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TW466593B - CVD TiN plug formation from titanium halide precursors - Google Patents

CVD TiN plug formation from titanium halide precursors Download PDF

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Publication number
TW466593B
TW466593B TW089107861A TW89107861A TW466593B TW 466593 B TW466593 B TW 466593B TW 089107861 A TW089107861 A TW 089107861A TW 89107861 A TW89107861 A TW 89107861A TW 466593 B TW466593 B TW 466593B
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Taiwan
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precursor
tin
patent application
scope
substrate
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TW089107861A
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Chinese (zh)
Inventor
John J Hautala
Johannes F M Westendorp
Takenao Nemoto
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Tokyo Electron Ltd
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    • H10P14/43
    • H10W20/01
    • H10W20/056

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  • Chemical Vapour Deposition (AREA)
  • Electrodes Of Semiconductors (AREA)

Abstract

A method of depositing high quality titanium nitride (TiN) films and filling small contacts having high aspect ratio features using TiN. The method uses a CVD process with titanium tetraiodide (TiI4) as a precursor material. The method allows TiN films with a thickness greater than about 0.3 μm to be deposited without cracking. For sufficiently high TiN deposition rates and sufficiently low TiN resistivities the preferred process temperature is at least about 500 DEG C. The method varies process pressure to obtain a seamless TiN plug fill in high aspect ratio structures.

Description

4 6 659 3 五、發明說明(υ 名蒼明範圍 本發明係關於積電路板之形成作用,並特別是來自鹵化 钬之氮化鈦膜之化學蒸氣沉積作用。 發明背景 積體電路板提供在電子設計中信號傳輸之路徑。在設計 中的積體電路板(ic)由許多包含在半導體基板的矽底層中 的活性晶體管組成的◊為了增加I C容量,故在基板的石夕底 層中的一個活性晶體管與在基板的石夕底層中的另一個活性 晶體管之間進行與金屬”網線"的大量交互連結。經由切入 基板之洞、道或溝進行電路板的交互連結,整體已知是金 屬交互連結。實際上與矽底層接觸之特殊的金屬連結點已 知是接觸點。洞、道或溝之其餘部份以稱為接點柱塞之導 電物質填充。因為晶體管密度持續增加,形成較高層級的 積體電路板,接點柱塞之直徑必須降低,以容許增加的交 互連結量、多層金屬化結構及較高的縱橫比之道。 直徑大於約0. 1 6微米之道典型係以如下方式填充。先利 用或CVD或PVD沉積約100埃之鈦(Ti)襯墊=該Ti層增強至 矽底層之電子接點。接著以將約5 0 0埃之氮化鈦(T i N )襯墊 沉積在T i層上。沉積作用可以是或C V D或P V D,以具有低壓 CVD(LPCVD)較佳,因為只有LPC VD會提供保形性,將其定 義成確實會再產生下層基板之表面形態學之能力,必須覆 蓋具有高縱橫比之亞微細粒結構之底部及側壁。T i層具有 金屬擴散阻擋物的作用,以避免T i在後續來自WF6之鎢(ff ) 沉積期間氟(F )的腐蝕浸蝕。T1 N也具有成為W之黏著層的4 6 659 3 V. Description of the invention (υ Name Cangming Scope The invention relates to the formation of printed circuit boards, and in particular the chemical vapor deposition of hafnium halide titanium nitride films. BACKGROUND OF THE INVENTION Integrated circuit boards are provided in Signal transmission path in electronic design. The integrated circuit board (ic) in the design is composed of many active transistors contained in the silicon substrate of the semiconductor substrate. To increase the IC capacity, one of the The active transistor and another active transistor in the Shi Xi bottom layer of the substrate make a large number of interactive connections with the metal "network cable". The circuit board is interactively connected through the hole, track or groove cut into the substrate, which is generally known as Intermetallic connection. In fact, the special metal connection point that is in contact with the bottom layer of silicon is known as the contact point. The rest of the hole, channel or trench is filled with a conductive substance called a contact plunger. As the density of transistors continues to increase, the formation of For higher-level integrated circuit boards, the diameter of the contact plunger must be reduced to allow for increased amounts of interconnections, multilayer metallization, and higher The aspect ratio aspect. The diameter greater than about 0.16 microns is typically filled in the following manner. First, a titanium (Ti) liner of about 100 angstroms is deposited by CVD or PVD = the Ti layer is reinforced to the underlying silicon substrate for electrical connection Point. Next, a titanium nitride (T i N) liner of about 500 angstroms is deposited on the Ti layer. The deposition can be either CVD or PVD, and it is better to have low pressure CVD (LPCVD) because only LPC VD will provide conformality, which is defined as the ability to indeed reproduce the surface morphology of the underlying substrate, which must cover the bottom and side walls of a submicron structure with a high aspect ratio. The Ti layer functions as a metal diffusion barrier To avoid the corrosion and etching of fluorine (F) during the subsequent deposition of T i from tungsten (ff) from WF6. T1 N also has an adhesion layer that becomes W

4 6 659 3 五、發明說明(2) 作用,因為W不會黏附於金屬氧化物上》雖然T i N提供極佳 的接點阻擋物,但是,T i N必須具有成為有效的阻擋物之 厚度(約5 0 0埃)。如果T i N厚度小於約5 0 0埃,T i金屬會擴 散至矽中。然後以C V D沉積之W填充其餘部份。利用W是因 為在形成接點柱塞時其低電阻係數及期可信賴度。W層提 供低電阻區,其在目前的I C導點性上具有重要性。接著將 接點柱塞表面浸蝕或磨光。生成之平面化表面是極佳的金 屬交互連結所必需的,並因此是極佳的I C功能所必需的。 晶體管密度持續增加,部件持續變小,即具有〇. 2 5微米 或更小的直徑。接點柱塞之直徑必須降低,以容許增加交 互連結數。但是,關於具有直徑小於約0 . 1 6微米之道,接 點柱塞金屬層之電阻受到T i N擴散阻擋層支配。因為T i N阻 擋層就當成擴散阻擋層的健全性能而言必須維持在約5 0 0 埃,接著會減少以W填充之接點柱塞部位。例如,具有 0 . 1 5微米直徑之結構可能具有W膜或在柱塞中央僅約3 0 0埃 之”核心"。因此,有效的柱塞電阻更會受到較高的電阻係 數TiN支配,更重要地是介於TiN與W層之間的界面電阻。 接著後續以W填充接點柱塞會提供接點柱塞無顯著效果 之整體電阻性之額外的程序步驟。此外,可以取消形成I C 的處理步驟,並只以T i N之接點柱塞填充道可以增加製造 效率,更甚於以TiN及W。因此,需要以CVD形成TiN接點柱 塞及取消在I C形成作用中的接點柱塞之W層之方法。 但是,以CVD沉積之T i N膜具有相對的高應力。具有高應 力之膜具有高強度之内分布力或力之組成,以抵抗膜之體4 6 659 3 V. Description of the invention (2) Function, because W will not adhere to metal oxides. "Although T i N provides an excellent contact barrier, T i N must have the ability to become an effective barrier. Thickness (about 50 0 Angstroms). If the T i N thickness is less than about 500 Angstroms, the T i metal will diffuse into the silicon. The remainder was then filled with CVD deposited W. W is used because of its low resistivity and reliability when forming a contact plunger. The W layer provides a low-resistance region, which is important in current IC conductance. The contact plunger surface is then etched or polished. The resulting planarized surface is required for excellent metal interaction and is therefore required for excellent IC functionality. The transistor density continues to increase, and the components continue to become smaller, that is, having a diameter of 0.25 microns or less. The diameter of the contact plunger must be reduced to allow for an increased number of interconnections. However, with respect to the way having a diameter of less than about 0.16 micrometers, the resistance of the metal layer of the contact plunger is dominated by the T i N diffusion barrier layer. Because the T i N barrier layer must be maintained at about 500 angstroms in terms of its sound performance as a diffusion barrier layer, the contact plunger portion filled with W will then be reduced. For example, a structure with a diameter of 0.15 micrometers may have a W film or only about 300 Angstroms in the center of the plunger. Therefore, the effective plunger resistance will be dominated by a higher resistivity TiN, More importantly, the interface resistance between TiN and W layers. Subsequent filling of the contact plunger with W will provide an additional procedural step of the overall resistivity of the contact plunger without significant effects. In addition, the formation of the IC can be eliminated Processing steps, and filling the track with only the T i N contact plunger can increase the manufacturing efficiency, even more than TiN and W. Therefore, it is necessary to form the TiN contact plunger by CVD and eliminate the contact in the IC formation function. Method to point the W layer of the plunger. However, the T i N film deposited by CVD has a relatively high stress. The film with high stress has a high strength internal distribution force or a composition of forces to resist the body of the film

4 6 659 3 五、發明說明(3) 積或形狀的改變,在膜受到外力時。高應力限制可沉積的 最大膜厚度。典型地是以CVD沉積之TiN膜之最大厚度是約 8 0 0埃,大於熟知的第一層氧化物。厚度超過約8 0 0埃之 TiN膜開始裂化,因為膜中的内應力之故。出現在TiN膜表 面上及定義成表面物質中的不連續狀之微裂化大至足以增 加膜之電阻,因此造成I C的非最佳性能。 雖然W層的絕對厚度可根據欲填充之道尺寸而改變,但 是其相對厚度是約8 0 %之道直徑。這是因為沉積膜不僅填 充具有接點柱塞之道的體積,而且也必須填充在接點柱塞 之”凹陷'’。將"凹陷”定義成在T i N中的成穴作用,其是在 道的填充期間形成的,以在柱塞頂端沉積更多的T i N消除 凹陷,生成封口層。因此,就0 . 2 5微米之部件而言,需要 具有2000埃(0.8 x2500埃)厚度之TiN膜。關於好的柱塞填 充,具有持續性、徹底的保形性及無缝性的這些膜厚度也 是重點。保形膜是一種確實會再產生下層基板之表面形態 學之膜。無縫膜是一種無裂化膜。 在指派於東京電子有限公司(Tokyo Electron Limited) 及全文併入本文以供參考之美國專利申請案序號第 08/964, 532號中揭示以TiN柱塞及以TiN層封口填充在基板 中的道之CVD法。利用TiCl4先質之CVD法之現有TiN沉積作 用沒有這些特色。關於TiCl4先質,在厚度超過約5 0 0 - -8 0 0埃時,則膜會均勻裂化。裂化是不可接受的,因為其 會防礙膜至下層之黏著性,造成膜之”片落π及因此危及後 續的處理。裂化也增加柱塞預期的電阻係數。4 6 659 3 V. Description of the invention (3) The product or shape changes when the membrane is subjected to external force. High stress limits the maximum film thickness that can be deposited. The maximum thickness of a TiN film typically deposited by CVD is about 800 Angstroms, which is larger than the well-known first layer oxide. TiN films with a thickness exceeding about 800 Angstroms begin to crack due to internal stresses in the films. The discontinuous microcracking that occurs on the surface of the TiN film and is defined as a surface material is large enough to increase the resistance of the film, thus causing non-optimal performance of the IC. Although the absolute thickness of the W layer can be changed according to the size of the track to be filled, the relative thickness is about 80% of the track diameter. This is because the deposited film not only fills the volume with the contact plunger, but also must be filled in the "depression" of the contact plunger. The "depression" is defined as the cavitation in T i N, which It is formed during the filling of the track to deposit more T i N on the tip of the plunger to eliminate pits and create a sealing layer. Therefore, for a component of 0.25 micrometers, a TiN film having a thickness of 2000 Angstroms (0.8 x 2500 Angstroms) is required. Regarding good plunger filling, these film thicknesses with continuous, thorough shape retention and seamlessness are also important. A conformal film is a film that does reproduce the surface morphology of the underlying substrate. Seamless film is a non-cracking film. U.S. Patent Application Serial No. 08/964, 532, assigned to Tokyo Electron Limited and incorporated herein by reference in its entirety, discloses a track filled with a TiN plunger and a TiN layer seal in a substrate. The CVD method. The existing TiN deposition using the TiCl4 precursor CVD method does not have these features. With regard to the TiCl4 precursor, when the thickness exceeds about 5 0-8 0 0 Angstroms, the film will crack uniformly. Cracking is unacceptable because it prevents the film from adhering to the underlying layer, causing the film to fall π and thus endangering subsequent processing. Cracking also increases the expected resistivity of the plunger.

O:\64\64000.PTD 第7頁 4 6 659 3 五、發明說明¢4) 因此,需要一種以Τ ί N膜之高品質保形性接點柱塞填充 高縱橫比之道之方法,不會裂化。這種膜可消除W沉積步 驟,並因此減少填充接點之處理步驟程序。這可以顯示出 會明顯降低設計製造之成本。 本發明的概述 最終及根據本發明的原理,其係揭示一種以T i Ν柱塞高 縱橫比之道及消除鎢(W)沉積步驟之方法。以C V D使來自碘 化鈦(T i I )先質沉積T i N柱塞。較佳的T i I先質是四碘化鈦 (T i 14)及以熱C V D沉積。 本發明也專注於以C V D沉積之T i N層完全填充具有小於約 0 . 1 6微米直徑之高縱橫比之道之方法。 本發明也專注於以Ti 14先質提供之TiN層之CVD形成在1C 道中之接觸柱塞之方法。該道是具有小於約〇. 1 6微米直徑 之高縱橫比之道。 根據本發明填充接點柱塞之T i N膜保有1 0 0 %在下層之形 態學。具有1 0 〇 %保形性之膜是有利的,因為其確實會再產 生下層基板之表面形態學,其容許最佳的I C功能。因此, 本方法適用於完全填充高縱橫比之部件。本方法的另一個 好處是消除沉積W的單獨處理步驟,同時節省時間及費 用。本方法也排除將W層黏附於T i N之問題。由以下伴隨的 圖形及其說明會使得本發明的這些及其它目的及優點魬而 易見。 圖形的概要說明 圖1是化學蒸氣沉積作用(CVD)之裝置圖示。O: \ 64 \ 64000.PTD Page 7 4 6 659 3 V. Description of the invention ¢ 4) Therefore, there is a need for a method of filling a high aspect ratio with a high-quality conformal contact plunger of Τ N film, Does not crack. This film eliminates W deposition steps and therefore reduces the number of process steps required to fill the contacts. This can show a significant reduction in design and manufacturing costs. SUMMARY OF THE INVENTION Finally and in accordance with the principles of the present invention, it is disclosed a method for eliminating the tungsten (W) deposition step by using a high aspect ratio of the T i N plunger. The T i N plunger was deposited with C V D from titanium iodide (T i I) precursor. The preferred T i I precursor is titanium tetraiodide (T i 14) and is deposited with thermal C V D. The present invention also focuses on a method of completely filling a TiN layer deposited in CVD with a high aspect ratio having a diameter of less than about 0.16 microns. The present invention also focuses on a method of contacting a plunger formed in a 1C channel by CVD of a TiN layer provided by a Ti 14 precursor. The track is a track having a high aspect ratio with a diameter of less than about 0.16 microns. The T i N film filling the contact plunger according to the present invention has a morphology of 100% in the lower layer. A film with 100% conformality is advantageous because it does reproduce the surface morphology of the underlying substrate, which allows for the best IC function. Therefore, this method is suitable for completely filling high aspect ratio parts. Another benefit of this method is that it eliminates the separate processing steps for depositing W, while saving time and money. This method also eliminates the problem of sticking the W layer to T i N. These and other objects and advantages of the present invention will be readily apparent from the accompanying drawings and descriptions thereof. BRIEF DESCRIPTION OF THE FIGURES Figure 1 is a diagram of a chemical vapor deposition (CVD) apparatus.

O:\64\64000.PTD 第8頁 修正4 6 65 9 3 修正 號 89107861 五、#明說明IB) 圊2是比較以鹵化鈦(TiX)為主之氮化鈦(TiN)膜中的應 力之圖形。 圖3是以碘化鈦(Til4)為主之TiN膜之SEM照片。 圖4 A及4B是以T i鹵化物為主之T i N膜之傳遞電子顯微照 像。 圖5是以C V D在1 . 5托壓力下沉積之T i N沉積1 0 : 1縱橫比結 構之SEM照片。 圖6是以C V D在1 . 0托壓力下沉積之T i N沉積1 0 : 1縱橫比結 構之SEM照片。 圖7是利用本發明及T i、T i N及鎢柱塞填充之接點電阻數 據之圖形。 圖示符號簡單說明 10 表示一化學蒸氣沉積(C VD )系統; 11 表示一CVD反應室; 12 表示一先質傳送系統; 13 表示一先質氣體來源; 1 4 表示一氣體出口; 15 表示一計量系統; 16 表示一氣體入〇 ; 20 表示一真空室; 21 表示一真空壓迫式室壁; 22 表示一基板支撐物或受體; 23 表示一半導體晶圓; 24 表示一真空泵; 25 表示一入口氣體來源;O: \ 64 \ 64000.PTD Page 8 Correction 4 6 65 9 3 Correction No. 89107861 V. #Explanation IB) 圊 2 is the stress in a titanium nitride (TiN) film based on titanium halide (TiX). Its graphics. FIG. 3 is a SEM photograph of a TiN film mainly composed of titanium iodide (Til4). 4A and 4B are transmission electron micrographs of a T i N film dominated by T i halides. Figure 5 is a SEM photograph of a Ti: N deposited 10: 1 aspect ratio structure with CVD deposited at a pressure of 1.5 Torr. Figure 6 is a SEM photograph of a Ti: N deposited 10: 1 aspect ratio structure with CVD deposited at 1.0 Torr. Fig. 7 is a graph of contact resistance data filled with the present invention and T i, T i N and a tungsten plunger. Brief description of the symbols 10 indicates a chemical vapor deposition (C VD) system; 11 indicates a CVD reaction chamber; 12 indicates a precursor transport system; 13 indicates a precursor gas source; 1 4 indicates a gas outlet; 15 indicates a Metering system; 16 means a gas inlet; 20 means a vacuum chamber; 21 means a vacuum pressure chamber wall; 22 means a substrate support or receiver; 23 means a semiconductor wafer; 24 means a vacuum pump; 25 means a Inlet gas source;

O:\64\64000.ptc 第9頁 2001.08. 23. 009 4 6 65 9 3案號89107861_qp年汶月曰 修正 五、發明說明(6) 26 表示一氣體來源; 27 表示一惰性氣體來源; 28 表示一喷射頭; 3 0 表示一密封的蒸發氣; 31 表示一圓筒狀蒸發室; 32 表示一垂直定向軸; 33 表示一圓筒壁; 34 表示一内表面; 35 表示一平坦的圓形封閉底部; 3 6 表示一蓋子; 37 表示一凸緣環; 38 表示一高溫容限的真空相容性金屬封口; 39 表示一載體氣體之來源; 40 表示一先質塊; 4 1 表示一真空泵; 42 表示一表面; 4 4 表示一加熱器; 45 表示一單獨的受控制加熱器; 46 表示一環狀凹陷的空氣間隔; 4 7 表示一環繞於同心圓外鋁壁或罐; 48 表示一矽酮泡棉絕緣物環狀層; 50 表示一傳送管; 51 表示一擋板; 52 表示一圓孔; 53 表示一控制閥;O: \ 64 \ 64000.ptc Page 9 2001.08. 23. 009 4 6 65 9 3 Case No. 89107861_qp Year of the Moon Rev. V. Description of Invention (6) 26 indicates a gas source; 27 indicates an inert gas source; 28 Indicates a spray head; 30 indicates a sealed evaporation gas; 31 indicates a cylindrical evaporation chamber; 32 indicates a vertical orientation axis; 33 indicates a cylindrical wall; 34 indicates an inner surface; 35 indicates a flat circular closed bottom 36 indicates a lid; 37 indicates a flange ring; 38 indicates a high-temperature tolerance vacuum-compatible metal seal; 39 indicates a source of carrier gas; 40 indicates a precursor block; 4 1 indicates a vacuum pump; 42 Indicates a surface; 4 4 indicates a heater; 45 indicates a single controlled heater; 46 indicates an annular recessed air gap; 4 7 indicates a concentric outer aluminum wall or can; 48 indicates a silicone Foam insulation ring layer; 50 represents a transfer tube; 51 represents a baffle; 52 represents a round hole; 53 represents a control valve;

O:\64\64000.ptc 第9a頁 2001.08. 23.010 4 6 89107861 五、發明說明(7) 54 表示一關閉閥; 55 ,56,57與58表示一壓力感應器: 6〇 表示一控制is ’以及 g I 表示一不易變之記憶體。 _細說明 在化學蒸氣沉積法(C VD)中’或利用熱能或電能將氣體 先質活化。一旦活化之後’氣體先質會以化學方式反應形 成膜。在圖1中例證較佳的C VD方法,並揭示在由 Westendorp等人在與本專利申請案同日提出申請及指派於 東京電子有限公司以將蒸氣由固態來源傳送至化學蒸氣沉 積室之裝置及方法(APPARATUS AND METHOD FOR DELIVERY OF VAPOR FROM SOLID SOURCES TO A CVD CHAMBER)為標 題之共同審理之申請案中,並將其全文併入本文以供參 考。化學蒸氣沉積(CVD)系統10包括CVD反應室11及先質傳 送系統1 2。在反應室中進行反應,將鹵化欽化合物,例 如,蛾化鈇(Til)轉化成TiN之阻擋層膜。 先質傳送系統12包括具有氣體出口 14之先質氣體來源O: \ 64 \ 64000.ptc Page 9a 2001.08. 23.010 4 6 89107861 V. Description of the invention (7) 54 represents a shut-off valve; 55, 56, 57 and 58 represent a pressure sensor: 60 represents a control is' And g I represents an immutable memory. _Detailed description In chemical vapor deposition (C VD) 'or using thermal energy or electrical energy to activate gas precursors. Once activated, the 'gas precursor will chemically react to form a film. The preferred C VD method is exemplified in Figure 1, and the device and APPARATUS AND METHOD FOR DELIVERY OF VAPOR FROM SOLID SOURCES TO A CVD CHAMBER) is the subject of a co-trial application and the entire text of which is incorporated herein by reference. The chemical vapor deposition (CVD) system 10 includes a CVD reaction chamber 11 and a precursor transfer system 12. The reaction is carried out in a reaction chamber to convert a halogenated ammonium compound, for example, Til, into a barrier film of TiN. The precursor delivery system 12 includes a precursor gas source having a gas outlet 14

〇:\64\64〇〇〇,ptc 第9b頁 2001. 08. 23.011 j η 65 9 3案號89107861 11]年0月>^曰 修正_ 五、發明說明(8) 1 3,將其經由具有氣體入口 16之計量系統1 5傳輸至CVD反 應室U中。來源1 3會產生來自個別的T i I化合物(以T i 14較 佳)之先質氣體,例如,T 1 I蒸氣。化合物在標準溫度及壓 力是一種固體狀態。以控制在將產生預期的先質蒸氣壓力 之溫度下加熱的方式(較佳)維持先質來源。較佳地是蒸氣 壓力是一種其本身足以將先質蒸氣傳送至反應室11,不使 用載體氣體較佳。計量系統1 5維持來自來源1 3之先質氣體 蒸氣以足以維持在反應室中以合乎經濟的方式能進行CVD 法之速度流入反應室11中。 反應室11是一種通常熟知的CVD反應器及包括以真空壓 迫式室壁21為邊界之真空室20。在室20中安置支撐基板, 如半導體晶圓23之基板支撐物或受體22。將室20維持在適 合於將臈,如TiN阻擋層沉積在半導體晶圓基板23上之CVD 反應性能之真空下。較佳的壓力範圍是0 . 2 - 5. 0托。以控 制真空泵2 4及包括傳送系統1 2和也包括在進行T i還原反應 中使用的例如氩(H2)、氮(N2)或氨(NH3)之還原氣體來源26 與如氬氣(Ar)或氦氣(He)之類的氣體之惰性氣體來源27之 入口氣體來源2 5等的操作維持真空。將來自來源2 5之氣體 經由位於與基板2 3對立的室20的一個末端(通常平行於及 朝向基板23)之喷射頭28進入室20中。 先質氣體來源13包括密封的蒸發器30,其包括具有垂直 定向軸3 2之圓筒狀蒸發室3 1。以高溫容限及非腐蝕性物質 (如合金INCONEL 600)構成的圓筒壁33為室31的邊界,其 内表面34經高度磨光及具有平滑性。壁33具有平坦的圓〇: \ 64 \ 64〇〇〇, ptc page 9b 2001. 08. 23.011 j η 65 9 3 case number 89107861 11] 0 years > ^ said amendment _ V. Description of the invention (8) 1 3 It is transferred into the CVD reaction chamber U via a metering system 15 having a gas inlet 16. Source 13 generates precursor gases from individual T i I compounds (preferably T i 14), for example, T 1 I vapor. The compound is in a solid state at standard temperature and pressure. The precursor source is maintained (preferably) in a manner that controls heating at a temperature that will produce the expected precursor vapor pressure. It is preferred that the vapor pressure is such that it is sufficient to transfer precursor vapor to the reaction chamber 11 without using a carrier gas. The metering system 15 maintains the precursor gas from the source 13 and the vapour flows into the reaction chamber 11 at a rate sufficient to be maintained in the reaction chamber and capable of performing the CVD method economically. The reaction chamber 11 is a generally known CVD reactor and includes a vacuum chamber 20 bounded by a vacuum pressure chamber wall 21. A support substrate, such as a substrate support or acceptor 22 of a semiconductor wafer 23, is placed in the chamber 20. The chamber 20 is maintained under a vacuum suitable for the CVD reaction performance of depositing a radon, such as a TiN barrier layer, on the semiconductor wafer substrate 23. The preferred pressure range is 0.2-5.0 Torr. In order to control the vacuum pump 24 and the delivery system 12 and also include a reducing gas source 26 such as argon (H2), nitrogen (N2) or ammonia (NH3) used in carrying out the T i reduction reaction, and such as argon (Ar) Or an inert gas source 27 such as a gas such as helium (He), the inlet gas source 25, and the like are maintained in a vacuum. The gas from the source 25 is introduced into the chamber 20 through an ejection head 28 located at one end of the chamber 20 opposite the substrate 23 (usually parallel to and toward the substrate 23). The precursor gas source 13 includes a sealed evaporator 30 including a cylindrical evaporation chamber 31 having a vertical orientation axis 32. A cylindrical wall 33 made of a high temperature tolerance and a non-corrosive substance (such as alloy INCONEL 600) is the boundary of the chamber 31. The inner surface 34 is highly polished and smooth. The wall 33 has a flat circle

O:\64\64000.ptc 第10頁 2001.08. 23.012 4 6 65 9 |號 89107861 «^革月 y 曰 修正 --------- ' 7 五、發明說明(9) 形封閉底部3 5及開口頂端’將其以與壁3 3相同的熱容限及 非腐蝕性物質的蓋子36密封。來源13的出口14位於蓋子36 中。在使用高溫時’如關於T i 14或T a B r 5 ’則將蓋子3 6密封 成凸緣環3 7,以高溫容限的真空相容性金屬封口 3 8 (如以C 形鎳管環繞INCONEL線圈彈簧構成的HELICOFLEX)將凸緣環 整合至壁33頂端。關於TaCl5及TaFs,則可利用熟知的彈性 體0-環封口 38密封蓋子。 經由蓋子36連結至容器31的是載體氣體之來源39,以惰 性氣體(如He或Ar)較佳《來源1 3包括一塊在容器31底部的 先質物質,如T i I ’以T i 14較佳,將其以在標準溫度及壓 力下的固體狀態裝入容器31中。以其中的Til固體塊密封 容器的方式將Til蒸氣裝入容器31中。將Tii當成先質塊4〇 供應’將其放置在容器31底部,在此加熱,以加熱成液體 狀態較佳’只要生成的蒸氣壓力是在可接受的範圍内。在 先質塊40是液體之處’則蒸氣會位於液體塊4〇高度之上。 因為壁33是垂直的圓筒,如果>111塊4〇是液體,則其表面 積會維持固定,無關於T i I的消耗高度。氣體與蒸汽可藉 真空泵41自容器31中抽空。 傳运系統12未受限於直接傳送先質4 〇,可在替換方式中 二起傳送先質40與來自氣體來源⑼可引入容器31之載 趙=:這樣的氣體可以是氣氣(Η」或惰性氣體,如氦氣 或氩氣Ur)。在利用栽體氣體之處,可將其引入容器 # ί於分布於先質塊40的整個頂端表面上,或可將 !•、桃^ =益3 1中、’以便於經由先質塊4 〇自容器3 1底部3 5向 政'> 透,以達到先質塊4〇以最大的表面積曝露於載體O: \ 64 \ 64000.ptc Page 10 2001.08. 23.012 4 6 65 9 | No. 89107861 «^ leather month y said correction -------- '7 V. Description of the invention (9) Shaped closed bottom 3 5 and the opening top 'seal it with a lid 36 of the same thermal tolerance and non-corrosive substance as the wall 33. The outlet 14 of the source 13 is located in the lid 36. When using high temperature, 'if it is T i 14 or T a B r 5', the cap 3 6 is sealed into a flange ring 37, and a vacuum-compatible metal seal 3 8 (such as a C-shaped nickel tube) HELICOFLEX, which consists of an INCONEL coil spring, integrates a flange ring to the top of the wall 33. With regard to TaCl5 and TaFs, the lid can be sealed with a well-known elastomer 0-ring seal 38. Connected to the container 31 via the lid 36 is a source 39 of carrier gas, preferably an inert gas (such as He or Ar). The source 13 includes a precursor material at the bottom of the container 31, such as T i I 'T i 14 Preferably, it is charged into the container 31 in a solid state at a standard temperature and pressure. Til vapor is charged into the container 31 in such a manner that the Til solid block is sealed therein. Supply Tii as a precursor block 40 and supply it and place it on the bottom of the container 31, and heat it here to heat it to a liquid state. As long as the generated vapor pressure is within an acceptable range. Where the precursor block 40 is liquid 'then the vapor will be above the liquid block 40 height. Because the wall 33 is a vertical cylinder, if the > 111 block 40 is a liquid, its surface area will remain fixed regardless of the consumption height of T i I. Gas and steam can be evacuated from the container 31 by a vacuum pump 41. The transport system 12 is not limited to the direct delivery of precursors 40. Two alternatives can be used to transfer precursors 40 and gas from the source 载 can be introduced into the container 31. Zhao =: Such a gas can be a gas (Η) Or an inert gas such as helium or argon Ur). Where the plant gas is used, it can be introduced into the container # ί distributed on the entire top surface of the precursor block 40, or can be! • 、 桃 ^ = 益 3 1 中, 'to facilitate the passage of the precursor block 4 〇 Penetrate from container 3 1 bottom 3 5 '> to reach the precursor block 40 and expose the carrier with the maximum surface area

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2001.08. 23.013 丄6 659各號89】迟迎和年p月4曰 條正_ 五、發明說明(10) j 氣體L還有另一種替換方式是將容器31中的液體蒸發。但 这些替換方式加入不希望的微粒及不提供以直接傳送 先質達到的控制的傳送速度,即不利用載體氣體傳送。因 此’以直接傳送先質較佳。 為了維持f容器3 1中的先質4 〇溫度,則將壁3 3的底部3 5 維持與加熱器4 4的熱傳輸,以維持先質4 〇在受控制的溫度 下丄以大於其溶點較佳,其會在缺少載體氣體下(即直接 傳送系統)產生大於約3托之蒸氣壓力,並在利用載體氣體 時會產^較低的蒸氣壓力,如約!托。確實的蒸氣壓力係 根據其它變異而定’如載體氣體量及基板23的表面積等。 在Τι I。的直接傳送系統中,特別是Ti,這樣的溫度是在 約180 °C至190 °C的範圍内。溫度不應該高至造成喷射頭28 t的氣體過早反應或另外在與晶圓23接觸之前。 就實施例的目的而言,採取18〇〇c的溫度是供加熱容器 31,部35的控制溫度。該溫度適合於以Tii4先質產生預期 的洛氣壓力。在容器31底部35提供該溫度,以避免先質蒸 ^在容器31壁33及蓋子36上濃縮,以熱接觸蓋子36外側之 單$的受控制加熱器45使蓋子維持在比在壁33底部35的加 熱器44更兩的溫度,例如,i90°C 。以容納在室壁33與環 繞於同心圓外鋁壁或罐4 7之間的環狀凹陷的空氣間隔4 6環 繞室壁33侧面。將罐47再以矽酮泡棉絕緣物48環狀層環 繞。在溫度範圍介於180 °C至190。(:及壓力大於約3托(以大 於5托較佳)之預期實施例t ’維持排列的該溫度會維持蒸 氣在以蓋子36、壁33側面及先質塊4〇表面42為邊界之容器2001.08. 23.013 丄 6 659 each number 89] Chi Ying and the year p. 4th article Zheng _ V. Description of the invention (10) j There is another alternative way of gas L is to evaporate the liquid in the container 31. These alternatives, however, add undesirable particles and do not provide a controlled transfer speed achieved by direct delivery of precursors, i.e. without carrier gas transfer. Therefore, it is better to use the direct delivery precursor. In order to maintain the temperature of the precursor 40 in the f container 31, the bottom 3 5 of the wall 3 3 is maintained in heat transfer with the heater 44 to maintain the precursor 40 at a controlled temperature so as to be greater than its solubility. The point is better, it will produce a vapor pressure greater than about 3 Torr in the absence of a carrier gas (ie, a direct delivery system), and will produce a lower vapor pressure when using a carrier gas, as about! Care. The exact vapor pressure depends on other variations, such as the amount of carrier gas and the surface area of the substrate 23. At Ti I. In direct transfer systems, especially Ti, such temperatures are in the range of about 180 ° C to 190 ° C. The temperature should not be so high as to cause the gas of the ejection head 28 t to react prematurely or otherwise before contacting the wafer 23. For the purpose of the embodiment, a temperature of 180 ° C is taken as the control temperature for heating the container 31, 35. This temperature is suitable to produce the expected Roh pressure with the Tii4 precursor. This temperature is provided at the bottom 35 of the container 31 to prevent the precursors from condensing on the wall 33 and the lid 36 of the container 31, and the lid is maintained at a lower temperature than the bottom of the wall 33 by a controlled heater 45 in thermal contact with the outside of the lid 36 The heater 44 of 35 is more than two temperatures, for example, i90 ° C. An air gap 4 6 is received around the side of the chamber wall 33 with an annular recessed air space contained between the chamber wall 33 and a concentric outer aluminum wall or tank 4 7. The tank 47 is then surrounded by a ring-shaped layer of silicone foam insulation 48. In the temperature range between 180 ° C and 190. (: And the expected embodiment t where the pressure is greater than about 3 Torr (preferably greater than 5 Torr), the temperature maintained in the arrangement will maintain the steam in a container bounded by the lid 36, the side of the wall 33, and the surface 40 of the precursor block 40

O:\64\64000.ptc 2001.08. 23.014 第12頁 4 6 6 5 9 3 五、發明說明(9) 31體積内。適合於維持預期壓力之溫度會隨主要包含成為 组或iS化组化合物之先質物質改變。 蒸氣流動計量系統1 5包括至少1 / 2英吋直徑或至少I 0毫 米内直徑之傳送管5 0,並以更大較佳,以便於在預期的流 動速度下提供不會有任何壓力降,其具有每分鐘至少約2 至40標準立方公分(seem)。傳送管50會自先質氣體來源 i3(以其上游末端連接至出口 14)廷伸至反應室(以其下游 末端連接至入口16)。也將自蒸發器出口 14至反應器入口 16之整個傳送管長度與反應器室20之噴射頭28以大於先質 物質4 0之蒸發溫度加熱較佳,例如,加熱至1 9 5 °C。 在傳送管50中提供位於圓孔52中央之擋板51 ,其以具有 約0 . 0 8 9英吋直徑較佳。以控制閥5 3調節自表1 5 6至表2 5 7之壓力降。在控制閥5 3之後經過圓孔5 2及進入反應室1 1 之該壓力降大於約1 0毫托,並將與流動速度成比例。在介 於蒸發器1 3出口 1 4與控制閥5 3之間的線5 0中提供關閉閥 5 4 ,以關閉蒸發器1 3容器3 1 。 在系統1 0中提供壓力感應器5 5 - 5 8,以提供訊息至用於 控制系統1 0之控制器60,其包括控制自傳送系統1 5至CVD 反應室11之室20内的先質氣體流動速度。壓力感應器包括 連接至介於蒸發器1 3出口 1 4與關閉閥5 4之間的傳送管5 0之 感應器5 5 ,以監控在蒸發容器3 1中的壓力。將壓力感應器 5 6連接至介於控制閥5 3與擋板5 1之間的傳送管5 0,以監控 圓孔52之上游壓力,同時將壓力感應器57連接至介於擋板 51與反應器入口 16之間的傳送管50,以監控圓孔52之下游O: \ 64 \ 64000.ptc 2001.08. 23.014 Page 12 4 6 6 5 9 3 V. Description of the invention (9) Within 31 volumes. The temperature suitable for maintaining the desired pressure will vary depending on the precursor material that mainly contains the compound that is the group or the iS group. The vapor flow metering system 15 includes a transfer tube 50 of at least 1/2 inch diameter or at least 10 mm inner diameter, and is preferably larger so as to provide no pressure drop at the expected flow rate, It has at least about 2 to 40 standard cubic centimeters per minute. The transfer tube 50 extends from the precursor gas source i3 (connected to the outlet 14 at its upstream end) to the reaction chamber (connected to the inlet 16 at its downstream end). It is also preferable to heat the entire transfer pipe length from the evaporator outlet 14 to the reactor inlet 16 and the ejection head 28 of the reactor chamber 20 at an evaporation temperature greater than that of the precursor substance 40, for example, to 19 5 ° C. A baffle 51 located in the center of the circular hole 52 is provided in the transfer tube 50 and preferably has a diameter of about 0.089 inches. Use the control valve 5 3 to adjust the pressure drop from Table 1 5 6 to Table 2 5 7. The pressure drop through the circular hole 5 2 and into the reaction chamber 11 after the control valve 53 is greater than about 10 mTorr and will be proportional to the flow velocity. A shut-off valve 5 4 is provided in a line 50 between the outlet 14 of the evaporator 13 and the control valve 53 to close the evaporator 13 container 3 1. A pressure sensor 5 5-5 8 is provided in the system 10 to provide a message to the controller 60 for controlling the system 10, which includes a precursor for controlling the self-conveying system 15 to the chamber 20 of the CVD reaction chamber 11 Gas flow speed. The pressure sensor includes a sensor 5 5 connected to a transfer pipe 50 between the outlet 14 of the evaporator 13 and the closing valve 54, to monitor the pressure in the evaporation vessel 31. Connect the pressure sensor 5 6 to the transfer pipe 50 between the control valve 53 and the baffle 51 to monitor the upstream pressure of the circular hole 52, and connect the pressure sensor 57 to the baffle 51 and A transfer tube 50 between the reactor inlets 16 to monitor downstream of the round hole 52

O:\64\64000.PTD 第13頁 466593 五、發明說明(ίο) 壓力。將另一個壓力感應器58連接至反應室之室20 ,以監 控在CVD室20中的壓力。 以回應由感應器5 5 - 5 8感應之壓力之控制器6 0達到控制 進入反應室1 1之CVD室2 0之先質蒸氣流動,特別是決定越 過圓孔之壓力降之感應器56及57。在使得經過圓孔52之先 質蒸氣流動不會抗流動之條件時,則經由傳送管5 2之實際 壓力蒸氣流動是由壓力感應器5 6及5 7監控之壓力的作用, 並可自在圓孔5 2的上游側面上之感應器5 6測量之壓力對在 圓孔5 2的下游側面上之感應器5 7測量之壓力比測定。 在使得經過圓孔5 2之先質蒸氣流動會抗流動之條件時, 則經由傳送管5 2之真實的壓力蒸氣流動只是由壓力感應器 5 7監控之壓力的作用。在任何實例中,以處理條件說明之 控制器6 0可測定存在的抗流動或非抗流動。在以控制器 6 0進行測定時*可經由計算的控制器6 0測定先質氣體的流 動速度。 較佳地是自貯存在以控制器6 0取得的不易變之記憶體6 1 中之查詢表或擴程表之訂正之流動速度數據計算先質氣體 真實的流動速度。在測定先質氣體真實的流動速度時,以 一或數個可變圓孔控制閥5 3之密閉線圈回饋控制、經由抽 空泵24或控制降低來自來源2 6及27之惰性氣體之CVD室壓 力或以控制由加熱器44、45控制之室31内先質氣體之蒸氣 壓力可維持預期的流動速度。 廣泛地使用純度9 9. 9 9 %之Ti 14。其在室溫下(18 °C-2 2 °C )是紫黑色固體,具有約1 5 0 °c的熔點及具有濕度敏感O: \ 64 \ 64000.PTD Page 13 466593 V. Description of the invention (ίο) Pressure. Another pressure sensor 58 is connected to the chamber 20 of the reaction chamber to monitor the pressure in the CVD chamber 20. The controller 60 responding to the pressure sensed by the sensors 5 5-5 8 reaches the precursor vapor flow entering the CVD chamber 2 1 of the reaction chamber 1 1, especially the inductor 56 and the pressure drop that determines the pressure drop across the circular hole 57. In the condition that the precursor vapor flow through the circular hole 52 is not resistant to flow, the actual pressure vapor flow through the transfer tube 52 is the effect of the pressure monitored by the pressure sensors 56 and 57, and can be freely rounded. The ratio of the pressure measured by the sensor 56 on the upstream side of the hole 5 2 to the pressure measured by the sensor 57 on the downstream side of the circular hole 5 2 is determined. In the condition that the precursor vapor flow through the circular hole 5 2 is resistant to flow, the actual pressure vapor flow through the transfer tube 52 is only the effect of the pressure monitored by the pressure sensor 57. In any instance, the controller 60, described in terms of processing conditions, can determine the presence or absence of anti-flow. When measuring with the controller 60 *, the flow velocity of the precursor gas can be measured via the calculated controller 60. Preferably, the true flow velocity of the precursor gas is calculated from the corrected flow rate data stored in the lookup table or extended range table stored in the non-volatile memory 6 1 obtained by the controller 60. When measuring the true flow velocity of precursor gas, use the closed coil feedback control of one or several variable circular hole control valve 53, reduce the CVD chamber pressure of inert gas from sources 26, 27 through the evacuation pump 24 or control Or, by controlling the vapor pressure of the precursor gas in the chamber 31 controlled by the heaters 44, 45, the desired flow velocity can be maintained. Ti 14 with a purity of 99.9% is widely used. It is a purple-black solid at room temperature (18 ° C-2 2 ° C), has a melting point of about 150 ° C, and is humidity sensitive

O:\64\64000.PTD 第14頁 4 6 G 5 Q ^ _。0 案號89107861 彳。年尸月日 修正_ ' y 五、發明說明(13) 性。根據圖1的展示,將固態T i 14先質物質4 0密封在使先 質物質表面積達到最大的圓筒狀抗腐腐蝕性金屬容器31 中。將來自或T i 14之蒸氣以高導電傳送系統接傳送至反應 室1 1内,即不利用載體氣體。將反應室1 1加熱至至少約 1 ο 〇 °c的溫度,以避免蒸氣濃縮或副產物沉積。為了精確 控制沉積膜之厚度,故希望不使用載體氣體。 為了獲得大於約3托(以大於5托較佳)的充份的蒸氣壓 力,故將固態T i 14先質加熱至約1 8 0 °C - 1 9 0 °C的溫度範 圍,以完成將T i 14蒸氣經控制直接傳送至反應室11内。需 要以該壓力維持越過在南導電傳送系統中限定圓孔之固定 壓力降,同時在約0. 1-2.0托為範圍的操作下將至多約50 seem之Til4先質傳送至處理室。為獲得該壓力的溫度就 Ti 14 而言是185 °C。 利用平行板RF放電,在此啟動的電極是氣體傳送喷射 頭,並以晶圓或基板23之受體或臺階是RF接地。將Ti 14蒸 氣與在已加熱至溫度介於約300 °C- 500 °C之基板上的含氨 (NH3)的處理氣體組合。可使用或單獨或組合的氬(Ar)、 氮(N2)、氫(H2)及氦(He)當成處理氣體。 以來自Ti 14先質之TiN膜沉積作用之要求如下。沉積溫 度必須低於約6 5 0 °C,以維護在基板或晶圓2 3上的下層物 質之完整性。沉積速度必須大於每分鐘約3 0 0埃,以提供 可接收的輸出量。可改變室壓力,以獲得預期的膜厚度。 例如,以3000 seem之NH3及25 seem之Til4(不使用載體氣 體)在約5 5 0 °C的晶圓溫度下,以約2 . 0托之壓力會O: \ 64 \ 64000.PTD P.14 4 6 G 5 Q ^ _. 0 Case number 89107861 彳. Year corpse month day correction _ 'y V. Description of invention (13). According to the display of Fig. 1, the solid Ti 14 precursor substance 40 is sealed in a cylindrical anticorrosive metal container 31 which maximizes the surface area of the precursor substance. The vapor from or Ti 14 is transferred to the reaction chamber 11 by a highly conductive transfer system, that is, no carrier gas is used. The reaction chamber 11 is heated to a temperature of at least about 1 ° C to avoid vapor concentration or by-product deposition. In order to precisely control the thickness of the deposited film, it is desirable not to use a carrier gas. In order to obtain a sufficient vapor pressure greater than about 3 Torr (preferably greater than 5 Torr), the solid Ti 14 precursor is heated to a temperature range of about 180 ° C-190 ° C to complete the process. The Ti 14 vapor is controlled to be sent directly into the reaction chamber 11. This pressure needs to be maintained to maintain a fixed pressure drop across the circular hole defined in the south conductive transmission system, while at the same time transmitting up to about 50 seem of Til4 precursor to the processing chamber under the operation of about 0.1-2.0 Torr. The temperature to obtain this pressure is 185 ° C in the case of Ti 14. Utilizing parallel plate RF discharge, the electrode activated here is a gas transfer jet, and the receiver or step of the wafer or substrate 23 is RF grounded. The Ti 14 vapor is combined with an ammonia (NH3) -containing process gas on a substrate that has been heated to a temperature between about 300 ° C and 500 ° C. Argon (Ar), nitrogen (N2), hydrogen (H2), and helium (He) can be used as a process gas or alone or in combination. The requirements for TiN film deposition from the precursor of Ti 14 are as follows. The deposition temperature must be lower than about 6 50 ° C to maintain the integrity of the underlying material on the substrate or wafer 2 3. The deposition rate must be greater than about 300 Angstroms per minute to provide an acceptable output. The chamber pressure can be changed to obtain the desired film thickness. For example, with NH3 of 3000 seem and Til4 of 25 seem (without carrier gas) at a wafer temperature of about 5 50 ° C, a pressure of about 2.0 Torr will

O:\64\64000.ptc 第15頁 2001.08. 27.017 4 6 659 3 五、發明說明(12) 得到每分鐘約5 0 0〜6 0 0埃為範圍之沉積速度。在這些相同 =件了,以約U托之髮力會得到每分鐘約綱埃之沉積 速度及以約1. 0托之壓力會得到每分鐘約15〇埃之沉積速 m」必須小於約1x1 〇ia達因,平方公分及具有大於約 接八=ί ί化極限◊沉積獏之電阻係數以小於約25Q微歐 hi A二^ 。膜應該在鬲縱橫比結構中展現出1 0 0 %保形 本文使用的高縱橫比結構具有大於約8. 〇及至多 : ί包括具有10_0或甚至更高的縱橫比之結構。 > #有ί、孔或溝等。後續的沉積膜,如鋁(a υ膜不 Λ,。在膜中必須有少量雜質,理想上是小 量、,如H e ° Λ最後,必須使用在商業上合理的處理氣體 置’如He、Ar、η2及心。 浐Ϊ ϋ中Δ供使CVD…膜沉積之較佳的範圍,以括弧内 ^ \条件。Slin代表以每分鐘計之標準公升及W/cm2 疋母千方公分計之瓦特。O: \ 64 \ 64000.ptc Page 15 2001.08. 27.017 4 6 659 3 V. Description of the invention (12) The deposition rate in the range of about 50 to 60 angstroms per minute is obtained. In these same cases, a deposition rate of about Angstroms per minute will be obtained with a force of about U Torr and a deposition rate of about 15 Angstroms per minute at a pressure of about 1.0 Torr must be less than about 1x1 〇ia dyne, square centimeters and having a resistivity greater than about 8 八 ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ ◊ 貘 电阻 The resistivity to less than about 25Q micro-ohm hi A 2 ^. The film should exhibit 100% conformality in a 鬲 aspect ratio structure. The high aspect ratio structures used herein have greater than about 8.0 and at most: ί includes structures having an aspect ratio of 10_0 or even higher. ># 有 ί, 孔 或 沟 etc. Subsequent deposition of films, such as aluminum (a υ film is not Λ). There must be a small amount of impurities in the film, ideally a small amount, such as He e ° Λ Finally, a commercially reasonable processing gas must be used, such as He , Ar, η2, and the heart. Ϋ Δ is the best range for CVD ... film deposition, in brackets ^ \ conditions. Slin stands for standard liters per minute and W / cm2 疋 female thousand cubic centimeters Watt.

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表2 400°C-650〇C(55〇r) V儿仅速度 一確+1 ---- 跡300埃/分鐘(300埃份簕 腰JJ 1-15X109達因/平方公分《,達因/平方公分) 無裂化之膜厚度 >4000 埃 電画sg — 85*400微歐姆公分(<200微歐姆公分) 0.5-5原子%(<2原子%) 需要的處理氣體… ------_ ~5-40 seem Til4(25 seem T1I4) 第16頁 466593 五、發明說明(13) 根據本發明Ti 14先質經CVD沉積之TiN膜符合所有的預期 標準,未在後續的沉基A 1層上出現裂化,並在具有縱橫比 甚至大於1 0 . 0之部件中展現1 0 0 %保形性。較高的沉積溫度 造成較低的電阻係數,較低的殘留碘濃度及較高的沉積速 度,未犧牲保形性及裂化極限。 根據本發明利用T i丨4先質沉積之T i N膜具有比利用其它 鹵化钽先質(如T i C 14)沉積之T i N膜更大的裂化極限。圖2 是比較以Ti 14及1^(:14為主之TiN膜之裂化應力。圓形代表 在5 8 0 °C下自T i C 14先質沉積之T i N膜。三角形代表在5 5 0 °C 下自Ti 14先質沉積之TiN膜。箭頭代表在TiCl4膜中發現裂 化的點。以急速降低的膜應力(以達因/平方公分測定)及 少許降低的膜厚度(以埃測定)對應於蔓延的裂化。 根據圖2的展示,以T i C 14為主的膜就小於約1 0 0 0埃之厚 度而言展現出快速降低的膜應力。在大於約6 0 0埃之膜上 利用以T i C 14為主的先質沉積之T i N膜之掃描式電子顯微照 像(SEM)上觀察到蔓延的裂化。在具有厚度大於4 0 0 0埃之 T i 14膜中的任合點上未發現裂化證據。圖3根據本發明沉 積之2 0 0 0埃無裂化之以Ti 14為主之TiN膜及以其填充之溝 的掃描式電子顯微照像(S E Μ )。在二氧化矽層6 2上沉積— 2 0 0 0 埃之 T i Ν 膜 6 0。 與利用以TiCl4先質沉積之ΊΊΝ膜比較,就利用以Ti 14先 質沉積之T i N膜較大的裂化極限而言,一個原因是在膜中Table 2 400 ° C-650 ° C (55 ° r) V is only +1 speed ---- trace 300 angstroms / minute (300 angstroms of waist JJ 1-15X109 dyne / cm2 ", Dyne / Cm²) Non-cracked film thickness> 4000 Angstroms sg — 85 * 400 microohm centimeters (< 200 microohm centimeters) 0.5-5 atomic% (< 2 atomic%) required processing gas ...- ----_ ~ 5-40 seem Til4 (25 seem T1I4) Page 16 466593 V. Description of the invention (13) According to the present invention, the TiN film deposited by the CVD of Ti 14 precursor meets all the expected standards. Cracking occurred on Shenji A 1 layer, and showed 100% shape retention in parts with aspect ratios even greater than 10.0. Higher deposition temperature results in lower resistivity, lower residual iodine concentration, and higher deposition rate without sacrificing shape retention and cracking limits. A TiN film deposited using the Ti4 precursor according to the present invention has a larger cracking limit than a TiN film deposited using other tantalum halide precursors, such as TiC14. Figure 2 compares the cracking stress of TiN films with Ti 14 and 1 ^ (: 14 as the main component. The circle represents the T i N film deposited from the T i C 14 precursor at 5 80 ° C. The triangle represents 5 TiN film deposited from Ti 14 precursor at 50 ° C. Arrows indicate the points where cracking was found in the TiCl4 film. Rapidly reduced film stress (measured in dyne / cm2) and slightly reduced film thickness (in angstroms) (Measurement) corresponds to spreading cracking. According to the display of FIG. 2, the film based on TiC14 exhibits a rapidly decreasing film stress for a thickness of less than about 100 Angstroms. At a thickness of more than about 600 Angstroms Spreading cracking was observed on scanning electron microscopy (SEM) of a T i N film predominantly deposited with T i C 14 on the film. T i having a thickness greater than 4 0 0 Angstroms was observed. No evidence of cracking was found at any of the joints in the 14 film. Figure 3 Scanning electron micrograph of a Ti 14 film mainly composed of Ti 14 without cracking and deposited in accordance with the present invention and filled with trenches (SE M). Deposited on the silicon dioxide layer 62-2 0 0 Angstrom T i N film 60. Compared with the ΊΊN film deposited with the TiCl4 precursor, the use of Ti 14 For the larger cracking limit of the T i N film deposited by the precursor, one reason is that

O:\64\64000.PTD 第17頁 4 6 6 5 9 3 五、發明說明(14) 本質上較小的粒子尺寸。與由較大的T i N粒子組成的膜比 較,由小粒子矩陣組成的膜可能展現出裂化繁衍。圖4是 分別在5 5 0 °C及5 8 0 °C下沉積利用以T i 14及了 i C丨4為主之先質 以根據本發明之C V D沉積之T i N膜之傳遞電子顯微照像 (TEM)。根據在圖4的展示,以丁丨14為主之膜具有實質上較 小的粒子。較小的粒子侵於以T i 14為主之T i N膜知裂化極 限的可能原因11 根據圖5及圖6的展示,在所有其它條件相同時,膜的保 形性係根據在具有高縱橫比部件之結構中的處理壓力有 關。這些條件如下:5 5 0 °C的溫度、3 s 1 m之N H3流動及2 5 sccro之1^14流動。圖5是以CVD在1.5托壓力下沉積之TiN填 充1 0 : 1縱橫比結構之SEM照片。圖6是以CVD在1 . 0托壓力下 沉積之T i N填充1 0 : 1縱橫比結構之SEM照片。 在高縱橫比結構中,需要以非常高度的飽和方法形成不 具有M鑰匙孔"之好柱塞。當在道中形成接觸柱塞之沉積的 T i N未完全填充道,則會發生”鑰匙孔效應,留下不含T i N 之稱為鑰匙孔之區域。當道具有實質上垂直的壁時,即壁 實質上垂直於底座時,則會發生該效應。在具有斜壁的道 中,則可排除鑰匙孔效應。發現需要以降低至小於約1. 5 托之處理壓力填充這些結構,同時維持約3 s 1 m NH3及2 5 seem Til4之氣體流動。好的柱塞填充有可能是在較低的 流速下,但是只會犧牲沉積速度。反之,較高的沉積速度 可能具有比在表2中陳述的那些流速高。 圖7展示電試驗結構的接點電阻數據。根據本發明,將O: \ 64 \ 64000.PTD Page 17 4 6 6 5 9 3 V. Description of the invention (14) The particle size is essentially small. Compared with a film composed of larger T i N particles, a film composed of a matrix of small particles may exhibit crack propagation. Fig. 4 shows the electron transfer of Ti Ni film deposited by CVD according to the present invention using the precursors based on T i 14 and i C 丨 4 deposited at 5 50 ° C and 5 80 ° C, respectively. Microphotograph (TEM). According to the display in Fig. 4, the film mainly composed of D14 has substantially smaller particles. The possible reasons for the smaller particles to invade the T i N film, which is dominated by T i 14 The processing pressure in the structure of the aspect ratio component is related. These conditions are as follows: a temperature of 5 50 ° C, a flow of N H3 of 3 s 1 m, and a flow of 1 ^ 14 of 2 5 sccro. Fig. 5 is an SEM photograph of a TiN filled 10: 1 aspect ratio structure deposited by CVD at a pressure of 1.5 Torr. FIG. 6 is a SEM photograph of a Ti: N filled 10: 1 aspect ratio structure deposited by CVD at 1.0 Torr. In a high aspect ratio structure, it is necessary to form a good plunger without an M-key hole in a very highly saturated method. When the T i N formed in the track contacting the plunger does not completely fill the track, a "keyhole effect" will occur, leaving an area called the keyhole without T i N. When the track has a substantially vertical wall, That is, the effect occurs when the wall is substantially perpendicular to the base. In channels with inclined walls, the keyhole effect can be eliminated. It was found that these structures need to be filled with a processing pressure reduced to less than about 1.5 Torr while maintaining about 3 s 1 m NH3 and 2 5 seem Til4 gas flow. Good plunger filling may be at a lower flow rate, but it will only sacrifice the deposition rate. Conversely, higher deposition rates may have a higher rate than in Table 2. The stated flow rates are high. Figure 7 shows the contact resistance data of the electrical test structure. According to the present invention,

O:\64\64000.PTD 第18頁 466593 五、發明說明(15) ^ 來自Ti I*先質沉積之Ti及TiN枉塞(實心圓)與利用Ti I先質 沉積典型的Ti/Tin與W柱塞填充之柱塞(空心圓)比較。接 點尺寸是0 _ 3微米及縱橫比是4 : 1。根據圖7的展示,以τ 土 及TiN取代一般的Ti、TiN及W層填充接點柱塞會造成相同 的接點電阻。這暗示以減少金屬界面更補償自W成為T丨N所 增加之整體物質電阻。 因此以T i I*之柱塞填充法是一種在I C設計的形成作用中 取代目前的W柱塞之可行方法。利用本發明之接觸電阻與 標準的W柱塞相同。這是值得注意地,總之TiN之整體電阻 比W大15至20倍,其具有10微歐姆公分之電阻係數《這強 調單一法與減少柱塞中的界面數的優點。 以本發明的方法沉積之膜展示出I C形成作用的特徵化重 要性。膜具有對低交互連結抗阻而言足夠低的電阻係數, 沉積速度對輸出考量而言足夠了(大於100埃/分鐘),並可 沉積厚度大於0. 3微米之膜,沒有裂化。可利用本發明的 方法填充直徑小至0. 1 5微米及縱橫比大於1 0 : 1之部件。 當然在申請書中展示及說明的本發明具體實施例只是使 本技藝熟練的發明者做為參考的具體實施例,並不是以做 為限制。例如,可以PECVD沉積Ta膜,可以熱CVD、PECVD 及電漿處理熱C V D沉積T a Nx膜,如分別在來自鹵化鈕先質 進行Ta 薄膜之PECVD(PECVD OF Ta FILMS FROM TANTALUM HALIDE PRECURSORS)、來自齒化钽先質之TaN薄膜之熱CVD (THERMAL CVD OF TaN FILMS FROM TANTALUM HALIDE PRECURSORS)、來自函化钽先質進行的TaN膜之電漿增強O: \ 64 \ 64000.PTD Page 18 466593 V. Description of the invention (15) ^ Ti and TiN plugs (filled circles) from Ti I * precursor deposition and the typical Ti / Tin with Ti I precursor deposition and Comparison of W plunger filled plungers (hollow circles). The contact size is 0 _ 3 microns and the aspect ratio is 4: 1. According to the display in Fig. 7, replacing general Ti, TiN and W layers with τ soil and TiN to fill the contact plunger will result in the same contact resistance. This implies that reducing the metal interface more compensates for the overall increase in material resistance from W to T, N. Therefore, the plunger filling method with T i * is a feasible method to replace the current W plunger in the formation of the IC design. The contact resistance using the present invention is the same as a standard W plunger. It is worth noting that, overall, the overall resistance of TiN is 15 to 20 times greater than W, which has a resistivity of 10 micro-ohm centimeters, which emphasizes the advantages of a single method and reduces the number of interfaces in the plunger. The films deposited by the method of the present invention show the importance of characterizing the formation of IC. The film has a resistivity sufficiently low for low cross-link resistance, a deposition rate sufficient for output considerations (greater than 100 Angstroms / minute), and a film having a thickness greater than 0.3 micron without cracking. The method of the present invention can be used to fill components with a diameter as small as 0.15 microns and an aspect ratio greater than 10: 1. Of course, the specific embodiments of the present invention shown and described in the application are only specific embodiments for the inventors skilled in the art as a reference, and are not intended to be limiting. For example, Ta films can be deposited by PECVD, and T a Nx films can be deposited by thermal CVD, PECVD, and plasma treatment. For example, PECVD OF Ta FILMS FROM TANTALUM HALIDE PRECURSORS for Ta thin films from halogenated precursors. THERMAL CVD OF TaN FILMS FROM TANTALUM HALIDE PRECURSORS

O:\64\64000.PTD 第19頁 466593 五、發明說明(16) CVD (PLASMA ENHANCED CVD OF TaN FILMS FROM TANTALUM HAUDE PRECURSORS)及來自i化組先質之Ta薄 膜之電渡處理熱CVD (PLASMA TREATED THERMAL CVD OF TaN FILMS FROM TANTALUM HALIDE PRECURSORS)巾之揭 示,全部是由Hautala及Westendorp發明及指定予東京電 子有限公司,並且是與本專利中請案同日提出申請之共同 審理申請案,並特別將其全文併入本文以供參考。根據另 一個實施例,可將以CVD沉積來自鹵化鈕先質之T i N用於枉 塞形成作用,如在為標題之共同審理申請案中之揭示,其 是由Hautala等人發明及指定予東京電子有限公司,與本 專利申請案同日提出申請,並特別將其全文併入本文以供 參考。而且,可以C V D沉積T a / T a Nx雙層,並可根據本發明 將TaNx用於柱塞填充,如分別在以來自鹵化钽先質之CVD Ta 及 TaNx 膜之整合作用(INTEGRATION OF CVD Ta AND TaNx FILMS FROM TANTALUM HALIDE PRECURSORS)及以來自鹵化 鈕先質之CVD TaNx柱塞形成作用(CVD TaNx PLUG FORMATION FROM TANTALUM HALIDE PRECURSORS)令之揭 示,兩者係由Hautala及Westendorp發明及指定予東京電 子有限公司,與本專利申請案同曰提出申請之共同審理申 請案,並特別將其全文併入本文以供參考。因此,可以不 違背本發明的精神及以下的申請專利範圍下進行或再分_類 這些具體實施例的各種變化、改良或替換。O: \ 64 \ 64000.PTD Page 19 466593 V. Description of the invention (16) CVD (PLASMA ENHANCED CVD OF TaN FILMS FROM TANTALUM HAUDE PRECURSORS) and electrothermal treatment thermal CVD (PLASMA) TREATED THERMAL CVD OF TaN FILMS FROM TANTALUM HALIDE PRECURSORS), all of which were invented and designated by Tokyo Electronics Co., Ltd. by Hautala and Westendorp, and are jointly reviewed applications filed on the same day as the application for this patent, and in particular It is incorporated herein by reference in its entirety. According to another embodiment, T i N from a halide neoprene precursor can be deposited by CVD for congestion formation, as disclosed in the co-trial application under the title, which was invented and designated by Tokyo Electronics Co., Ltd. filed an application on the same day as this patent application, and the entire contents thereof are specifically incorporated herein by reference. Furthermore, T a / T a Nx bilayer can be deposited by CVD, and TaNx can be used for plunger filling according to the present invention, such as the integration of CVD Ta and TaNx films from tantalum halide precursors (INTEGRATION OF CVD Ta AND TaNx FILMS FROM TANTALUM HALIDE PRECURSORS) and CVD TaNx PLUG FORMATION FROM TANTALUM HALIDE PRECURSORS order, both of which were invented by Hautala and Westendorp and designated by Tokyo Electron Limited The company co-examined the application with the patent application, and specifically incorporated the entire text of this application for reference. Therefore, various changes, improvements, or replacements of these specific embodiments can be made or sub-classified without departing from the spirit of the present invention and the scope of the following patent applications.

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Claims (1)

4 6 659 3 案號 89107861 4年俨月曰 修正 六'申請專利範圍 1. 一種填充具有在其中沉積鈦(Ti)膜之基板中的部件之 方法,其包含將T i _化物先質以加熱至足以使該先質蒸發 之溫度,以提供該先質之蒸氣至含有該基板之反應室内, 接著將該蒸氣與含有氮氣之處理氣體組合,以化學蒸氣沉 積(CVD)沉積該TiN的方式沉積鹵化鈦(TiN)。 2. 根據申請專利範圍第1項之方法,其中該部件具有大 於8 . 0之縱橫比。 其中該部件具有大 其令該鹵化敛先質 其中將該基板加熱 其中以約5-40 seem 其中以約1 0 0 - 6 0 0埃 其f該含氮氣之氣 其中該氨氣具有以 1其中該方法是熱 3. 根據申請專利範圍第1項之方法 於約0 . 1 6微米之直徑。 4. 根據申請專利範圍第1項之方法 是四碘化鈦(Ti 14)。 5. 根據申請專利範圍第4項之方法 至約4 0 0 °C - 6 5 0 °C為範圍的溫度。 6. 根據申請專利範圍第4項之方法 為範圍的速度提供該先質。 7. 根據申請專利範圍第4項之方法 /分鐘為範圍的速度沉積該TiN。 8. 根據申請專利範圍第1項之方法 體是氨氣。 9. 根據申請專利範圍第8項之方法 約3 s 1 m為範圍的流速。 1 0.根據申請專利範圍第1項之方法 CVD 法。 1 1. 一種在反應室中的基板的高縱橫比部件中提供保形4 6 659 3 Case No. 89107861 Rev. 6 of the 4th year of the 'Amendment Patent Application Scope 1. A method of filling a component in a substrate having a titanium (Ti) film deposited therein, which includes heating a T i _ compound precursor to heat A temperature sufficient to vaporize the precursor to provide the precursor vapor into a reaction chamber containing the substrate, and then combine the vapor with a nitrogen-containing processing gas to deposit the TiN by chemical vapor deposition (CVD) Titanium halide (TiN). 2. The method according to item 1 of the scope of patent application, wherein the component has an aspect ratio greater than 8.0. Wherein the part has a large precursor to make the halogenated condensate therein, the substrate is heated therein to about 5-40 seem among which about 1 0 0-6 0 0 angstroms thereof f the nitrogen-containing gas wherein the ammonia gas has 1 in which This method is thermal 3. The method according to item 1 of the patent application range is about 0.16 microns in diameter. 4. The method according to item 1 of the scope of patent application is titanium tetraiodide (Ti 14). 5. According to the method in the scope of patent application No. 4 to a temperature of about 4 0 ° C-6 5 0 ° C. 6. Provide the precursor to the speed of the scope according to the method of scope 4 of the patent application. 7. Deposition the TiN at a rate in the range of 4 per minute of the method of patent application. 8. The method according to item 1 of the scope of patent application is ammonia. 9. The method according to item 8 of the scope of patent application. The flow velocity in the range of about 3 s 1 m. 10. Method according to item 1 of the scope of patent application CVD method. 1 1. A conformation provided in a high aspect ratio component of a substrate in a reaction chamber O:\64\64000.ptc 第丨頁 2001. 08. 23. 024 '4 6 659 t號 89107861 _年t月巧曰_修正 六、申請專利範圍 性無縫氮化鈦(T 1 N )柱塞之方法,其包含在該室中小於1. 5 托之壓力,同時在足以使該先質蒸發之溫度下將四碘化鈦 提供至該室,接著將該蒸氣與在約5-40 seem為範圍之流 動下之含有氮氣之處理氣體組合,以化學蒸氣沉積法沉積 該TiN。 12. —種積體電路基板,其包含以在來自Ti鹵化物先質 之T i膜上沉積之保形性無縫Τ ί N膜填充之高縱橫比部件, 該T i Ν膜能夠支撐以約1 - 1 5 X 1 09達因/平方公分為範圍之應 力及具有以約8 5 - 4 0 0微歐姆公分為範圍之電阻。 13. 根據申請專利範圍第12項之基板,其中該TiN膜具有 至少約4000埃之厚度。 其中該TiN膜具有 其中該T i _化物 其中以將該T i鹵 1 4.根據申請專利範圍第1 2項之基板 小於約2原子%之雜質。 1 5.根據申請專利範圍第1 2項之基板 先質是四碘化鈦。 1 6.根據申請專利範圍第1 2項之基板 化物先質加熱至足以使其蒸發的方式提供至反應室,接著 將該蒸氣與含有氮氣之處理氣體組合,並以化學蒸氣沉積 法在該基板上沉積該TiN。O: \ 64 \ 64000.ptc Page 丨 2001. 08. 23. 024 '4 6 659 t No. 89107861 _year t month Qiao Yue _ Amendment 6. Application for patent scope seamless titanium nitride (T 1 N) column A method of plugging, comprising a pressure in the chamber of less than 1.5 Torr, while providing titanium tetraiodide to the chamber at a temperature sufficient to evaporate the precursor, and then applying the vapor with about 5-40 seem The TiN is deposited by a chemical vapor deposition method for a combination of process gas containing nitrogen under a flowing range. 12.-A integrated circuit substrate comprising a high aspect ratio component filled with a shape-preserving seamless T film deposited on a Ti film derived from a Ti halide precursor, the T i Ν film being capable of supporting A stress in the range of about 1-1 5 X 1 09 dyne / cm 2 and a resistance in the range of about 8 5-4 0 microohms. 13. The substrate according to item 12 of the application, wherein the TiN film has a thickness of at least about 4000 angstroms. Wherein the TiN film has the T i _ compound wherein the T i halide 1. The substrate according to item 12 of the patent application scope is less than about 2 atomic% impurities. 1 5. The substrate precursor according to item 12 of the scope of patent application is titanium tetraiodide. 16. The substrate compound precursor according to item 12 of the scope of the patent application is heated to provide sufficient evaporation to the reaction chamber, and then the vapor is combined with a processing gas containing nitrogen, and the substrate is chemically vapor-deposited on the substrate. This TiN is deposited on. O:\64\640GO.ptc 第2頁 2001.08. 23. 025O: \ 64 \ 640GO.ptc Page 2 2001.08. 23. 025
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