TW201023986A - Object cleansing method and object cleansing system - Google Patents
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201023986 • 六、發明説明·· - 【發明所屬之技術領域】 本發明係有關以半導體基板/玻璃基板/透鏡/磁碟構 件/精密機械加工構件/模製樹脂構件等作為對象物(特別是 ^ 在表面上具有鋁配線等鋁材料之半導體基板),來處理該對 象物之預定部位或預定面的方法及該系統(例如,對象物清 洗方法及對象物清洗系統),更具體而言,有關進行部位或 面的清洗、在該部位不使用之物的去除與剝離、對象物表 ®面之研磨與加工等之方法及該系統(例如,如阻劑剝離裝 置、聚合物剝離裝置及清洗裝置之類的半導體製造裝置、 印刷基板清洗裝置、光罩清洗裝置等之處理方法)。 【先前技術】 在半導體之則處理步驟中,對i片晶圓,重複進行% 至100次的清洗。該清洗的對象,係對元件可靠度造成影 響之阻劑膜或聚合物膜等有機物或微粒等。在此清洗步踢 ❿中’般而β使用驗清洗液與酸清洗液之組合與其他硫 酸與過氧化氫混合_之藥品,此外,在用財除該殘留 Γ洗==使用大量的純水。此外 面,一▲使用電衆灰各壯班 洗係使用其他清洗裝置“㈣殘留物與雜f之清[Technical Field] The present invention relates to a semiconductor substrate/glass substrate/lens/disc member/precision machined member/molded resin member or the like (particularly ^ a method of processing a predetermined portion or a predetermined surface of the object on a semiconductor substrate having an aluminum material such as aluminum wiring on the surface, and the system (for example, an object cleaning method and an object cleaning system), and more specifically, a method of cleaning a part or a surface, removing and peeling off a substance not used in the part, polishing and processing the surface of the object surface, and the like (for example, a resist stripping device, a polymer stripping device, and a cleaning device) Processing methods such as a semiconductor manufacturing apparatus, a printed circuit board cleaning apparatus, and a mask cleaning apparatus. [Prior Art] In the processing step of the semiconductor, the cleaning of the i wafer is repeated from 100 to 100 times. The object to be cleaned is an organic substance or a fine particle such as a resist film or a polymer film which affects the reliability of the element. In this cleaning step kicking, the combination of the cleaning solution and the acid cleaning solution is mixed with other sulfuric acid and hydrogen peroxide, and in addition, the residue is washed in the waste == use a large amount of pure water . In addition, one ▲ use electric ash and each class to wash the line using other cleaning devices "(4) residue and miscellaneous f clear
多使用胺系之有機二,於去除聚合物膜方W .辟用於卜.+劑。此樂液亦可使用於阻劑的去除。 在此,使;上魂所示的習知技術 液係有以下缺點:n令麻认 尤〜云除溥膜之滎 的排水處理設備,3):了貝过’ 2)環境負荷大且必須有特別 ‘、’、了確保工作人員的安全衛生裝置必 320816 201023986 須大型化,且在所使用藥液之清洗中,為了沖洗藥液而必 須有大量的純水,4)利用1台裝置無法進行去除薄膜到清 洗之處理。 此外,若限定於不使用藥液之清洗步驟,目前有下述 之主要技術。首先,超音波清洗裝置係現在最廣泛使用之 清洗技術’除了純水之外亦可與各種清洗液組合。缺點係 因氣穴(cavitation)現象(如後述與本發明的氣穴現象之作 用機序不同)而可能有損及軟質材料、脆性材料與微細圖案 之疑慮。因此,雖提高頻率等來因應,但會產生與清洗力 之衝突。其次,喷水清洗裝置,係適用於比較大型系統的 清洗物。缺點係必須有高壓力(數Mpa至20Mpa),而不適 用於具有微細圖案之對象物。而且,刷子清洗裝置係除了 純水以外也可與各種清洗液組合。缺點係不適合於有深的 溝與孔之表面。而且,由於對象物表面與刷子直接接觸’ 故有產生灰塵與刮痕的可能性。 此外,具有僅對水蒸氣照射之清洗裝置。由此裝置亦 不使用藥液之點來看,其環境負荷非常小。但是’此裝置 有以下缺點:1)由於不利用液滴,故對如晶圓上之光阻劑 與異物之比較強力地接合之對象物效果小’ 2)由於蒸氣產 生器的壓力為唯一的參數,故無法調整對象物之最適條件。 因此,近年來,建議使用一種組合水蒸氣與液體微粒 子而進行照射之清洗裝置(如後述之專利文獻1)。在該技術 中’首先氣化之水(水蒸氣體)浸潤到阻劑膜中且到達阻劑 膜與對象物表面之界面,而弱化此界面之阻劑膜的接合 4 320816 201023986 力,以使阻劑膜從對象物表面浮起(剝離,lift off)。接著, -產生一種縣,係㈣含有伴_定切壓力的液狀水微 粒子之霧狀的水(水霧體)會物理性作用於阻劑膜而使該阻 劑膜從界面剝離。然後,在專利文獻!之段落號碼刪9, ’記載有作為該技術的基本原理而利用熱效果現象之氣穴現 象。具體而言’為-種機制,係混合常溫的純水與高^的 水蒸氣時’藉由上述熱交換而產生具有某種程度的頻率 (ΙΟΚΗζ至1MHz)之振動。然後,利用此振動,使水分子分 ❹解為氫離子與氫氧化物離子,且將上述不穩定之離子再次 回到水分子時產生之高能量轉換為機械性衝擊。 [專利文獻 1] W020061/018948 【發明内容】 (發明所欲解決之課題) 但是,使用組合專利文獻1所示之水蒸氣與水而進行 照射之清洗裝置時,會發生以下問題:第一,由於利用水 _分子的浸透之反應所需要之某種程度的時間之現象,以及 霧狀的霧直接碰撞到阻劑膜與微粒而去除膜與污垢之即時 的現象,故有對水分子的浸透時間限制處理時間之問題, 以及第二’清洗力不充分而無法充分地去除對象物的污 垢,或相反地清洗力太強而損及對象物之事態經常發生之 問題。此時’採取一些對策’例如’前者的情況,提高喷 出壓力,後者的情況降低喷出壓力。如此,以現狀而言, 僅利用流體力學的作用(碰撞力等),可進行清洗力的調 整。但是,此時,有一些疑慮,即在前者中,由於提高喷 320816 5 201023986 出壓力而使蒸氣溫度升高而無法以耐熱性低的材料作為對 象’或碰撞力太強而可能發生對對象物的損害。另一方面, 在後者中,有一個問題,係由於喷出壓力低而可避免損及 對象物之事態但對象物之清洗不夠充分。因此,本發明的 第一目的係在提供一種手段,其係水分子之浸透時間不會 受到制限而在不損及對象物之前提下確實地進行清洗。 而且’本案發明人等依其經驗發現,以水與水蒸氣之 多相流來清洗半導體基板時,形成在該半導體基板表面之 鋁很快就產生腐蝕。如此,於施行下一個處理前若銘受到 腐触時,半導體裝置便可能無法進行運作,且亦導致良率 變差之事態。因此,本發明的第二目的係在提供一種手段, 係即使在以水與水蒸氣之多相流來清洗半導體基板時,形 成在該半導體基板表面之鋁亦不易受到長期間腐蝕。 (解決課題之手段) 本案發明人係著眼於前述之與之前的作用機序完全 不同的氣穴現象,且藉由控制在對象物上之該氣穴現象的 程度,發現可有效且容易地實施適合於對象物的處理,而 完成本發明。 並且,本案發明人為了提高洗淨力,並非著眼於氣體 的壓力而是著眼於包含在多相流體之液㈣速度,而不斷 地進行精心之研究以提高該速度。於是,發現使用某特定 的喷嘴來提高液滴速度時,如前述不會導致對象物之龜裂 以及表面圖案的崩潰而可利用充分的衝擊力來去除附著在 對象物之去除姆象物,而完成本發明。 201023986 本發明(1)係一種對象物清洗方法,係包含透過喷嘴照 ^ 射藉由以混合部混合水蒸氣與水而產生之包含連續相的水 蒸氣與分散相的水滴之多相流體之步驟而清洗對象物之方 法, “ 而前述混合部係設置在前述喷嘴的上游侧,且具有内 λ 壁面的一部分開口之水導入部, 而前述喷嘴為超高速喷嘴, 前述混合部的内壁面與喷嘴的内壁面形成大致連續 ❹性的曲面, 而從前述混合部之内壁面將水混合至流動於前述混 合部内之前述水蒸氣,且從前述混合部之内壁面使水沿著 前述喷嘴之内壁面移動,並由前述喷嘴的出口喷射前述多 相流體。 本發明(2)係於前述發明(1)的方法中,前述喷嘴具有 隨著從噴嘴上游側朝向喷嘴出口而縮徑,並且,以成為最 _ 小剖面積之喉部為邊界而擴徑之末端變寬之構造。 '本發明(3)係於前述發明(1)或(2)的方法中,前述混合 部為筒狀。 本發明(4)係於前述發明(1)至(3)中任一個方法中,將 前述水滴的速度設為100至600m/s的範圍。 本發明(5)係於前述發明(1)至(4)中任一個方法中,前 述多相流體到達對象物時的溫度為50°C以上,且前述多相 流體到達對象物時之pH為7至9的範圍。 本發明(6)係於前述發明(5)的方法中,前述多相流體 7 320816 201023986 喷射出口與對象物的距離為 30mm以下。 , 本發明(7)係於前述發明(1)至(6)中任一個方法中,前 述對象物為於表面具有銘配線等銘材料的半導體基板。 本發明(8)係藉由透過喷嘴來照射包含水蒸氣與水滴 之多相流體來清洗對象物之系統,具有:供應水蒸氣之水 蒸氣供應手段(例如’減氣供應部(A));供應㈣的水之 水供應手段(例如,純水供應部(B));以及照射多相流體之 喷嘴;其特徵為: 刖述混合部(例如’混合部144)係設置在前述喷嘴的 ❹ 上游’且具有可由内壁面將水混合至流動之前述水蒸氣之 内壁面的一部分開口之水導入部(例如,144a), 而剛述喷嘴係超高速喷嘴(例如,喷嘴141), 刖述此合部的内壁面與喷嘴的内壁面係形成大致連 續性的曲面。 本發明(9)係於前述發明(8)的方法中,前述噴嘴具有 隨著從噴嘴上游侧朝向喷嘴出口而縮徑,並且,以成為最❹ 小剖面積之喉部為邊界而擴徑之末端變寬之構造。 本發明(10)係於前述發明(8)或的系統中,前述混合 部為筒狀。 ,下,就本說明書之各用語的意義加以說明。首先, 所月、夂滴」,例如係指除了來自水的水滴以外,亦包含 來^濕飽和蒸氣之微小的水滴之概念。所謂「多相流體」, 係指具有2流體與3流體等複數的流體成分之流體,例如, 可列舉出1)飽和水蒸氣與沸點以下之純水液滴,2)加熱水 8 320816 201023986 蒸氣與沸點以下之純水液滴,3)於前述1}或2)中復組合惰 -性氣體或乾淨的高壓空氣。但是,使用在不用在意對象物 的氧化與化學反應之用途時,亦可使用氧氣體與其他活性 氣體。此外,由使用鋁來防止腐蝕之觀點來看,最好是使 用屬於僅水與水蒸氣之二相流或組合上述二相流與惰性氣 體者。所謂「對象物」並沒特別限定,例如,可列舉出電 子零件、半導體基板、玻璃基板、透鏡、磁碟構件、精密 機械加工構件’模製樹脂構件。所謂「處理」係指只要為 :對象物施加者,則並沒特別限定,例如,可列舉出剝離、 π洗、加工❺所謂「水」係指於半導體裝置製造的清洗步 驟等會在忍對象物上之微小異物與金屬離子等之污染的 用途上j吏用作為純水或超純水之程度的特性之水,而於 在不在思產生在對象物上之微小異物與金屬離子等污染之 用途上,復包含層級低的自來水。所謂「系統」,係指除 了將各構成要素收納成—體之「1置」以外,只要是在各 ⑩構成要素配置在物理性離隔之位置(例如機器設備),或各 構成要素彼此間未以可傳達資訊之方式連接時,整體具備 有具有申請專利範圍所規定的功能之構成要素,即符合該 系統。所明「超南速噴嘴」,係指可將液滴加速到音速以 上之喷嘴。 在此,為了使與在對象物處理之該領域已知之其他的 作用機序之氣穴現象的差異更加明確,而參照圖式,對本 發明之液滴碰撞時的氣穴現象加以詳述。再者,在此記載 之作用機序係僅為予測。因此,本發明不受到該作用機序 9 320816 201023986 之任何限定。 首先就氣穴現象之一般性的概念說明如下。 一般而言,當液體的溫度比該壓力之飽和溫度還高 時,開始沸騰,而液體的壓力即使變為比該溫度之飽和壓 力還低,液體亦開始沸騰。亦即蒸氣泡在液體中產生。如 此並非因溫度變化,而是因減壓效果而產生沸騰之氣泡係 通常稱為氣穴現象氣泡。由於該氣泡收縮、崩潰而產生高 壓,且產生侵蝕•噪音等。此現象稱為氣穴現象。 以往於使用在清洗之超音波清洗裝置中,藉由如以下 之作用機序,產生氣穴現象(第24圖)。 1. 利用超音波產生器傳送音波到媒液中。 2. 音波係以快速週期反覆進行壓縮與減壓而通過媒 液中。 3. 在從壓縮移轉到減壓的過程中,局部性地減壓至飽 和水蒸氣壓以下。 4. 在此開始產生氣泡(常溫沸騰)之成長。 5. 此外,溶解在媒液中的不凝結氣體亦混入到增大的 成長蒸氣氣泡。 6. 氣泡持續成長。 7. 氣泡係受到之後的壓縮力而隔熱地壓縮而具有高 能量。 8. 氣泡到最後被壓破而崩潰。 9. 被壓破時,局部性地變成極大的衝擊能量,而分解 位於周圍的污垢。 10 320816 201023986 * ίο.音波通常係藉由通過媒液中的行進波以及在液面 - 反射之反射波而產生駐波。 11.此時氣六現象係沿著最大音壓體而在媒液中產生 為條紋狀。 接著,依據本發明之方法,關於產生的液滴碰撞時之 氣穴現象,就可考慮之產生機制,以過去報告之例為參考 進行說明(martin Rein,、Drop-Surface Interaction(CismThe use of an amine-based organic second is used to remove the polymer film. This liquid can also be used for the removal of the resist. Here, the conventional technical liquid system shown by Shangshen has the following disadvantages: n. The drainage treatment equipment of the 认 认 〜 云 云 云 云 云 云 云 云 , , 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 There is a special ', ', to ensure that the safety and health of the staff must be 320816 201023986 must be large, and in the cleaning of the used liquid, in order to rinse the liquid must have a large amount of pure water, 4) can not use one device The process of removing the film to the cleaning is performed. Further, if it is limited to the washing step in which the chemical liquid is not used, the following main techniques are currently available. First, ultrasonic cleaning devices are now the most widely used cleaning technology. In addition to pure water, they can be combined with various cleaning solutions. Disadvantages are due to the cavitation phenomenon (which is different from the cavitation phenomenon described later in the present invention), which may damage the soft material, the brittle material, and the fine pattern. Therefore, although the frequency is increased, etc., there is a conflict with the cleaning power. Secondly, the water spray cleaning device is suitable for cleaning large-scale systems. The disadvantage is that there must be high pressure (several Mpa to 20 MPa), but not for objects with fine patterns. Moreover, the brush cleaning device can be combined with various cleaning liquids in addition to pure water. Disadvantages are not suitable for surfaces with deep grooves and holes. Moreover, since the surface of the object is in direct contact with the brush, there is a possibility of generating dust and scratches. In addition, there is a cleaning device that illuminates only water vapor. The environmental load of the device is also very small when the device is not used. However, 'this device has the following disadvantages: 1) Since the droplets are not used, the effect of strongly bonding the object such as the photoresist on the wafer and the foreign matter is small ' 2) Since the pressure of the vapor generator is unique The parameters, so it is impossible to adjust the optimum conditions of the object. Therefore, in recent years, it has been proposed to use a cleaning device that combines water vapor with liquid fine particles (for example, Patent Document 1 to be described later). In this technique, 'the first vaporized water (water vapor) infiltrates into the resist film and reaches the interface between the resist film and the surface of the object, and weakens the bond of the resist film of the interface 4 320816 201023986, so that The resist film is lifted off from the surface of the object. Next, a county is produced, and (4) a mist-like water (water mist) containing liquid water microparticles having a constant cutting pressure physically acts on the resist film to peel the resist film from the interface. Then, in the patent literature! The paragraph number is deleted as 9, and the cavitation phenomenon using the thermal effect phenomenon as a basic principle of the technique is described. Specifically, it is a mechanism that generates a vibration having a certain frequency (ΙΟΚΗζ to 1 MHz) by mixing the above-mentioned heat exchange with pure water of normal temperature and high water vapor. Then, by using this vibration, the water molecules are decomposed into hydrogen ions and hydroxide ions, and the high energy generated when the unstable ions are returned to the water molecules again is converted into a mechanical impact. [Patent Document 1] W020061/018948 [Problem to be Solved by the Invention] However, when a cleaning device that combines water vapor and water shown in Patent Document 1 is used, the following problems occur: First, Water molecules are soaked by the phenomenon of a certain amount of time required for the water-molecular impregnation reaction, and the fog-like mist directly collides with the resist film and the particles to remove the film and the dirt. The problem of the time limit processing time, and the second 'cleaning force is insufficient enough to sufficiently remove the dirt of the object, or conversely, the cleaning power is too strong to damage the object. At this time, 'take some measures', for example, the former is used to increase the discharge pressure, and the latter is to lower the discharge pressure. Thus, in the current state, the cleaning force can be adjusted only by the action of fluid mechanics (collision force, etc.). However, at this time, there is some doubt that in the former, the vapor temperature rises due to the increase of the pressure of the spray 320816 5 201023986, and the material with low heat resistance cannot be used as the object 'or the collision force is too strong and the object may occur. Damage. On the other hand, in the latter, there is a problem in that the ejection pressure is low and the situation of the object is prevented from being damaged, but the cleaning of the object is insufficient. Accordingly, a first object of the present invention is to provide a means for ensuring that the permeation time of water molecules is not restricted and that the cleaning is carried out before the object is not damaged. Further, the inventors of the present invention have found from their experience that when a semiconductor substrate is cleaned by a multiphase flow of water and water vapor, aluminum formed on the surface of the semiconductor substrate is quickly corroded. As a result, the semiconductor device may not operate when it is subjected to corrosion before the next process, and it also causes a situation in which the yield is deteriorated. Accordingly, a second object of the present invention is to provide a means for forming aluminum on the surface of the semiconductor substrate to be less susceptible to long-term corrosion even when the semiconductor substrate is cleaned by multiphase flow of water and water vapor. (Means for Solving the Problem) The inventors of the present invention focused on the aforementioned cavitation phenomenon completely different from the previous action sequence, and found that the degree of the cavitation phenomenon on the object can be effectively and easily implemented. The present invention has been completed in accordance with the treatment of an object. Further, in order to improve the detergency, the inventors of the present invention did not pay attention to the pressure of the gas but focused on the velocity of the liquid (four) contained in the multiphase fluid, and continually conducted careful research to increase the speed. Therefore, it has been found that when a specific nozzle is used to increase the droplet velocity, the above-described object can be removed without causing cracking of the object and collapse of the surface pattern, and sufficient impact force can be used to remove the removed object attached to the object. The present invention has been completed. 201023986 The present invention (1) is a method for cleaning an object, comprising the step of irradiating a multiphase fluid containing water droplets of a continuous phase and water droplets of a dispersed phase which are produced by mixing water vapor and water with a mixing portion through a nozzle. In the method of cleaning the object, the mixing unit is provided on the upstream side of the nozzle, and has a water introduction portion that is partially open in the inner λ wall surface, and the nozzle is an ultrahigh-speed nozzle, and the inner wall surface of the mixing portion and the nozzle The inner wall surface forms a substantially continuous curved surface, and water is mixed from the inner wall surface of the mixing portion to the water vapor flowing in the mixing portion, and water is caused to flow along the inner wall surface of the nozzle from the inner wall surface of the mixing portion In the method of the invention (1), the nozzle has a diameter reduction from the upstream side of the nozzle toward the nozzle outlet, and The structure in which the throat of the small cross-sectional area is a boundary and the end of the diameter is widened. The invention (3) is the method of the invention (1) or (2), the aforementioned In the method of any one of the inventions (1) to (3), the speed of the water droplets is in the range of 100 to 600 m/s. The invention (5) is based on In any one of the above inventions (1) to (4), the temperature at which the multiphase fluid reaches the object is 50 ° C or higher, and the pH of the multiphase fluid reaching the object is in the range of 7 to 9. The invention (6) is the method of the invention (5), wherein the distance between the ejection outlet of the multiphase fluid 7 320816 201023986 and the object is 30 mm or less. The invention (7) is based on the aforementioned inventions (1) to (6) In any one of the methods, the object is a semiconductor substrate having a material such as a wiring on the surface. The invention (8) is a system for cleaning an object by irradiating a multiphase fluid containing water vapor and water droplets through a nozzle. And a water vapor supply means for supplying water vapor (for example, 'reduction gas supply part (A)); a water supply means for supplying water (for example, a pure water supply part (B)); and a nozzle for irradiating the multiphase fluid; The feature is: a description mixing unit (for example, 'mixing unit 144) is provided in the foregoing a nozzle upstream of the nozzle and having a water introduction portion (for example, 144a) that can mix water to the inner wall surface of the water vapor flowing from the inner wall surface, and the nozzle system is a super high speed nozzle (for example, the nozzle 141). According to a seventh aspect of the invention, in the method of the invention (8), the nozzle has a nozzle that faces from the upstream side of the nozzle toward the nozzle outlet. In the system of the invention (8) or the system of the invention (8), the mixing portion is cylindrical, and the end portion of the invention is (8). Next, the meaning of each term in this manual is explained. First, the month, the drop, for example, refers to the concept of tiny droplets of water that are saturated with vapor, in addition to water droplets from water. The "multi-phase fluid" refers to a fluid having a plurality of fluid components such as two fluids and three fluids, and examples thereof include 1) saturated water vapor and pure water droplets having a boiling point or less, and 2) heating water 8 320816 201023986 vapor With pure water droplets below the boiling point, 3) complex inert gas or clean high pressure air in the above 1} or 2). However, oxygen gas and other reactive gases can also be used when it is used without ignoring the oxidation and chemical reaction of the object. Further, from the viewpoint of using aluminum to prevent corrosion, it is preferable to use a two-phase flow which is only water and water vapor or a combination of the above two-phase flow and an inert gas. The "object" is not particularly limited, and examples thereof include an electronic component, a semiconductor substrate, a glass substrate, a lens, a disk member, and a precision machined member' molded resin member. The term "treatment" is not particularly limited as long as it is applied to the object, and examples thereof include peeling, π washing, and processing. The term "water" refers to a cleaning step in the manufacture of a semiconductor device. In the use of a small foreign matter or a metal ion or the like, the water is used as a characteristic of pure water or ultrapure water, and the foreign matter and metal ions which are generated on the object are not contaminated. In use, it includes a layer of tap water with a low level. The term "system" refers to a position (for example, a device) in which each of the 10 constituent elements is physically separated from each other except for the "1" setting in which each component is stored as a body, or between the components. When connected in such a way as to convey information, the overall constituent elements having the functions specified in the scope of the patent application are in compliance with the system. The term "super south speed nozzle" means a nozzle that accelerates a droplet above the speed of sound. Here, in order to clarify the difference between the cavitation phenomenon of the other action sequence known in the field of object processing, the cavitation phenomenon at the time of collision of the droplet of the present invention will be described in detail with reference to the drawings. Furthermore, the operational sequence described herein is only predictive. Therefore, the present invention is not limited by this action sequence 9 320816 201023986. First, the general concept of cavitation is explained below. In general, when the temperature of the liquid is higher than the saturation temperature of the pressure, boiling starts, and even if the pressure of the liquid becomes lower than the saturation pressure of the temperature, the liquid starts to boil. That is, vapor bubbles are generated in the liquid. Therefore, it is not a bubble that is caused by a change in temperature but is caused by a decompression effect. It is usually called a cavitation bubble. High pressure is generated due to shrinkage and collapse of the bubble, and erosion, noise, and the like are generated. This phenomenon is called cavitation. Conventionally, in the ultrasonic cleaning device used for cleaning, cavitation is generated by the following action sequence (Fig. 24). 1. Use the ultrasonic generator to transmit sound waves into the medium. 2. The sound wave is compressed and decompressed in a fast cycle and passed through the medium. 3. During the transfer from compression to decompression, local pressure is reduced to below the saturated water vapor pressure. 4. At this point, the growth of bubbles (normal temperature boiling) begins to occur. 5. In addition, non-condensable gases dissolved in the vehicle are also mixed into the enlarged growth vapor bubbles. 6. Bubbles continue to grow. 7. The bubble is compressed in a heat-insulated manner by the subsequent compressive force and has high energy. 8. The bubble collapses and collapses at the end. 9. When crushed, it becomes a localized impact energy and decomposes the dirt around it. 10 320816 201023986 * ίο. Sound waves usually generate standing waves by passing the traveling waves in the medium and the reflected waves reflected at the liquid level. 11. At this time, the gas six phenomenon is streaked in the vehicle liquid along the maximum sound pressure body. Then, according to the method of the present invention, the mechanism for generating cavitation in the collision of the generated droplets can be considered, and the example of the past report is used as a reference (martin Rein, Drop-Surface Interaction (Cism).
Internation Centre For Mechanical Sciences Courses andInternation Centre For Mechanical Sciences Courses and
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Lectures) pp.39-102, Martin Eein ed., Springer-Verlag, 2002,) ° 1. 當液滴以某種速度碰撞固體邊界界面時,液滴的運 動能量轉換為壓力能源’在液滴與固體邊界界面之接觸面 中’產生高壓(第25圖)。 2. 產生之壓力係作為壓力波(壓縮波)將液滴内部傳 播到上方’而到達液滴與周圍氣體之邊界界面,亦即自由 界面(第20圖)。 3.水的音響阻抗係遠比周圍氣體的音響阻抗大而導 ’ I—力波係大致刚%反射。亦即,由於朝 壓力波的周圍氣體之傳播變得非常小故結果可將在自由 界面上之壓力變化抑制在較小程度(第π圖)。 由界面上之壓力變化變小’係由於產生抵消壓 縮波之膨脹波、亦A _ 力即產生比周圍更低的壓力波,且傳播到 液體内部之故。 5 ·傳播到液滴 内部之膨脹波係降低液滴内部的壓 11 320816 201023986 力。液滴的溫度若為30°C左右,約降低0.04氣壓,若為 60°C左右,約降低0.2氣壓,若為80°C左右,約降低0.5 氣壓,如此一來便開始沸騰,而產生氣泡且成長(第28, 29 圖)。 6. 所產生的蒸氣泡一邊成長一邊亦導入液體中之不 凝結氣體,而變得更大。 7. 充分成長之氣泡達到成長極限,便開始反彈亦即收 縮。由於收縮過程比起膨脹過程急劇產生,故氣泡急劇收 縮,且氣泡内部壓力比開始成長時的壓力高而可達到極高 的壓力。此高壓力係稱為氣泡崩潰時壓力。 8. 氣泡崩潰亦因受到氣泡周圍條件的擾亂而誘發。此 外,氣泡並非一定單獨崩潰,而是作為氣泡集積之氣泡群 而崩潰。根據報告,此時之氣泡崩潰壓力為單一氣泡崩潰 壓力之數百倍程度以上。 9. 在液滴内部產生之氣泡崩潰壓力,係作為壓力波 (壓縮波)傳播於液滴内部,而到達液滴與固體面之接觸 面,使於固體面上產生非常大的壓力。此係液滴碰撞時產 生的氣穴現象之崩潰壓力,利用此壓力進行清洗。 在本發明中本質上重要的是,藉由水蒸氣,而將液滴 周圍之熱環境保持在充分的高溫,或防止液滴引起之熱的 外漏。因此,液滴内部之膨脹波所引起之壓力下降即使不 顯著,亦為可產生充分的氣泡之條件。因有此特性,故如 其他發明,即使液滴具有快速的速度而不會與固體表面碰 撞,只要為可產生某些程度的壓縮波之速度便足夠。 12 320816 201023986 發明比較時,藉由具有以2位數程度 -速度之液滴’來產生氣穴現象之點乃本發明最特 (發明的功效) 々 依據本發明,與藉㈣出壓力的赌(流體力學的作 .用)來控制對於對象物的衝擊力之習知的方法不同,而係構 成為湘因液滴碰撞對象物表面而產生的液滴碰撞時之氣 穴現象來處理對象物,故可得到解決下列的疑虞與問題之 ❹效果,該問題係起因於喷出壓力的高低之習知的問題,具 體而言為’碰撞力變得太強有產生造成對象物的損害之疑 慮,以及由於低的喷出壓力故傷及對象物之事態雖可避免 但對象物的清洗不充分之問題。並且,碰撞時之液滴的溫 度與此液滴碰撞時之氣穴現象有很大的相關,故藉由變更 Μ的溫度可容易控制該氣穴現㈣程度(發生的有無與 程度)。此外’在低喷出壓力下,只要提高液滴溫度便可有 ❷效地執行對象物的處理,故可避免起因於高喷出壓力之問 題。並且,氣體為水蒸氣時,即使招致由該水蒸氣熱移動 到其他媒體之事態時,從水蒸氣之潛熱所利用的結果,可 避免整個系統整體的溫度降低之事態。 本發明之更具體的作用•效果如以下述。(i)以因液滴 碰撞後產生之高速侧喷流與氣泡崩潰所引起之衝擊波、以 及以因衝擊波產生之連鎖反應的衝擊力(氣穴現象)而產生 成為膜剝離的起因之膜上的龜裂與孔。(2)產生因液滴所致 之喷流與衝擊波’及因衝擊波所致之連鎖反應以及高速侧 13 320816 201023986 喷流,以(1)所述之龜裂與孔為起點捲起膜而使之剝離。(3) 利用具有大的熱溫度能量之水的蒸氣使對象物材料脆化, ' 或產生應力來弱化對象物與基底之界面的密接力。(4)按照 對象物,使上述功能的組合變化,藉此亦可擴展清洗對象 與去除對象。(5)不僅去除雜質,亦可將本發明應用於蝕刻 〜 步驟與離子植入步驟後之不使用的光阻劑的去除與蝕刻步 · 驟後之不使用的聚合物之去除的用途。 此外,依據本發明(1)至(4)及(8)至(10),藉由使用超 高速喷嘴,使水滴的速度變快。因此,將液滴細分化而使 〇 液滴直徑變小。因此,不易產生具有成為晶圓之龜裂與圖 案之崩潰的原因之大的直徑之液滴,而即使提高壓力該問 題亦不易產生。 並且,使用超高速喷嘴時,在喷射水蒸氣與水滴之多 相流體,以及空氣與水滴之多相流體中,觀測到表示下列 二點之特異的動作。 第一,可清楚得知藉由使用超高速喷嘴來喷射水蒸氣 q 與水之多相流體,於喷嘴内之出口附近觀測到如壓力波之 類的物體(第30例)。據此,得到以下之效果:在喷嘴内液 滴更細分化而使液滴直徑變小,故即使升高壓力,亦不會 引起晶圓的龜裂與表面圖案的崩潰之問題。 第二,氣體壓力與液滴速度及/或平均粒徑之關係。在 提高氣體壓力時,在空氣與水之多相流體中,隨著壓力升 高液滴速度亦變高,相反地在水蒸氣與水的情況時,係可 進行測量到預定之壓力為止,但超過預定壓力時則無法進 14 320816 201023986 '行測量(第28例)。再者,可得知觀察氣髏壓力與水滴之平 •均粒徑的關係時,在空氣與水之多相流體中’該粒徑並非 取決於氣體壓力,而在水蒸氣與水的情況時’係當超過預 定壓力時平均粒徑的資料即成為無訏信度者(第29例)。此 係指有一種區域的壓力,其在·空氣與水之2多相流體中為 可進行測量’而在水蒸氣與水之2多相流體中為不可測 量。亦即,係指在該壓力下,水蒸氟與水之多相流體,係 與空氣與水之多相流體至少表示一沙不同的動作。關於該 =作之差異點並不明確,而至於無^測量之主要原因,可 能為液滴速度太快或液濟直徑太 ^ 藉由在噴嘴上游侧,從前述現舍部之壁面將水混合至 則逑水蒸氣,於壁面形成水膜而從噴嘴出口喷出,且喷出 水滴與水蒸氣之多相流體。喷出之浪滴孫藉由碰撞對象物 表面,並藉由前述之作用機序而在浪滴内局部性地產生低 % ^部’而可在對象物表面產生氣穴現象。 此^卜,由於具有末端變寬之構造,亦即使用於照射之 為,隨者從喷嘴上游側朝向噴嘴出口而縮徑,並且,以成 混、剖面積之喉部為邊界而擴徑之構造,故藉由在前述 噴繁所犯合之水使水膜形成於噴嘴内壁’且水蒸氣通過 1的中心部分而噴出。此蛑.^ ^ ^ 口之間‘并口 時,水蒸軋係於喉部到喷嘴出 水如迷。 幻該加速之水蒸氣牵引之方式使 上越,’依f本發可達到町之效果:除了择由 '穴現象所得到之充分的衝擊之外,《水與: 320816 15 201023986 之多相流來清洗半導體基板時,形成在該… 之銘長期間不易腐#。例如,可得到以5、導體基板表面 蝕刻後,若利用本發明(5)之方法,來/效果:於鋁之乾 劑,則到下個步驟為止之時間銘配線不,]離對象物上的阻 依據本發明(6),可達到以下之欵果腐蚀。 出口與對象物之距離短,故多相流戢不办因夕相流體噴射 二氧化碳而使pH不容易偏向酸性,、易導入大氣中之 鋁腐蝕的效果。 可更有效發揮防止 【實施方式】 :態畢竟僅為最佳的例示,完全C技= 以下’作為最佳形態,而採用Γ晶 作為對象物處理裝置,來具體說明本發明凊洗裝置」為例 減:最佳形態之2多相流體’係包含藉由混合水 蒸乳與水而產生之連續相的水蒸氣與分散相的水滴。在 此’ 「水滴」係由適當地處理由忌諱化學藥品的材料所構 成之對象物的純水所構成(此外,溼度高的水蒸氣之一部 分)。此外,前述的多相流體亦可任意地包含氬、氮等之惰 性氣體、乾淨的高壓空氣。但是,從防止鋁的腐蝕之觀點 來看,任意氣體最好是氬或惰性氣體。 ” 在此,使用水蒸氣的理由,除了比熱高之外,係可利 用潛'、、、且即使在伴隨流體的壓力之變化液滴所具有的熱 量被奪走之狀況下’溫度幾乎*會降低之點來看為有利之 320816 16 201023986 *故。水滴與氣體在流體混合部混合時,於水滴與氣體之間 產生熱移動’或與水滴及混合部以及配管等的内壁之間產 生熱移動。此外,由於利甩喷嘴部加速而放出到大氣時產 生減壓膨脹,故氣體的溫度會下降。此時,水滴的溫度是 否降低’係由氣體的潛熱所決定。未含有多的潛熱之氣體, 例如,將惰性氣體或乾淨的高壓空氣與純水混合時,氣體 的溫度會降低而難以控制溫度。另一方面,氣體為水蒸氣 時’由於具有預定量的潛熱,故與比較低溫的水滴混合時, 内壁奪走熱時’亦可利用熱的移動使氣想的溫 度不-易降低’而有可容易控制溫度之傾曰水落 乳的潛熱若不充分,而隨著一部分的 一疋水?、、、 滴,茈# I A zL Μ各 蒸氣液化產生液 育此便會對產生於處理對象物表面之衡擊 再者,此多相流體最後在喷嘴之喉部加逮〜 度雖會降低,但利用水蒸氣所具 虿之潛熱’可減低流體的溫度。 ❹ 處理裝置之磬艚缉法 第1圖係本發明的一實施形態之對象物處理裝置1〇〇 的整體圖。本裝置100的構成係具有··水蒸氣供應部(A); 純水供應部(B);水蒸氣流體調整部(C);多相流體照射部 (D) ’以及晶圓保持•旋轉•上下機構部(E)。以下,對各 部加以詳述。 (A)水蒸氣供應部 水蒸 應官1.11 ; 氣供應部(A)的構成包含:用以供應純水之水供 加溫到預定溫度DirC)以上而產生水蒸氣,並 320816 17 201023986 控制水蒸氣的產生量且對水蒸氣進行加壓到預定値Cl(MP) * 之蒸氣產生器112 ;掌管蒸氣的供應及該停止之可開關的 -水蒸氣開關閥113 ;用以測量從蒸氣產生器112供應到下 游的水蒸氣的壓力之壓力計114;用以調整蒸氣供應壓力 到所希望的値之水蒸氣壓力調整閥115;調整供應水蒸氣 〜 内的微小液滴量之附有溫度控制機構之加熱蒸氣產生器兼 · 飽和蒸氣濕度調整器116;以及作為安全裝置之释壓閥 117。 (B) 純水供應部 〇 純水供應部(B)的構成包含:用以供應純水之水供應 管121;用以使純水具有熱能量之附有純水溫度控制機構 的加熱部122;掌管純水供應的停止及重新供應之純水開 關閥123 ;用以確認純水的流量之純水流量計124 ;以及為 2流體時掌管對下游之純水的停止供應及重新供應之2流 體產生用純水開關閥125。 (C) 水蒸氣流體調整部 〇 水蒸氣流體調整部(C)係具有用以調整水蒸氣流體的 溫度與飽和水蒸氣的濕度之附有水蒸氣流體溫度控制機構 的加熱部131 〇 (D) 多相流體照射部 多相流體照射部(D)係具備:用以對對象物照射多相 流體之可移動於前後左右方向(第1圖之X軸喷嘴掃描範 圍或Y轴喷嘴掃描範圍)的照射喷嘴141;用以順暢地進行 喷嘴的移動之彈性配管142;用以測量多相流體之喷嘴正 18 320816 201023986 * 前的壓力之壓力計143 ;以相對於蒸氣配管而在壁面形成 - 水膜之方式導入純水之氣液混合部144 ;以及用以順暢地 導入純水到氣體配管内之孔口 145。在此,噴嘴141係超 高速喷嘴。所謂「高速喷嘴」,若為可對液滴加速到音速 " 以上之喷嘴,則無特別限定,例如,可列舉出音速喷嘴。 • 第30圖係本最佳形態之音速喷嘴及混合部的剖面圖。音速 喷嘴的形狀無特別限定,而具有末端變寬喷嘴構造,其係 喷嘴的内部,隨著由圖式上方的喷嘴上游侧朝向位於圖式 G 下方之喷嘴出口急速縮徑,並且,以成為最小剖面積a3 之位置(喉部)為邊界,且以流體不從内壁剝離之方式比較 和緩地擴徑,並在喷嘴出口剖面積成為a2。喉部之剖面積 A3係以音速除流量來算出。喉部之剖面積A3沒特別限定, 例如,為3.0至20.0mm2。此外,擴張率(A3/A2)係利用以 下列的數學式1表示之式子所算出。 [數學式1]Lectures) pp.39-102, Martin Eein ed., Springer-Verlag, 2002,) ° 1. When a droplet collides with a solid boundary interface at a certain velocity, the kinetic energy of the droplet is converted to a pressure energy 'in the droplet High pressure is generated in the contact surface of the solid boundary interface (Fig. 25). 2. The generated pressure acts as a pressure wave (compressed wave) that propagates the inside of the droplet to the upper side and reaches the boundary interface between the droplet and the surrounding gas, that is, the free interface (Fig. 20). 3. The acoustic impedance of water is much larger than the acoustic impedance of the surrounding gas, and the I-force wave system is approximately as far as % reflection. That is, since the propagation of the gas around the pressure wave becomes very small, the pressure change at the free interface can be suppressed to a small extent (Fig. π). Since the pressure change on the interface becomes smaller, the expansion wave which cancels the compression wave is generated, and the A _ force generates a lower pressure wave than the surroundings, and propagates to the inside of the liquid. 5 · Propagation into the droplets The internal expansion of the wave system reduces the pressure inside the droplets. 11 320816 201023986 Force. When the temperature of the droplet is about 30 ° C, it is reduced by about 0.04 atmosphere. If it is about 60 ° C, it is reduced by about 0.2 atmosphere. If it is about 80 ° C, it is lowered by about 0.5 atmosphere, so that boiling starts and bubbles are generated. And grow up (Figures 28, 29). 6. The generated vapor bubbles are also introduced into the liquid and become larger than the non-condensable gas in the liquid. 7. When the bubble of full growth reaches the limit of growth, it begins to rebound and shrinks. Since the shrinkage process is sharply generated compared to the expansion process, the bubble is rapidly contracted, and the internal pressure of the bubble is higher than the pressure at the start of growth, and an extremely high pressure can be achieved. This high pressure is called pressure when the bubble collapses. 8. Bubble collapse is also induced by disturbances in the surrounding conditions of the bubble. In addition, the bubbles do not necessarily collapse alone, but collapse as a group of bubbles that accumulate bubbles. According to the report, the bubble collapse pressure at this time is more than a hundred times the pressure of a single bubble collapse. 9. The bubble collapse pressure generated inside the droplet propagates as a pressure wave (compression wave) inside the droplet and reaches the contact surface between the droplet and the solid surface, causing a very large pressure on the solid surface. This is the collapse pressure of the cavitation phenomenon that occurs when the droplet collides, and is cleaned by this pressure. It is essential in the present invention to maintain the thermal environment around the droplets at a sufficiently high temperature by water vapor or to prevent the leakage of heat caused by the droplets. Therefore, even if the pressure drop caused by the expansion wave inside the droplet is not significant, it is a condition that a sufficient bubble can be generated. Because of this characteristic, as in other inventions, even if the droplets have a rapid velocity without colliding with the solid surface, it is sufficient as long as a certain degree of compression wave can be generated. 12 320816 201023986 In the comparison of inventions, the point of generating cavitation by the droplets with a 2-digit degree-speed is the most special (the effect of the invention) 々 according to the invention, and the gambling of the (four) pressure (The method of fluid mechanics is used to control the impact force on the object, and the method is to treat the object by the cavitation phenomenon when the droplet collides with the surface of the object. Therefore, the following problems can be solved by solving the following problems and problems, which are conventional problems due to the level of the discharge pressure, specifically, the fact that the collision force becomes too strong and causes damage to the object. Suspicion and the problem that the object is damaged due to the low discharge pressure, but the cleaning of the object is insufficient. Moreover, the temperature of the droplet at the time of collision is highly correlated with the cavitation phenomenon at the time of collision of the droplet, so that the degree of the gas pocket (the presence or absence and degree of occurrence) can be easily controlled by changing the temperature of the helium. Further, under the low discharge pressure, the treatment of the object can be performed efficiently by increasing the temperature of the droplet, so that the problem caused by the high discharge pressure can be avoided. Further, when the gas is water vapor, even if the heat of the water vapor is transferred to another medium, the temperature of the entire system can be prevented from being lowered as a result of the latent heat of the water vapor. More specific effects and effects of the present invention are as follows. (i) a shock wave caused by a high-speed side jet and a bubble collapse caused by a collision of a droplet, and an impact force (cavitation phenomenon) caused by a chain reaction by a shock wave, which is caused by a film peeling cause Cracks and holes. (2) Producing a jet-and-shock wave due to droplets and a chain reaction due to shock waves and a jet on the high-speed side 13 320816 201023986, and rolling up the film with the crack and hole as described in (1) Stripping. (3) The object material is embrittled by the vapor of water having a large heat temperature energy, or stress is generated to weaken the adhesion of the interface between the object and the substrate. (4) The combination of the above functions can be changed in accordance with the object, whereby the cleaning object and the removal object can be expanded. (5) The present invention can be applied not only to the removal of impurities but also to the removal of the photoresist which is not used after the etching-step and ion implantation steps, and the use of the polymer which is not used after the etching step. Further, according to the inventions (1) to (4) and (8) to (10), the speed of water droplets is made faster by using an ultrahigh speed nozzle. Therefore, the droplets are subdivided to make the droplet diameter smaller. Therefore, it is difficult to produce droplets having a diameter which is a cause of cracking of the wafer and collapse of the pattern, and the problem is not easily generated even if the pressure is increased. Further, when an ultrahigh-speed nozzle is used, an action indicating the following two points is observed in the multiphase fluid which ejects water vapor and water droplets, and the multiphase fluid of air and water droplets. First, it is clear that an object such as a pressure wave is observed near the outlet in the nozzle by using an ultra-high-speed nozzle to eject a multiphase fluid of water vapor q and water (the 30th example). According to this, the effect is obtained in that the droplets are more subdivided in the nozzle and the droplet diameter is made smaller, so that even if the pressure is raised, the problem of cracking of the wafer and collapse of the surface pattern is not caused. Second, the relationship between gas pressure and droplet velocity and/or average particle size. When the gas pressure is increased, in the multiphase fluid of air and water, the droplet velocity becomes higher as the pressure increases, and conversely, in the case of water vapor and water, the measurement can be performed until the predetermined pressure is reached, but When the predetermined pressure is exceeded, it is not possible to enter 14 320816 201023986 'line measurement (28th case). Furthermore, it can be known that when observing the relationship between the gas pressure and the average particle size of the water droplets, in the multiphase fluid of air and water, the particle diameter does not depend on the gas pressure, but in the case of water vapor and water. 'The data of the average particle size when the pressure exceeds the predetermined pressure becomes the unbelief (the 29th case). This refers to the pressure of a zone that is measurable in the multiphase fluid of air and water and not unmeasurable in the multiphase fluid of water vapour and water. That is, under this pressure, the multiphase fluid of water and fluorine is distilled, and the multiphase fluid of air and water represents at least a different action of sand. The difference between the = is not clear, and as for the main reason for the measurement, it may be that the droplet velocity is too fast or the liquid crystal diameter is too large. By mixing the water from the wall surface of the present housing portion on the upstream side of the nozzle As a result, the water vapor forms a water film on the wall surface and is ejected from the nozzle outlet, and a multiphase fluid of water droplets and water vapor is ejected. The ejected wave drowner can generate cavitation on the surface of the object by colliding with the surface of the object and locally generating a low % portion in the wave droplet by the aforementioned action sequence. Since the structure has a widened end, even if it is used for irradiation, the diameter is reduced from the upstream side of the nozzle toward the nozzle outlet, and the diameter is expanded by the throat of the mixed and sectional area. According to the structure, the water film is formed on the inner wall of the nozzle by the water which is caused by the spray, and the water vapor is ejected through the central portion of the nozzle 1 .蛑.^ ^ ^ Between the mouths ‘and the mouth, the water is steamed in the throat to the nozzle water. The way of accelerating the steaming of the steam makes it better, and the effect of the town can be achieved. In addition to the full impact of the 'cavity phenomenon, the water and the multi-phase flow of 320816 15 201023986 come. When the semiconductor substrate is cleaned, it is formed during the length of the ... For example, after the surface of the conductor substrate is etched by 5, the method of (5) of the present invention is used, and the effect is: in the case of the aluminum dry agent, the wiring is not in the next step, and the object is not removed from the object. According to the invention (6), the following corrosion can be achieved. Since the distance between the outlet and the object is short, the multiphase flow does not cause the effect of the corrosion of the aluminum in the atmosphere because the carbon dioxide is injected into the fluid, so that the pH is not easily biased toward acidity. It can be more effectively prevented. [Embodiment]: The state is only an optimum example, and the following is the best mode. The following is the best mode, and the use of twins as the object processing device to specifically describe the washing device of the present invention is Example: The best form of the 2 multiphase fluid' is a water droplet containing a continuous phase of water vapor and water produced by mixing water with water and a dispersed phase. Here, the "water droplet" is composed of pure water which is an object which is formed by appropriately processing a material which is resistant to chemicals (in addition, a part of water vapor having a high humidity). Further, the above-mentioned multiphase fluid may optionally contain inert gas such as argon or nitrogen, and clean high-pressure air. However, from the viewpoint of preventing corrosion of aluminum, any gas is preferably argon or an inert gas. Here, the reason for using water vapor is that, in addition to being higher than the heat, it is possible to use the potential, and even if the heat of the liquid droplets is taken away with the change of the pressure of the fluid, the temperature is almost * It is advantageous to reduce the point. 320816 16 201023986 *There is a heat transfer between the water droplets and the gas when the water is mixed with the gas mixing portion or between the water droplets and the mixing portion and the inner wall of the pipe or the like. In addition, since the pressure of the gas is lowered when the nozzle portion is accelerated and released to the atmosphere, the temperature of the gas is lowered. At this time, whether the temperature of the water droplet is lowered is determined by the latent heat of the gas. For example, when an inert gas or clean high-pressure air is mixed with pure water, the temperature of the gas is lowered and it is difficult to control the temperature. On the other hand, when the gas is water vapor, 'because of a predetermined amount of latent heat, it is relatively low-temperature water droplets. When mixing, when the inner wall takes away heat, 'the heat can also be used to make the temperature of the gas not easy to decrease' and the latent heat of the falling water can be easily controlled. Insufficient, and with a part of the water, 、, 滴, 茈 # IA zL Μ each vapor liquefaction liquid production will be the balance of the surface of the object to be treated, this multiphase fluid is finally in the nozzle Although the throat is increased, the degree is lowered, but the latent heat of the steam is used to reduce the temperature of the fluid. ❹ The processing method of the apparatus is shown in Fig. 1 is an object processing apparatus according to an embodiment of the present invention. The overall configuration of the device 100. The configuration of the device 100 includes a steam supply unit (A), a pure water supply unit (B), a steam fluid adjustment unit (C), and a multi-phase fluid irradiation unit (D). And the wafer holding/rotating and the upper and lower mechanism parts (E). The following sections detail each part. (A) Water vapor supply part steaming 1.11; The gas supply part (A) consists of: supply of pure water The water is heated to a predetermined temperature DirC) to generate water vapor, and 320816 17 201023986 controls the amount of water vapor generated and pressurizes the water vapor to a predetermined 値Cl(MP)* vapor generator 112; Supply and stop switchable - water vapor switch valve 113; for measurement The steam generator 112 supplies a pressure gauge 114 to the pressure of the downstream water vapor; a water vapor pressure regulating valve 115 for adjusting the steam supply pressure to the desired enthalpy; and adjusting the amount of the minute droplets in the supply water vapor~ The heating steam generator of the temperature control mechanism and the saturated vapor humidity regulator 116; and the pressure relief valve 117 as a safety device. (B) The pure water supply unit 〇 the pure water supply unit (B) comprises: for supplying pure a water supply pipe 121; a heating portion 122 with a pure water temperature control mechanism for making pure water having thermal energy; a pure water switching valve 123 for stopping and resupply the supply of pure water; for confirming pure water A pure water flow meter 124 for flow rate; and a pure water switching valve 125 for generating 2 fluids for stopping supply and resupply of pure water downstream for 2 fluids. (C) The steam fluid adjusting unit (C) has a heating unit 131 (D) with a steam fluid temperature control mechanism for adjusting the temperature of the steam fluid and the humidity of the saturated steam. The multiphase fluid irradiation unit multiphase fluid irradiation unit (D) includes a movable front and rear direction (the X-axis nozzle scanning range or the Y-axis nozzle scanning range in FIG. 1) for irradiating the multi-phase fluid to the object. Irradiation nozzle 141; elastic pipe 142 for smoothly moving the nozzle; pressure gauge 143 for measuring the pressure of the multiphase fluid nozzle before 18 320816 201023986 *; forming a water film on the wall surface with respect to the steam pipe In this manner, the gas-liquid mixing portion 144 of the pure water is introduced; and the orifice 145 for smoothly introducing the pure water into the gas pipe is introduced. Here, the nozzle 141 is an ultra high speed nozzle. The "high-speed nozzle" is not particularly limited as long as it can accelerate the droplet to the speed of sound < Above, for example, a sonic nozzle can be cited. • Figure 30 is a cross-sectional view of the sonic nozzle and mixing section of this best mode. The shape of the sonic nozzle is not particularly limited, and has an end widening nozzle structure which is formed by the nozzle opening, which is rapidly reduced in diameter from the upstream side of the nozzle above the drawing toward the nozzle outlet located below the pattern G, and is minimized. The position (throat) of the sectional area a3 is a boundary, and the diameter is relatively gently expanded so that the fluid does not peel off from the inner wall, and the cross-sectional area at the nozzle outlet becomes a2. The sectional area of the throat A3 is calculated by dividing the flow rate by the speed of sound. The sectional area A3 of the throat is not particularly limited, and is, for example, 3.0 to 20.0 mm 2 . Further, the expansion ratio (A3/A2) is calculated by the equation expressed by the following mathematical formula 1. [Math 1]
Α3 φ2 _ \jc+ if aH- A2 φ3 2 filΑ3 φ2 _ \jc+ if aH- A2 φ3 2 fil
、2/ (*-i) 2/r <1 一 (广 1) /r ftH-l NIX (r-1) Μ \/κ fc+l ——一 [卜㈤ (d)八, > J i κ— 1 L UJ (式1) 在此,K為氣體的比熱(定壓比/定容比熱),而Ρ!為喷 嘴之喉部的壓力,;P2係噴嘴出口之壓力。藉由該擴張率與 喉部之剖面積A3,求取喷嘴出口之剖面積A2。在此,噴 嘴出口之剖面積A2並沒特別限定,例如,為7.0至 28.0mm2。此外,喷嘴的長度係考慮噴嘴的材料、粗糙度、 19 320816 201023986 流速(雷諾數(Reynolds number))等之各種參數,而可設定 適當値。此外,擴徑的程度係考慮勘度、密度、流速等之 各種參數,而可設定適宜値4嘴出π的形狀並沒特別限 定’亦可為圓形。再者,混合部的内壁面與喷嘴的内壁面 係形成為大致連續性的曲面。混合部亦可作為筒狀體而接 合在喷嘴上游,或形成在喷嘴内的上游部。接合有混合部 壁面與噴魅㈣,祕合部分係、最好以―邊藉由混合部 形成水膜而一邊沿著壁面而到達之液體,亦於喷 ❹ 成水膜而流動之方式所形成,而無特·定,亦可為有配 管之接頭等,最好是據錄财核為㈣面_之程产 的障害物之程度而平滑地形成為1。此外,關於混^ H4,於後面加以詳述。 口叫 (E)晶圓保持•旋轉•上下機構部 晶圓保持·旋轉·上下機構部⑻的構成包含··可 •保持對象物(晶圓)之基座151;用以使基座m 、栽 轉馬達152;藉由使基座151移動於上下方向而可^旋 嘴141的出口與晶圓的距離之晶圓上下驅動機構⑼嘴 以供應冷卻對象物(晶圓)的冷卻水之冷卻水管154用、,用 止及重新進行冷卻水的供應之可開關的冷卻水開^停 155;用以調整冷卻水的流量之冷卻水流量調整閥w _ 及用以測量冷卻水的流量之冷卻水流量計Η?。 以 以上,概略說明了本最佳形態之對象物處理较置 體構成,接著,就多相流體照射部(1))之混合部144加r ^ 述。混合部144具有内壁面之一部分開口之水乂詳 年入部 32〇8l6 20 201023986 • 144a(第30圖),係在噴嘴上游侧,以前述水蒸氣之行進方 • 向為基準而以90度以下之角度可將水從前述混合部之壁 面混合至水蒸氣。混合部最好為圓筒形,而與混合部噴嘴 接合之剖面的内徑,最好與前述喷嘴的入口之内徑相同。 ' 在此’第2圖係將該混合部144設為附有溫度控制機 ' 構之多相流體量液混合部時.的詳細構成圖。重要的是在混 合部144中’於混合部内壁將水蒸氣之液化與水的氣化之 相互變北現象的發生減少到最少α因此,如第2圖所示, β 該混合部144最好是採取如下述之構造。 1) 為了穩定地混合’氣體及液體之各流體的方向係 在混合部具有未達90度的角度。 2) 液體流體的配管直控或裝設於配管之孔口係在_混 合部遠比氣體流體之流路的剖面積小。 3) 藉由安裝加熱器於混合部,將混合部的内壁溫度 控制成適合以下的條件。更内壁的溫度係在混合部内之壓 φ 力下不從該液體的飽和溫度偏離太大(±20%以内)。此外, 更内壁的溫度係在混合部内之壓力下不從該氣體的飽和溫 度偏離太大(±20%以内)。此外,隨著時間經過,混合部之 内壁係接近流體的飽和溫度,故於不會在意直到多相流的 狀態穩定為止的時間之用途上,而在充分實施混合部的保 溫之條件下,可去除此加熱器之加熱功能。 在利用混合液滴與氣體之多相流體處理對象物之裝 置中,於起動該裝置之時間點,流體混合部為常溫。然後, 有該部分與水蒸氣之溫度差時,在該液體混合裝置之内部 21 320816 201023986 產生溫度的不岣勻,藉此方式,因一部分的蒸氣產生相變. 化而成為水滴等,而使多相流體之送出壓力變為不穩定, 而難以穩疋地供應一定的衝擊波到處理對象物表面上故 到裝置穩定運作為止需要時間。亦即,設置加熱器到多相 流體調整部時’由起動當初可將流體混合部設定為與水蒸, 氣的溫度相同的溫度,而使之不易產生混合部内之氣液相. 變化’且裝置可對於對象處理面施加穩定的衝擊波。 1-攻現象控鼓理(氣泡崩渣相 關參數) 本最佳形態之清洗裝置,係藉由調整氣體壓力、多相 ❹ 流體内之水混合流量、氣體溫度、混合之水的溫度、喷嘴 形狀、由喷嘴出口到對象物之距離、對象物的溫度、喷嘴 與對象物間之相對性移動時間,而具有控制液滴的溫度、 液滴之流速、液滴之大小、液滴之數目、處理對象物表面 之溫度、每單位時間之多相流體照射面積之功能。上述氣 泡崩潰相關參數中,液滴的流速、溫度、液滴密度係特別 重要。藉由控制上述參數,可在處理對象物表面上,得到 ❹ 由液滴所產生之喷流與由氣泡崩潰所致之衝擊波,以及由 前述衝擊波產生之連鎖反應的衝擊力,且可在清洗等中進 行有效的處理。流速係有助於液滴碰撞時的液滴内之氣泡 的崩潰所致之衝擊波的產生,而溫度則有助於液滴内之氟 泡的產生。此外,液滴密度愈多產生衝擊波之機率愈高。 例如,液滴的數目若為零,則不會產生因液滴的碰撞所致 之衝擊波。但是,液滴之數目變得太密時,可能造成爹相 流體的速度降低與溫度降低而使衝擊波的產生機率降够。 32〇816 22 201023986 • 在此,所謂液滴密度,係表示多相流體内之單位體積•每 * 單位時間之所有液滴數,而正確測量高速移動之//級 (order)的微小液滴之測量器尚未開發,故以導入到多相流 體之純水量代用。 ^ 氣穴現象測量手段 ' 本發明之系統係具備有一測量手段,用以在某條件下 將多相流照射於對象物或測量用樣本後,而在該條件下測 量產生何種程度的氣穴現象。在此,以現在的技術,不可 ❹ 能一邊監視氣穴現象(衝擊波)的大小(氣穴現象之強度)與 密度(單位面積•每時間之發生數)而一邊進行剝離•清洗 程序。因此,在本系統中採用的手法,係在預先的實驗中 改變與氣穴現象的產生有關之參數,並進行程序處理,且 s從該結果得到之以下的資料來判斷氣穴現象的大小。 (1) 以定量的方法測量對象物或測量用樣本之物理性 變化之物理性變化測量手段 ^ •照射多相流體於金屬表面時之金屬表面的凸凹度 •照射於阻劑表面時之阻劑剝離面積及殘渣的多少 •附著在晶圓整面之異物的去除率 (2) 可感知氣穴現象之雜音的大小之音響的測量手段 •利用音響感測器感知之氣穴現象的雜音之大小 (3) 以定量的方法測量對象物或測量樣本之視覺的變 化之視覺性變化測量手段 •以高速照相機所攝影之阻劑剝離過程之影像資料 例如,多相流體溫度與照射該多相流體之金屬表面的 23 320816 201023986 凸凹度之資料係如第9圏所確認。此 各參數之相關關係,係由 .且劑剝離性能與 認。口圖之資料為其,所f積,多數資料所確 二阻_面積會體 傷,而損及本裝 =之 以==喷嘴之最大_力二::亦 產不錢_的耐高壓零件之結果且 © 地製造安全的裝置。將喑 合易且便且 μ%嘴料縣物間的距 但是,如前所述:表第:第乂2圖、第23_果。 . r d±…、表不利用以尚速碰撞的液滴產生之衝 Z、’、之权的單位而表示為沒單位之相對値。 11 ’在習知技術(例如專敎獻υ中,除了使用超 ❹ 2嘴χ外,亦_於裝置上與本最佳形態差異不 大=構成。但是’在習知技術中,於對象物之處理時完全 不著眼=所謂「衝擊波」之物理力,因此,於對象物上完 玉不進行使衝擊波產生•不產S之控制。此外,在習知技 術之條件下’「氣穴現象」係完全在前端成衫細錐狀之 ^嘴内發生’該產生之衝擊波之壽命極短而在到達對象物 鈿/肖失具體而έ,流動於喷嘴内之多相流體靠近喷嘴尖 端^時加快錢。然後’起因於該流速加快為而成為減壓 狀L之結果,液體引起氣穴現象而產生衝擊波。依據加藤 洋/σ著、稹書店出版之「氣穴現象」,液體衝擊波管内的 氮氣泡之崩潰持續時間為2至3从秒。流速4〇〇m/秒之流 24 320816 201023986 ' 體的秒鐘之移動時間僅1.2mm,而於喷嘴喉部到嗔嘴 .出口之間氣泡崩潰現象會消失。再者,即使在噴嘴出口發 生氣泡崩潰,而將對象物距離設定在1.2mm以下於橼造上 而言係有困難。另一方面,在本發明中,喷嘴係以對多相 ’ 流體進行加速或擴張照射面積的功能為中心。而且,與氟 , 穴現象的發生相關之氣泡崩潰相關參數,只要著眼於對象 物上之氣穴現象,基本上在任何處所皆可作調整,例如, 亦可在喷嘴前面之流體配管的任何處所之流體混合部進 ❹行。具體而言,只要在第1圖之α所示之箭頭符號的範園 内(由蒸氣產生'器到喷嘴出口之間)可於任何處所進行控 制。以下,將主要的氣泡崩潰相關參數加以詳述。 歧止鋁埤鈕 本最佳形態之對象物清洗方法,除了上述之衝擊力 外’亦具有防止銘腐钱之效果。在此,亦可藉由調整氣禮 溫度、混合之水的溫度、噴嘴形狀、從喷嘴出口到對象物 ❹之距離、對象物的溫度 '噴嘴與對象物間之相對性移動時 間’而可控制防止腐蝕效果。上述相關參數中,特別是, 多相流體到達對象物時之溫度,以及多相流體到達對象物 時之ρΗ特別重要。藉由控制上述參數,可在鋁表面上, 形成達成防止腐蝕效果之特殊的保護膜。以下,與主要的 氣泡崩潰相關參數一起,就有關鋁腐蝕防止之參數加以詳 述。 (1)流體之溫度 該衝擊波係主要為液滴碰撞處理對象物表面時產生 320816 25 201023986 之氣穴現象與因氣穴現象的崩潰而產生者。氣穴現象係在 水等液體的一部分產生低壓部分時產生之空洞,而有氣體 及液體的溫度愈高愈容易產生之傾向。亦即,液滴的溫度 愈高,在水滴内之氣泡愈容易發生,隨之,在處理對象物 表面上成為大的能源之衝擊波的基礎之氣泡崩潰多數發 生’例如,將該處理方法利用於阻劑膜的去除時,可去除 ’ 接合比較強的阻劑膜與異物等。另一方面,若將多相流體 與水滴的溫度設定成較低程度,隨之,在處理對象物表面 上可抑制衝擊波的產生,而可進行強度較弱的對象物之清 ❹ 洗。但是,由於對象物的耐熱性之制限等而於可設定之溫 度的高度上產生限制。此外,在溫度太高之狀態下與對象 物之距離變為長時,可能產生液滴内之氣體成分脫落而不 易產生氣泡核之事宜,而從喷嘴出口到對象物之距離為約 2至30mm之距離設為可忽略。此外,供應到喷嘴内之水 蒸氣的溫度最好是50至120它,較理想的是80至115。(:, 更佳的是90至11(TC。再者,混合到前述水蒸氣之水的溫 度最好是0至40。(: ’較理想的是10至35。(:,更佳的是20 至 3〇。(:。 在此,特別是,多相流體到達對象物時的溫度最好是 5〇ΐ以上,較理想的是80它以上,更佳的是9〇它以上。此 外,多相流體之溫度的測量,係利用實施例記載的方法來 進仃。藉由設定在該範圍,使在對象物表面上之鋁,形成 達到防止腐#效果之特殊的膜。 (2)液滴的速度 320816 26 201023986 • 由於液滴的速度愈高則液滴碰撞處理對象物表面時 • 之衝擊變為愈大,故變得容易產生内部壓力差,結果變得 容易產生氣泡崩潰而產生氣穴現象。亦即,若將液滴的速 度設定為較高程度,隨之,於處理對象物表面上產生大的 ^ 能量之衝擊波,例如,將該處理方法利用於阻劑膜的去除 • 時,可去除接合比較強的阻劑膜與異物等。另一方面,若 將液滴的速度設定為較低程度,隨之,在處理對象物表面 上可抑制衝擊波的產生,而可進行強度較弱的對象物之清 ❹洗。此外藉由提高液滴的速度,使得多相流體曝露於空氣 之時間變短,故難以導入大氣中的二氧化碳,而難偏向酸 性,故可更適當地發揮防止腐蝕的效果。液滴的速度為100 至600m/s,較理想的是200至500m/s,更佳的是250至 350m/s。藉由設定為該範圍的流體速度,可得到氣穴現象 之衝擊力。再者,設為液滴之速度與流體的速度大致一致, 而設為「流量」/「喷嘴剖面積」。此外,在此,流量係設 @ 為水蒸氣流量(m3/s),而喷嘴剖面積係設為噴嘴出口之剖 面積(m2) 〇 (3)其他參數 首先,關於噴嘴,如前述使用超高速喷嘴。藉由使用 此喷嘴使得流體的流速改變且衝擊波的大小亦改變。原則 上,使用流速大的喷嘴時變得容易得到衝擊波。再者,藉 由使用超高速噴嘴來照射包含水蒸氣與水滴之多相流體, 而以水蒸氣之壓力、與水滴的速度及直徑之關係,來觀測 特殊的動作。水蒸氣壓只要為0.05至0.25Mpa,則無特別 27 320816 201023986 限定,特別是水蒸氣壓在015MPa以上之條件下,水蒸氣 與水滴之多相流體係顯示與空氣及水滴之多相流體大有不 同之動作。接著,關於從噴嘴出口到對象物之距離,一般 的適應値為2至3〇mm之範圍(最適範圍2至1〇ηπη),最好 是5mm以下’較理想的是3mm以下,更佳的是2mm。若 縮小喷嘴的出口到晶圓之距離,則同樣地阻劑剝離性能會 提升,而具有最適距離而太接近時,則剝離性能會降低。 相反地欲抑制剝離性能、清洗性能時只要離最適距離遠即 可。再者’從喷嘴出口到對象物之距離愈近,愈難導入大 氣中的二氧化碳,而變得難以偏向酸性。 此外’欲得到特別高的衝擊力時,重要的是液滴碰撞 到對象物時,周圍由水蒸氣所覆蓋。在此,水蒸氣的流量, 係水蒸氣的質量流量最好為〇 〇83至1 〇kg/min,較理想的 疋 0.025 至 0.75kg/min,更佳的是 〇 33 至 〇 5〇kg/min。此 外’氣液混合比(液/氣)最好為〇 〇〇〇18至〇 〇1。液滴直徑 最好為2至25 。液滴直徑若變大則表面積會變小,故 導入大氣中的二氧化碳之量變少,而變得難以偏向酸性。 又,液滴直徑係使用丁81公司製造的機器,並利用PDA 〇Phase D〇ppiei· Anem〇metry :位相多普勒法),而無特別 圯載時,設為在距喷嘴出口之5mm的位置進行測量。流體 流量/噴出口剖面積最好是〇.5至32 〇 kgcm-2min-i。 為了使水在壁面形成水膜,將水混合到多相流體時, 例如,最好是將對水施加的壓力,設為利用水蒸氣的壓力 使水不逆流的程度。對水施加的壓力並無特別限定,例如, 28 320816 201023986 ' 若為導入水蒸氣壓力以上,且施加不會喷射水之程度的壓 • 力便可導入。更具體而言,水導入的壓力最好滿足下式。 (水蒸氣的壓力+ 〇.〇2MPa) < (水導入的壓力)< (水蒸氣的 壓力+ 1.0MPa) 水導入的壓力太低時,水係以脈流導入,流體的特性 變得不穩定。此外,壓力太高時,水會飛散至喷嘴直徑方 向的中心部,而難以形成一樣的水膜,而且亦會阻礙蒸氣 © 的加速。此外,以在壁面形成水膜之觀點而言,最好是不 對喷射方向加壓,更佳的是對著水蒸氣的通過方向而由垂 直方向來供應。. 多相流體到達對象物時的pH最好是7.0至9.0,更理 想的是7.0至8.0,更佳的是7.0至7.5。由於藉由設定為 該範圍的pH,而在對象物表面上的形成特殊的膜,故可 得到鋁的防止腐蝕效果。此外,pH測量方法係設為依據實 ❹施例記載的方法。 [實施例] 多相流體到達對象物時的溫度之測量方法 第31圖係進行多相流體到達對象物時的溫度測量之 裝置的概略圖。在直徑6叶、厚度0.625mm之梦晶圓W 之上利用帶TA貼合熱電偶TH(鋁鉻熱電偶 JIS C1602),且將喷嘴141的流體喷射出口與對象物的距離, 與水蒸氣壓力,以及純水流量等之諸條件設定為與對象物 處理時相同的値,並對熱電偶照射1分鐘,且將成為穩定 29 320816 201023986 狀態時之溫度設為多相流體到達對象物時之溫度。 多相,_透體到達對象物時之pH的測詈方法 第32圖係進行多相流體到達對象物時的pH之測量的 裝置之概略圖。經由配管P將喷嘴141的喷出口連接於冷 卻管C(例如,格式蛇型冷凝器(Graham condenser)),且將 凝集的水回收到容器r,並利用HSZ8802之方法來測量該 水的pH。此外’前述凝集作業係以不接觸空氣之方式進行。 第1例 在以下的條件下,在鋁表面對多相流體(作為氣體使 用蒸氣的情況與使用空氣的情況)照射10分鐘。將處理前 後之AFM(atomic force microscopy,原子力顯微鏡)照片表 示於第3圖。於第5圖表示表面粗糙度的資料。此外,在 本例中表面粗糙度’係以AFM附屬的輪廓分析之方法進 行測量。 蒸氣的壓力:〇.2Mpa 蒸氣的温度:13〇°C 純水的流量:300cc/min 純水的溫度:20°C GAP 5 mm 噴嘴掃描:固定 第2例 在與第1例相同條件之下,在鋼表面對多相流體(作 為氣體使甩蒸氣之情況與使用空氣之情況)照射1〇分鐘。 將處理前後之AFM照片表示於第4圖。於第6圖表示表 320816 30 201023986 * 面粗糙度的資料。 .·-第3例 專利文獻1所示之蒸氣清洗技術,係利用条氣的化學 反應與喷流之機械性作用來剝離阻劑,故於阻劑之剝離需 ^要以分计算的時間。本手法亦為了確認是否為相同的機 制,故進行高速視頻之視覺化。第7圖係表示,除了將噴 嘴掃描速度為io〇mm/sec以外在與第1例相同條件下’照 射多相流體,且從石英晶圓的下部觀察之1線正光阻劑剝 ®離時之經時性變化的情況。如第7圖所示’阻劑係剝離的 區域一邊漸漸擴大且一邊急快速地剝離。 ΆΛΜ. 除了將噴嘴掃描速度設為40mm/sec之點以外在與第 1例相同條件下,對著植入高濃度離子後之梦晶圓照射多 相流體,且觀察i線正光阻劑剝離之經時性變化的倩況。 將結果表示於第8圖。 ft 列至第8例 在以下的條件下,改變多相流體的氣體及溫度,且對 著鋁表面照射多相流體10分鐘。將處理前後之AFM照片 表示於第9圖。將表面粗糙度的資料表示於第1〇圖。此外’ 照射前的處理對象之鋁的表面’係Ra為34.9nm。 氣體壓力:〇.2Mpa 液體流量:300cc/min Gap : 10mm 對由低溫空氣(20°C)與低溫純水液滴(20°C )構成的多 31 320816 201023986 相流體進行照射的結果,得到Ra為30.5nlVt的表面。將表 面的AFM照片表示於第9圖(a),且將表面粗糙度的資料 表示於第10圖(a)(第5例)。接著,照射由高溫空氣 與低溫純水液滴(2〇°c)所構成之多相流體的結果,得到 為96.4nm的表面。將表面的AFM照片表米於第9圖(b) 且將表面粗糙度的資料表示於第10圖(b)(第6例)β然後, 照射由高溫空氣(13〇°C)與高温純水液滴(6〇°C)構成的多才目 流體的結果,得到Ra為86.3nm的表面。將表面的 照片表示於第9圖(c)’且將表面粗糙度的資料表示於第 圖(c)(第7例)。(c)的表面粗輪度係比(b)稍小’而挺輪的部 分之密度比(b)還大,故可看出(c)比(b)受到更多衝擊波的 影響。再者,照射由水蒸氣與低溫純水液滴(20¾)構成的 多相流體之結果’得到Ra為257nm的表面。將表面的 照片表示於第9圖(d),並將表面粗糙度的資料表示於第^ 圖(d)(第8例)。由以上的結果,隨著溫度上存衝擊波變大 尤其是’使用水蒸氣於氣體時,可清楚知道對處理對象表 面施加最大的衝擊波。 對Ra為348.8nm的A1防钱銘表面,在與第5例至第 8例相同條件下,使多相流體的氣體及溫度產生變化來加 以照射。照射由2(TC的空氣與20t的純水液滴構成之多相 机體的結果,得到Ra為3 80nm的表面。將表面之AFM昭 片表示於第11圖(a) ’且將表面粗糙度的資料表示於第U 圖(c)(第9例)。接著,照射由130〇C水蒸氣與2(η:的純水 320816 32 201023986 • 液滴構成之多相流體的結果,得到Ra為440nm的表面。 ' 將表面之AFM照片表示於第11圖(b),且將表面粗糙度的 資料表示於第11圖(d)(第10例)。 第11例 , 對Ra為8.1nm的SUS表面,在與第5例至第8例相 同條件下,使多相流體的氣體及溫度產生變化來加以照 射。照射由130°C的水蒸氣與20°C的純水液滴構成的多相 流體之結果,得到Ra為19.gnm的表面。將表面的AFM照 Ο 片表示在第12圖(a),且將表面粗糙度的資料表示於第12 圖(b)(第11例)。 第12例 對Ra為75.5nm的鈦表面,在與第5例至第8例相同 條件下,使多相流體的氣體及溫度產生變化來加以照射。 照射由130°C的水蒸氣與2(TC的純水液滴構成的多相流體 之結果,可得到Ra為98nm的表面。將表面的AFM照片 ⑩表示在第13圖(a),且將表面粗糙度的資料表示第13圖 (b)(第12例)。利用鈦,能以目視看到干涉條紋。於表面亦 有可能形成氧化皮膜。 第13例 對Ra為1.9nm的矽表面,在與第5例至第8例相同 條件下,使多相流體的氣體及溫度產生變化來加以照射。 照射由130°C的水蒸氣與20°C的純水液滴構成的多相流體 之結果,可得到Ra為7.6nm的表面。將表面的AFM照片 表示於第14圖(a),且將表面粗糙度的資料表示於第14圖 33 320816 201023986 (b)(第 13 例)。 第14例至笫25例 在第14例至第25例中,檢討於阻劑塗佈條件下之剝 離的情況是否有差異。將HMDS(六甲基二發氮焼, hexamethyldisilazane)的有無、Bake 溫度變化為 9〇°c、11〇 °C,且觀察該條件變化的影響。得到處理後之表面輪廓可 能不取決於基底處理HMDS之結果。實驗係在以下之條件 下進行。 使用樣本:I線阻劑 照射時間:以目視觀察到剝離為止 氣體壓力:〇.2Mpa 液體流量:300cc/min 喷嘴掃描:固定 Gap : 10mm 第15圖(a)至(c)係表示,在無HMDS、Bake9〇(Jc之條 件下塗佈_膜’且以上述條件照射該樣本後,以顯微鏡 觀察處理剝離邊界界面之情況,係表示第15圖⑷至⑴以 AFM觀察之情況。第15圖(a)係照射由2(Γ(:的空氣與2〇 °C的純水構成的多相流體後’以顯微鏡觀察表面的情況, 第15圖(d)係對應之AFM照片(第14例)。第15 _)係照 射由!30。(:的空氣與贼的純水構成的多相流體後,以顯 微鏡觀察表面的情況’而第15圖(e)係對應之AFM照片(第 15例)。第15圖⑷係照射由13(rc的水蒸氣與紙的純水 構成的多相流體後,以顯微鏡觀察表面的情況,第15圖⑴ 320816 34 201023986 * 係對應之AFM照片(第16例)。 在無 HMDS,BakellCTC 之條 件下塗佈阻劑膜,並以上述條件照射該樣本後,以顯微鏡 /觀察處理剝離邊界界面之情況,第16 _至⑴係表示以 Ο 觀察之情況。第16圖⑷係照射由2(TC的空氣與2 〇 C的,水構成的多相流體後,並以顯微鏡觀察表面之情 第16圖(d)係對應之AFM照片(第17例)。第16圖(外 1’、、射130C的工氣與90 C的純水構成的多相流體後,利 用顯微鏡觀察表面的情況,f 16圖⑷係對應之遍照片 第18例)。第16圖⑷係照射由城的水蒸氣與抓的 窗水構成的多相流體後,簡微鏡觀察表_情況,第16 圖«)係對應之AFM照片(第19例)。 第17圖(a)至(c)係表不’在有HMDS,赃的條 % 私下塗靜舰’且在上述條件下㈣該樣本後以顯微 二觀察處理剝離邊界界面之情況,第17圖⑹至(⑽表示 2/FM觀察之情況。第17圖⑷係照射由跳的空氣與 C的純水構成的多相流體後,且利用顯微鏡觀察表面的 ^況’第17圖⑷係對應之AFM照片(第2。例)。第17圖 德)係照㈣130。(:的空氣與9G。⑶純水構成❹相流體 昭’並以顯微鏡觀察細之情況,第〗7圖(e)係對應之應 片(第21例)第17圖(^)係照射由13〇。(:的水蒸氣與2〇 的純水構成的多相流體後’而以顯微鏡觀察表面的情 /,苐17圖(f)係對應之AFM照片(第22例)。 第18圖⑷至(c)係表示,在有HMDs、^ke11〇t>c之條 320816 35 201023986 件下塗佈阻劑膜,且以上述條件照射該樣本後,並以顯微t 鏡觀察處理剝離邊界界面之情況,第18圖(d)至(f)係以 AFM觀察之情況 '第18圖⑷係照射由加^的空氣與 。(:的純水構成的多相流體後,以顯微鏡觀察表面之情況, 第18圖(d)係對應之AFM照片(第23例)。第18圖作)係照 射由13〇t的空氣與90°C的純水所構成的多相流體後,且 利用顯微鏡觀察表面之情況,第18圖〇)係對應之AFM照 片(第24例)。第18圖⑷係照射由130eC的水蒸氣與20 。(:的純水構成的多相流體後,而以顯微鏡觀察表面的情❽ 況’第18圖(f)係對應之AFM照片(第乃例)。 第26例 將液滴直徑及流速的關係表示於第19圖。將水蒸氣 壓力設為—定(G.2MPa),且以各種之純水流量,測量液滴 的流速液滴直餐。將結果表示於第19圖。表示以 =量之液滴速度V•直徑d的關係。V與d皆接近於正規 刀布’其平均值係分别為28〇油與1〇"拉左右。, 2/ (*-i) 2/r <1 a (wide 1) /r ftH-l NIX (r-1) Μ \/κ fc+l ——一[卜(五) (d)八, > J i κ — 1 L UJ (Formula 1) Here, K is the specific heat of the gas (constant pressure ratio / constant volume specific heat), and Ρ! is the pressure of the throat of the nozzle, and the pressure of the outlet of the P2 nozzle. The cross-sectional area A2 of the nozzle outlet is obtained by the expansion ratio and the sectional area A3 of the throat. Here, the sectional area A2 of the nozzle outlet is not particularly limited, and is, for example, 7.0 to 28.0 mm2. In addition, the length of the nozzle is determined by considering the material of the nozzle, the roughness, and various parameters such as the flow rate of 19 320816 201023986 (Reynolds number). Further, the degree of expansion is considered in consideration of various parameters such as the degree of investigation, the density, the flow rate, and the like, and the shape suitable for the π of the nozzle is not particularly limited, and may be circular. Further, the inner wall surface of the mixing portion and the inner wall surface of the nozzle are formed into a substantially continuous curved surface. The mixing portion may be joined as a cylindrical body upstream of the nozzle or formed upstream of the nozzle. The mixing portion wall surface and the spray enchantment (4) are joined, and the secret portion is preferably formed by a liquid which is formed along the wall surface by forming a water film by the mixing portion, and also flows by squirting into a water film. There is no special setting, but it can also be a joint with piping, etc., and it is preferable to smoothly form the obstacle by the degree of the obstacle that the financial core is (4). In addition, the hybrid H4 will be described in detail later. (E) Wafer holding, rotation, upper and lower mechanism, wafer holding, rotation, and up-and-down mechanism unit (8) include a base 151 for holding an object (wafer); The rotation motor 152 is cooled by cooling the cooling object (wafer) by moving the susceptor 151 in the vertical direction by the distance between the outlet of the nozzle 141 and the wafer. The water pipe 154 is used to open and close the switchable cooling water for stopping the supply of the cooling water; the cooling water flow regulating valve w _ for adjusting the flow rate of the cooling water and the cooling for measuring the flow rate of the cooling water Water flow meter? In the above, the object processing of the present preferred embodiment is described as a structure, and then the mixing unit 144 of the multiphase fluid irradiation unit (1) is described. The mixing portion 144 has a water enthalpy that is partially open to the inner wall surface. The entangled portion 32 〇 8l6 20 201023986 • 144a (Fig. 30) is on the upstream side of the nozzle, and is 90 degrees or less based on the direction of the water vapor. The angle can mix water from the wall surface of the aforementioned mixing portion to water vapor. Preferably, the mixing portion has a cylindrical shape, and the inner diameter of the cross section joined to the nozzle of the mixing portion is preferably the same as the inner diameter of the inlet of the nozzle. Here, Fig. 2 is a detailed configuration diagram in which the mixing unit 144 is provided with a multiphase fluid amount mixing unit of a temperature controller. It is important to reduce the occurrence of the mutual northward phenomenon of the liquefaction of water vapor and the vaporization of water to the minimum α in the mixing portion 144 in the mixing portion 144. Therefore, as shown in Fig. 2, the mixing portion 144 is preferably the same. It is constructed as follows. 1) The direction in which the fluids of the gas and the liquid are stably mixed is at an angle of less than 90 degrees in the mixing portion. 2) The direct control of the liquid fluid or the orifice installed in the piping is much smaller than the cross-sectional area of the flow path of the gas fluid in the _ mixing section. 3) By installing a heater in the mixing section, the temperature of the inner wall of the mixing section is controlled to suit the following conditions. The temperature of the inner wall is not too large (±20% or less) from the saturation temperature of the liquid under the pressure φ force in the mixing portion. Further, the temperature of the inner wall is not too large (±20% or less) from the saturation temperature of the gas under the pressure in the mixing portion. Further, as the time passes, the inner wall of the mixing portion approaches the saturation temperature of the fluid, so that it is not intended to be used until the state of the multiphase flow is stabilized, and under the condition that the heat retention of the mixing portion is sufficiently performed, Remove the heating function of this heater. In the apparatus for processing an object by using a multiphase fluid in which a droplet and a gas are mixed, the fluid mixing portion is at a normal temperature at the time of starting the apparatus. Then, when there is a difference between the temperature and the temperature of the water vapor, the temperature is not uniform in the interior of the liquid mixing device 21 320816 201023986, whereby a part of the vapor is phase-changed and becomes a water droplet or the like. The delivery pressure of the multiphase fluid becomes unstable, and it is difficult to stably supply a certain shock wave to the surface of the object to be processed, so that it takes time until the device operates stably. That is, when the heater is provided to the multi-phase fluid adjusting portion, the fluid mixing portion can be set to the same temperature as the water vapor and the gas temperature, so that it is less likely to generate a gas-liquid phase in the mixing portion. The device can apply a stable shock wave to the object processing surface. 1- Attacking Phenomenon (Air Bubble Dregs Related Parameters) This best mode cleaning device is based on adjusting the gas pressure, the water mixing flow in the multiphase helium fluid, the gas temperature, the temperature of the mixed water, and the nozzle shape. The distance from the nozzle outlet to the object, the temperature of the object, and the relative movement time between the nozzle and the object, and the temperature of the droplet, the flow rate of the droplet, the size of the droplet, the number of droplets, and the treatment The function of the temperature of the surface of the object and the irradiation area of the multiphase fluid per unit time. Among the above parameters related to bubble collapse, the flow rate, temperature, and droplet density of the droplets are particularly important. By controlling the above parameters, the jet generated by the droplet and the shock wave caused by the collapse of the bubble, and the impact of the chain reaction generated by the shock wave can be obtained on the surface of the object to be processed, and can be cleaned, etc. In the effective processing. The flow rate contributes to the generation of shock waves caused by the collapse of the bubbles in the droplets at the time of droplet collision, and the temperature contributes to the generation of fluoro bubbles in the droplets. In addition, the higher the droplet density, the higher the probability of generating a shock wave. For example, if the number of droplets is zero, no shock wave due to collision of droplets will occur. However, when the number of droplets becomes too dense, the speed of the 爹 phase fluid may be lowered and the temperature may be lowered to reduce the probability of generation of the shock wave. 32〇816 22 201023986 • Here, the density of droplets means the number of droplets per unit volume in a multiphase fluid • every * unit time, and correctly measures the droplets of the high speed moving / order The measuring device has not been developed yet, so it is substituted with the amount of pure water introduced into the multiphase fluid. ^ Measurement method of cavitation phenomenon' The system of the present invention has a measuring means for measuring the degree of cavitation under the condition of irradiating the multiphase flow to the object or the measurement sample under certain conditions. phenomenon. Here, according to the current technology, it is impossible to monitor the cavitation phenomenon (shock wave) (the intensity of cavitation) and the density (the number of occurrences per unit time) while performing the peeling and cleaning process. Therefore, the technique used in the present system changes the parameters related to the generation of cavitation in a prior experiment, and performs program processing, and s determines the size of the cavitation phenomenon from the following data obtained from the result. (1) Measurement method of physical change of physical change of object or measurement sample by quantitative method ^ Concavity and convexity of metal surface when irradiating multiphase fluid on metal surface • Resistor when irradiated on resist surface The area of the peeling area and the amount of the residue • The removal rate of the foreign matter attached to the entire surface of the wafer (2) The measuring method of the sound that can detect the noise of the cavitation phenomenon • The size of the noise of the cavitation phenomenon perceived by the acoustic sensor (3) Measuring means for visually measuring changes in the visual value of an object or a measuring sample in a quantitative manner. Image data of a resist stripping process photographed by a high-speed camera, for example, multiphase fluid temperature and irradiation of the multiphase fluid 23 320816 201023986 The surface of the metal is as confirmed in Section 9. The correlation between these parameters is determined by the peeling performance of the agent. The data of the mouth map is its product, the product of the f, the majority of the data is indeed the second resistance _ the area will be physically injured, and the damage to the equipment = = the maximum of the nozzle _ force two:: also does not produce _ high-pressure parts As a result, and manufacturing a safe device. The distance between the objects of the county and the county is as follows: Table 1: Fig. 2, Fig. 23. r d±..., the table is unfavorable for the unit of the weight Z, ', and the weight of the droplet generated by the fast collision, which is expressed as the relative unit of no unit. 11 'In the conventional technology (for example, in addition to the use of more than 2 mouthpieces, the difference between the device and the best form is not large = composition. But in the conventional technology, in the object At the time of the treatment, there is no such thing as the physical force of the so-called "shock wave". Therefore, the jade is not controlled on the object, and the control of the shock wave is not performed. In addition, under the condition of the prior art, "the cavitation phenomenon" It is completely inside the mouth of the thin-tailed shape of the front end of the shirt. The life of the shock wave generated is extremely short, and when the object is reached, the specific phase of the shock wave is lost, and the multiphase fluid flowing in the nozzle is accelerated near the tip of the nozzle. Money. Then 'causes that the flow rate is accelerated to become the result of the decompression L, the liquid causes cavitation and generates shock waves. According to Kato Yang / σ, the "cavitation phenomenon" published by the bookstore, the nitrogen in the liquid shock wave tube The duration of the bubble collapse is 2 to 3 seconds. The flow rate is 4〇〇m/sec. 24 320816 201023986 ' The movement time of the body is only 1.2mm, and the bubble collapses between the nozzle throat and the mouth. The phenomenon will disappear. Again, that is, Bubble collapse occurs at the nozzle outlet, and it is difficult to set the object distance to 1.2 mm or less. On the other hand, in the present invention, the nozzle is used to accelerate or expand the irradiation area of the multiphase 'fluid. The function of the bubble is related to the bubble collapse related parameters related to the occurrence of fluorine and acupoint phenomenon. As long as the cavitation phenomenon on the object is focused on, it can be adjusted basically in any place, for example, in front of the nozzle. The fluid mixing section of any space of the fluid piping is carried out. Specifically, it can be controlled in any space as shown by the arrow symbol shown by α in Fig. 1 (between the steam generating device and the nozzle outlet). In the following, the main parameters related to bubble collapse will be described in detail. The method of cleaning the object in the best form of the aluminum alloy button, in addition to the above-mentioned impact force, also has the effect of preventing the money of the rot. By adjusting the temperature of the gas, the temperature of the mixed water, the shape of the nozzle, the distance from the nozzle outlet to the object, the temperature of the object, the relative between the nozzle and the object The movement time can be controlled to prevent the corrosion effect. Among the above related parameters, in particular, the temperature at which the multiphase fluid reaches the object and the ρΗ when the multiphase fluid reaches the object are particularly important. By controlling the above parameters, it is possible to On the surface, a special protective film for preventing corrosion is formed. Hereinafter, the parameters related to the prevention of aluminum corrosion are detailed together with the parameters related to the main bubble collapse. (1) Temperature of the fluid The shock wave system is mainly a droplet collision. When the surface of the object is treated, the cavitation phenomenon of 320816 25 201023986 and the collapse of the cavitation phenomenon occur. The cavitation phenomenon is a cavity generated when a part of the liquid such as water generates a low pressure portion, and the temperature of the gas and the liquid is higher. The higher the temperature of the droplets, the higher the temperature of the droplets, and the more easily the bubbles in the water droplets occur. Accordingly, the bubble collapse which is the basis of the shock wave that becomes a large energy source on the surface of the object to be treated occurs. When the treatment method is utilized for the removal of the resist film, the resist film and foreign matter which are relatively bonded can be removed.On the other hand, if the temperature of the multiphase fluid and the water droplets is set to a low level, the generation of the shock wave can be suppressed on the surface of the object to be treated, and the object having a weak strength can be cleaned. However, there is a limit to the height at which the temperature can be set due to the limitation of the heat resistance of the object or the like. Further, when the distance from the object becomes long in a state where the temperature is too high, there is a possibility that the gas component in the droplet falls off and the bubble core is not easily generated, and the distance from the nozzle outlet to the object is about 2 to 30 mm. The distance is set to be negligible. Further, the temperature of the water vapor supplied into the nozzle is preferably from 50 to 120, more preferably from 80 to 115. (:, more preferably 90 to 11 (TC. Further, the temperature of the water mixed with the aforementioned steam is preferably 0 to 40. (: 'It is desirable to be 10 to 35. (:, better yet 20 to 3 〇. (: Here, in particular, the temperature at which the multiphase fluid reaches the object is preferably 5 〇ΐ or more, more preferably 80 Å or more, and more preferably 9 〇 or more. The measurement of the temperature of the multiphase fluid is carried out by the method described in the examples. By setting it in this range, the aluminum on the surface of the object is formed into a special film which prevents the effect of the rot #2. The speed of the drop is 320816 26 201023986 • The higher the velocity of the droplet is, the larger the impact becomes when the droplet collides with the surface of the object to be treated. Therefore, the internal pressure difference is likely to occur, and as a result, the bubble collapses and gas is generated. Acupoint phenomenon, that is, if the velocity of the droplet is set to a high degree, a large shock wave of the energy is generated on the surface of the object to be processed, for example, the treatment method is utilized for the removal of the resist film. It can remove the relatively strong resist film and foreign matter. On the other hand, if the speed of the liquid droplets is set to a low level, the generation of the shock wave can be suppressed on the surface of the object to be processed, and the object of the weaker object can be cleaned and washed. The speed makes the time for exposing the multiphase fluid to the air to be short, so it is difficult to introduce carbon dioxide in the atmosphere, and it is difficult to be biased toward acidity, so that the effect of preventing corrosion can be more appropriately exhibited. The velocity of the droplets is 100 to 600 m/s, It is preferably 200 to 500 m/s, more preferably 250 to 350 m/s. By setting the fluid velocity in this range, the impact of cavitation can be obtained. Furthermore, the velocity of the droplet and the fluid are set. The speed is approximately the same, and is set to "flow rate" / "nozzle sectional area". Here, the flow rate is set to @ water vapor flow rate (m3/s), and the nozzle sectional area is set to the sectional area of the nozzle outlet (m2) 〇(3) Other parameters First, regarding the nozzle, the ultrahigh-speed nozzle is used as described above. By using this nozzle, the flow velocity of the fluid is changed and the magnitude of the shock wave is also changed. In principle, it is easy to obtain a shock wave when using a nozzle having a large flow velocity. Furthermore, by using an ultra-high-speed nozzle to irradiate a multi-phase fluid containing water vapor and water droplets, a special action is observed by the relationship between the pressure of the water vapor and the speed and diameter of the water droplets. The water vapor pressure is 0.05. Up to 0.25Mpa, there is no special 27 320816 201023986. Especially when the water vapor pressure is above 015MPa, the multiphase flow system of water vapor and water droplets shows a different action from the multiphase fluid of air and water droplets. Then, Regarding the distance from the nozzle outlet to the object, the general adaptation 値 is in the range of 2 to 3 mm (optimal range 2 to 1 〇 ηπη), preferably 5 mm or less 'more preferably 3 mm or less, more preferably 2 mm. If the distance from the exit of the nozzle to the wafer is reduced, the resist stripping performance is improved as well, and when the optimum distance is too close, the peeling performance is lowered. On the contrary, it is desirable to suppress the peeling performance and the cleaning performance as long as it is far from the optimum distance. Furthermore, the closer the distance from the nozzle outlet to the object, the more difficult it is to introduce carbon dioxide in the atmosphere, and it becomes difficult to be acidic. In addition, when it is desired to obtain a particularly high impact force, it is important that the liquid droplets are covered by the water droplets when they collide with the object. Here, the flow rate of water vapor, preferably the mass flow rate of water vapor is 〇〇83 to 1 〇kg/min, more preferably 疋0.025 to 0.75 kg/min, more preferably 〇33 to 〇5〇kg/ Min. Further, the gas-liquid mixture ratio (liquid/gas) is preferably 〇 〇 18 to 〇 〇1. The droplet diameter is preferably from 2 to 25. When the droplet diameter is increased, the surface area is reduced, so that the amount of carbon dioxide introduced into the atmosphere is small, and it becomes difficult to be acidic. Further, the droplet diameter was a machine manufactured by Ding 81 Co., Ltd., and PDA 〇Phase D〇ppiei· Anem〇metry: phase Doppler method), and when there was no special load, it was set at 5 mm from the nozzle outlet. The position is measured. The cross-sectional area of the fluid flow/discharge port is preferably 〇.5 to 32 〇 kgcm-2min-i. In order to form water into the water film on the wall surface and to mix the water into the multiphase fluid, for example, it is preferable to set the pressure applied to the water to such an extent that the water does not flow back by the pressure of the water vapor. The pressure applied to the water is not particularly limited. For example, 28 320816 201023986 ' If it is introduced above the water vapor pressure and the pressure is not applied, the pressure can be introduced. More specifically, the pressure of water introduction preferably satisfies the following formula. (pressure of water vapor + 〇.〇2MPa) < (pressure of water introduction) < (pressure of water vapor + 1.0 MPa) When the pressure of water introduction is too low, the water is introduced as a pulsating flow, and the characteristics of the fluid become Unstable. In addition, when the pressure is too high, the water will scatter to the center of the diameter direction of the nozzle, and it is difficult to form the same water film, and it also hinders the acceleration of the vapor ©. Further, from the viewpoint of forming a water film on the wall surface, it is preferable not to pressurize the spray direction, and it is more preferable to supply it in the vertical direction against the passage direction of the water vapor. The pH of the multiphase fluid reaching the object is preferably 7.0 to 9.0, more preferably 7.0 to 8.0, more preferably 7.0 to 7.5. Since a special film is formed on the surface of the object by setting the pH in this range, the corrosion preventing effect of aluminum can be obtained. Further, the pH measuring method is a method described in accordance with the examples. [Embodiment] Method for measuring temperature when multiphase fluid reaches an object Fig. 31 is a schematic view showing a device for measuring temperature when a multiphase fluid reaches an object. A thermocouple TH (aluminum chrome thermocouple JIS C1602) is attached to the dream wafer W having a diameter of 6 leaves and a thickness of 0.625 mm, and the distance between the fluid ejection outlet of the nozzle 141 and the object is compared with the water vapor pressure. The conditions such as the pure water flow rate and the like are set to the same enthalpy as when the object is processed, and the thermocouple is irradiated for 1 minute, and the temperature at which the temperature is stabilized is 29 320816 201023986, and the temperature at which the multiphase fluid reaches the object is set. . Multiphase, Measure method of pH when the body reaches the object Fig. 32 is a schematic view of a device for measuring the pH when the multiphase fluid reaches the object. The discharge port of the nozzle 141 is connected to a cooling pipe C (for example, a Graham condenser) via a pipe P, and the agglomerated water is recovered to the vessel r, and the pH of the water is measured by the method of HSZ8802. Further, the aforementioned agglutination operation is carried out without contact with air. First Example Under the following conditions, a multiphase fluid (a case where steam was used as a gas and air was used) was irradiated on an aluminum surface for 10 minutes. The AFM (atomic force microscopy) photograph before and after the treatment is shown in Fig. 3. Figure 5 shows the surface roughness data. Further, in this example, the surface roughness was measured by the AFM-affiliated profile analysis method. Vapor pressure: 〇.2Mpa Vapor temperature: 13〇°C Pure water flow rate: 300cc/min Pure water temperature: 20°C GAP 5 mm Nozzle scan: Fixed the second case under the same conditions as the first case The multiphase fluid (as a gas for the vapor and the use of air as a gas) was irradiated on the steel surface for 1 minute. The AFM photographs before and after the treatment are shown in Fig. 4. Figure 6 shows the table 320816 30 201023986 * Surface roughness data. . . . - 3rd example The steam cleaning technique shown in Patent Document 1 utilizes the mechanical action of the strip gas and the mechanical action of the jet to peel off the resist, so the stripping of the resist needs to be calculated in minutes. This method also visualizes high-speed video in order to confirm whether it is the same mechanism. Fig. 7 is a view showing the case where the multi-phase fluid is irradiated under the same conditions as in the first example except that the nozzle scanning speed is io 〇 mm/sec, and the one-line positive photoresist is removed from the lower portion of the quartz wafer. The case of time-dependent changes. As shown in Fig. 7, the area where the resist is peeled off gradually expands and rapidly peels off. ΆΛΜ. In the same conditions as in the first example, the multi-phase fluid was irradiated against the dream wafer implanted with high-concentration ions, and the i-line positive photoresist was peeled off, except that the nozzle scanning speed was set to 40 mm/sec. The situation of change over time. The results are shown in Fig. 8. From ft to eighth, the gas and temperature of the multiphase fluid were changed under the following conditions, and the multiphase fluid was irradiated against the aluminum surface for 10 minutes. The AFM photographs before and after the treatment are shown in Fig. 9. The surface roughness data is shown in Figure 1. Further, the surface Ra of the aluminum to be treated before the irradiation was Ra of 34.9 nm. Gas pressure: 〇.2Mpa Liquid flow rate: 300cc/min Gap : 10mm The result of irradiation with a large amount of 31 320816 201023986 phase fluid composed of low temperature air (20 ° C) and low temperature pure water droplets (20 ° C), obtained Ra It is a surface of 30.5 nl Vt. The AFM photograph of the surface is shown in Fig. 9(a), and the data of the surface roughness is shown in Fig. 10(a) (the fifth example). Next, as a result of irradiating a multiphase fluid composed of high-temperature air and low-temperature pure water droplets (2 ° C), a surface of 96.4 nm was obtained. The AFM photo of the surface is shown in Fig. 9(b) and the surface roughness data is shown in Fig. 10(b) (sixth example). Then, the irradiation is performed by high temperature air (13 〇 ° C) and high temperature pure As a result of the multi-purpose fluid composed of water droplets (6 〇 ° C), a surface having an Ra of 86.3 nm was obtained. The photograph of the surface is shown in Fig. 9(c)' and the data of the surface roughness is shown in Fig. (c) (the seventh example). The surface coarse rotation of (c) is slightly smaller than (b) and the density of the portion of the thick wheel is larger than (b), so it can be seen that (c) is more affected by shock waves than (b). Further, the result of irradiation of a multiphase fluid composed of water vapor and low-temperature pure water droplets (203⁄4) was used to obtain a surface having Ra of 257 nm. The photograph of the surface is shown in Fig. 9(d), and the data of the surface roughness is shown in Fig. (d) (8th example). As a result of the above, as the shock wave is increased in temperature, especially when water vapor is used in the gas, it is clear that the maximum shock wave is applied to the surface to be treated. The surface of the A1 anti-money surface having a Ra of 348.8 nm was irradiated with the gas and temperature of the multiphase fluid under the same conditions as in the fifth to eighth examples. As a result of irradiating a multi-camera composed of 2 (the air of TC and 20 t of pure water droplets), a surface having an Ra of 380 nm was obtained. The AFM of the surface was shown in Fig. 11 (a) 'and the surface roughness was The data is shown in Figure U (c) (Example 9). Next, the result of irradiating a multiphase fluid consisting of 130 〇C water vapor and 2 (η: pure water 320816 32 201023986 • droplets gives Ra Surface of 440 nm. 'AFM photograph of the surface is shown in Fig. 11(b), and the surface roughness data is shown in Fig. 11(d) (10th example). In the eleventh case, the Ra is 8.1 nm. The SUS surface was irradiated with the gas and temperature of the multiphase fluid under the same conditions as in the fifth to eighth examples. The irradiation consisted of water vapor at 130 ° C and pure water droplets at 20 ° C. As a result of the phase fluid, a surface having an Ra of 19. gnm was obtained. The AFM of the surface was shown in Fig. 12(a), and the surface roughness data was shown in Fig. 12(b) (the eleventh example). In the twelfth case, the surface of the titanium having a Ra of 75.5 nm is subjected to the change of the gas and temperature of the multiphase fluid under the same conditions as in the fifth to eighth examples. As a result of irradiating a multiphase fluid composed of water vapor of 130 ° C and 2 (a pure water droplet of TC), a surface having an Ra of 98 nm was obtained. The AFM photograph 10 of the surface is shown in Fig. 13 (a), and The surface roughness data is shown in Fig. 13(b) (12th example). With titanium, interference fringes can be visually observed. It is also possible to form an oxide film on the surface. The thirteenth case has a Ra surface of Ra of 1.9 nm. Irradiating the gas and temperature of the multiphase fluid under the same conditions as in the fifth to eighth examples. Irradiating the multiphase fluid composed of water vapor at 130 ° C and pure water droplets at 20 ° C As a result, a surface having Ra of 7.6 nm was obtained. The AFM photograph of the surface was shown in Fig. 14 (a), and the surface roughness data was shown in Fig. 14 320816 201023986 (b) (13th example). From the 14th case to the 25th case, in the 14th to the 25th cases, it is reviewed whether there is a difference in the peeling condition under the resist coating condition. The presence or absence of HMDS (hexamethyldiazepine, hexamethyldisilazane), Bake The temperature change was 9 ° ° C, 11 ° ° C, and the effect of the change in the condition was observed. The profile may not depend on the results of the substrate treatment of HMDS. The experiment was carried out under the following conditions: Sample use: I line resist irradiation time: visually observed the gas pressure after peeling: 〇. 2Mpa liquid flow rate: 300cc/min nozzle scanning : Fixed Gap : 10 mm Fig. 15 (a) to (c) shows that the peeling boundary interface was treated by microscopic observation after coating the sample under the conditions described above without HMDS and Bake9 (Jc) and irradiating the sample under the above conditions. In the case of Fig. 15, (4) to (1) are observed by AFM. Fig. 15(a) is an AFM photograph corresponding to the case where the surface is observed by a microscope after the irradiation of 2 (Γ(: air and a multiphase fluid composed of pure water of 2 °C), and Fig. 15 (d) The 14th example). The 15th _) is the AFM photo corresponding to the radiation of 30: (: the air of the thief and the pure water of the thief, and the surface is observed by a microscope] and Fig. 15 (e) (15th example) Fig. 15 (4) is a case where the surface is observed by a microscope after irradiating a multiphase fluid composed of 13 (r water vapor and paper pure water, Fig. 15 (1) 320816 34 201023986 * corresponding AFM Photograph (16th example). The resist film was applied under the conditions of no HMDS and BakellCTC, and after irradiating the sample under the above conditions, the boundary interface was peeled off by microscope/observation treatment, and the 16th to the (1) In the case of observation, Fig. 16 (4) is an AFM photograph corresponding to the multi-phase fluid consisting of 2 (the air of TC and 2 〇C of water, and the surface is observed by a microscope) (Fig. 16(d)) 17 cases). Figure 16 (Using the external 1', the 130C gas and the 90 C pure water, the multiphase fluid is used. Micromirror observation of the surface, f 16 (4) corresponds to the 18th case of the photo. Figure 16 (4) is the multi-phase fluid composed of the water vapor of the city and the captured window water, the microscopic observation table _ In the case, the 16th figure «) corresponds to the AFM photograph (19th example). Figure 17 (a) to (c) show that 'in the case of HMDS, 赃% of the privately coated squid' and under the above conditions (4) After the sample, the peeling boundary interface is treated by microscopic observation. Fig. 17 (6) to (10) show the case of 2/FM observation. Fig. 17 (4) is the irradiation of the multiphase composed of the jumping air and C pure water. After the fluid, the surface of the surface is observed by a microscope. Figure 17 (4) corresponds to the AFM photograph (2nd example). Figure 17 is a photograph (4) 130. (: Air and 9G. (3) Pure water constitutes a ❹ phase The fluid is shown in the microscope and is observed by a microscope. The 7th figure (e) corresponds to the film (21st case) and the 17th figure (^) is irradiated by 13〇. (: water vapor and 2〇 pure After the multiphase fluid consisting of water, the surface is observed by a microscope, and Fig. 17 (f) corresponds to the AFM photograph (22nd example). Fig. 18 (4) to (c) show that HMDs, ^ke11〇t>c strip 320816 35 201023986 coated resist film, and irradiated the sample under the above conditions, and observed the peeling boundary interface by microscopic t-mirror, Fig. 18 (d) (f) is the case of observation by AFM. [Fig. 18 (4) is a case where the surface of the multiphase fluid composed of pure air is added and the surface is observed by a microscope, Fig. 18 (d) Corresponding AFM photograph (23rd example). Fig. 18 is a case where a multiphase fluid composed of 13 〇t of air and 90 °C of pure water is irradiated, and the surface is observed by a microscope, Fig. 18 ) A corresponding AFM photograph (24th example). Figure 18 (4) is irradiated with water vapor of 130eC and 20 . (A: A multi-phase fluid composed of pure water, and a condition of observing the surface by a microscope. Fig. 18(f) corresponds to an AFM photograph (the first example). The 26th example relates the relationship between the droplet diameter and the flow rate. It is shown in Fig. 19. The water vapor pressure is set to - (G. 2 MPa), and the flow rate of the droplets is measured at various pure water flows, and the results are shown in Fig. 19. The relationship between the droplet velocity V and the diameter d. Both V and d are close to the regular knife cloth's average value is 28 〇 oil and 1 〇 "
第27你L 第20圖係表示關於純水的流量(TlOOmL/min時之v 將蒸氣壓力P及與噴嘴之距離h設為參數時的結果。 hi為了進Μ較’空氣與液滴之混合喷流的結果亦以 π °由圖可知作為對象之液滴速度係 200 至 300m/s :右’而液滴直徑係1〇鋒左右。 ''''''飢^體1力息速度的關係、 使水的狀里改變為200cc/min’ JL使氣體的壓力改變 36 320816 201023986 ’為0.05、(U、0.2Mpa ’並使用音速噴嘴來喷射水蒸氣與水 '的多相流體,以及空氣與水的多相流體,且科用 LDA(LaserDopplerAnemometry:雷射杜卜勒流速計)於距喷 出口 5、10mm之位置測量該液滴的速度(第33圖)。此外, ’ LDA之測量係利用TSI公司製造的LD A来進行測量直到 可取得10000個液滴之資料為止,在各條件下進行3次測 量。使用水蒸氣與水的多相流體時,觀測到相較於5mm的 位置’於10mm的位置液滴之速度比較快。此外,空氣與 ©水之多相流體的情況’係可看出愈提高空氣的壓力,液滴 的速度變愈高之傾向。另一方面,水蒸氣與水的情況,原 因不明’但觀測到愈提高水蒸氣的壓力,液滴的速度變愈 南且兩至預定値’在〇.2Mpa之下’依據測量値液滴速度 會變低。但是’推測此可能為錯誤。在其他條件下,測量 為不到10秒之程度,而水蒸氣與水之多相流體僅在水蒸氣 壓〇.2Mpa之條件下,測量需要數分鐘。因此,可推測在 參該條件下大部分觀測到雜訊。. 盖^例(氣艚壓力與液滴直徑之關係、 將水的流量設為200cc/min ’且使氣體的壓力變化為 0.05、0.1、〇.2Mpa而使用音速喷嘴來噴射水蒸氣與水之多 相流體、以及空氣與水之多相流體’且利用pDA於距喷出 口之5、l〇mm的位置測量該液滴的直徑(第34圖)。此外, PDA的測量係進行測量到取得10000個液滴的資料為止, 在各條件下測量3次。空氣與水之多相流體的情況,係即 使使空氣的壓力產生變化,液滴之速度幾乎不產生變化。 320816 37 201023986 另一方面,水蒸氣與水的情況,雖眉 ^ 席口不明’但若提高水 蒸氣關力,直到預定㈣止幾乎看不到液滴之 變 化,而在0.2鄭下,觀測_滴的直徑急速變小之^象。 但是,推測此可能為錯誤。在其他條件下,測量為不到ι〇 秒之程度,而^氣與水之多相流體僅在錢氣壓〇购& 之條件下’測量需要數分鐘。因此,可推測在該條件下大 部分觀測到雜訊。' 第30例(喷嘴内之壓 在水蒸氣麼(U、〇.2Mpa之條件下,將純水流量設為 1〇〇CC/min,並使用石英喷嘴來喷射水蒸氣與水之多相流 體。如此-來,在石英喷嘴的尖端觀到測遷力波。將此情 況表示於第35圖。此外’第35 _係在Q ¥的條件 下之喷射的情況,第35圖(b)係在〇 2Mpa的條件之喷射的 情況。此外為了進行比較,在氣體麼力0.1、0.2Mpa之條 件下皮將純水流量⑤為i QQee/min,並使用石英喷嘴來照 λ工1與水之多相流體。但是,於石英喷嘴尖端觀測不到 壓力波將此情況表示於第36圖。此外,第36圖⑷係在 〇.應的條件下之喷射的情況,第36圖(b)係在〇.2Mpa 的條件下之嘴射的情況。 (第1實施例至第36實施例) 、有最佳形態的音速喷嘴(第30圖)之清洗裝 置在以下之條件下’將水蒸氣與水之多相流體喷射到對 象物,且洗效果 、物理破壞及配線之耐腐蚀性(第 1表、第2矣、 衣)°再者,就對象物而言’係使用具有鋁配線 38 320816 201023986 • 之矽晶圓,其係對i線負光阻劑(東京應化THMRip3300) , 塗佈1/zm之厚度,並在90°C下烘乾120分鐘後,且以 365nm曝光20秒,並在室溫下利用TMAH (〔N(CH3)4〕 +ΟΚΓ)進行顯影者。No. 27, L Figure 20 shows the flow rate of pure water (the result of setting the vapor pressure P and the distance h from the nozzle as a parameter at T100 mL/min. hi is more mixed with 'air and liquid droplets. The result of the jet flow is also π ° as shown in the figure. The droplet velocity is 200 to 300 m/s: right' and the droplet diameter is about 1 。. '''''' Relationship, change the shape of the water to 200cc/min' JL to change the pressure of the gas 36 320816 201023986 'Multi-phase fluid of 0.05, (U, 0.2Mpa 'and use sonic nozzle to spray water vapor and water', and air The multiphase fluid with water, and the LDA (LaserDopplerAnemometry) is used to measure the velocity of the droplet at 5, 10 mm from the discharge port (Fig. 33). In addition, the measurement system of 'LDA The measurement was performed using LD A manufactured by TSI Corporation until three times of measurement was possible, and three measurements were performed under each condition. When a multiphase fluid of water vapor and water was used, a position of 5 mm was observed. At a position of 10mm, the velocity of the droplet is faster. In addition, the air and the water are In the case of the phase fluid, it can be seen that the higher the pressure of the air, the higher the tendency of the droplet to become higher. On the other hand, the case of water vapor and water is unknown, but the higher the pressure of the water vapor is observed, the liquid The speed of the drop becomes southerly and two to the predetermined 値 'under 〇.2Mpa'. The droplet velocity will become lower depending on the measurement. But 'presumably this may be an error. Under other conditions, the measurement is less than 10 seconds. The multiphase fluid of water vapor and water only needs to be measured for several minutes under the condition of water vapor pressure of .2Mpa. Therefore, it is speculated that most of the noise is observed under the condition of this condition. The relationship between the pressure and the droplet diameter, the flow rate of water is set to 200 cc/min', and the pressure of the gas is changed to 0.05, 0.1, M.2 MPa, and the sonic nozzle is used to spray the multiphase fluid of water vapor and water, and the air and The multiphase fluid of water' and the diameter of the droplet are measured by pDA at a position of 5, 10 mm from the discharge port (Fig. 34). In addition, the measurement of the PDA is measured until the data of 10,000 droplets is obtained. , measured 3 times under various conditions. Air In the case of a multiphase fluid with water, the velocity of the droplets hardly changes even if the pressure of the air changes. 320816 37 201023986 On the other hand, in the case of water vapor and water, the eyebrows are not clear. Increase the water vapor pressure until the predetermined (four) stop can hardly see the change of the droplet, and under 0.2 Zheng, the diameter of the observation_drop is rapidly reduced. However, it is speculated that this may be an error. Under other conditions, The measurement is not to the extent of ι〇秒, and the multiphase fluid of qi and water is only measured for several minutes under the conditions of money pressure && Therefore, it is speculated that most of the noise is observed under this condition. 'Thirtyth case (the pressure inside the nozzle is in water vapor (U, 〇. 2Mpa, the pure water flow rate is set to 1〇〇CC/min, and the quartz nozzle is used to spray the multiphase fluid of water vapor and water) In this way, the force wave is observed at the tip of the quartz nozzle. This is shown in Figure 35. In addition, the '35th _ series is the case under the condition of Q ¥, Fig. 35 (b) In the case of the injection of 〇2Mpa conditions. In addition, for comparison, the pure water flow rate 5 is i QQee/min under the condition of gas force 0.1, 0.2Mpa, and quartz nozzle is used to take λ work 1 and water. Multiphase fluid. However, no pressure wave is observed at the tip of the quartz nozzle. This is shown in Fig. 36. In addition, Fig. 36 (4) is the case of injection under the condition of 〇., Fig. 36 (b) The case of the nozzle under the condition of 22Mpa. (The first embodiment to the thirty-sixth embodiment) The cleaning device having the best form of the sonic nozzle (Fig. 30) under the following conditions 'water vapor and The multiphase fluid of water is sprayed onto the object, and the washing effect, physical damage, and corrosion resistance of the wiring (Table 1, 2矣, clothing) ° Again, in terms of the object 'use the aluminum wiring 38 320816 201023986 • after the wafer, which is tied to the i-line negative photoresist (Tokyo should THMRip3300), coated 1 / zm The thickness was dried at 90 ° C for 120 minutes, and exposed at 365 nm for 20 seconds, and developed at room temperature using TMAH ([N(CH3)4) + ΟΚΓ).
39 320816 201023986第ι表 遵_遽*3839 320816 201023986第ι表 遵_遽*38
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In Ο 00 _> 0寸 1001- 100 10 0 ‘6 00 _ 0寸 1001. 320816 ο 201023986^ 第2表 e 項_璲*38 10天後 之配線 的腐蝕 碟 墀 m 碱 碟 碱 m m 碟 m m m 墀 m 墀 磲 峨 物理 破壞 1_ 媒 m m 碱 磔 墀 m 碟 #. m 磲 m 聚合物 去除 I ! Μ 4i •Μ Μ 液滴 直徑 〇> σ> 1 1 C0 r— CO 〇> 〇> 1 1 00 GO σ> 03 1 1 明?:S , \φ v! 〇 ο 5 〇 Ύ— 〇 〇 〇 δ Ο τ-~ ο 〇 〇 〇 Τ Ο Ο ο 〇 τ~ ο δ Ο τ- Ο ο τ- Ο Ο »— Ο 〇 Ϊ— 〇 T— 〇 ο 〇 〇 〇 ό 〇 d 6 Ο ο ο Ο Ο 6 〇 水蒸氣 壓力 /MPa 0. 20 0; 20 0. 23 0. 23 0.05 0. 05 0. 20 0. 20 0. 23 0. 23 0. 05 0. 05 0. 20 0. 20 0. 23 0. 23 鉍鳋_ 敢跑I 10 10 10 1〇 ΙΟ ΙΟ ΙΟ to u> to ΙΟ ΙΟ tD ίΩ ΙΟ ΙΩ \ 〇 卜 Ο 〇} 〇 卜 〇 〇> Ο 〆 ο σ> 〇 卜 Ο 〇> ο 卜 ό α> ο ο σ> Ο 卜 Ο 0> 〇 〇 σ> 液滴 速度 /me"*1 〇 CO ο § 〇 ο 〇 to Ο ΤΓ- ο ο t— 〇 〇 c〇 ο ο C0 ο S ο (Ο ο ο r* ο τ- Ο g ο § 〇 〇 <〇 〇 〇 <D 混合 水溫 /¾ 导 导 〇 σ Ο ο 〇 ο ο ο 穿 Ο Ο 〇 寸 流體 溫度 /°C g 1— to ο τ~ g ο τ- S S τ—· T— τ- ο CSI Τ™*· S τ— 8 ΊΤ~ S τ— r— S S | <Μ CM to <Μ 寸 1Ω ΟΙ 苳 Φ <Μ & C0 Csl 苯 0) CM ο C0 5 ΟΙ C9 3ε Ο CO 10 CQ CO CO :s 遥 Μ 4Κ ίΚ 41 320816 201023986 比較例 第1比較例係流體溫度太低之情況。流體溫度太低時 去除聚合物,且10天後配線腐蝕。 第2比較例、第3比較例係液滴速度太慢的情況與太 快的情況。太慢時聚合物殘留,太快時可看到配線之物理 性破壞。 第4比較例、第5比較例係pH太低之情況與太高之 情況。pH太低時不會產生保護膜,且10天後看到配線的 腐蝕。pH太高時會產生因pH高引起之配線的腐蝕。 42 320816 201023986 ^ 第3表In Ο 00 _> 0 inch 1001- 100 10 0 '6 00 _ 0 inch 1001. 320816 ο 201023986^ 2nd table e item _璲*38 Corrosion of wiring after 10 days 墀m Alkali dish alkali mm dish mmm 墀m 墀磲峨 physical destruction 1_ medium mm alkali 磔墀m disc #. m 磲m polymer removal I ! Μ 4i • Μ Μ droplet diameter 〇 > σ > 1 1 C0 r - CO 〇 > 〇 > 1 1 00 GO σ> 03 1 1 Ming? :S , \φ v! 〇ο 5 〇Ύ—〇〇〇δ Ο τ-~ ο 〇〇〇Τ Ο Ο ο 〇τ~ ο δ Ο τ- Ο ο τ- Ο Ο »— Ο 〇Ϊ — 〇 T— 〇ο 〇〇〇ό 〇d 6 Ο ο ο Ο Ο 6 〇Water vapor pressure / MPa 0. 20 0; 20 0. 23 0. 23 0.05 0. 05 0. 20 0. 20 0. 23 0. 23 0. 05 0. 05 0. 20 0. 20 0. 23 0. 23 铋鳋 _ dare to run I 10 10 10 1〇ΙΟ ΙΟ ΙΟ to u> to ΙΟ ΙΟ tD ίΩ ΙΟ Ι \ \ 〇 Ο 〇 〇 〇 〇〇 〇〇 gt ό ό ό ό & & & & & & & & & & ό ό ό ό ό ό ό ό ό ό ό ό ό ό ό ό ό ό ό 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴 液滴Ο - ο ο t — 〇〇c〇ο ο C0 ο S ο (Ο ο ο r* ο τ- Ο g ο § 〇〇 〇〇〇 &〇〇〇; 〇〇〇 < D mixed water temperature / 3⁄4 Guide 〇 σ Ο ο 〇ο ο ο Ο Ο 〇 流体 fluid temperature / ° C g 1 - to ο τ ~ g ο τ - SS τ - · T - τ - ο CSI Τ TM * · S τ - 8 ΊΤ ~ S τ - r — SS | <Μ CM to <Μ inch 1Ω ΟΙ 苳Φ < &Amp; C0 Csl benzene 0) CM ο C0 5 ΟΙ C9 3ε Ο CO 10 CQ CO CO: s remote Μ 4Κ ίΚ 41 320816 201023986 Comparative Example 1 Comparative Example of case-based fluid temperature is too low. When the fluid temperature was too low, the polymer was removed and the wiring was corroded after 10 days. In the second comparative example and the third comparative example, the case where the droplet velocity is too slow is too fast. When the polymer is too slow, the polymer remains, and when it is too fast, the physical damage of the wiring can be seen. The fourth comparative example and the fifth comparative example are cases where the pH is too low and the case is too high. When the pH is too low, no protective film is produced, and after 10 days, the wiring is corroded. When the pH is too high, corrosion of the wiring due to high pH occurs. 42 320816 201023986 ^ Table 3
配線腐蚀 10天後 之配線 的腐蝕 I I 處理後 m 碟 磲 物理 破壞 _I 聚合物 去除 |去除 梛 去除I I去除I 去除ι 處理條件 诨趔f ^ ^ \ σ> 〇〇 T-C • •. CD Ό> 液/氣 混合比 0.010 0.010 0.010 〇 _ 〇 〇 0.010 丨水蒸氣 壓力 /MPa 〇 CO 〇 〇 κ ο 〇 ο 喷嘴對 象物間 距離 /mm to IO ΙΟ u> to 玉乂 ο CD 〇 cad ο ο5 to cd to o ㈣7« Ο TO to 〇E> Ο 石 ο 〇〇 o « 混合 水溫 /X S ο 04 ο CM s s 流體 溫度 /¾ 呂 in o to o 比較例1 j比較例2 比較例3 比較例4 比較例 201023986 [產業上之運用利用] 本發明係可你 液晶、磁頭、磁微 例如’有關半導體裝置、 械加工零件、模製=基板、照相機等之透鏡、精密機 磨光等的處理2 等之不使用物的去除•洗淨· 加工等的領域之去=用石夕製程技術之微細構造體、模製 本發明最好使用^ 等’亦可活用本發明。並且, 【圖式簡單說明】、心諱化學藥品之材料的處理。 〇 第2 裝置的整體構成圖。 的多相流體氣液混合部震置之附有溫度控制機構 第3圖係表示 10 〇 第5圈4系矣-.. 分鐘後之表面粗^:第1例中之於紹表面照射多相流體10 粗輪度的資料之圖。 鐘後表7^第1例中之於鋼表面照射多相流體10分 後之表面粗糙度的資料之圖。 邊二7:2示第3例中之在塗佈於透明晶圓之阻劑- i(a ^ ,, ,L 〜邊從背面以高速攝影機觀測阻劑剝離 喝往的結果之圖。 $ 圖係表示第4例中之因注入高濃度離子後的多相 320816 201023986 ‘ 流體照射所致之阻劑剝離資料的圖。 - 第9圖係表示第5例至第8例的結果之圖。 第10圖係表示第5例至第8例的結果之圖。 第11圖係表示第9例至第10例的結果之圖。 " 第12圖係表示第11例的結果之圖。 - 第13圖係表示第13例的結果之圖。 第14圖係表示第12例的結果之圖。 第15圖⑷至⑴係表示第14例至第16例的結果之圖。 ❹ 第16圖(a)至(f)係表示第17例至第19例的結果之圖。 第17圖⑻至⑴係表示第20例至第22例的結果之圖。 第18圖⑷至⑴係表示第23例至第25例的結果之圖。 第19圖係表示第26例的結果之圖。 第20圖係表示第27例的結果之圖。 第21圖係表示因多相流體之熱能量的不同所引起之 衝擊波的大小變化之圖。 魏 第22圖係表示因多相流體之速度的不同所引起之衝Corrosion of wiring after 10 days of wiring corrosion II Physical damage after processing m _ I Polymer removal | Removal 梛 Removal II Removal I Removal ι Processing conditions 诨趔 f ^ ^ \ σ> 〇〇 TC • •. CD Ό> Liquid/gas mixture ratio 0.010 0.010 0.010 〇 _ 〇〇 0.010 丨Water vapor pressure / MPa 〇CO 〇〇κ ο 〇ο Nozzle object distance /mm to IO ΙΟ u> to 乂 乂 CD CD 〇 cad ο ο5 to cd To o (4)7« Ο TO to 〇E> Ο石ο 〇〇o « Mixed water temperature / XS ο 04 ο CM ss Fluid temperature / 3⁄4 ü in o to o Comparative Example 1 j Comparative Example 2 Comparative Example 3 Comparative Example 4 Comparison Example 201023986 [Industrial use and utilization] The present invention is a process for processing liquid crystals, magnetic heads, magnetic micro-such as 'semiconductor devices, machined parts, moldings=substrates, cameras, etc., precision machine polishing, etc. 2 In the field of removal of unusable materials, cleaning, processing, etc., the fine structure of the stone-making process, molding, and the present invention are preferably used. In addition, [simplified description of the drawings], processing of materials for heart sputum chemicals.整体 The overall structure of the second device. The multi-phase fluid gas-liquid mixing part is attached with a temperature control mechanism. Fig. 3 shows the surface roughness of the 10th ring after 4th 4-.. minutes. A diagram of the data of the fluid 10 coarse wheel. Table 7 of the data of the surface roughness of the steel surface after irradiation of the multiphase fluid for 10 minutes in the first example of the table. Side 2:7:2 shows the result of the stripping agent-i (a ^ , , , L ~ side coated on the transparent wafer in the third example), and the result of peeling off the resist from the back side by a high-speed camera. The figure shows the multi-phase 320816 201023986' of the resist stripping data by fluid irradiation in the fourth example after injecting high-concentration ions. - Figure 9 shows the results of the fifth to eighth examples. Fig. 10 is a view showing the results of the fifth to eighth examples. Fig. 11 is a view showing the results of the ninth to tenth examples. < Fig. 12 is a view showing the results of the eleventh example. Fig. 14 is a view showing the results of the thirteenth example. Fig. 14 is a view showing the results of the twelfth example. Fig. 15 (4) to (1) are diagrams showing the results of the fourteenth to sixteenth examples. a) to (f) are graphs showing the results of the 17th to the 19th examples. Fig. 17 (8) to (1) show the results of the 20th to 22nd examples. Fig. 18 (4) to (1) indicate the 23rd. Fig. 19 is a diagram showing the results of the twenty-sixth example. Fig. 20 is a diagram showing the results of the twenty-seventh example. Fig. 21 is a diagram showing the difference in thermal energy due to the multiphase fluid. Cited The size variation of the shock wave in FIG. FIG. 22 are diagrams Wei vary the speed of a multiphase fluid due to the overshoot
G 擊波的大小變化之圖。 第23圖係表示因多相流體之密度的不同所引起之衝 擊波的大小變化之圖。 第24圖係表示因超音波所致之氣穴現象產生的機制 之圖。 第25圖係表示液滴碰撞時產生之氣穴現象的機制之 圖。 第26圖係表示液滴碰撞時產生之氣穴現象的機制之 45 320816 201023986 圖。 第27圖係表示液滴碰撞時產生之氣穴現象的機制之 圖。 第28圖係表示液滴碰撞時產生之氣穴現象的機制之 圖。 第29圖係表示液滴碰撞時產生之氣穴現象的機制之 機制之圖。 第30圖係表示音速喷嘴及混合部的構造之圖。 第31圖係多相流體溫度的測量裝置之概略圖。 第32圖係多相流體之pH的測量裝置之概略圖。 第33圖係表示氣體壓力與水滴速度的關係之圖。 第34圖係表示氣體壓力與水滴直徑的關係之圖。 第35圖(a)及(b)係表示在英喷嘴内產生之壓力波的情 況之圖。 第36圖(a)及(b)係表示在石英噴嘴内未產生壓力波的 情況之圖。 【主要元件符號說明】 100 對象物處理裝置 111 水供應管 112 蒸氣產生器 113 水蒸氣開關閥 114 壓力計 115 水蒸氣壓力調整閥 附有温度控制機構之加熱蒸氣產生器兼飽和蒸氣 46 320816 116 201023986 ’ 濕度調整器 -117 釋壓閥 121 水供應管 122 附有純水溫度控制機構之加熱部 ^ 123 純水開關閥 124 純水流里計 125 2流體產生用純水開關閥 131 附有水蒸氣流體溫度控制機構之加熱部 ❹ 141 照射喷嘴 142 彈性配管 143 壓力計 144 附有溫度控制功能之多相流體氣液混合部 145 孔口 151 可裝載•保持對象物之基座 152 旋轉馬達 ^ 153 晶圓上下驅動機構 154 冷卻水管 155 冷卻水開關閥 156 冷卻水流量調整閥 157 冷卻水流量計 47 320816G The map of the magnitude of the shock wave. Fig. 23 is a view showing changes in the magnitude of the shock wave due to the difference in density of the multiphase fluid. Figure 24 is a diagram showing the mechanism of cavitation caused by ultrasonic waves. Fig. 25 is a view showing the mechanism of the cavitation phenomenon generated when the droplet collides. Figure 26 is a diagram showing the mechanism of cavitation caused by droplet collisions. 45 320816 201023986 Figure 27 is a diagram showing the mechanism of the cavitation phenomenon generated when a droplet collides. Figure 28 is a diagram showing the mechanism of cavitation generated when a droplet collides. Fig. 29 is a view showing the mechanism of the mechanism of the cavitation phenomenon generated when the liquid droplet collides. Fig. 30 is a view showing the structure of a sonic nozzle and a mixing portion. Figure 31 is a schematic view of a measuring device for the temperature of a multiphase fluid. Figure 32 is a schematic view of a measuring device for the pH of a multiphase fluid. Figure 33 is a graph showing the relationship between gas pressure and water droplet velocity. Figure 34 is a graph showing the relationship between the gas pressure and the diameter of the water droplets. Fig. 35 (a) and (b) are views showing a state of pressure waves generated in the British nozzle. Fig. 36 (a) and (b) are views showing a state in which no pressure wave is generated in the quartz nozzle. [Description of main components] 100 Object processing device 111 Water supply pipe 112 Vapor generator 113 Water vapor switching valve 114 Pressure gauge 115 Water vapor pressure regulating valve with temperature control mechanism heating steam generator and saturated steam 46 320816 116 201023986 'Humidity regulator-117 Pressure relief valve 121 Water supply pipe 122 Heating section with pure water temperature control mechanism ^ 123 Pure water switching valve 124 Pure water flow meter 125 2 Pure water switching valve for fluid generation 131 Water vapor fluid Temperature control unit heating unit 141 141 Irradiation nozzle 142 Elastic piping 143 Pressure gauge 144 Multiphase fluid gas-liquid mixing unit 145 with temperature control function Hole 151 Mounting and holding object pedestal 152 Rotating motor ^ 153 Wafer Upper and lower drive mechanism 154 cooling water pipe 155 cooling water switching valve 156 cooling water flow adjustment valve 157 cooling water flow meter 47 320816
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Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI462148B (en) * | 2013-07-10 | 2014-11-21 | 億力鑫系統科技股份有限公司 | Fluid nozzle and fluid nozzle device |
| CN104415930A (en) * | 2013-09-03 | 2015-03-18 | 亿力鑫系统科技股份有限公司 | Method for cleaning substrate, fluid ejection head and fluid ejection head device |
| TWI579061B (en) * | 2011-02-17 | 2017-04-21 | 水科學股份有限公司 | Serial nozzle and substrate processing apparatus having the series of nozzles |
| CN112535962A (en) * | 2019-09-20 | 2021-03-23 | 三菱电机株式会社 | Processing liquid generating method, processing liquid generating mechanism, semiconductor manufacturing apparatus, and semiconductor manufacturing method |
| US20240190391A1 (en) * | 2022-12-13 | 2024-06-13 | Hyundai Motor Company | Cleaning apparatus |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JP3127251B2 (en) * | 1991-03-08 | 2001-01-22 | 四国化工機株式会社 | Dew condensation prevention device for filling nozzle in filling device |
| JPH10144650A (en) * | 1996-11-11 | 1998-05-29 | Mitsubishi Electric Corp | Semiconductor material cleaning equipment |
| US6332470B1 (en) * | 1997-12-30 | 2001-12-25 | Boris Fishkin | Aerosol substrate cleaner |
| US7451774B2 (en) * | 2000-06-26 | 2008-11-18 | Applied Materials, Inc. | Method and apparatus for wafer cleaning |
| US6586708B1 (en) * | 2001-09-04 | 2003-07-01 | Cusick, Iii Joseph B. | Water vapor cooled nozzle used in the MIG and TIG arc welding process |
| CN2661319Y (en) * | 2003-12-02 | 2004-12-08 | 王宝玉 | Vapor/water atomization shower nozzle for humidifying tobacco leaf |
| TWI252782B (en) * | 2004-08-06 | 2006-04-11 | Univ Nat Cheng Kung | Ultrasonic micro nozzle system |
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- 2008-12-17 TW TW97149103A patent/TWI469832B/en active
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI579061B (en) * | 2011-02-17 | 2017-04-21 | 水科學股份有限公司 | Serial nozzle and substrate processing apparatus having the series of nozzles |
| TWI462148B (en) * | 2013-07-10 | 2014-11-21 | 億力鑫系統科技股份有限公司 | Fluid nozzle and fluid nozzle device |
| CN104415930A (en) * | 2013-09-03 | 2015-03-18 | 亿力鑫系统科技股份有限公司 | Method for cleaning substrate, fluid ejection head and fluid ejection head device |
| CN112535962A (en) * | 2019-09-20 | 2021-03-23 | 三菱电机株式会社 | Processing liquid generating method, processing liquid generating mechanism, semiconductor manufacturing apparatus, and semiconductor manufacturing method |
| US20240190391A1 (en) * | 2022-12-13 | 2024-06-13 | Hyundai Motor Company | Cleaning apparatus |
Also Published As
| Publication number | Publication date |
|---|---|
| TWI469832B (en) | 2015-01-21 |
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