200902741 九、發明說明: 【發明所屬之技術領域】 …申凊案主㈣下專獅請案的優先權:美國專利臨時 申請號60/915,967’申請曰2〇〇7年5月*曰,及美國專利 申請號11/937,164,申請曰2〇〇7年u月8曰,該等文件 全二内容以引用方式併入本文中以用於所有有。 【先前技術】 此蟄中習知電子工業中用於物理氣體沉積(pvD)的賤擊 目標的物理特性大大地影響所製薄膜的最終特性,事實 上’有助於增強高品質薄膜裝置及電路結構製造的目標特 性是: 細小且均勻細粒結構; 该等個別顆粒的隨機及均勻隨機結晶定向; 以在觀規模觀看時遍及該目標的整個本體大體上不變的一 微結構; 可自一目標複製到另一目標的一微結構;及 大體上100%岔貫及提供顆粒間高強度結合的一微結構。 尤其在鈕(Ta)及鈮(Nb)目標中極難得到此等特性,此起 因於高純度鈕及鈮是經由電子束融化及澆鑄到冷水冷卻模 中加以提煉及純化的事實。形成的鑄模具有許多極大顆 粒,其長寬皆以公分乘公分來測量。這些極大顆粒需要大 里且ep貝的熱機處理以減低顆粒尺寸,及減低個別顆粒的 結晶對齊(減低紋理)。熱機處理在減低顆粒尺寸、所產生 隨機結晶及所產生微結構的均勻中有限度,通常自鑄模產 200902741 的目祆材料仍包含說成顆粒尺寸及紋理帶狀區的大程 X不句勻’其中具有—共同顆粒尺寸及紋理並非整個目標 的全部顆粒尺寸及紋理的特點。 *美國專利號6,193,821中提出此問題的重要性及大小規 =’、其中先側锻造或侧輾壓數個鑄模,接著再加以翻倒鍛 L或翻倒輾壓。美國專利公開號細川謂9 A1說明一 種衣程’其利用翻倒锻造,接著拉回锻造,然後側锻造, 及最後是父又輾壓製程,以提供具有口⑻丨與丨丨丨丨}定向 的-顆粒混合。在美國專利號6,331,233及7,iqi,447中, 發明人明確指出-複雜的三步驟製程,包含多個變形及退 火零件。雖然該複雜處理路線成功地精煉顆粒尺寸,但該 處理仍造成一主導的{111}紋理。 美國專利公開號2005/0155856 A1說明一鈕濺擊目標, 其在該目標厚度的-有限部分之上具有—優先的(222)定 向,該專利公開案聲稱改良該濺擊膜厚度的均勻。 其他專利案明白以鈕金屬粉末而非固體钽鑄模開始的固 有有利點,美國專利號5,58G,516及6,521,173說明组粉冷 壓縮成數個短金屬條,其接著可作大範圍的熱/機械製程^ 術處理,以產生可製出濺擊目標的數個完全密實短金屬 條。美國專利號6,770,154說明一粉末短金屬條強化到完 全密度’接著是健及退火,以提供__但非隨機的Z 粒結構。美國專利號7,081,148在美國專利號6,77〇,154的 該等製程之上擴充以包括一作為結果的钽濺擊目標,其是 至少99.99%純钽。 200902741 美國專利號7,067,197說明—粉末冶金製程,其在壓實 前先表面氮化短粉。接著可藉由一連串至少23個不同處理 步驟壓實該表面氮化粉末,該等處理步驟必須保留該粉末 的高含氮量。最不獲讚賞的步驟之_是噴霧沉積,但未提 及使用何類型噴霧沉積技術,即電漿噴霧、低壓電槳沉積、 火想喷霧、高速氧燃料等,它們是目前所用眾多製程中的 一些製程。 世界專利號WO 2006/117145及WO 2006/117144說明用 以產生鈕塗層的數個冷噴霧製程,該等文件以引用方式併 入本文中以用於該等冷喷霧製程的揭露。 因紐及组結合到支持板的製程皆極昂貴的事實,對用過 目標的恢復或再處理或修復亦有經濟上的興趣,再加上必 須更換整個目標前,在濺擊中只用掉一平面目標的約乃 至30%及一旋轉目標的約6〇至7〇%的事實。因此,從未 用過的鈕的收回令人極感興趣。 美國專利公開號2004/0065546 A1揭露一種氫化該鈕目 標的方法,以使鈕變脆以容許鈕與支持板分開,磨成粉末, 及再作為製造鑄模中的粉末原料使用。美國專利公開號 2006/0032735討論雷射光束及其他聚焦能源為同步炼化及 熔接粉末的使用,該粉末饋入一用過目標的磨損面積以填 補濺擊所產生的空間。當然所有這些技術產生大量熱且需 要在修復前將支持板自該目標移除,此外,如熟諳此藝者 所習知,當發生熔化時,粉末以定向方式固化及作為結果 的微結構具有堅固的紋理成分。 200902741 一目標在可使用前,必須以機器加工到最終設定尺寸, 及接著焊接、銅焊或擴散結合到一高熱傳導支持板以安裝 在濺擊機器中。 濺擊目標用以製造各式各樣的薄膜’應用範圍有窗戶玻 璃用的反射及低發射率塗層(鈮)、光生伏打膜(鉬)、窄通濾 波器(钽-鈮)等。然而它們最為人知的用途可能是在積體電 路中,其中使用層狀濺擊膜以製造基本切換裝置,以及用 以連接該等切換裝置的電路結構,用以製造功能性電子零 件(積體電路、平板顯示器等)。如上述,製造的薄膜品質, 及因此使用薄膜技術所製造的產品品質’皆高度取決於濺 擊出它們的目標的品質。 冷喷霧或動力喷霧(參閱美國專利號5,302,414、 6,502,767 及 6,759,085; Van Steenkiste 等人發表的”Analysis of Tantalum Coatings Produced by the Kinetic Spray Process (由動力喷霧製程產生之钽塗層之分析)",熱噴霧科技期 刊’第13(2)卷,2004年6月,第265至273頁;美國專 利號6,139,913及美國專利公開號2005/0120957及 2005/0252450)是一新興工業科技,其正用以解決許多工業 製造挑戰(亦參閱如美國專利號6,924,974 ; 6,444,259 ; 6,491,2〇8及6,9〇5,728)。所有以上參考文件以引用方式併 入本文中’以用於其對冷噴霧或動力噴霧的揭露。 冷喷霧利用一高速氣體噴射流以使尺寸通常大約小於 4 4微米的粉末快速地加速到高速,以便該等粉末撞擊一表 面時結合到該表面以形成〜完整、結合良好且密實的塗 200902741 層。已有人建議將鈕粉冷喷霧到各種基板(包括鋼)上(例如 參閱 Van Steenkiste 等人發表的”Anaiysis 〇f Tantaium Coaitngs Produced by the Kinetic Spray Process(由動力喷霧 製程產生之鈕塗層之分析)”,熱噴霧科技期刊,第13卷, 第2期,2004年6月,第265至273頁;Marx等人發表 的"Cold spraying - innovative layers for new applications(冷 喷霧-用於新應用之革新層)"’熱噴霧科技期刊,第15 卷’第2期,2006年6月’第177至183頁;及Gartner 等人發表的"The Cold Spray Process and its Potential for Industrial Applications(冷喷霧製程及其用於工業應用之潛 力)”,熱噴霧科技期刊,第15卷,第2期,2006年6月, 第223至232頁)。此冷噴霧不用像使用傳統熱喷霧製程一 樣必須將粉末加熱到接近或超過其熔點的溫度便完全達 成。能以低溫形成緻密塗層的事實提出許多有利點。此類 有利點包括無氧化、高密度沉積物、固態壓實、無熱引起 的應力’在此情形中尤其是無大量基板變熱。 達成動力喷霧例如能藉由將具有微粒直徑大於65微米 的组開始粉末注入一溶岩型(de Laval-type)喷嘴,以一超音 速氣流帶走,及因阻力效應而加速到高速。微粒的動能經 由塑性變形而轉變成與基板表面撞擊時的張力及熱。微粒 在製程中熔化。 在製造用於物理氣體沉積(PVD)領域的陰極或電子濺擊 目標靶心的情形中,較佳是有限的基板變熱。目標材料常 是高熔溫("TM")耐熔金屬(鈕的TM是攝氏2998度),而支 200902741 撐目標的支持板是因其高熱傳導性來選定,及通常是銅或 (,名的™疋攝氏660度),兩者皆是低熔溫材料。因此, '去使用*要將粉末加熱到或接近纽點的其他熱喷霧製 程在低炫溫支持板上沉積耐料屬。目前實施方法是使目 標完全與支持板分開,及接著使用焊接、銅焊、擴散結合 或爆炸結合技術以使目標與支持板結合-起。因冷噴霧或 動力噴霧未實質上加熱粉末,因此可用以直接在支持板上 k數個目;^ ’以及不需將目標自支持板移除便可修復用 過的目標。 【發明内容】 本發明目的造-種濺擊目標,其遍及該目標的整個 本體具有一均句細小及隨機結晶的微結構。 本發明再-目的為提供—種製程,其可具成本效益地產 生此微結構,及從—目標到另_目標地複製該結構。較 佳地’該製程不需熔化。此類製程的數個範例包括冷喷霧 或動力喷霧製程。 本發明又-目的為提供—種具成本效益的修復或恢復製 私其提供該修復目標如原有者的相同或較佳微結構。 本發明又一目的為研發-目標恢復製程,其藉由一不需 熔化的方法,如冷噴霧或動力喷霧等。 我們已發現-種不用±述複雜製程而容許直接製造具有 Ik機定向的細粒結構以通過該目標的整個厚度的技術及 數個參數&種各4直接在該支持板上製造數個具該期 望微結構的目標及料簡單地修制過目標的技術^該技 200902741 術不使用-炫化製程。此類製程的數個範例包括如㈣限 於)组粉等細金屬粉末的冷喷霧或動力喷霧。 此外’本發明提供—種濺擊方法,藉此任何上述減擊目 標作數個錢擊條件處理及藉此受賤擊。本發明中可使用任 何合適濺擊方法。合適的轉方法包括(但不限於)磁電管 激擊、脈衝雷射轉、離子束濺擊、三極體_,及其組 合。 此外’本發明提供―種濺擊目標,其包括基本上小於A* 微米的-均勻細粒結構,該濺擊目標由電子背向散射繞射 儀("EBSD”)測量時不具有較佳紋理定向(即基本上包含數 個隨歧向顆粒)’包含基本上小於44微米的數個顆粒, 及遍及該目標的本體顯示無顆粒尺寸或紋理帶狀。 此外,本發明提供_種目標,其在退火狀態中包括一各 方等大顆粒尺寸’顆粒尺寸小於開始粉末微粒尺寸。 此外,本發明提供一種具有晶狀體顆粒結構的濺擊目 標,其特徵為大體上無微粒間的擴散,由電子背向散射燒 射儀("EBSD”)測量時不具有較佳紋理定向,及遍及該目標 的本體顯示無顆粒尺寸或紋理帶狀。 此外,本發明提供-種依-添加方式製造__賤擊目標組 件的製程,其藉由在—單—步驟中,,經由_粉末嘴霧直接 在用於該目標組件的支持板上沉積該等目標材料,該沉積 物及基板以機器加工到最終目標組件設定尺寸。 本發明亦提供一種製造一薄膜的方法,包括以下步驟·· (a)濺擊上述錢擊目標; 12 200902741 (b)自該目標中移除數個金屬原子; 在一基板上形成包括上述金屬的一薄膜。 【實施方式】200902741 IX. Description of invention: [Technical field to which the invention belongs] ... the priority of the application for the singer (4) The priority of the lion's request: the US patent provisional application number 60/915,967' application 曰 2〇〇7 May*曰, and U.S. Patent Application Serial No. 11/937,164, filed on Jan. 28, the entire contents of each of which is hereby incorporated by reference. [Prior Art] The physical properties of the slamming target for physical gas deposition (pvD) in the conventional electronics industry greatly influence the final characteristics of the film produced, in fact 'helping to enhance high quality thin film devices and circuits The target characteristics of structural fabrication are: a fine and uniform fine-grained structure; a random and uniform random crystal orientation of the individual particles; a microstructure that is substantially constant throughout the entire body of the target when viewed at a viewing scale; A microstructure that is replicated to another target; and a microstructure that is substantially 100% coherent and provides high intensity bonding between the particles. Especially in button (Ta) and niobium (Nb) targets, it is extremely difficult to obtain such characteristics, which are caused by the fact that the high-purity knob and crucible are refined and purified by electron beam melting and casting into a cold water cooling mold. The resulting mold has many extremely large particles whose length and width are measured in centimeters by centimeters. These very large particles require large heat and ep shell heat treatment to reduce particle size and reduce the crystal alignment of individual particles (reduced texture). The heat treatment is limited in reducing the particle size, the random crystallization generated, and the uniformity of the resulting microstructure. Usually, the target material from the mold production 200902741 still contains the large-scale X of the particle size and the texture band. Among them, the common particle size and texture are not the characteristics of the entire particle size and texture of the entire target. * U.S. Patent No. 6,193,821 addresses the importance of this problem and the size gauge =', where the first side is forged or side-punched by several molds, followed by tipping forging or tipping. U.S. Patent Publication No. 9 A1 describes a clothing process 'which utilizes tipping forging, then pulls back forging, then side forging, and finally the father and the squeezing process to provide orientation with mouth (8) 丨 and 丨丨丨丨} - particle mixing. In U.S. Patent Nos. 6,331,233 and 7, iqi, 447, the inventors have explicitly pointed out that the complicated three-step process comprises a plurality of deformation and anneal parts. Although this complex processing route successfully refines the particle size, the process still produces a dominant {111} texture. U.S. Patent Publication No. 2005/0155856 A1 describes a button splash target having a -priority (222) orientation above the -finite portion of the target thickness, the patent publication claiming to improve the uniformity of the thickness of the splash film. Other patents understand the inherent advantages of starting with a button metal powder rather than a solid tantalum mold. U.S. Patent Nos. 5,58G,516 and 6,521,173 illustrate the cold compression of a group of powder into several short metal strips which can then be used for a wide range of heats. / Mechanical process ^ to process a number of fully dense short metal strips that produce a splash target. U.S. Patent No. 6,770,154 teaches a powdered short metal strip reinforced to full density' followed by a hardening anneal to provide a __ but non-random Z-grain structure. U.S. Patent No. 7,081,148 is extended over the processes of U.S. Patent No. 6,77, 154 to include a resulting splatter target which is at least 99.99% pure ruthenium. 200902741 U.S. Patent No. 7,067,197 describes a powder metallurgy process for surface nitriding short powder prior to compaction. The surface nitrided powder can then be compacted by a series of at least 23 different processing steps which must retain the high nitrogen content of the powder. The least appreciated step is spray deposition, but there is no mention of what type of spray deposition technology is used, namely plasma spray, low pressure paddle deposition, fire spray, high velocity oxygen fuel, etc., which are currently used in many processes. Some of the processes. World Patent Nos. WO 2006/117145 and WO 2006/117144 describe several cold spray processes for producing button coatings, which are incorporated herein by reference for use in the disclosure of such cold spray processes. The fact that the process of integrating the support board into the support board is extremely expensive is also economically interesting for the recovery or reprocessing or repair of the used target. In addition, it is only used in the splash before the entire target has to be replaced. The fact that a plane target is about 30% and a rotating target is about 6〇 to 7〇%. Therefore, the retraction of buttons that have never been used is of great interest. U.S. Patent Publication No. 2004/0065546 A1 discloses a method of hydrogenating the button to make the button brittle to allow the button to be separated from the support sheet, ground into a powder, and used as a powder material in the manufacture of the mold. U.S. Patent Publication No. 2006/0032735 discusses the use of laser beam and other focused energy sources for simultaneous refining and welding of powders that feed a used area of wear to fill the space created by splashing. Of course all of these techniques generate a large amount of heat and require the support plate to be removed from the target prior to repair. Furthermore, as is well known to those skilled in the art, when melting occurs, the powder solidifies in a targeted manner and the resulting microstructure is sturdy. Texture composition. 200902741 A target must be machined to the final set size before being used, and then welded, brazed or spread bonded to a high heat transfer support plate for installation in a splash machine. Splash targets are used to make a wide variety of films. Applications range from reflective glass for window glass to low emissivity coatings, photovoltaics (molybdenum), and narrow-pass filters (钽-铌). However, their most well-known use may be in integrated circuits in which a layered splash film is used to fabricate basic switching devices, and circuit structures for connecting the switching devices to fabricate functional electronic components (integrated circuits) , flat panel display, etc.). As mentioned above, the quality of the films produced, and thus the quality of the products produced using the film technology, are highly dependent on the quality of the target that splashes them out. Cold spray or power spray (see U.S. Patent Nos. 5,302,414, 6,502,767 and 6,759,085; "Analysis of Tantalum Coatings Produced by the Kinetic Spray Process" by Van Steenkiste et al.) ;, Journal of Thermal Spray Technology, Vol. 13(2), June 2004, pp. 265-273; US Patent No. 6,139,913 and US Patent Publication No. 2005/0120957 and 2005/0252450) is a new industrial technology To solve many of the industrial manufacturing challenges (see also, for example, U.S. Patent Nos. 6,924,974; 6,444,259; 6,491, 2, 8 and 6, 9, 5, 728), the entireties of each of Or the disclosure of a power spray. The cold spray utilizes a high velocity gas jet to rapidly accelerate a powder having a size of typically less than about 44 microns to a high speed so that the powder bonds to a surface upon impacting a surface to form a complete, bonded Good and dense coating of 200902741 layer. It has been suggested to spray the button powder on various substrates (including steel) (see, for example, Van Steenkiste, etc.) Published "Anaiysis 〇f Tantaium Coaitngs Produced by the Kinetic Spray Process", Journal of Thermal Spray Technology, Vol. 13, No. 2, June 2004, p. 265 To 273 pages; Marx et al., "Cold spraying - innovative layers for new applications" " Thermal Spray Technology Journal, Vol. 15 'No. 2, 2006 June pp. 177-183; and "The Cold Spray Process and its Potential for Industrial Applications by Gartner et al., Journal of Thermal Spray Technology, 15th Vol. 2, June 2006, pp. 223-232). This cold spray does not have to be fully heated by heating the powder to a temperature close to or above its melting point, as with conventional thermal spray processes. The fact that a dense coating can be formed at a low temperature raises many advantages. Such advantageous points include no oxidation, high density deposits, solid compaction, no heat induced stress 'in this case in particular no substantial substrate heating. The achievement of the power spray can be carried out, for example, by injecting a powder having a particle diameter of more than 65 μm into a de Laval-type nozzle, carrying it away in a supersonic flow, and accelerating to a high speed due to a resistance effect. The kinetic energy of the particles is transformed by plastic deformation into tension and heat when striking the surface of the substrate. The particles melt during the process. In the case of manufacturing a cathode or electron splatter target body for the field of physical gas deposition (PVD), it is preferred that the substrate be heated to a limited extent. The target material is often a high-melting temperature ("TM") refractory metal (the button's TM is 2,998 degrees Celsius), while the support plate of the 200902741 support target is selected for its high thermal conductivity, and is usually copper or (named TM 660 660 ° C), both are low melting temperature materials. Therefore, 'to use*' to heat the powder to or near the other thermal spray process deposits the resistant material on the low temperature support plate. The current implementation method is to separate the target completely from the support plate, and then use welding, brazing, diffusion bonding or explosion bonding techniques to combine the target with the support plate. Since the cold spray or power spray does not substantially heat the powder, it can be used to repair the used target directly on the support plate by a number of targets; ^ ' and without removing the target from the support plate. SUMMARY OF THE INVENTION The object of the present invention is to create a splash target having a fine-grained and randomly crystallized microstructure throughout the body of the object. It is a further object of the present invention to provide a process that can cost-effectively generate the microstructure and replicate the structure from the target to the other. Preferably, the process does not require melting. Several examples of such processes include cold spray or power spray processes. The present invention is also directed to providing a cost effective repair or recovery process which provides the same or preferred microstructure of the repair target as the original. Still another object of the present invention is a development-target recovery process by a method that does not require melting, such as a cold spray or a power spray. We have found that it is possible to directly manufacture a fine-grained structure having an Ik machine orientation to pass the entire thickness of the target and a plurality of parameters & 4 each directly on the support plate without using a complicated process. The target of the desired microstructure and the technique of simply modifying the target ^ This technique 200902741 does not use the - smashing process. Several examples of such processes include cold spray or power spray of fine metal powders such as (d) limited to group powders. Further, the present invention provides a method of splashing whereby any of the above-mentioned mitigation targets are subjected to a plurality of money-stroke conditions and thereby subjected to slamming. Any suitable splash method can be used in the present invention. Suitable transfer methods include, but are not limited to, magnetron shock, pulsed laser turn, ion beam splash, triode, and combinations thereof. In addition, the present invention provides a splash target that includes a uniform fine grain structure that is substantially smaller than A* microns, which is not preferred when measured by an electron backscatter diffractometer ("EBSD"). The texture orientation (i.e., substantially comprising a plurality of particles along the distraction) comprises a plurality of particles substantially less than 44 microns, and the body throughout the target exhibits no particle size or texture band. Further, the present invention provides a target, It includes a large particle size 'particle size' in the annealed state that is smaller than the starting powder particle size. Furthermore, the present invention provides a splash target having a crystalline particle structure characterized by substantially no interparticle diffusion, by electrons The Backscatter Burner ("EBSD") does not have a good texture orientation when measured, and the body throughout the target shows no grain size or texture banding. In addition, the present invention provides a process for manufacturing a _ snip target component by depositing the smear target directly on a support plate for the target component via a _ powder nozzle. The target material, the deposit and the substrate are machined to the final target assembly size. The present invention also provides a method of manufacturing a film comprising the steps of: (a) splashing the above-mentioned money target; 12 200902741 (b) removing a plurality of metal atoms from the target; forming a metal including the above on a substrate a thin film. [Embodiment]
我們已發現不用上述複雜處理而容許直接製造數個目標 的-種技術及數個參數’及料直接在該支持板上製造數 個具有該期望微結構的目標’及可以或不用先將用過的目 t自支持板移除以簡單地修復用過目標的—種技術。該技 術不使用一熔化製程,此類製程的數個範例包括如(但不限 於)短粉等細金屬粉末的冷喷霧或動力喷霧。 該技術亦可用於一濺擊目標的恢復或修復。 至於與金屬粉末形成—氣體粉末混合物的氣體通常使用 一惰性氣體。根據本發明的惰性氣體包括(但不限於)氬、 氦或較不起反應的氮,或其:或多者的混合物。在特殊情 形中亦可使用空氣。若符合安全規定,亦會考慮使用氫 或氫與其他氣體的混合物’及由於氫的極高音速而有利地 ^用。事實上’氫的音速比氦的音速A3G%,氦的音速依 次:為氮的音速的3倍。空氣在攝氏Μ度及工大㈣(_) 的曰速疋每秒344公尺,而相較於空氣的原子量28 %, 具有原子量2.016的氫是最輕元素,其密度約比空氣小14 倍且具有每秒1308公尺的音速。 在該製程的一較佳版本中,該噴霧包括以下步驟: 提供—噴霧孔毗鄰待由濺擊塗裝的一表面; 提供一微粒材料粉末到該噴霧孔,該微粒材料選自以下各 物組成的群:鈮、鈕、鎢、鉬、鈦、锆,其至少二者的混 13 200902741 合物或其與另一者或其他 150料4^ am 。屬的合金,該粉末具有0.5至 150彳政未(μΓη)的微粒尺寸, 芏 10至44 η半兮』 土疋5至80微米’及最佳是 川至44祕未,該粉末是在壓力下; 在一升高不流動覆力提供一情性氣體到該喷霧孔, 该微粒材料及氣體的—噴霧到待塗裝的 ,、 使該喷霧孔位於-低周Μ力區域;; ; =周Μ力大體上小於該噴霧孔前面的不 供該微粒材—的讀大量加速職待塗裝表面上 及 藉此該塗層退火時,該美彡泠 这基板塗佈一硬化塗層。請注意,該 硬化塗層可在退火前或退火後自該基板移除。 在該製程的另-較佳版本中,利用—冷噴霧搶執行該喷 霧’及使該待塗裝目標及冷噴霧搶位在壓力低於80千帕 (kPa)或高於(U百萬帕(Mpa)的—惰性小室内。 本申請案從頭到尾使用冷喷霧—詞,應了解在僅參昭至 冷喷霧製程的例子中可以使用—動力喷霧製程以代替該冷 喷霧製程。 在該製程的另-較佳版本中,利用—動力裝置以執行該 喷霧。相較於冷喷霧製程使用小於5〇微米的微粒直徑具有 較高微粒速度及通常較低微粒溫度,動力製程使用在Μ 至2 0 0微米之間的較大微粒尺寸分布及較高微粒溫度以產 生塗層。由於動能與微粒直徑的立方及微粒速度的平方成 正比,因此可用於塑性變形的總動能通常大於冷噴霧製程 者。執行該動力喷霧是利用在該咽喉區域後面的一較長喷 14 200902741 嘴長度(如280毫米(mm)對標準80毫米)及較高氣體溫度 (例如高於攝氏200度,但遠低於該材料的熔點)。相較於 利用較短噴嘴產生的塗層,較高微粒速度改良該等塗層特 性,造成高等級的塑性變形、增加的黏合、較低有孔性及 較高'工作硬化。 通常,耐熔金屬具有至少99%的純度,如99.5%或 99.7%,99.9%,基於金屬雜質,有利地具有至少99.95% 的純度,特別是至少99.995%或至少99.999%的純度,尤 其是至少99.9995%的純度。 通常若使用一合金以代替單一耐熔金屬,則至少該耐熔 金屬(但較佳是該合金整體)具有該純度,以便可產生一對 應高純度塗層。 在根據本發明的數個實施例之一中,粉末中如氧、碳、 氮或氫等非金屬雜質的總含量應有利地少於1,000 ppm, 較佳少於5 00 ppm,及更佳少於150 ppm。 在根據本發明的數個實施例之一中,氧含量是50 ppm或 更少,氮含量是25 ppm或更少,及碳含量是25 ppm或更 少〇 金屬雜質含量有利地是500 ppm或更少,較佳是100 ppm 或更少,及最佳是50 ppm或更少,尤其是10 ppm或更少。 此類金屬粉末可在市面購買,或可利用一還原劑還原耐 熔金屬化合物及較佳後續去氧化來配製。例如,在升高溫 度的一氫氣流中還原氧化鎢或氧化钥。該配製例如揭示在 Schubert,Lassner 的”Tungsten(鎢)” 一書中(Kluwer 學術/ 15 200902741 充電出版社,紐約,1999年)’或Brauer的”Handbuch der Praparativen Anorganischen Chemie"(Ferdinand Enke Verlag Stuttgart,1981 年,第 1530 頁)一文中。 在钽及鈮的例子中,實施該配製在大部分例子中是藉由 一鹼族金屬或鹼土族金屬以還原鹼族庚烷氟一钽酸鹽及鹼 土族金屬庚烷氟一鈕酸鹽,或如钽酸庚烷氟化鈉、钽酸庚 烷氟化鉀、钽酸庚烷氟鈮鐵化鈉或鈕酸庚烷氟鈮鐵化鉀等 氧化物。實施該還原可在例如因加入鈉而熔化的鹽中,或 在有利地使用鈣或鎂蒸汽的氣相中。亦可混合該耐熔金屬 化合物與鹼族或鹼土族金屬及加熱該混合物。氩氣環境可 為有利’熟諳此藝者已知許多合適製程,亦已知可選出合 適反應條件的製程參數。例如在美國專利號4,483,819及 世界專利號98/37249中說明數個合適製程。 例如世界專利號WO 01/12364及歐洲專利號 EP-A-1200218中所揭露,若期望低的氧含量,則用以配製 具一低氧含量的純粉末的再一製程包括使用一鹼土族金屬 作為還原劑以還原一耐熔金屬氫化物。 此外’本發明相關於一種用以再處理一濺擊目標(金屬陰 極濺擊中的金屬源)的製程,其中一氣體流量與一材料粉末 形成一軋體/粉末混合物’該材料選自以下各物組成的群: 鈮、钽、鎢 '鉬、鈦、锆,或其二或多者的混合物,或其 與其至少二者或與其他金屬的合金,該粉末具有〇5至15〇 微米的微粒尺寸,其中給予該氣體流量一超音速,及導引 該超音速喷射流到待再處理或製造的物件表面上。 16 200902741We have found that the technology and several parameters that allow the direct manufacture of several targets without the above complicated processing, and the production of several targets having the desired microstructure directly on the support board, may or may not be used first. The purpose of the self-support board removal is to simply repair the used technology. The technique does not use a melting process, and several examples of such processes include cold spray or power spray of fine metal powder such as, but not limited to, short powder. This technique can also be used for recovery or repair of a splash target. As the gas which forms a gas powder mixture with the metal powder, an inert gas is usually used. The inert gas according to the present invention includes, but is not limited to, argon, helium or less reactive nitrogen, or a mixture of: or more. Air can also be used in special situations. If safety regulations are met, hydrogen or a mixture of hydrogen and other gases will also be considered and advantageously used due to the extremely high sonic speed of hydrogen. In fact, the speed of sound of hydrogen is higher than the speed of sound of A3G%, and the speed of sound of 氦 is: three times the speed of sound of nitrogen. The air is at 344 meters per second in the Celsius temperature and the idling speed of the (4) (_), compared to 28% of the atomic weight of air. Hydrogen with an atomic weight of 2.016 is the lightest element, and its density is about 14 times smaller than air. Has a speed of sound of 1308 meters per second. In a preferred version of the process, the spray comprises the steps of: providing a spray aperture adjacent a surface to be coated by splashing; providing a particulate material powder to the spray aperture, the particulate material being selected from the group consisting of The group: 铌, knob, tungsten, molybdenum, titanium, zirconium, at least two of them mixed 13 200902741 or its other or other 150 material 4 ^ am. An alloy of the genus, the powder having a particle size of 0.5 to 150 未 (μΓη), 芏10 to 44 η 兮 兮 疋 5 to 80 μm and the best is Chuanzhi 44 secret, the powder is under pressure Providing an inert gas to the spray hole at an elevated non-flowing force, spraying the particulate material and the gas to the surface to be coated, so that the spray hole is located in the low-period force region; ; = Μ Μ force is substantially smaller than the front of the spray hole is not for the particulate material - read a large number of accelerated service coating surface and thereby annealing the coating, the substrate is coated with a hard coating . Note that the hardened coating can be removed from the substrate before or after annealing. In another preferred version of the process, the spray is performed using a cold spray and the target to be coated and the cold spray are subjected to a pressure of less than 80 kPa or higher (U million). Mpa - Inert chamber. This application uses a cold spray from beginning to end. It should be understood that in the example of the cold spray process only, a power spray process can be used instead of the cold spray. Process. In another preferred version of the process, a power device is utilized to perform the spray. A particle diameter of less than 5 microns is used to have a higher particle velocity and generally a lower particle temperature than a cold spray process. The power process uses a larger particle size distribution between Μ and 200 microns and a higher particle temperature to produce a coating. Since kinetic energy is proportional to the cube of the particle diameter and the square of the particle velocity, it can be used for total plastic deformation. The kinetic energy is usually greater than the cold spray process. The power spray is applied using a longer spray 14 behind the throat area. 200902741 mouth length (eg 280 mm (mm) versus standard 80 mm) and higher gas temperature (eg higher than 200 degrees Celsius , but much lower than the melting point of the material. Compared to coatings produced with shorter nozzles, higher particle velocities improve the coating properties, resulting in high levels of plastic deformation, increased adhesion, and lower porosity. And higher 'work hardening. Typically, the refractory metal has a purity of at least 99%, such as 99.5% or 99.7%, 99.9%, based on metal impurities, advantageously having a purity of at least 99.95%, in particular at least 99.995% or at least 99.999 % purity, especially at least 99.9995% purity. Generally, if an alloy is used instead of a single refractory metal, at least the refractory metal (but preferably the alloy as a whole) has this purity so that a corresponding high purity can be produced. In one of several embodiments according to the present invention, the total content of non-metallic impurities such as oxygen, carbon, nitrogen or hydrogen in the powder should advantageously be less than 1,000 ppm, preferably less than 500 ppm, and More preferably less than 150 ppm. In one of several embodiments according to the present invention, the oxygen content is 50 ppm or less, the nitrogen content is 25 ppm or less, and the carbon content is 25 ppm or less. The content is advantageously 500 ppm or Less, preferably 100 ppm or less, and most preferably 50 ppm or less, especially 10 ppm or less. Such metal powders can be purchased commercially or a reducing agent can be used to reduce refractory metal compounds and It is preferably formulated for subsequent deoxidation, for example, reduction of tungsten oxide or oxidized key in a hydrogen stream at elevated temperature. This formulation is disclosed, for example, in Schubert, Lassner's "Tungsten" (Kluwer Academic / 15 200902741). Charging Press, New York, 1999) 'or Brauer's Handbuch der Praparativen Anorganischen Chemie" (Ferdinand Enke Verlag Stuttgart, 1981, p. 1530). In the examples of ruthenium and osmium, the preparation is carried out in most of the examples by reducing an alkali heptane fluoromonitate and an alkaline earth metal heptane fluoro-monate by an alkali metal or an alkaline earth metal. Or an oxide such as sodium heptane citrate, potassium heptane citrate, sodium heptane fluoroantimonate or potassium hexanoate. The reduction can be carried out, for example, in a salt which is melted by the addition of sodium, or in a gas phase in which calcium or magnesium vapor is advantageously used. The refractory metal compound may be mixed with an alkali or alkaline earth metal and the mixture may be heated. An argon atmosphere can be advantageous. Many suitable processes are known to those skilled in the art, and process parameters for selecting suitable reaction conditions are also known. Several suitable processes are described, for example, in U.S. Patent No. 4,483,819 and World Patent No. 98/37,249. For example, as disclosed in the World Patent No. WO 01/12364 and the European Patent No. EP-A-1200218, if a low oxygen content is desired, a further process for formulating a pure powder having a low oxygen content includes the use of an alkaline earth metal. As a reducing agent to reduce a refractory metal hydride. Further, the present invention relates to a process for reprocessing a splash target (a metal source in a metal cathode splash), wherein a gas flow rate forms a rolled body/powder mixture with a material powder. The material is selected from the following a group consisting of: ruthenium, osmium, tungsten 'molybdenum, titanium, zirconium, or a mixture of two or more thereof, or an alloy thereof with at least two or with other metals, the powder having 〇5 to 15 〇 micron particles Dimensions in which the gas flow is given a supersonic velocity and the supersonic jet is directed to the surface of the article to be reprocessed or manufactured. 16 200902741
κ... —濺擊目標是金屬陰極濺擊中的一金屬源。此等減擊目 標用在積體電路、半導體及其他電氣、磁性及光學產品的 製造中。在濺擊製程期間,通常是不均勾地磨掉濺擊目標 的金屬表面,導致該表面上的一溝槽。為避免被支持板的 材料污染或甚至冷卻液的不利穿透,該等濺擊目標不會用 到該耐熔金屬目標用完為止,卻是迅速提前停止使用,因 此當必須用到一新濺擊目標時僅用掉較小量的昂貴耐熔金 屬。由於需要移除支持板及連接到新耐熔金屬板,因此大 多數濺擊目標僅能當作廢料賣掉,或回收其材料。然而, 支持板在此是濺擊目標中較低價值的一部分。 因此需要一種技術用以提供一濺擊目標的再處理或不必 為此拆卸支持板而恢復一濺擊目標的可能性,或提供直接 /儿積濺擊材料到支持板或用於一旋轉目標支持管的可能 性。 马此目的 一、救擎目標中的溝槽再加滿該特殊耐熔 金屬’ k佳不使⑽化來完成,例如可藉由上述冷喷霧或 動力製程來完成。為此目的’將該氣體/粉末混合物的超音 速喷射流導制該賴上及在構槽的整個長度及形狀之上 移動。按需要残錢此動作以重新加滿_,以使該賤 擊目標的表面再形成-幾乎完全平坦面積及/或該加滿材 稍“㈣擊目標的表面。較佳地,接著將該氣體/粉末 忍合物的超音速喷射料引㈣_目標的其餘表面上, 及導引到制擊目標表面的整個長度、寬度及形狀之上, 直到得到完全覆蓋該卿目標表面的—均勾厚度平面層。 17 200902741 接著可藉由傳統製程研磨拋光所得粗糙表面,以便得到想 要的平滑表面。 我們注意到’若原目標是由傳統鑄模冶金或粉末冶金技 術製成’财翁隸將料_目標更細㈣粒尺寸及 更隨機的結構。若原目標是由冷噴霧製成,則修復將具有 與原目標類似若難以區別的微結構。然而在原目標盥祕 復地帶之間將有一明顯分界線,其可在該目標的剖面見蝌 在製造-新_目標期間,該目標是直接施加到一支持 板。依目標的構造而定’因此將該氣體/粉末混合物的超音 速喷射流^丨翁崎目標的切板的整個表面上,及導 引到該濺擊目標表面的整個長度、寬度及形狀之上,直到 得到完全覆蓋錢擊目標表面的—均勻且夠厚的平面層, 或僅塗裝該電漿的接觸面積,其造成可觀的材料節省。 較佳是具有2至20毫米之間厚度的目標,更佳在3·〇至 15毫米之間,又更佳在5至12毫来之間,又更佳在8至 10毫米之間。 所得目標的純度及氧含量應偏離該粉末者不超過5%, 及較佳不超過1%。 若在-惰性氣體下塗裝該待再處理_目標,則可有利 地達成此目的。氬因密度比空氣高而有利地作為該惰性氣 體使用’尤其若濺擊目標是位在防止氬漏掉或流出且持續 罐的-容器中’氬傾向於覆蓋待塗袭物件且依然存 在。前面已討論過根據本發日紅作的其他情性氣體。 根據本發明的製程特別適於數個賤擊目標的處理或製 18 200902741 造,一方面因藉由熱機製程的製造期間常發生可在不同間 隔改變的較佳結晶定向’因此未得到均勻紋理,反而是所 謂的帶狀’即發生不同較佳定向的數個區域。在熱機製程 中’僅能用極複雜且昂貴的製程來避免此情形發生。相較 下藉由根據本發明的製程可得到一均句隨機紋理,其中 在°亥财炼金屬目標的厚度之上未出現可偵測到的較佳定 向0 同樣地,在该等目標中得到一均勻且隨機的微粒尺寸分 布及顆粒尺寸分布,以便若非期望,亦未得到不同微粒尺 寸或顆粒尺寸的帶狀。轉目標巾的顆粒尺寸或紋理帶狀 特別糟’原因是會造成濺擊速率及膜均句的變化。 在將粉末施加到該濺擊目標且熔化粉末的製程中,由經 驗得知會發生氣泡及難生長4根據本發明的製程中亦 不會見到此情形發生。 在邊目標的施加後,通常會研磨及拋光該濺擊目標的表 面以得到一合適的平滑表面,可藉由根據先前技藝的傳統 製程來實施此製程。 在一新濺擊目標的製造中,將該目標施加到一支持構 件,例如施加到一支持板,此板通常是銅或鋁,或此等金 屬的至者與鉸的合金製成的板。此支持板可包含數個 通道,其中有一冷卻媒質。 該支持板及因而該濺擊目標可以是平面、桿、圓柱、塊 或其他任何想要形狀的形式,亦可附加額外的結構性零 件,液體冷卻線圈及/或較大冷卻液貯槽及/或複雜凸緣或 19 200902741 其他機械或電氣結構。 根據本發明製造的目標,或在一濺擊目標的製造或再處 理期間產生的目標,可具有高純度及低氧含量。 作為結果的目標具有一氣體雜質含量,其偏離製造此目 標的開始粉末含量不超過50%,或不超過2〇%,或不超過 10%,或不超過5% ’或不超過1%。在此相關情況中,應 了解偏離一詞特指增加;所得目標因此應有利地具有一氣 體雜質含量,其超過該開始粉末含量不超過50%。 在該表面上硬化的粉末較佳具有一氧含量,其偏離該開 始叙末的氧含量不超過5%,尤其是不超過1〇/〇。 在一有利實施例中,該等目標並且具有一至少97%的密 度,較佳大於98%,尤其是大於99%或99.5%〇該目標的 密度在此是該目標的密閉本質及有孔性的測度。—目標的 97/。在度表示該目標具有該大塊材料的一密度。一密 閉、戌乎元全無細孔的目標通常具有超過99·5%的一密 度判疋氆度可藉由此一目標的一剖面影像(剖面)的影像 分析,或藉由氦固縮測定(helium pykn〇metry),後者方法 較不利,原因是在極密實目標的例子中,未偵測到存在於 目標中又自表面移除的細孔’因此測到比實際存在者低的 有孔(生。判定密度可藉由影像分析,首先在顯微照片的影 像』面中判疋待調查目標的總面積,及接著使此面積與該 等細孔的面積相關聯。藉由此方法,亦記錄早自該表面移 除及靠近基板介面的細孔.在濺擊目標的製造及再處理 中’至少97%的高密度是特別重要的,較佳大於_,尤 20 200902741 其是大99%或99.5%。 該等目標顯示高機械強度,造成原时其高密度及該等 微粒的高變形,在鉅的例子中,若與該金屬粉末形成一氣 體/粉末混合物的氣體是氮,該等強度因此至少8〇百萬帕 (MPa) ’更佳至少1〇〇百萬帕,最好至少14〇百萬帕。藉 由在喷務後提供-退火或擴散結合熱處理可更增加該喷霧 粉末的此機械強度及可塑性。 若使用氦,該強度通常是至少15〇百萬帕,較佳至少17〇 百萬帕,更佳至少200百萬帕,及最佳是大於250百萬帕。 轉明亦提供-種製造—薄膜的方法,包括以下步驟: ⑷藉由冷喷霧或動力喷霧以製造該期望賤擊目標; (b)濺擊上述濺擊目標; (c) 自該目標移除數個金屬原子;及 (d) 在基板上形成包括有數個金屬原子的一薄膜。 根據本發明的該等金屬原子包括(但不限於)銳、组 '鶴、 =鈦、鍅、鉻、釩、鎂、錫、鉛、鋁、鋅、銅、铑、銀、 二、鈷、鐵、釕、銖、鎵、銦、銻,其二或多者的混合物, 或其二或多者的合金,或與具有上述特性的其他金屬的合 、依該薄膜的應用而定,會要求在製造該漉擊目標中使 用何種金屬或金屬原子的組合。 ,發明的另—實施财,在步驟⑷之後可加入-步 Γ ’其包括供應—反應氣體到該等金屬原子。—反應氣體 疋包括有-成分的氣冑,其可態中或一且沉積到一基 板上與該等金屬原子起反應,以形成一金屬或合金化合 21 200902741 物作為-非限定範例,該反應氣體可 石夕氣體。 …氧氮及/或一含 藉由本方法施加的薄膜可具有任何期望 厚度將依期望的最终使 *又’ k薄膜的 、便用應用而疋。通常, 二以是至少。.5奈米㈣,在一些情形中是至少、太旱度 在一些例子中是至少5奈米,在其他例子中是2:;〇卡: 米,在一些情形中是至少25 不 5。奈米,在一_境中… 其他情形中是至少 ^ 境中疋至少75奈米,及在其他環境中 疋乂 100奈米。而且,該膜厚度可達到10微米’在—些 例子令達到5微米,在其他例子中達到2微米,在一奸 形中達到1微求,及在其他情形中達到〇·5微米。該^ 度可為所述任何值,或可在任何上述值之間。根據本發明 的薄膜的有利點在於’該薄膜可具有一絕佳均勾及極小表 面粗糖度。令人驚言牙地,在類似的磁電管濟擊條件下,相 較於傳統鑄模輾壓式鈕目標製成的膜不均勻在4.抓至 15.4%之間’藉由冷噴霧鈕目標製成的薄膜不均勻卻在 1.5%至4%之間(如表j所示)。改良的薄膜均勻是冷喷霧目 標呈現隨機均勻紋理及細粒尺寸大體上小於44微米的特 點的結果。 根據本發明的薄膜的用途包括各種不同應用中使用的產 品。在一實施例中,根據本發明製造的一薄膜可用在薄膜 電晶體(TFT)-液晶顯示器(LCD)應用中。而且,在另一實施 例中’本發明包括一種用於太陽能電池應用、感應器應用、 半導體裝置及CMOS(互補金氧半)科技用金屬閘的薄膜。 22 200902741 在一實施例中,本發明指向一種tft-lcd裝置,其包含數 個鉬薄螟,其作為具絕佳均勻的閘極。另一實施例指向數 個薄膜太陽能電池應用,其中本發明包括數個太陽能電 池’其中鉬(M〇)薄膜作為背面接點以及障壁層。該薄膜圩 用於噴墨列印頭應用(例如钽作為一加熱元件(一高度抗腐 蝕金屬材料)、_氣蝕障壁及一純化層(如TkO5)使用,提 供一較高電崩潰),或建築用玻璃塗層,該薄膜可以是一平 板顯示器或一平板顯示器的一部分,或作為磁碟機儲存體 的一磁性薄膜材料,及光學塗層。根據本發明的薄膜可取 代根據先前技藝的傳統薄膜。 由於該等金屬濺擊目標的整個厚度中的均勻細粒尺寸及 紋理,因該冷噴霧目標是具有隨機顆粒定向的細粒非帶 狀,因此得自此類目標的薄膜具有絕佳均勻。 太陽能裝置為此藝所習知。例如,以下有關太陽能電池 裝置的專利及參考文件以引用方式併入本文中’用於數個 太陽能電池裝置的揭露(鉬薄膜作為障壁層以及背端接 點)··美國專利號7,053,294(在撓性金屬基板上製造的薄膜 太陽能電池)、美國專利號4,915,745(薄膜太陽能電池及製 造方法)' The Fabrication and Physics of High-efficiency CdTe Thin Film Solar Cells (高效率鎘-碲薄膜太陽能電池 的製造及物理)(由Alvin, Compaan及Victor Karpov發表, 2003年’國家可更新能源實驗室),及Development of Cu(In, Ga)Se2 Superstrate Thin Film Solar Cells(Cu(In,Ga)Se2 超基 板薄膜太陽能電池的發展)(由Franz-Josef Haug發表,2001 23 200902741 年,蘇黎克的瑞士聯邦科技機構的博士論文)。 通常,一太陽能電池可包括: A) —覆蓋玻璃; B) —頂電接觸層; C) 一透明接點; D) —頂接合層; E) 一吸收層; F) —背面電接點;及 G) —基板。 根據本發明,藉由使用如上述動力或冷噴霧製程製造的 數個濺擊目標以製造一薄膜。該濺擊目標較佳是一粉末混 合物,至少一粉末來自以下金屬:組、銳、錮、銘、鋅、 碲、銅或金。根據本發明的膜可作為一背面電接點以及障 壁層使用。 根據本發明,為製造一半導體裝置,藉由上述動力或冷 喷霧製程製造一濺擊目標。藉由冷喷霧製造該濺擊目標, 較佳利用一粉末混合物,至少一粉末來自以下金屬:组、 鈮、鉬、鎢、鉻、鈦、铪及錘。此類目標製出的薄膜作為 障壁層使用。該等障壁層的使用為此藝所習知。例如,以 下有關障壁層的專利以引用方式併入本文中用於數個障壁 層的揭露:Semiconductor Carrier film, and Semiconductor Device and Liquid Crystal Module Using The Same(半導體 載膜,及使用該膜之半導體裝置及液晶模組)(美國專利號 7,164,205),Methods of forming an interconnect on a 24 200902741 semiconductor substrate(在半導體基板上形成一互連之方 法)(美國專利號 5,612,254),Fabrication of Semiconductor device(tungsten, chromium or molybdenum, and barrier layer)(半導體裝置(鎢、鉻或鉬,及障壁層)之製造)(美國專 利號7,183,206),全部文件揭示半導體裝置。 具有根據本發明使用一冷喷霧或動力製程所製造薄膜的 半導體裝置包括鈦、钽、鈮、鎢、鉻、铪及锆,及其氮化 物、矽化物或矽氧化物製成的膜。此等膜可作為障壁層使 用及可取代傳統的鈕膜。例如,以下專利說明钽(Ta)障壁 層及以引用方式併入本文中用於钽障壁層的揭露: Tantalum Barrier Layer for Copper Metallization(用於銅金 屬化之钽障壁層)(美國專利號6,953,742),Method of Preventing Diffusion of Copper through a Tantalum-comprising Barrier Layer(防止銅擴散通過一含组 障壁層之方法)(美國專利號6,919,275),及Methodof Depositing a TaN seed Layer(沉積一氮化组(TaN)種子層之 方法)(美國專利號6,911,124)。 根據本發明的磁性薄膜材料是藉由使用上述動力或冷喷 霧製程所製造的濺擊目標來製造。藉由冷喷霧製造該滅擊 目標較佳具有一合成粉末混合物,至少二粉末至少來自以 下金屬:鉑、鈷、鎳、鉻、鐵、鈮、鍅,天生元素。此磁 性膜材料可用於硬碟儲存裝置及磁性隨機存取記憶體 (MRAM)以取代傳統磁性薄膜材料。該等傳統磁性薄膜材 料為此藝所習知··例如,以下專利以引用方式併入本文中 25 200902741 用於硬碟儲存裝置用的磁性薄膜材料的揭露:Magnetic Materials Structures, Devices and Methods(磁性材料結構、 裝置及方法)(美國專利號 7,128,988),Method and Apparatus to Control the Formation of Layers useful in Integrated Circuits(控制積體電路中有用層形成之方法及裝置)(美國 專利號 6,669,782) ’ Magnetic Recording Medium and Method for Its Production(磁性記錄媒體及其製造方法)(美國專利 號 5,679,473),Magnetic Recording Medium(磁性記錄媒 體)(美國專利號4,202,932)。硬碟機為此藝所習知。 光學塗層為此藝所習知:例如,以下揭示光學塗層的專 利以引用方式併入本文中用於數個光學塗層的揭露: Optical Reflector for Reducing Radiation Heat Transfer to Hot Engine Parts(用以減低輻射熱傳遞至熱引擎零件之光 學反射層)(美國專利號 7,208,230),Thin Layer of Hafnium Oxide and Deposit Process(氧化铪薄層及沉積方法)(美國專 利號 7,192,623) ’ Anti-reflective (AR) Coating for Highκ... — The target of splashing is a source of metal in the splash of metal cathode. These mitigation targets are used in the manufacture of integrated circuits, semiconductors, and other electrical, magnetic, and optical products. During the splashing process, the metal surface of the splash target is usually rubbed off unevenly, resulting in a groove on the surface. In order to avoid the material contamination of the support plate or even the unfavorable penetration of the coolant, the splash target will not be used up until the refractory metal target is used up, but it is quickly stopped in advance, so when a new splash must be used Only a small amount of expensive refractory metal is used when hitting the target. Due to the need to remove the support plate and connect to the new refractory metal plate, most splash targets can only be sold as scrap or recycled. However, the support board is here a part of the lower value of the splash target. There is therefore a need for a technique to provide re-processing of a splash target or the possibility of recovering a splash target without having to disassemble the support plate, or to provide direct/spray material to the support plate or for a rotating target support. The possibility of tube. For this purpose, the groove in the target of the rescue is filled with the special refractory metal, which can be accomplished by, for example, the above-mentioned cold spray or power process. For this purpose, the supersonic jet of the gas/powder mixture is guided to the top and moved over the entire length and shape of the grooving. If necessary, the action is to refill _ so that the surface of the slamming target is reformed - almost completely flat area and / or the filling material is slightly "(4) the surface of the target. Preferably, the gas is then applied / Powdered-kneaded supersonic jet material (4) _ the remaining surface of the target, and guided over the entire length, width and shape of the target surface of the target, until the full thickness of the target surface is covered Plane layer 17 200902741 The rough surface obtained by conventional polishing can be polished to obtain the desired smooth surface. We noticed that if the original target is made by traditional mold metallurgy or powder metallurgy technology, the target is _ target Finer (four) grain size and more random structure. If the original target is made of cold spray, the repair will have similar microstructures that are similar to the original target, but there will be a clear dividing line between the original target and the secret zone. It can be seen in the profile of the target during the manufacturing-new_target period, which is directly applied to a support plate. Depending on the construction of the target, the gas/powder is thus mixed. The supersonic jet of the object is superimposed on the entire surface of the cutting board of the Ogaki target and guided over the entire length, width and shape of the surface of the splash target until it is completely uniform and sufficient to cover the surface of the target a thick planar layer, or only the contact area of the plasma, which results in considerable material savings. Preferably, the target has a thickness of between 2 and 20 mm, more preferably between 3 and 15 mm, More preferably between 5 and 12 milliliters, and even more preferably between 8 and 10 millimeters. The purity and oxygen content of the target to be obtained should not deviate from the powder by no more than 5%, and preferably not more than 1%. This can be advantageously achieved by applying the to-be-processed target under inert gas. Argon is advantageously used as the inert gas because of its higher density than air. Especially if the target of splashing is to prevent argon from leaking or flowing out In the continuous tank-container, 'argon tends to cover the object to be coated and still exists. Other identifiable gases according to the present day have been discussed. The process according to the invention is particularly suitable for the treatment of several slamming targets. Or system 18 200902741 made, one side Since the preferred crystal orientation which can be changed at different intervals during the manufacturing process of the thermal mechanism often occurs, a uniform texture is not obtained, but rather a so-called strip shape, that is, several regions in which different preferred orientations occur. This can be avoided only by extremely complicated and expensive processes. A uniform random texture can be obtained by the process according to the invention, wherein no detectable is found above the thickness of the target of the metal Preferred orientations to 0 Similarly, a uniform and random particle size distribution and particle size distribution are obtained in the targets so that, if not desired, ribbons of different particle sizes or particle sizes are not obtained. The size or texture is particularly bad. The reason is that it will cause the splash rate and the change of the film. In the process of applying the powder to the splash target and melting the powder, it is known from experience that bubbles will occur and it is difficult to grow. This situation will not be seen in the process of the invention. After application of the edge target, the surface of the splash target is typically ground and polished to provide a suitable smooth surface, which can be performed by conventional processes in accordance with prior art techniques. In the manufacture of a new splash target, the target is applied to a support member, such as a support plate, which is typically copper or aluminum, or a plate of such metal and hinged alloy. This support board can contain several channels with a cooling medium. The support plate and thus the splash target may be in the form of a plane, rod, cylinder, block or any other desired shape, plus additional structural components, liquid cooling coils and/or larger coolant reservoirs and/or Complex flange or 19 200902741 Other mechanical or electrical structures. The object produced in accordance with the present invention, or the target produced during the manufacture or reprocessing of a splash target, may have a high purity and a low oxygen content. The resulting target has a gaseous impurity content that deviates from the starting powder content at which this target is made by no more than 50%, or no more than 2%, or no more than 10%, or no more than 5% ' or no more than 1%. In this context, it should be understood that the term deviation is specifically meant to increase; the object of the invention should therefore advantageously have a gaseous impurity content which exceeds the starting powder content by no more than 50%. The powder hardened on the surface preferably has an oxygen content which deviates from the beginning of the beginning by an oxygen content of not more than 5%, especially not more than 1 Torr. In an advantageous embodiment, the targets have a density of at least 97%, preferably greater than 98%, especially greater than 99% or 99.5%. The density of the target is here the closed nature and porosity of the target. Measure. - 97/ of the target. The degree indicates that the target has a density of the bulk material. A closed, almost non-porous target usually has a density of more than 99.5%. The image can be analyzed by a cross-sectional image (profile) of the target or by tamping. (helium pykn〇metry), the latter method is less advantageous because in the case of extremely dense targets, the pores that are present in the target and removed from the surface are not detected. Therefore, a hole lower than the actual one is detected. (Determination. The density can be determined by image analysis, first in the image of the photomicrograph), and the total area of the object to be investigated is determined, and then the area is correlated with the area of the pores. The pores removed from the surface and close to the substrate interface are also recorded. At least 97% of the high density is particularly important in the manufacture and reprocessing of the splash target, preferably greater than _, especially 20 200902741 which is a large 99 % or 99.5%. These targets show high mechanical strength, resulting in their high density and high deformation of the particles. In the giant case, if the gas forming a gas/powder mixture with the metal powder is nitrogen, Equal strength is therefore at least 8 million (MPa) 'More preferably at least 1 MPa, preferably at least 14 MPa. This mechanical strength and plasticity of the spray powder can be further increased by providing an annealing or diffusion bonding heat treatment after spraying. If hydrazine is used, the strength is usually at least 15 MPa, preferably at least 17 MPa, more preferably at least 200 MPa, and most preferably greater than 250 MPa. The method of film comprising the steps of: (4) manufacturing the desired target by cold spray or power spray; (b) splashing the splash target; (c) removing a plurality of metal atoms from the target; (d) forming a thin film comprising a plurality of metal atoms on the substrate. The metal atoms according to the invention include, but are not limited to, sharp, group 'cranes, = titanium, tantalum, chromium, vanadium, magnesium, tin, lead , aluminum, zinc, copper, antimony, silver, di-, cobalt, iron, antimony, bismuth, gallium, indium, antimony, a mixture of two or more thereof, or an alloy of two or more thereof, or with the above characteristics The combination of other metals, depending on the application of the film, will require the use of the target in the manufacture of the target. a combination of a metal or a metal atom. In addition, after the step (4), a step -4 can be added, which includes supplying a reaction gas to the metal atoms. The reaction gas 疋 includes a component-containing gas enthalpy. In a state or a state, deposited on a substrate and reacted with the metal atoms to form a metal or alloy compound 21 200902741 as a non-limiting example, the reaction gas can be a gas, a gas, and/or a The film comprising the film applied by the method may have any desired thickness which will eventually be used to make the film of the desired film. Typically, the second is at least .5 nanometers (four), in some cases at least The dryness is at least 5 nanometers in some cases, 2: in other examples; Leica: meters, in some cases at least 25 not 5. Nano, in a _ environment... In other cases, at least ^ 75 at least 75 nm in the environment, and 疋乂 100 nm in other environments. Moreover, the film thickness can be as large as 10 micrometers, and in some cases, up to 5 micrometers, in other examples up to 2 micrometers, in a trait, up to 1 micro-finish, and in other cases up to 5 micrometers. The ^ can be any of the stated values or can be between any of the above values. The film according to the invention is advantageous in that the film can have an excellent uniformity and a very small surface roughness. Surprisingly, under the similar magnetrons, the film made by the target of the traditional mold-pressing button is uneven. 4. It is caught between 15.4%. The resulting film is not uniform but is between 1.5% and 4% (as shown in Table j). The improved film uniformity is the result of a cold spray target exhibiting a random uniform texture and a fine particle size substantially less than 44 microns. The use of the film according to the invention includes products used in a variety of different applications. In one embodiment, a film made in accordance with the present invention can be used in thin film transistor (TFT)-liquid crystal display (LCD) applications. Moreover, in another embodiment, the invention includes a film for solar cell applications, inductor applications, semiconductor devices, and metal gates for CMOS (Complementary Metal Oxygen) technology. 22 200902741 In one embodiment, the invention is directed to a tft-lcd device comprising a plurality of molybdenum thin ruthenium as a gate having an excellent uniformity. Another embodiment is directed to a number of thin film solar cell applications in which the invention includes a plurality of solar cells' wherein a molybdenum (M〇) film serves as a back contact and a barrier layer. The film is used in ink jet print head applications (for example, as a heating element (a highly corrosion-resistant metal material), a cavitation barrier and a purification layer (such as TkO5) to provide a higher electrical breakdown), or The building is coated with glass, which may be part of a flat panel display or a flat panel display, or a magnetic thin film material as a disk drive storage, and an optical coating. The film according to the present invention can be substituted for a conventional film according to the prior art. Due to the uniform fine particle size and texture throughout the thickness of the metal splash target, since the cold spray target is a fine particle non-band shape with random particle orientation, the film obtained from such a target has excellent uniformity. Solar devices are well known for this art. For example, the following patents and references for solar cell devices are incorporated herein by reference 'disclosure for several solar cell devices (molybdenum film as barrier layer and backside contact). US Patent No. 7,053,294 Thin film solar cells fabricated on a metal substrate), US Patent No. 4,915,745 (Thin-film solar cells and manufacturing methods) 'The Fabrication and Physics of High-efficiency CdTe Thin Film Solar Cells (Manufacture and physics of high-efficiency cadmium-tantalum thin film solar cells) (published by Alvin, Compaan and Victor Karpov, 2003 National Renewable Energy Laboratory), and Development of Cu(In, Ga) Se2 Superstrate Thin Film Solar Cells (Cu(In,Ga)Se2 super-substrate thin film solar cells) Development) (published by Franz-Josef Haug, 2001 23 200902741, Ph.D. the Swiss Federal Institute of Science and Technology, Zurich). Typically, a solar cell can include: A) - a cover glass; B) a top electrical contact layer; C) a transparent contact; D) a top bond layer; E) an absorber layer; F) a backside electrical contact; And G) - substrate. In accordance with the present invention, a film is produced by using a plurality of splash targets made by a power or cold spray process as described above. Preferably, the splash target is a powder mixture from at least one of the following metals: group, sharp, enamel, indium, zinc, bismuth, copper or gold. The film according to the present invention can be used as a back surface electrical contact and a barrier layer. According to the present invention, in order to fabricate a semiconductor device, a splash target is produced by the above-described power or cold spray process. The splash target is produced by cold spray, preferably using a powder mixture from at least one of the following metals: group, bismuth, molybdenum, tungsten, chromium, titanium, niobium and hammer. Films made from such targets are used as barrier layers. The use of such barrier layers is well known in the art. For example, the following patents relating to barrier layers are incorporated herein by reference for disclosure of several barrier layers: Semiconductor Carrier Film, and Semiconductor Device and Liquid Crystal Module Using The Same, and semiconductor devices using the same. And a liquid crystal module) (U.S. Patent No. 7,164,205), Methods of forming an interconnect on a 24 200902741 semiconductor substrate (Method for forming an interconnection on a semiconductor substrate) (U.S. Patent No. 5,612,254), Fabrication of Semiconductor device (tungsten, chromium) Or molybdenum, and barrier layer) (manufacture of semiconductor devices (tungsten, chromium or molybdenum, and barrier layers)) (U.S. Patent No. 7,183,206), the entire disclosure of which is incorporated herein. A semiconductor device having a film produced by using a cold spray or a power process according to the present invention comprises titanium, tantalum, niobium, tungsten, chromium, hafnium and zirconium, and a film thereof made of a nitride, a telluride or a tantalum oxide. These films can be used as a barrier layer and can replace conventional button films. For example, the following patent describes a Ta (Ta) barrier layer and the disclosure of a barrier layer for inclusion herein: Tantalum Barrier Layer for Copper Metallization (U.S. Patent No. 6,953,742) , Method of Preventing Diffusion of Copper through a Tantalum-comprising Barrier Layer (Method for preventing copper from diffusing through a barrier layer containing layers) (U.S. Patent No. 6,919,275), and Methodof Depositing a TaN seed Layer (TaN) Method of seed layer) (US Patent No. 6,911,124). The magnetic film material according to the present invention is produced by using a splash target manufactured by the above-described power or cold spray process. Preferably, the target is produced by cold spray having a synthetic powder mixture, at least two of which are derived from at least the following metals: platinum, cobalt, nickel, chromium, iron, ruthenium, osmium, a natural element. This magnetic film material can be used in hard disk storage devices and magnetic random access memories (MRAM) to replace conventional magnetic film materials. Such conventional magnetic thin film materials are known in the art. For example, the following patents are incorporated herein by reference. 25 200902741 The disclosure of magnetic thin film materials for hard disk storage devices: Magnetic Materials Structures, Devices and Methods Material Structure, Apparatus, and Method) (U.S. Patent No. 7,128,988), Method and Apparatus to Control the Formation of Layers useful in Integrated Circuits (U.S. Patent No. 6,669,782) Magnetic Recording Medium and Method for Its Production (U.S. Patent No. 5,679,473), Magnetic Recording Medium (U.S. Patent No. 4,202,932). Hard disk drives are well known for this art. Optical coatings are known in the art: for example, the following disclosure of optical coatings is incorporated herein by reference for the disclosure of several optical coatings: Optical Reflector for Reducing Radiation Heat Transfer to Hot Engine Parts (for Reduced radiant heat transfer to the optical reflective layer of the heat engine parts) (US Patent No. 7,208,230), Thin Layer of Hafnium Oxide and Deposit Process (US Patent No. 7,192,623) 'Anti-reflective (AR) Coating For High
Index Gain Media(用於高係數增益媒體之抗反射(AR广塗 層)(美國專利號7,170,915^根據本發明,藉由使用根據本 發明的薄膜以製造數個光學塗層。藉由上述動力或冷噴霧 製程以製造該濺擊目標。該濺擊目標由铪、鈦或鍅製成。 將該氧化物材料硬壓在該濺擊目標上。可藉由上述目標的 反應式磁電管濺擊以製造該氧化膜,以取代藉由真空熱壓 或熱等壓壓平製程所製目標濺擊出的傳統氧化薄膜。 喷墨列印頭(含钽)為此藝所習知:根據本發明,藉由使 26 200902741 用根據本發明的薄膜以製造一喷墨列印頭,藉由上述動力 或冷喷霧製程以製造該濺擊目標。該濺擊目標由鈕或鈮製 成。藉由以矽烷及/或氧的反應濺擊以製造該膜,其可取代 如美國專利號6,962,407所述鈕-矽-氧抗腐蝕膜。例如,以 下揭示噴墨列印頭的專利以引用方式併入本文中用於數個 喷墨列印頭的揭露:Inkjet recording head, method of manufacturing the same, and inkjet printer(喷墨記錄頭,其 製造方法,及喷墨印表機(美國專利號6,962,407),Print head for Ink-Jet Printing A method for Making Print Heads(用於噴墨列印之列印頭,製造列印頭之方法(美國專 利號 5,859,654)。 用於平板顯示器的TFT-OLED(薄膜電晶體有機發光二 極體)裝置結構為此藝所習知。根據本發明,藉由使用上述 動力或冷喷霧製程製造的濺擊目標以製造一薄膜。該濺擊 目標由鎢、鉻、銅或鉬製成。由該冷喷霧目標濺擊成以作 為閘極層的膜可取代TFT-OLED中的傳統薄膜層。例如, 美國專利號6,773,969中揭示TFT-OLED。 TFT-LCD(用於平板顯示器的薄膜電晶體液晶顯示器) 中’液晶顯不裔包括· A) —玻璃基板; B) —源極; C) 一汲極; D) —閘極絕緣體; E) 一閘極; 27 200902741 F) —非晶矽、多晶系或單晶矽層; G) — η摻雜矽層; Η) —鈍化層; I) 一像素透明電極; J) 一共用電極; Κ)一聚醯亞胺對準層;及 L)一儲存電容電極。 其中該閘極為如鉬、鎢、鋁等金屬。 用於TFT LCD的另—綱要圖表中,使用以纟目完全覆蓋的 铭閘極以避免|g擴散形成的小丘。通常,翻覆蓋層用以阻 止J丘开/成所需的厚度大約是扇埃(人)。具低阻抗(約《Ο8 微馱姆Λ刀)的鉬全覆蓋鋁膜成功地整合到具高效能的非 曰曰系Si’H TFT製造中。說明半導體領域中的tft的其他 專利如下:美國專利號 6,992,234, 6,489,222, 6,613,697, 八乂引用方式併入本文中以用於半導體領域中TFT的使 用根據本發明,藉由使用上述動力或冷噴霧製程所製濺 擊目&以製造—薄膜。該鱗目標由翻、鶴或铭製成。該 減擊目標製成的膜可取代TFT丄CD中的傳統紹及/或钥層。 由於該等金相擊目標的整個厚度中的均㈣粒尺寸及 紋理’得自此類目標的膜具有絕佳均^該冷噴霧目標是 具有隨機顆粒定向的細粒非帶狀。 在本發明的—特殊實施例中提供-種極賴 <=在此實施 例中,該薄膜是至少1〇〇埃,在一些例子中是至少埃, 在八他例子中是至少5〇〇 士矣。在此實施例中,該薄膜可 28 200902741 達到5,000埃,在一些例子中達到3,000埃,在其他例子 中達到2,500埃’及在一些情形中達到2,000埃。 除了各種不同基板上的金屬薄膜外,亦可藉由反應濺擊 或離子植入以產生MOx(氧化),MNX(氮化),MSix(矽化), 及其任何組合(如MOxSiy等),其中M是金屬。根據本發 明的金屬原子包括(但不限於)銳、钽、鎢、鉬、欽、錯、 絡、飢、鎮、錫、錯、銘、辞、銅、錄、銀、金、姑、鐵、 釕、銖、鎵、銦、銻’其二或多者的混合物。 關於許多應用’玻璃並非完美,尤其是建築用途。一方 面’在氣候較寒冷區域,玻璃在遠紅外線(室溫輻射)中的 低反射造成加熱建築物所需熱能的不良損失。另一方面, 在氣候炎熱的地帶,玻璃在近紅外線(太陽輻射)中的高透 射增加建築物冷卻所需的能量。 建築用玻璃塗層為此藝所習知:例如,以下揭示建築用 玻璃塗層的專利以引用方式併入本文中用於數個建築用玻 璃塗層的揭露:D.C. reactively sputtered antireflection coatings(D.C.反應濺擊抗反射塗層)(美國專利號 5,270,858),Multilayer antireflection coating using zinc oxide to provide ultraviolet blocking(使用氧化鋅以提供紫 外線阻斷之多層抗反射塗層(美國專利號5,147,125), Coated architectural glass system and method(具塗層之建築 用玻璃系統及方法(美國專利號3,990,784), Electrically-conductive, light-attenuating antireflection coating(導電、光衰減抗反射塗層(美國專利號5,091,244)。 29 200902741 俨虞:《明,猎由使用上述動力或冷喷霧製程所製濺擊目 標以製造一薄膜。該減擊目標! ^目 墼射… 單知由鋅I成。在該鋅目標的濺 n ,在小室(如空氣或氧)中弓丨入氧,藉此 鋅薄膜。由該濺擊目標製成的薄膜可取代破璃 統氧化鋅層。 *現今在玻璃上小心設計的塗層可克服所有這些缺點。此 等塗層的目的是為控制能量輸送通過玻璃以用於更有效加Index Gain Media (Anti-Reflection for High Coefficient Gain Media (AR Wide Coating) (U.S. Patent No. 7,170,915) according to the invention, by using a film according to the invention to make several optical coatings. a power or cold spray process to produce the splash target. The splash target is made of tantalum, titanium or tantalum. The oxide material is hard pressed onto the splash target. The reactive magnetron can be splashed by the above target The oxide film is fabricated to replace the conventional oxide film which is splashed by a target made by vacuum hot pressing or hot isostatic pressing. The ink jet printing head (including ruthenium) is known to the art: according to the present According to the invention, the splash target is manufactured by using the film according to the present invention to make an ink jet print head by using the above-described power or cold spray process. The splash target is made of a button or a cymbal. The film is made by splashing with a reaction of decane and/or oxygen, which can replace the button-矽-oxygen anti-corrosion film as described in U.S. Patent No. 6,962,407. For example, the disclosure of the ink jet print head is hereby incorporated by reference. Used in this paper for several inkjet print heads Inkjet recording head, method of manufacturing the same, and inkjet printer (inkjet recording head, method of manufacturing the same, and inkjet printer (U.S. Patent No. 6,962,407), Print head for Ink-Jet Printing A method for Making Print Heads (printing head for ink jet printing, method of manufacturing a printing head (U.S. Patent No. 5,859,654). TFT-OLED (Thin Film Transistor Organic Light Emitting Diode) device structure for flat panel display Conventionally, according to the present invention, a film is produced by using a splash target manufactured by the above-described power or cold spray process. The splash target is made of tungsten, chromium, copper or molybdenum. A film formed as a gate layer can be substituted for a conventional film layer in a TFT-OLED. For example, a TFT-OLED is disclosed in US Pat. No. 6,773,969. A TFT-LCD (Thin Film Transistor Liquid Crystal Display for Flat Panel Display) Afro include: A) - glass substrate; B) - source; C) a drain; D) - gate insulator; E) a gate; 27 200902741 F) - amorphous germanium, polycrystalline or single crystal矽 layer; G) — η doping矽 layer; Η) — passivation layer; I) one pixel transparent electrode; J) a common electrode; Κ) a polyimide aligning layer; and L) a storage capacitor electrode. The gate is extremely metal such as molybdenum, tungsten or aluminum. In the other outline of the TFT LCD, the gates that are completely covered by the eye are used to avoid the hills formed by the diffusion of |g. Usually, the thickness required to turn over the cover layer to prevent the J-opening/forming is about a fan (human). The molybdenum-coated aluminum film with low impedance (about Ο8 micro Λ Λ) was successfully integrated into the high-performance non-lanthanide Si'H TFT fabrication. Other patents describing tft in the field of semiconductors are as follows: U.S. Patent No. 6,992,234, 6, 489, 222, 6, 613, 697, incorporated herein by reference in its entirety for the use in the the the the the the the the The splashed eye & is made to make a film. The scale target is made of a turn, a crane or a charm. The film made by the target of the reduction can replace the conventional and/or key layer in the TFT丄CD. Since the average (four) grain size and texture of the entire thickness of the metallographic targets are excellent, the film obtained from such a target has a fine particle non-band shape with random particle orientation. Provided in a particular embodiment of the invention - <RTIgt; </ RTI> <RTIgt; </ RTI> In this embodiment, the film is at least 1 angstrom, in some examples at least angstroms, and in the eight examples it is at least 5 〇〇. Gentry. In this embodiment, the film can reach 5,000 angstroms in 28 200902741, 3,000 angstroms in some instances, 2,500 angstroms in other instances, and 2,000 angstroms in some cases. In addition to metal films on a variety of different substrates, it is also possible to generate MOx (oxidation), MNX (nitride), MSix (deuterated), and any combination thereof (such as MOxSiy, etc.) by reactive sputtering or ion implantation. M is a metal. The metal atoms according to the present invention include, but are not limited to, sharp, bismuth, tungsten, molybdenum, chin, wrong, collateral, hunger, town, tin, wrong, inscription, recital, copper, recorded, silver, gold, aunt, iron, A mixture of two or more of ruthenium, osmium, gallium, indium, and yttrium. Regarding many applications, glass is not perfect, especially for architectural purposes. On one side, in colder climates, the low reflection of glass in far infrared (room temperature radiation) causes a poor loss of heat energy required to heat the building. On the other hand, in areas with hot climates, the high penetration of glass in near-infrared (solar radiation) increases the energy required to cool a building. Glass coatings for construction are known in the art: for example, the following disclosure of glass coatings for construction is incorporated herein by reference for disclosure of several architectural glass coatings: DC reactively sputtered antireflection coatings Splashing anti-reflective coating) (U.S. Patent No. 5,270,858), Multilayer antireflection coating using zinc oxide to provide ultraviolet blocking (U.S. Patent No. 5,147,125) using zinc oxide to provide ultraviolet blocking. Coated architectural glass system and method (US Patent No. 3,990,784), Electrically-conductive, light-attenuating antireflection coating (US Patent No. 5,091,244) 29 200902741 俨虞: "Ming, hunting is made by using the above-mentioned power or cold spray process to create a film with a splash target. The target of the reduction! ^ 墼射射... I know it is made of zinc I. In the zinc target Splashing n, in the chamber (such as air or oxygen) bow into the oxygen, thereby taking the zinc film. By the splash target Broken glass film system may be substituted zinc oxide layer. * Now on glass coating may be carefully designed to overcome all these drawbacks. The purpose of this coating and the like to control the energy delivery is by adding more effective for the glass
熱或空調。該等塗層是多層金屬及陶€,其準確組合物是 依特定需要而制定。熱反射(所謂的低發射率)塗層允許最 大量日光通過’但接著阻斷光撞擊—物件時產生的熱(溫室 效應)。 用於大面積玻璃塗層的最重要金屬化合物是(但不限 於)Si〇2、SiN4、Sn〇2、Zno、Ta205、Nb205 及 Ti〇2。藉由 矽(Si)、鋅(Sn)、鈕(Ta)、鈮(Nb)及鈦(Ti)金屬目標的反應濺 擊可传到這些薄膜塗層。藉由上述動力或冷噴霧製程以製 造該等激擊目標。 根據本發明可使用的其他領域薄膜是光學塗層等塗層。 光學塗層包括反射及抗反射材料,提供選擇性透射的塗層 (即濾波器)’及非線性光學應用。如Ti〇2薄膜及Nb205薄 膜等範例是由钽及鈮濺擊目標所反應濺擊成的。 用於汽車應用,需要透射70%可見光及反射100%(或接 近)紅外線(IR)及紫外線(UV)的塗層,以符合汽車製造商設 定的目標。 用於薄膜用途的上述領域包括磁性薄膜材料。薄膜材料 30 200902741 科學對磁碟機儲存技術的衝擊是—重大革命,從鐵酸鹽讀 寫頭及微粒磁碟轉變為薄膜磁碟及讀寫頭。薄膜磁碟的未 來世代需要高矯頑力及高感應。薄膜媒體亦必須是平滑的 且比目前㈣表面更薄以達成較高記《度。垂直記錄顯 然是最有前途以達成極高記《度的科技。磁性薄膜材料 的數個範例如用於儲存應用祕、鉻、錄、鐵、銳、錯、 删及翻的合金。根縣發明,藉由制上述動力或冷 製程所製造的濺擊目標以製造—薄膜。該濺擊目標由以下 金屬中至少二者的合成物所製成:鈷、鉻、鎳、鐵、鈮、 鍅、硼及鉑。 ^如上述’該薄膜亦包括半導體應用。在—Ar_N2周圍 裱境中減擊组以形成一氮化组(TaN)層,其作為一銅層與用 於半導體晶片的-石夕基板之間的一擴散障壁層使用,以確 保使用尚導電銅的互連。 因此本發明亦相關於數個濺擊目標,其包括耐炼金屬 銳组、鶴、翻、鈦、錯、鉻、鈒及釕,與金屬鎮、錫、 釔、鋁、鋅、銅、鍺、銀、金、鈷、鐵、銖、鎵、銦、銻、 其一或多者的混合物,或其二或多者的合金,或與具有上 述特性的其他金屬的合金。 較佳地’由鎢、鉬、鈦、鍅或其二或多者的混合物,或 其二或多者的合金,或與其他金屬的合金形成的目標,極 佳疋钽或鈮形成的目標’藉由冷喷霧或動力喷霧施加到一 待塗裝基板的表面。在該等冷喷霧目標中,相較於該等粉 末的氧含罝,該金屬的氧含量幾乎不變。與藉由電漿喷霧 31 200902741 次猎由真空„製成的目標相比,此等 目標顯示相當程度較古&、務或動力喷霧 失數^ “的讀。此外,依粉末特性及塗声 ;:’可製造此等冷細動力嗔霧目標無任何㈣ 或具有小紋理。 1」、、又埋 7人驚冴地’已發現減少該冷喷霧或動 :量:該等賤擊薄膜層的密度及其他特性獲得改善^ 金:::中的乳職擊速率’因此影響薄膜的均勾。用於 玉4膜,由於氧對該薄膜電阻係數的影 氧是不良的。 “辰度的 我們已發明-種_擊目標及製造触目標的方法,該 鈕目標具有大體上小於44微米的均勻細粒結構,由電子; 向散射繞射儀("EBSD”)測量時不具有較佳紋理定向,及遍 及該目標的本Μ示無齡尺寸或㈣帶狀,及亦具有可 目標複製到另-目標的一微結構。此外,我們已發明 一種用以修復此類目標以及某些熱等壓壓平式(HIP式)目 ;^的製程’其在修復前完整複製該目標的微結才冓。當用以 修復較差微結構的其他目標時,歸復區段具有改良微結 構,就像以此技術製成整個目才票。該技術不受形狀或材料 限制’已用以製造平面、縱斷面及圓柱形目標及噴霧一系 列目標組成物。 ’ 本發明所作改良包括熱處理以改良該目標的微粒間結合 及應力減低,以及設計該目標組件的材料以使同樣喷霧應 力的效應減到最小,及容許整個組件的熱處理以免除傳統 支持板材料所需的拆卸步驟。 32 200902741 藉由冷噴霧科技的熱管理材料 此等金屬矩陣合成物的目標為產生一合成材料,… 加銦或鶴的低熱膨係數以減低加熱槽相對财晶片的差另: 膨脹及收縮的同時’維持該等金屬元素的高熱傳導性。 傳統上’該:業已研發出鎢-銅(WCu)或鉬-銅(MoCu)金 屬矩陣σ成物’藉由燒結錮或鎢(稱為”骨架”),接著在溫 度及塵力下㈣化的銅滲透,以產成―金屬輯合成物。 ”此技術相關連的困難在於此技術是個昂貴的操作。該渗 透溫度通常在攝氏_度或更高的範圍。 / 卜目如WCu或MoCu合成物加熱槽製造需要先製造 鎮塊’切片成-適當尺寸’接著是銅滲透。然、後最終使用 者需要進—步將它切片«當厚度及蚊尺寸。冷噴霧可 直接製造極薄、同質分布的合成物。 相較於’燒結及滲透"操作,冷喷霧是更不昂貴的操作, 因冷喷霧是在遠低於該等材料熔點的溫度由粉末製出零件 的直接途徑。 以下準備數個範例: 範例1是一平面鈕濺擊目標製造、測試及薄膜評估。 乂尺寸為15至38微米的纽粉(Amperit # 151,特級,商 業純度(>99.95钽),H.C. STarch公司製造)冷喷霧額定厚度 1/8,直徑3·1"的二平面圓板’以提供3〇〇吋的總厚度。 §亥氣體,在一例子中是氮,在另一例子中是氦,預熱到攝 氏6〇〇度,並在3百萬帕(MPa)的一不流動壓力使用。使 用冷氣體科技公司(德國Ampfing)的市售Kinetiks搶噴霧 33 200902741 該粉末及氣體。噴霧後,該圓盤以機器加工到額定ι/4”厚 度,及在濺擊前抛光該濺擊表面(參閱圖1)。該等目標通過 程序中的一標準焚燒,然後使用數個標準條件,用以使用 -直流電(DC)磁電管濺擊單元來製造數個薄膜。 圖2顯示,賤擊後的目標表面。為比較目的,亦在相同條 件下漱擊一標準輾恩式圓盤目標。以下表i中顯示所製造 的4等膜的測侍特性。们顯示由該等冷喷霧目標製成的 膜-有佳均勻’因容許製程巾使用較低膜厚度及以較 乂時間姓缝小電路產生較少组廢料,因此是極吸引積體 電路(’’1C”)製造商的—特點。對於電氣及物理特性兩者及 追求減小^上的電路結構尺寸,改善均勾是極為重要 的相車乂於一傳統目標,一冷喷霧目標的極細及隨機顆粒 結構直接造成此均勻改呈。 圖4所不用過的目標表面可直接說明此均勻改善。圖4 义特寫.兒明-輾壓式鑄模冶金目標(上圖)及出(氮)冷喷霧 丁 (下圖)才目車乂於冷噴霧目標的表面,濺擊後,該輾壓 、' U雜色且不規則的表面。造成冷喷霧目標的較 平滑非雜色表Φ是ϋ較均勻減理微結構,其依次產生一 較均勻減擊速率及作為結果的膜(參閱圖3)。表i中亦顯示 全部三個膜的電阻係數及表面形態都類似。因此,可認定 冷喷霧目標製成的賤擊膜與μ式鑄模製,的傳統目標-樣好或更好。圖3亦顯示由該等目標製成的膜具有不同的 内部形恶,11喷霧目標造成—柱狀内部結構(圖3Α),氮噴 霧目標造成-各方等大内部結構(圖3Β),及健式目標造 34 200902741 成一較無圖形的内部結構(圖3C)。 表1.數個濺擊膜的特性 薄膜特性 膜 編 號 製程 厚度(奈米) 平均 厚度 (奈米) 膜厚度 不均勻 Rs (歐嫁sq) 電阻係數 (歐姆 妙) 微 結 構 表 面 形 態 106 CSHe 230,168,197 198 1.50% 8.642±2.4°/〇 1.71E-04 平滑 107 CSHe 157,170,170 166 3.40% 10.281±3.6% 1.71E-04 城 平滑 109 csn2 288^88^27 268 3.50% 8.713±3.6°/〇 2.33E-04 平滑 110 csn2 288^04^06 233 4.00% 7.867i4.0% 1.83E-04 各方等大 平滑 111 雛式 4.30% 8.42U4.4% 112 雛式 244 244 5.00% 7.87&M.2% 1.92E-04 無圖形 平滑 113 雛式 15.40% 4.120*12% 114 雛式 275^48^30 251 7.40% 6.76U7.9% 1.70E-04 無圖形 平滑 範例2管狀鈕目標預成型品製造及微結構分析 使用範例1的相同操作參數以製造數個管狀钽預成型品 (參閱圖5)。數個樣本是自該等預成型品切下及在不同溫度 退火。然後準備數個冶金底座,及在該等同樣喷霧及退火 的樣本上執行微結構分析。表2顯示該等特性的摘要。所 有樣本皆來自一預成型品,其使用的一粉末具有15.9微米 (微粒計數式分布)及大約26微米(整體式分布)的一開始中 間尺寸。 表2.同樣噴霧及後續退火的冷喷霧钽的微結構特性摘要 35 200902741 條件 同樣 沉積 退火 攝氏942度 退火 攝氏1150度 退火 攝氏1450度 熱等壓 壓平(HIP) 攝氏1300度 粉末尺寸㈣ 15.9 15.9 15.9 15.9 15.9 顆粒尺寸(m) 12 12 6.7 10.6 5.5 顆粒形狀 長形 長形 各方等大 各方等大 各方等大 再結晶 否 否 是 是 是 結晶定向 隨機 隨機 隨機 隨機 隨機 表2及圖6顯示在同樣喷霧、退火兩者與熱等壓壓平(HIP) 條件中的冷喷霧鈕的特徵特點。圖中顯示製程溫度。所有 退火是保持溫度達1.5小時,及熱等壓壓平(HIP)週期是保 持溫度達3小時。開始粉末尺寸似乎是控制作為結果的顆 粒尺寸,甚至在高溫退火後亦是如此。因此特有地,冷噴 霧材料的顆粒尺寸小於44微米,而甚至大規模工作的鑄模 材料通常將具有60至100微米的顆粒尺寸,甚至更大尺 寸。此較細顆粒尺寸又是該目標造成較均勻膜的一重要特 徵,然而,為造成結果,必須與一完全無紋理微結構相結 合。 圖6說明同樣喷霧材料的扁平或長形或晶狀體結構,其 在退火期間再結晶成數個各方等大顆粒,退火前後皆極細 粒結構,及甚至在廣泛退火後,顆粒尺寸仍等於或小於原 粉末微粒尺寸。 由電子背向散射繞射儀(EBSD)檢查四個冷噴霧樣本及 一個電漿噴霧樣本,以判定所呈現結晶紋理的本質。全部 36 200902741 都是通過厚度的樣本,及全部定向以用於電子背向散射繞 射儀(EBSD),因此喷霧方向是垂直向下。 在材料科學的相關情況中”紋理”表示”結晶較佳定向”。 此等定向在一樣本中完全隨機,則說該樣本不具有紋理。 若該等結晶定向並非隨機,卻具有一些較佳定向,則該樣 本具有一弱、強,或中間紋理。電子背向散射繞射儀(EBSD) 藉由應用Kikuchi繞射圖案而得到樣本的定向資訊,該繞 射圖案是將樣本蓋瓦約攝氏70度時形成。 該等樣本在經過安裝、抛光及利用表3所示步進尺寸蝕 刻後,由電子背向散射繞射儀(EBSD)以高解析度(2與4微 米步進尺寸)或較低解析度(50微米)描繪其特徵。基於樣本 的顆粒尺寸選取步進尺寸,以確保在合理時間完成電子背 向散射繞射儀(EBSD)掃描時未錯過小特徵。 表3 製程 EBSD步進 EBSD區域 指數% CS, 1450〇c 2μπι 330μιηχ300 94 CS, 1150°C 2μπι 330μιηχ300 95 CS, 942〇C 2μπι 280μηιχ250 66 CS,無退火 4μηι 3區域’ 330μηιχ150 71 至 73 電漿噴霧 50μιη 2.95mm><9 96 結果一冷喷霧,在攝氏1450度退火 圖7A中顯示相關3個正交方向的紋理圖。定向在{100} 方向的20°内的顆粒以藍色表示,在{111}方向的20。内以 黃色表示,及在{110}方向的20°内以紅色表示,當定向錯 37 200902741 误減少時顏色漸暗。灰色㈣定向在三定向之間的顆粒。 圖中顏色的隨機分布是由該等個別輪的隨機分布造成。 若該等顆粒呈現任何特定紋理,料顏色中的—者會有優 勢’意即若大部分顆粒定向在{100}方向中,黃色會是主要 顏色。 曰 該等極地圖(圖7B)亦顯示完全缺少對稱,再指明該微結 構中缺少紋理。由該等紋_及極地圖可認定該樣本具有 無紋理帶狀的_隨機紋理,及料顆粒是隨機定向,具有 小顆粒尺寸且無系統特徵。 攝氏 1150 疳禍' 如圖8中該等紋理圖及極地圖所示,該紋理是隨機的。 該顆粒結構比在攝氏丨彻度退火的樣本者更細。 攝氏942磨银小 如圖9所不’此樣本亦具有—隨機紋理。然而,該指數 化比率遠低於先前樣本,指明該材料保留—高張力-該材 料在較低退火溫度未再結晶❶ 同樣也士Π °亥等紋理圖及極地圖所示(參閱圖1 〇及11), 發現3亥紋理是隨機的,且通過該厚度是均勻隨機。在此例 中’以下3個紋理圖代表3個檢查區,第—個是沉積第一 材料者(該喷霧層的底部),及最後—個是沉積最後材料者 (3亥贺霧層的頂部):所有圖皆顯示相關該垂直方向(通過厚 度方向)的紋理是隨機的。 結果一電漿哈 38 200902741 ••亥基板或支持板(圖12至13的紋理圖的下部)具有各方 等大的極大顆粒,其具有輾壓式及過度退火圓盤的一紋理 特點。紋理圖中的該等顆粒主要是藍色及黃色,及數個極 地圖H3,其僅包括該紋理顆粒圖的較低三分之一部分,在 {1 〇〇}//ND及.{11丨}//ND顯示數個峰值(雖然是較弱峰值), 其中ND表示垂直於該樣本表面。該等H3極地圖的三重 對稱是輾壓的證據。 该電漿沉積材料顯示數個柱狀顆粒,具有許多低角度邊 界(顆粒圖中以紅色表示)。如該等極地圖H1(紋理顆粒圖的 上部二分之一)中所示及藉由該圖中藍色的優勢,該紋理主 要疋{100}//ND。極地圖H1是有效軸對稱的。 該等柱狀顆粒下方更粗糙的各方等大地帶的起源及原因 未知。 由於包括的點數極小,因此Η1及H3極地圖兩者皆弄成 15°平滑角半寬(相較於平常的1〇。),以避免非必要峰值的 導入。 簡言之,以上電子背向散射繞射儀(EBSD)分析顯示在該 等同樣冷噴霧及退火冷喷霧目標中一完全隨機非紋理微結 構,無關於退火溫度。電漿喷霧目標顯示重大紋理。 範例3钽-鈮(TaNb)冷喷霧目標 將一 50/50體積百分比的鈮-钽(NbTa)矩形目標直接冷噴 霧在一銅支持板上。圖14顯示由於該沉積物中的同樣嘴霧 應力,因此在該銅支持板中產生3毫米(mm)的彎曲。支持 板必須是平的以緊靠其配對凸緣密封。因該等應力在機哭 39 200902741 加工期間將只重新分布而造成連續變形,因此無法以機器 加工除去該彎曲。由於同樣噴霧鈕、鈕-鈮(TaNb)及冷噴霧 沉積物通常具有極有限的可塑性(圖15),因此亦無法機械 地壓去該彎曲。 然而,實驗顯示藉由退火可大大地提高可塑性。圖Μ 顯示一鈕沉積物在攝氏95〇度退火15小時後,可塑性地 變形而得到一永久變形。將銅支持板自該目標移除;接著 將該目標退火,彎平及以機器加工(圖17)。 由此範例亦明顯看出,用於藉由冷喷霧的耐熔金屬目 標,傳統的銅及IS支持板材料並不理想。M傳統銅及銘 支持板具有高熱傳導性,但其彈性係數趨低(促成變形), 具有大熱膨脹係數(”CTE”)無法與該等耐熔金屬匹配(促成 變形及退火期間增加該目標與支持板之間結合失敗的可能 性)’及具有低熔點(當黏合支持板時妨礙退火製程)。表4 顯示如鉬、鈦或316不銹鋼的材料具有較佳特性組合以抵 抗冷喷霧製程期間的彎曲(高彈性係數),或會容許在耐熔 金屬所需的高溫退火(熱膨脹係數("CTE")與該等耐熔金屬 者相近及高溶點)。 可使用冷噴霧以製造—多層式目標,其克服該熱膨脹係 數(CTE )不匹配及上述造成不良結果的問題。不直接在該 支持板上噴霧可濺擊的目標材料,卻可先喷霧一薄塗層或 數個塗層,其具有一熱膨脹係數(”CTE”)介於該支持板與該 目標材料者之間。此等中間層可具有〇 25至2 〇毫米 的厚度。噴霧此一層的一方式是使用一粉末混合物,其包 200902741 括該支持板材料及該目標材料 __.目標及支持板材料胜,14 ,.,, ~ ' π~~~--- 材料 熱傳導性 '--- 單性係數 熱膨脹係數 熔點 ------ 卡公分/公分2 秒它 X10'6PSI 公分/公分°c °C 銅 ------ ---------- —_ 0.94 -----—__ 1 17 16.5 1083 鋁 0.53 10 23.6 660 鈮 0.12 17 7.3 2468 纽 0.13 27 6.5 2996 鉬 .34 47 4.9 2610 鈦 0.22 16.8 8.4 1668 316 不錄鋼 28 14 〜1350 KNbTal 日標的濺墼 將該偽合金(钽及鈮粉末依然在化學上有區別)目標放置 在一 18"x5"的平面磁電管陰極濺擊器中。目標設定尺寸是 4”xl7"x 大約 0.125”。 進行三個測試:直金屬沉積、氧化物沉積及氮化物沉積。 使用的條件及得到的結果說明如下。 直金屬沉積 進行濺擊是使用在100 seem的氬氣,利用ι·〇 x 1〇_3托 (基本壓力4x 1〇_5托)的一濺擊壓力,5〇千瓦,55〇伏, 約略73瓦/平方吋。目標自一開始極佳地濺擊,無電弧形 成,無穩定度所需的真實"燒毁,,時間。 在一承物玻璃片上沉積1401埃的一最終膜厚度(如一 Dektak 2A顯微斷面測量儀所測量p此為沉積時間為上埃 41 200902741 瓦平方寸移的-速率’稍高於用於鈮及鈕的個別速 率°版電阻為3·7歐姆/平方(如利用4 ρί•探針在該承物玻 璃片上所測量)。算出此結果是51·8〇_歐姆公分。 該算出結果高於大約28口_歐姆公分的期望電阻係數。此 材料對背景屋力(雜質)敏感,及需要用栗抽吸到低的_5至 -6托範圍以用於適當電阻係數數值。該膜的日光吸收是 〇_4U如按照ASTM 5903及Ε490所測量及計算)。 氧化物沉積 #進行錢擊是使用在⑽_的氬及在90 sccm的氧(較低 氧位準造成逐漸切換到金屬模式),在12至3托,3 〇千 瓦(44瓦/平方叶),在副伏。此為在氧化物模式比在金屬 模式中具有較高Μ電壓的少數材料之_。制該Μ〇χ D.C·在20 赫操作的Sparc_le單元上供應一添加物。再 仔到-極穩定濺擊製程,無電弧形成且無問題產生。減擊 良率疋至屬比率的40%。此製程提供—極美觀透明膜,透 射中具有些微粉紅色彩’反射中具有些微綠色彩,最終膜 厚度疋4282埃。算出折射率是2·8,此折射率高於個別纽 及鈮氧化物的折射率(大約2.2至2.3)。 氮化物沉積 進行滅擊是使用在100咖的氣及在2〇〇咖的氣, 大約2·0 X 1G-3托的轉壓力。該氮化物鮮令人滿意且 十分穩定n即使在嘗試許多製程參數後仍無法產生 一透明氮化物塗層。利用該MDX及Sparc_le單元的3〇 千瓦運作良好1擊良率是金屬比率的m最終膜厚度 42 200902741 =歐姆/平方是刪埃(126G微歐姆公分)。測得日光吸 光為0.5 9。 一些觀察結果是: 在金屬模式中濺擊令人滿意; 在氧化物模式中丨賤擊極佳。 未注意到電孤,此表示該目標中的氧化物含量是穩定的’ 及該目標在沉積期間未構成—介電層。極高指數氧化物, 其將量化及用於變化的測量以作為由於位置及時間的一化 學函數。 絕佳明確跑道’該跑道中無變色點。 整個目標以一良好速率沉積。 在最大功率5千瓦(kW)運作目標,5千瓦換算成75瓦/平 方吋一參考鈦(Ti)或鎳-鉻(Ni_Cr)是在35瓦/平方吋濺擊。 目標功率在1千瓦增加巾斜升,未注意财問題。 在高功率,就目標膨脹、過度加熱而言’未注意到有問題。 良好疋尺寸穩定性,在該等夾頭或邊緣無問題產生。 fe例5. —銅支持板上的一冷喷霧鈕-鈮(TaNb)目標的退火 及弄平 冷喷霧一 17”xl.5”x〇.3〇〇鈕-鈮(TaNb)沈積物在一 〇 5〇〇 厚度銅支持板上。在喷霧該純鈕_鈮(TaNb)前,在該銅上喷 霧大約0.030"厚的一 50%銅50%(TaNb)層,以提供一中間 遵從熱膨脹係數(CTE)層。該同樣喷霧組件具有大約〇·2吋 的一中點彎曲。接著將該目標組件在攝氏825度真空退火 1.5小時一正足以在該鈮中導入恢復及使它可延展。一旦 43 200902741 冷卻,將該目標組件放置在一壓平機中,成功地壓平到 0.010吋之内,及完成機器加工。 範例6.大約50/50百分比組成的.^^(M〇Ti)濺擊目標, 其中藉由熱等壓壓平(HIP)及藉由冷噴霧製造。該M〇Ti合 金系統未呈現100%固體溶性,及包含數個有害易碎中間 相。當鉬(Mo)及鈦(Τι)在液態中鑄成合金時,此等相是無 法避免的。研發HIP參數的目標是為使此等相的形成減到 最小。但由於該二元素的互相擴散,若想達成全足密度, 同樣是無法避免此等相的形成。圖19清楚顧示此等有害相 在攝氏825度、15,000 ksi進行熱等壓壓平出辽丨達7小時 的粉末中出現。大約15至20微米厚度的一第三相材料地 帶包圍鈦粉及鉬粉兩者(圖19),然而,顯示鉬與鈦未互相 擴散,及藉由冷喷霧產生的目標中僅存在鉬及鈦的純元素 相。圖20顯示即使在攝氏700度退火15小時後,大體上 無互相擴散,及在此放大率下,無可見的有害相形成。 里一以製造备二銅(WCu)合成物熱管理材料的冷喳稼倏#列 出如下: 设備·冷氣體科技公司(德國)Kinetiks 3000或Kinetiks 4000 冷噴霧條件:氮氣在攝氏600至900度,壓力在2〇至4 〇 百萬帕(MPa) ’粉末饋入速率在3〇至9〇克,及噴霧距離 10至80毫米。 較佳條件:攝氏8〇〇至900度及壓力3至3.8百萬帕,功 率饋入速率每分鐘30至50克,及噴霧距離20至4〇毫米。 使用粉末: 44 200902741 鎢(W) : AMPERIT 140,25/10微米微粒切片,燒結;及 銅(Cu) : AMPERIT 190,35/15微米,氣體原子化。 兩種材料皆由H.C. Starck公司製造。藉由混合約50體積 百分比的W與50體積百分比的銅以製造該冷喷霧WCu 樣本,及饋送通過CGS冷喷霧系統的粉末進料器以製造 WCu合成物。該等基板可以是不銹鋼或鈦。合成結構與基 板之間的結合絕佳。圖21A及21B中顯示W-Cu(50/50體 積百分比)的微結構。 以下表格顯示該同樣喷霧WCu具有193 W/m-K的熱傳導 性,及13.49 ppm/°C的熱膨脹係數。在華氏1600度(攝氏 871度)經過2小時及4小時的退火顯示熱傳導性及熱膨脹 係數兩者的重大改善。清楚地證明退火是一重要步驟,用 以重大地增強熱傳導性及用以減低熱膨脹係數以用於冷喷 霧熱管理材料。 樣本識別 熱傳導性 W/mK 熱膨脹係數 ppm/C 照原狀 193 13.49 2 小時 X 1600F 281 11.8 4 小時 X 1600F 276 11.82 藉由冷喷霧技術製造的該等熱管理產品具有以下組合 物: 鎢-銅(WCu)化合物:具有鎢(W)含量從10%至85%不等 鉬-銅(MoCu)化合物:具有鉬(Mo)含量從10%至85%不等。 用於熱管理應用,藉由冷喷霧製程製造的化合物的主要特 徵是: 45 200902741 ⑷銅扁平微結構,亦可使用其他金屬,如:銀、铭或金。 ()鉬或鎢將大體上維持其微粒形態或成團微粒。亦可使用 八材料如氮化銘(A1N)、碳化石夕(Sic)等。圖21A及B中 顯示W-CU(50/50體積百分比)的微結構。 所有上述參考文件全部内容以引用方式併入本文中以用 於所有有用目的。 雖然顯示及說明某些特定結構以具體表現本發明,但熟 諳此藝者應明白,不背離該基本創新概念的精神及範圍, 可作出該等組成部分的各種不同修改及重新配置,及該等 組成部分不限於本文中所示及所述的特定形式。 【圖式簡單說明】 圖1(A)說明藉由使用氦氣的冷賴所製造的數個平面式叙 目標; 圖1(B)說明藉由使用氮氣的冷喷霧所製造的數個平面式麵 目標; 工’一 圖2説明滅擊後藉由冷喷霧所製造的數個平面式组目標; 圖3以掃描電子顯微鏡(”SEM”)顯微照片說明藉由氦冷喷 霧、氮冷«及輾壓式短金錢所預備的數個目標轉出 的數個钽薄膜; 圖4A以特寫鏡頭說明滅擊後的輾壓式目標,顯示該輕壓 式目標的雜色及不規則表面; 圖4B以特寫鏡頭說明濺擊後的氦冷噴霧式目標,顯示該 氦冷喷霧式目標的較平順、非雜色表面; 圖5說明根據本發明的數個鈕管狀預成型品; 46 200902741 圖6以顯微照片說明垂直於喷霧方向所取得的數個同樣喷 霧及退火的結構; ’、 圖7AU說明使用冷喷霧及在攝氏咖度退火的數個社 果; 、、° 圖8說明使用冷喷霧及在攝氏115〇度退火的數個結果; 圖9說明使用冷喷霧及在攝氏942度退火的數個結果; 圖10說明該基板具有數個各方等大的極大顆粒,其具有輾 壓過及過度退火板特有的一紋理; 圖11說明根據本發明的數個極地圖; 圖12說明該電漿噴霧式鈕樣本,其具有數個各方等大的極 大顆粒,其具有輾壓過及過度退火板特有的一紋理; 圖13說明根據本發明的數個極地圖; 圖14說明冷喷霧鈕-鈮(TaNb)目標,沉積物超過44〇毫米 長,110毫米寬及7毫米厚,請注意在該銅支持板的中央 引起3毫米弯曲; 圖15說明用於同樣喷霧鈕的負載對偏斜,請注意因易碎裂 縫造成的沉積物失敗,未呈現任何塑性變形; 圖16說明在彎曲測試期間偏斜〇 〇8吋後,在钽沉積物中 得到的永久變形; 圖17說明退火及弄直後的一目標,直邊尺證明已成功地移 除該彎曲; 圖18說明一鉬-鈦(M〇Ti)目標的微結構及該等有害相,及 熱等壓壓平("HIP")期間為合併該粉末所產生的相互擴散 帶; 47 200902741 圖19說明由冷喷霧產生的一同樣喷霧鉬_鈦目 構’其只包含元素姻及元素钬,及無有害相心的微結 圖別說明在攝氏700度及L5小時退火後的冷喷霧翻喊, 顯不相較於—熱等壓壓平("HIP”)目標(圖19),大體上益古 害相形成; …有 圖21A說明鎢-銅(w_Cu)(5〇/5〇體積百分比)的微結構; 圖21B說明具有一扁平結構的銅(Cu)。【主要元件符號說明】 r /- k 48Hot or air conditioning. These coatings are multi-layered metals and ceramics, the exact composition of which is tailored to specific needs. The heat reflection (so-called low emissivity) coating allows the maximum amount of sunlight to pass through, but then blocks the heat generated by the impact of the object (greenhouse effect). The most important metal compounds for large-area glass coatings are (but are not limited to) Si〇2, SiN4, Sn〇2, Zno, Ta205, Nb205, and Ti〇2. These thin film coatings can be transmitted by reactive sputtering of yttrium (Si), zinc (Sn), button (Ta), niobium (Nb) and titanium (Ti) metal targets. The slamming targets are manufactured by the above-described power or cold spray process. Other areas of film that can be used in accordance with the present invention are coatings such as optical coatings. Optical coatings include reflective and anti-reflective materials that provide selective transmission of coatings (i.e., filters)' and nonlinear optical applications. Examples such as Ti〇2 film and Nb205 film are splashed by sputum and sputum splash targets. For automotive applications, it is required to transmit 70% visible light and reflect 100% (or close) infrared (IR) and ultraviolet (UV) coatings to meet the automotive manufacturer's goals. The above areas for film applications include magnetic film materials. Thin Film Materials 30 200902741 The impact of science on disk storage technology is a major revolution, shifting from ferrite read and write heads and particle disks to thin film disks and read/write heads. The future generation of thin film disks requires high coercivity and high inductance. The film media must also be smooth and thinner than the current (iv) surface to achieve a higher score. Vertical recording is clearly the most promising way to achieve extremely high-tech. Several examples of magnetic thin film materials are used, for example, for the storage of alloys of application, chromium, recording, iron, sharp, offset, deletion and turning. Geno County invented the manufacture of a film by sputtering targets made by the above-mentioned power or cold process. The splash target is made from a composition of at least two of the following metals: cobalt, chromium, nickel, iron, ruthenium, osmium, boron, and platinum. ^ The film as described above also includes semiconductor applications. The shock group is formed in the surrounding environment of -Ar_N2 to form a nitride layer (TaN) layer, which is used as a diffusion barrier layer between the copper layer and the -shixi substrate for the semiconductor wafer to ensure that the use is still conductive. Copper interconnection. Therefore, the present invention is also related to several splash targets, including metal-resistant fine sets, cranes, turns, titanium, aluminum, chrome, niobium and tantalum, and metal towns, tin, antimony, aluminum, zinc, copper, antimony, Silver, gold, cobalt, iron, ruthenium, gallium, indium, antimony, a mixture of one or more thereof, or an alloy of two or more thereof, or an alloy with other metals having the above characteristics. Preferably 'by tungsten, molybdenum, titanium, niobium or a mixture of two or more thereof, or an alloy of two or more thereof, or an alloy with other metals, the target of excellent bismuth or bismuth formation' Apply to the surface of a substrate to be coated by a cold spray or a power spray. In these cold spray targets, the oxygen content of the metal is almost constant compared to the oxygen containing enthalpy of the powders. Compared with the target made by vacuum spray 31 200902741, the target shows a considerable degree of reading of the older & In addition, depending on the characteristics of the powder and the sound of the coating;: 'There can be any such cold and fine power fog target without any (4) or with a small texture. 1", and buried 7 people with horror 'have been found to reduce the cold spray or movement: the amount: the density and other characteristics of the slamming film layer are improved ^ Gold::: the milk strike rate' Affect the uniformity of the film. For the Jade 4 film, oxygen is poorly affected by the oxygen resistance of the film. "We have invented - a method of hitting a target and making a touch target, the button target has a uniform fine grain structure of substantially less than 44 microns, measured by electrons; when measured by a scattering diffractometer ("EBSD") There is no better texture orientation, and the present invention shows no age or (4) strips throughout the target, and also has a microstructure that can be copied to another target. In addition, we have invented a process for repairing such targets and certain hot isostatically pressed (HIP-type) targets, which completely replicate the target before repair. When used to repair other targets of poor microstructures, the recovery section has an improved microstructure, just like this technique. This technique is not limited by shape or material 'has been used to make planar, longitudinal and cylindrical targets and spray a range of target compositions. 'The improvements made by the present invention include heat treatment to improve the interparticle bonding and stress reduction of the target, and designing the material of the target assembly to minimize the effects of the same spray stress, and allowing heat treatment of the entire assembly to eliminate conventional support sheet materials. Required removal steps. 32 200902741 Thermal management materials by cold spray technology The goal of these metal matrix compositions is to produce a synthetic material, ... with a low thermal expansion coefficient of indium or crane to reduce the difference between the heating bath and the wafer: another expansion and contraction 'Maintain the high thermal conductivity of these metal elements. Traditionally, the tungsten-copper (WCu) or molybdenum-copper (MoCu) metal matrix sigma has been developed by sintering tantalum or tungsten (referred to as "skeleton"), followed by temperature and dust (four) The copper penetrates to produce a metal-composite. "The difficulty associated with this technology is an expensive operation in this technology. The permeation temperature is usually in the range of Celsius or higher. / The manufacturing of the heating tank of the WCu or MoCu composition requires the first fabrication of the town block - sliced into - appropriate The size 'follows the copper infiltration. Then, the end user needs to step in and slice it «in thickness and mosquito size. Cold spray can directly produce a very thin, homogeneously distributed composition. Compared to 'sintering and infiltration" Operation, cold spray is a less expensive operation, because cold spray is a direct way to make parts from powder at temperatures well below the melting point of the materials. Here are a few examples: Example 1 is a flat button splash Target manufacturing, testing and film evaluation. 纽 New size powder of 15 to 38 microns (Amperit # 151, premium grade, commercial purity (>99.95钽), manufactured by HC STarch) Cold spray rated thickness 1/8, diameter 3 · 1 " two-plane circular plate 'to provide a total thickness of 3 。. § Hai gas, in one case is nitrogen, in another example is 氦, preheated to 6 degrees Celsius, and at 3 One million kPa (MPa) Flow pressure used. Commercially available Kinetiks rush spray 33 using cold gas technology company (Ampfing, Germany) 200902741 The powder and gas. After spraying, the disc is machined to a nominal ι/4" thickness and polished before splashing. Splash the surface (see Figure 1). These targets are incinerated by a standard in the program and then used in several standard conditions to fabricate several films using a direct current (DC) magnetron splash unit. Figure 2 shows the target surface after the sniper. For comparison purposes, a standard 辗 disc target is also struck under the same conditions. The measurement characteristics of the produced 4th film are shown in the following Table i. We show that the film made from these cold spray targets - good uniformity - is extremely attractive because it allows the process towel to use a lower film thickness and a smaller number of scraps generated by a smaller circuit. ''1C') The characteristics of the manufacturer. For both electrical and physical properties and the pursuit of reducing the size of the circuit structure, the improvement of the hook is extremely important for a traditional target, a cold spray target The extremely fine and random particle structure directly causes this uniform change. The target surface used in Figure 4 can directly explain this uniform improvement. Figure 4 义明. 儿明-辗压式模模金属冶金 target (above) and out (nitrogen) Cold spray Ding (below) only looks at the surface of the cold spray target. After splashing, the rolling, 'U motley and irregular surface. A smoother non-color table that causes the cold spray target Φ It is a more uniform mitigation microstructure, which in turn produces a more uniform attack rate and the resulting film (see Figure 3). Table i also shows that all three films have similar resistivity and surface morphology. Identify the sniper film and μ made of cold spray target The traditional goal of mold-casting is better or better. Figure 3 also shows that the membranes made from these targets have different internal forms of evil, 11 spray targets create - columnar internal structure (Figure 3Α), nitrogen spray The target causes - the internal structure of the parties (Fig. 3Β), and the construction of the target 34 200902741 into a relatively unpatterned internal structure (Fig. 3C). Table 1. Characteristics of several splash films Film characteristics Film number Process thickness ( Nano) Average thickness (nano) Uneven film thickness Rs (European marriage sq) Resistivity coefficient (Omtical) Microstructure surface morphology 106 CSHe 230,168,197 198 1.50% 8.642±2.4°/〇1.71E-04 Smoothing 107 CSHe 157,170,170 166 3.40% 10.281±3.6% 1.71E-04 City smoothing 109 csn2 288^88^27 268 3.50% 8.713±3.6°/〇2.33E-04 Smoothing 110 csn2 288^04^06 233 4.00% 7.867i4.0% 1.83E -04 All parties and other large smooth 111 prototype 4.30% 8.42U4.4% 112 prototype 244 244 5.00% 7.87 & M.2% 1.92E-04 no graphic smoothing 113 prototype 15.40% 4.120*12% 114 275^48^30 251 7.40% 6.76U7.9% 1.70E-04 No graphic smoothing example 2 Tubular button target prefabrication Model Manufacturing and Microstructure Analysis The same operating parameters of Example 1 were used to make several tubular tantalum preforms (see Figure 5). Several samples were cut from the preforms and annealed at different temperatures. Several metallurgical mounts are then prepared and microstructure analysis is performed on the same sprayed and annealed samples. Table 2 shows a summary of these characteristics. All samples were from a preform using a powder having a starting mid-size of 15.9 microns (particle count distribution) and approximately 26 microns (integral distribution). Table 2. Microstructure characteristics of cold spray crucibles for the same spray and subsequent annealing. Abstract 35 200902741 Conditions also deposited annealing Celsius 942 degrees Annealing 1150 degrees Annealing 1450 degrees Celsius hot isostatic pressing (HIP) 1300 degrees Celsius powder size (4) 15.9 15.9 15.9 15.9 15.9 Particle size (m) 12 12 6.7 10.6 5.5 Particle shape Long and long, all sides, equal parties, large parties, etc., large recrystallization, whether it is crystallographically oriented random random random random list 2 and 6 shows the characteristics of the cold spray button in the same spray, annealing and hot isostatic pressing (HIP) conditions. The process temperature is shown in the figure. All annealing was maintained for a temperature of 1.5 hours, and the hot isostatic flattening (HIP) cycle was maintained for 3 hours. Starting the powder size appears to control the resulting particle size, even after high temperature annealing. Thus, in particular, the cold spray material has a particle size of less than 44 microns, and even large scale working mold materials will typically have a particle size of 60 to 100 microns, or even larger. This finer particle size is an important feature of the target to result in a more uniform film, however, in order to produce a result, it must be combined with a completely textureless microstructure. Figure 6 illustrates a flat or elongated or crystalline structure of the same spray material which recrystallizes into several large particles during annealing, has a very fine grain structure before and after annealing, and even after extensive annealing, the particle size is still equal to or less than The original powder particle size. Four cold spray samples and one plasma spray sample were examined by an electron backscatter diffractometer (EBSD) to determine the nature of the crystal texture presented. All 36 200902741 are all samples of thickness, and are all oriented for use in an electron backscatter scatterer (EBSD), so the spray direction is vertically downward. In the context of materials science, "texture" means "crystal orientation is preferred". These orientations are completely random in a sample, and the sample is said to have no texture. If the crystalline orientation is not random, but has some preferred orientation, the sample has a weak, strong, or intermediate texture. Electronic Backscattering Diffraction (EBSD) The orientation information of the sample is obtained by applying a Kikuchi diffraction pattern formed when the sample tiling is about 70 degrees Celsius. The samples were mounted, polished, and etched using the step size shown in Table 3, with an electronic backscatter diffractometer (EBSD) at high resolution (2 and 4 micron step size) or lower resolution ( 50 micrometers) characterizes it. The step size is chosen based on the particle size of the sample to ensure that the small features are not missed when the electronic backscatter diffraction (EBSD) scan is completed in a reasonable amount of time. Table 3 Process EBSD Stepping EBSD Area Index% CS, 1450〇c 2μπι 330μιηχ300 94 CS, 1150°C 2μπι 330μιηχ300 95 CS, 942〇C 2μπι 280μηιχ250 66 CS, No Annealing 4μηι 3 Area '330μηιχ150 71 to 73 Plasma Spray 50μιη 2.95 mm><9> 96 Results A cold spray, annealed at 1450 degrees Celsius Figure 7A shows a texture map of the relevant three orthogonal directions. Particles oriented within 20° of the {100} direction are shown in blue, 20 in the {111} direction. The inside is indicated by yellow, and is indicated by red in 20° in the {110} direction. When the orientation error 37 200902741 is reduced, the color is darkened. Gray (four) aligns the particles between the three orientations. The random distribution of colors in the graph is caused by the random distribution of the individual wheels. If the particles exhibit any particular texture, the one in the color of the material will have the advantage that if the majority of the particles are oriented in the {100} direction, yellow will be the dominant color.曰 The polar map (Fig. 7B) also shows a complete lack of symmetry, indicating that there is no texture in the microstructure. From the pattern, the sample can be considered to have a texture-free _ random texture, and the material particles are randomly oriented, have small particle sizes and have no system characteristics. Celsius 1150 疳 ' As shown in the texture map and polar map in Figure 8, the texture is random. The particle structure is finer than the sample annealed at Celsius. Celsius 942 grinding silver is small as shown in Figure 9. This sample also has a random texture. However, the indexation ratio is much lower than the previous sample, indicating that the material remains—high tension—the material is not recrystallized at lower annealing temperatures, as well as the texture map and polar map shown in Figure ( (see Figure 1 〇 And 11), it is found that the 3H texture is random, and the thickness is uniform and random. In this example, 'the following three texture maps represent three inspection areas, the first one is the first material deposited (the bottom of the spray layer), and the last one is the last material deposited (3 Heha fog layer Top): All graphs show that the texture associated with this vertical direction (through the thickness direction) is random. The result is a plasma. 38 200902741 • The substrate or support plate (the lower part of the texture map of Figures 12 to 13) has extremely large particles of equal width, which have a texture characteristic of the rolled and overannealed disk. The particles in the texture map are mainly blue and yellow, and a number of polar maps H3, which only include the lower third of the texture grain map, at {1 〇〇}//ND and .{ 11丨}//ND shows several peaks (although it is a weaker peak), where ND is perpendicular to the sample surface. The triple symmetry of these H3 pole maps is evidence of pressure. The plasma deposition material shows several columnar particles with many low angle boundaries (shown in red in the particle map). As shown in the polar map H1 (the upper half of the texture grain map) and by the blue color in the figure, the texture is mainly 疋{100}//ND. The polar map H1 is effectively axisymmetric. The origin and cause of the rougher sides of the columnar particles are unknown. Since the number of points included is extremely small, both the Η1 and H3 polar maps are 15° smooth angle half width (compared to the usual one 〇.) to avoid the introduction of unnecessary peaks. In short, the above electron backscatter diffraction (EBSD) analysis shows a completely random non-textured microstructure in the same cold spray and annealed cold spray target, regardless of the annealing temperature. The plasma spray target shows a significant texture. Example 3: TaNb Cold Spray Target A 50/50 volume percent 铌-钽 (NbTa) rectangular target was directly cold sprayed onto a copper support plate. Figure 14 shows that a 3 mm (mm) bend is produced in the copper support plate due to the same nozzle fog stress in the deposit. The support plate must be flat to seal against its mating flange. Because of these stresses, the machine is crying 39 200902741 During processing, it will only redistribute and cause continuous deformation, so the bending cannot be removed by machining. Since the same spray button, Ta-b and cold spray deposits typically have very limited plasticity (Fig. 15), the bend cannot be mechanically pressed. However, experiments have shown that plasticity can be greatly improved by annealing. Figure Μ shows that a button deposit is plastically deformed to a permanent deformation after annealing for 15 hours at 95 °C. The copper support plate was removed from the target; the target was then annealed, bent and machined (Fig. 17). It is also apparent from this example that conventional copper and IS support plate materials are not ideal for refractory metal targets by cold spray. M traditional copper and Ming support plates have high thermal conductivity, but their elastic modulus is low (promoting deformation), and a large thermal expansion coefficient ("CTE") cannot match these refractory metals (promoting deformation and annealing to increase the target and The possibility of failure of the bond between the support plates) and the low melting point (which hinders the annealing process when bonding the support plates). Table 4 shows that materials such as molybdenum, titanium or 316 stainless steel have a better combination of properties to resist bending during cold spray processes (high modulus of elasticity), or to allow for high temperature annealing (thermal expansion coefficient) required for refractory metals. CTE") is similar to these refractory metals and has a high melting point). Cold spray can be used to make a multi-layer target that overcomes the thermal expansion coefficient (CTE) mismatch and the above-mentioned problems that cause undesirable results. Spraying a splashable target material directly on the support plate, but first spraying a thin coating or a plurality of coatings having a coefficient of thermal expansion ("CTE") between the support plate and the target material between. These intermediate layers may have a thickness of 〇 25 to 2 mm. One way to spray this layer is to use a powder mixture, which includes 200902741 including the support plate material and the target material __. Target and support plate material wins, 14 , .,, ~ ' π~~~--- material heat conduction Sex '--- Partial coefficient thermal expansion coefficient melting point ------ card cm / cm 2 seconds it X10'6PSI cm / cm °c °C copper ------ --------- - —_ 0.94 -----—__ 1 17 16.5 1083 Aluminum 0.53 10 23.6 660 铌0.12 17 7.3 2468 New 0.13 27 6.5 2996 Molybdenum.34 47 4.9 2610 Titanium 0.22 16.8 8.4 1668 316 Unrecorded steel 28 14 ~1350 KNbTal The sprinkling of the Japanese standard targets the pseudo-alloy (the bismuth and bismuth powders are still chemically different) in a 18"x5" planar magnetron cathode splatter. The target setting size is 4"xl7"x approximately 0.125". Three tests were performed: straight metal deposition, oxide deposition, and nitride deposition. The conditions used and the results obtained are explained below. Straight metal deposition for splashing is used in 100 seem of argon, using a splash pressure of ι·〇x 1〇_3 Torr (basic pressure 4x 1〇_5 Torr), 5 〇 kW, 55 〇, approximate 73 watts per square foot. The target is excellently splashed from the beginning, no arc formation, no realism required for stability, burnout, time. A final film thickness of 1401 angstroms was deposited on a glass substrate (as measured by a Dektak 2A micro-section measuring instrument), which is a deposition time of the upper angstrom 41 200902741 watts squared shift - the rate is slightly higher than that used for 铌And the individual rate of the button is 3.7 ohms/square (as measured by the 4 ρί• probe on the glass plate). The result is calculated to be 51·8 〇 _ ohm centimeters. The expected resistivity of approximately 28 _ ohm centimeters. This material is sensitive to background house forces (impurities) and needs to be pumped to a low _5 to -6 Torr range for proper resistivity values. The absorption is 〇_4U as measured and calculated according to ASTM 5903 and Ε490). Oxide deposition# is performed using argon at (10)_ and oxygen at 90 sccm (lower oxygen levels cause gradual switching to metal mode), at 12 to 3 Torr, 3 〇 kW (44 watts/square) In the secondary volts. This is the _ of a few materials that have a higher erbium voltage in the oxide mode than in the metal mode. This Μ〇χ D.C. supplies an additive on the Sparc_le unit operating at 20 Hz. Once again, the - extremely stable splash process, no arc formation and no problem. The reduction rate is 40% of the ratio. This process provides a very aesthetically pleasing transparent film with a slight pink color in the reflection. The reflection has a slight green color and the final film thickness is 4282 angstroms. The refractive index is calculated to be 2·8, which is higher than the refractive index of individual lanthanum oxides (about 2.2 to 2.3). Nitride Deposition The attack is performed using a gas of 100 coffee and a gas of 2 coffee, approximately 2·0 X 1G-3 Torr. The nitride is freshly satisfactory and very stable. n A transparent nitride coating cannot be produced even after many process parameters have been tried. Using 3D kW of the MDX and Sparc_le units works well 1 shot yield is the metal ratio of m final film thickness 42 200902741 = ohms/square is ED (126G micro ohm centimeters). The daylight absorption was measured to be 0.59. Some observations are: Splatter is satisfactory in metal mode; sniper is excellent in oxide mode. The electrical isolation is not noted, which means that the oxide content in the target is stable 'and the target does not constitute a dielectric layer during deposition. Very high index oxides, which will be quantified and used for measurement of changes as a chemical function due to position and time. Excellent clear runway' No discoloration point in the runway. The entire target is deposited at a good rate. At a maximum power of 5 kW (kW) operating target, 5 kW converted to 75 watts/square 吋 a reference titanium (Ti) or nickel-chromium (Ni_Cr) is splashed at 35 watts per square foot. The target power is increased by 1 kW, and the towel is not inclined. At high power, there is no problem in terms of target expansion and overheating. Good 疋 dimensional stability, no problem at these chucks or edges. Fe Example 5. — A cold spray button on a copper support plate—Annealed and smoothed a TaNb target. A 17”xl.5”x〇.3〇〇-铌(TaNb) deposit On a 5 inch thick copper support plate. A layer of approximately 50% copper 50% (TaNb) thick was sprayed onto the copper prior to spraying the pure button (TaNb) to provide an intermediate coefficient of thermal expansion (CTE). The same spray assembly has a midpoint bend of approximately 〇·2吋. The target assembly is then vacuum annealed at 825 degrees Celsius for 1.5 hours to be sufficient to introduce recovery in the crucible and to make it ductile. Once 43 200902741 is cooled, the target assembly is placed in a flattening machine, successfully flattened to within 0.010 Torr, and machined. Example 6. Approximately 50/50 percent composition of the ^^(M〇Ti) splash target, which was produced by hot isostatic pressing (HIP) and by cold spray. The M〇Ti alloy system does not exhibit 100% solid solubility and contains several harmful brittle intermediate phases. When molybdenum (Mo) and titanium (Τι) are alloyed in a liquid state, such phases are unavoidable. The goal of developing HIP parameters is to minimize the formation of such phases. However, due to the mutual diffusion of the two elements, if the full density is to be achieved, the formation of such phases cannot be avoided. Figure 19 clearly shows that these harmful phases occur in powders that are hot isostatically pressed at 825 ° C and 15,000 ksi for 7 hours. A third phase material having a thickness of about 15 to 20 microns surrounds both titanium powder and molybdenum powder (Fig. 19), however, it shows that molybdenum and titanium do not diffuse, and that only molybdenum is present in the target produced by cold spray. The pure elemental phase of titanium. Figure 20 shows that even after annealing for 15 hours at 700 degrees Celsius, there is substantially no interdiffusion, and at this magnification, no visible harmful phase is formed. The following is a list of the following materials: Equipment Cold Air Technology (Germany) Kinetiks 3000 or Kinetiks 4000 Cold Spray Condition: Nitrogen at 600 to 900 Celsius Degrees, pressures from 2 〇 to 4 〇 MPa (MPa) 'Powder feed rate from 3 〇 to 9 〇, and spray distance from 10 to 80 mm. Preferred conditions are 8 Torr to 900 ° C and a pressure of 3 to 3.8 MPa, a power feed rate of 30 to 50 g per minute, and a spray distance of 20 to 4 mm. Powder used: 44 200902741 Tungsten (W): AMPERIT 140, 25/10 micron particle slicing, sintering; and copper (Cu): AMPERIT 190, 35/15 micron, gas atomization. Both materials are manufactured by H.C. Starck. The cold spray WCu sample was fabricated by mixing about 50 volume percent of W with 50 volume percent copper, and fed through a powder feeder of a CGS cold spray system to make a WCu composition. The substrates can be stainless steel or titanium. The combination between the composite structure and the substrate is excellent. The microstructure of W-Cu (50/50 volume percent) is shown in Figs. 21A and 21B. The table below shows that the same spray WCu has a thermal conductivity of 193 W/m-K and a coefficient of thermal expansion of 13.49 ppm/°C. Annealing at 1600 degrees Fahrenheit (871 degrees Celsius) for 2 hours and 4 hours showed a significant improvement in both thermal conductivity and coefficient of thermal expansion. Annealing is clearly demonstrated as an important step to significantly enhance thermal conductivity and to reduce thermal expansion coefficients for use in cold spray thermal management materials. Sample identification Thermal conductivity W/mK Thermal expansion coefficient ppm/C as it is 193 13.49 2 hours X 1600F 281 11.8 4 hours X 1600F 276 11.82 These thermal management products manufactured by cold spray technology have the following composition: Tungsten-copper ( WCu) compound: a molybdenum-copper (MoCu) compound having a tungsten (W) content ranging from 10% to 85%: having a molybdenum (Mo) content ranging from 10% to 85%. For thermal management applications, the main features of compounds produced by cold spray processes are: 45 200902741 (4) Copper flat microstructures, which can also be used with other metals such as silver, gold or gold. () Molybdenum or tungsten will generally maintain its particulate morphology or agglomerated particles. Eight materials such as Niobium (A1N), Carbonized Sith (Sic), etc. can also be used. The microstructure of the W-CU (50/50 volume percent) is shown in Figures 21A and B. All of the above references are hereby incorporated by reference in their entirety for all purposes for all purposes. While the present invention has been shown and described with respect to the specific embodiments of the present invention, it is understood that various modifications and arrangements of the various components can be made without departing from the spirit and scope of the basic inventive concept. The components are not limited to the specific forms shown and described herein. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1(A) illustrates several planar representations made by using a cold gas of helium; Fig. 1(B) illustrates several planes produced by cold spray using nitrogen gas. Figure 2; Figure 2 illustrates several planar group targets made by cold spray after killing; Figure 3 shows the scanning electron microscope ("SEM") photomicrograph by means of a cold spray, Nitrogen cooling « and several sputum films that are turned out by several targets prepared by rolling short money; Figure 4A shows the smashing target after the smashing in close-up, showing the variegated and irregular of the light-pressing target Figure 4B is a close-up illustration of a squirting spray target after splashing, showing a smoother, non-mosquito surface of the chilled spray target; Figure 5 illustrates a plurality of button tubular preforms in accordance with the present invention; 46 200902741 Figure 6 shows a number of identical sprayed and annealed structures taken perpendicular to the spray direction in a photomicrograph; ', Figure 7AU illustrates several fruits treated with cold spray and annealed at Celsius; ° Figure 8 illustrates several results using a cold spray and annealing at 115 degrees Celsius Figure 9 illustrates several results using a cold spray and annealing at 942 degrees Celsius; Figure 10 illustrates that the substrate has a plurality of maximal particles of equal width and the like, which have a texture unique to the stamped and overannealed sheets; A number of polar maps in accordance with the present invention are illustrated; FIG. 12 illustrates a sample of the plasma spray button having a plurality of maximal particles of equal width and the like, having a texture unique to the stamped and overannealed sheet; FIG. Figure 1 illustrates a cold spray button-tank (TaNb) target with deposits over 44 mm long, 110 mm wide and 7 mm thick. Please note that in the center of the copper support plate 3 Millimeter bending; Figure 15 illustrates the load pair deflection for the same spray button, please note that the deposit failure due to fragile cracks does not exhibit any plastic deformation; Figure 16 illustrates the skew after 弯曲 8吋 during the bending test , permanent deformation obtained in tantalum deposits; Figure 17 illustrates a target after annealing and straightening, the straight edge rule proves that the bend has been successfully removed; Figure 18 illustrates the microstructure of a molybdenum-titanium (M〇Ti) target And such harmful phases, and Isobaric flattening ("HIP") period is the interdiffusion zone produced by combining the powder; 47 200902741 Figure 19 illustrates a similar sprayed molybdenum-titanium structure produced by cold spray, which contains only elemental elements and elements钬, and the no-harm diagram of the micro-junction shows that the cold spray shouting after annealing at 700 °C and L5 hours is not comparable to the hot-press equalization ("HIP" target (Figure 19). ), substantially the formation of the sacred phase; ... Figure 21A illustrates the microstructure of tungsten-copper (w_Cu) (5 〇 / 5 〇 volume percent); Figure 21B illustrates copper (Cu) with a flat structure. [Main components Explanation of symbols] r /- k 48