波長 該數學分1317539 Picking up and applying for a patent: This method is used to establish a plasma etching process. The method includes the following steps: 4: placing a substrate in a vacuum chamber; etching by a plasma a material from the substrate, a passivation layer is deposited on the substrate by a plasma; 'execution of repeating the etching step and the deposition step is performed to - the etching step or sink corresponding to the process loop step The characteristic frequency of the foot is set to monitor a change in the plasma radiation intensity. The process circuit step is interrupted based on the monitoring step; and the substrate is removed from the vacuum chamber. 2. The method of claiming a patent, wherein the characteristic frequency is determined based on a sum of an etching step of the process loop step and a duration of the deposition step. 3. The method of claim 1, wherein the process application frequency is less than about 5 Hz. 4. The method of claim 2, wherein the process loop further comprises: a plurality of etching steps for each process loop. 5. The method of claim 1, wherein the process circuit further comprises: a plurality of deposition steps of each process loop. 6 The method of claim 1, wherein the monitoring step further comprises: monitoring the plasma radiation intensity in the plurality of wavelength regions. 7. The method of claim 6, wherein the step of monitoring the plurality of wavelength regions further comprises: performing a mathematical operation to obtain a plurality of 23 1317539 frequency knives S and knowing at least one characteristic frequency . The mathematical operation, the wavelengths, the mathematical points 8.如申請專利範圍帛7項之方法,其中 係快速傅立葉變換。 中’ s亥監視複數 ’以修正一背景 9·如申請專利範圍第7項之方法,其 個波長區域之步驟更包含··執行數學運算 電漿放射。 10.如申請專利範圍第6項之方法,其中 區域係透過5亥電漿放射光譜之數學分析而選取 ^U.如申請專利範圍第10項之方法,其中 析係主要分量分析。 12'種用於偵測分時多工製程中的不同材料之間 轉釔之方法,該方法係包含下列步驟: 、 置放一基板於一真空室之中· 執行該分時多工製程; 以—對應於製程迴路步驟之蝕刻步驟或沉積步驟的重 複率之特徵頻率而監視於一電漿放射強度之變化;8. The method of claim 7, wherein the fast Fourier transform is used. In the 'sho monitoring complex number' to correct a background. 9. As in the method of claim 7, the steps of the wavelength region further include performing a mathematical operation on plasma radiation. 10. The method of claim 6, wherein the region is selected by the mathematical analysis of the radiation spectrum of the 5th plasma, and the method is as described in claim 10, wherein the main components are analyzed. 12' method for detecting transition between different materials in a time division multiplexing process, the method comprising the steps of: placing a substrate in a vacuum chamber; performing the time division multiplexing process; Monitoring the change in the radiation intensity of a plasma corresponding to the characteristic frequency of the repetition rate of the etching step or the deposition step of the process loop step; 基於該監視步驟而中斷該分時多工製程;及 自該真空室而移除該基板。 13.如申請專利範圍第12項之方法,其中,該特徵頻 率係基於該分時多工製程之步驟的持續期間之總和而決定 14. 如申請專利範圍第a項之方法,其中,該特徵頻 率係小於約5 Hz。 15. 如申請專利範圍第12項之方法,其中,該監視步 24 1317539 驟更包合:監視於複數個波長區域之電漿放射強度。 16. 如申請專利範圍第15項之方法,其中,該監視複 數個波長區域之步驟更包含:執行數學運算,以求取複數-個頻率分量而得到至少一個特徵頻率。 17. 如申凊專利範圍第丨6項之方法其中,該數學運 算係快速傅立葉變換。 18. 如申請專利範圍第16項之方法,其中,該監視複 數個波長區域之步驟更包含:執行數學運算,以修正一背 景電漿放射。 | 19. 如申請專利範圍第15項之方法,其中,該等波長 區域係透過該電漿放射光譜之數學分析而選取。 20. 如申請專利範圍第IQ項之方法,其中,該數學分 析係主要分量分析。 拾壹、圈式: 如次頁。 鲁 25The time division multiplex process is interrupted based on the monitoring step; and the substrate is removed from the vacuum chamber. 13. The method of claim 12, wherein the characteristic frequency is determined based on a sum of durations of the steps of the time division multiplexing process. 14. The method of claim a, wherein the feature The frequency system is less than about 5 Hz. 15. The method of claim 12, wherein the monitoring step 24 1317539 is further included: monitoring the plasma radiation intensity in the plurality of wavelength regions. 16. The method of claim 15, wherein the step of monitoring the plurality of wavelength regions further comprises: performing a mathematical operation to obtain a plurality of frequency components to obtain at least one characteristic frequency. 17. The method of claim 6, wherein the mathematical operation is a fast Fourier transform. 18. The method of claim 16, wherein the step of monitoring the plurality of wavelength regions further comprises: performing a mathematical operation to correct a background plasma radiation. 19. The method of claim 15, wherein the wavelength regions are selected by mathematical analysis of the plasma emission spectrum. 20. The method of claim 12, wherein the mathematical analysis is a primary component analysis. Pick up, circle: as the next page. Lu 25
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