TWI525887B - Air-guiding electrode plate - Google Patents

Air-guiding electrode plate Download PDF

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TWI525887B
TWI525887B TW100141473A TW100141473A TWI525887B TW I525887 B TWI525887 B TW I525887B TW 100141473 A TW100141473 A TW 100141473A TW 100141473 A TW100141473 A TW 100141473A TW I525887 B TWI525887 B TW I525887B
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gas
micropores
conductive material
electrode plate
plasma
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TW100141473A
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TW201320448A (en
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翁敏航
陳威宇
吳奕達
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財團法人金屬工業研究發展中心
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Priority to CN201110406241.2A priority patent/CN103107057B/en
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E60/00Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
    • Y02E60/10Energy storage using batteries

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Description

導氣電極板Gas guiding electrode plate

本發明係關於一種電極板,特別是一種具有導氣及均勻電位分佈之導氣電極板。The present invention relates to an electrode plate, and more particularly to a gas guiding electrode plate having a gas guiding and a uniform potential distribution.

傳統係將電漿製程[例如:電漿輔助化學氣相蒸鍍、電漿輔助蝕刻或電漿高分子等]廣泛應用於各式產業,舉凡薄膜電晶體顯示器廠、太陽能廠或晶圓廠等。Traditionally, plasma processing [eg, plasma-assisted chemical vapor deposition, plasma-assisted etching, or plasma polymer] is widely used in various industries, such as thin-film transistor display plants, solar plants, or fabs. .

以太陽能廠沉積微晶矽質薄膜為例,其係選擇透過電漿增強型化學氣相沉積(plasma enhaced chemical vapor deposition,PECVD)裝置,而於該裝置通入氫氣及矽烷混合氣體,以沉積微晶矽質薄膜。在此之前,係先通入射頻電流使上、下電極之間產生反應所需之電場,以由電場散佈之電子撞擊通入之電漿生成氣體[例如:氬氣],並破壞該氣體原子或分子間之鍵結而形成電漿態,方能使電漿中之自由電子撞擊該氫氣及矽烷所混合之氣體分子,而逐漸離子化該混合氣體分子,以沉積形成微晶矽質薄膜。Taking a microcrystalline enamel film deposited by a solar power plant as an example, a plasma enhaced chemical vapor deposition (PECVD) device is selected, and a hydrogen gas and a decane gas mixture are introduced into the device to deposit micro Crystalline film. Prior to this, the RF current is first applied to generate an electric field required for the reaction between the upper and lower electrodes, so that electrons dispersed by the electric field collide with the plasma generated to generate a gas [for example, argon gas] and destroy the gas atom. Or a bond between the molecules to form a plasma state, so that the free electrons in the plasma collide with the gas molecules mixed by the hydrogen gas and the decane, and gradually ionize the mixed gas molecules to deposit a microcrystalline enamel film.

隨著業界產能及品質要求的不斷提升,係必須改善電漿中離子因電場直線加速作用,而產生離子過度轟擊成膜基板,導致沉積於基板之薄膜出現折曲度過大之現象。更因應成膜基板尺寸的逐漸增大,勢必為了加快沉積薄膜之速率及品質,而相對須提升電漿生成之速度及均勻性。As the industry's production capacity and quality requirements continue to increase, it is necessary to improve the linear acceleration of ions in the plasma due to the electric field, and the ions are excessively bombarded into the film-forming substrate, resulting in excessive bending of the film deposited on the substrate. In response to the gradual increase in the size of the film-forming substrate, it is necessary to increase the speed and uniformity of the plasma generation in order to speed up the rate and quality of the deposited film.

傳統係藉由輸入較高的射頻功率而提高上、下電極的操作頻率,以提升上、下電極間所產生之電場強度,使得電漿生成氣體能於電場中快速解離,達成提高氣體解離率而快速生成電漿態之目的。The traditional method is to increase the operating frequency of the upper and lower electrodes by inputting higher RF power, so as to increase the electric field intensity generated between the upper and lower electrodes, so that the plasma generated gas can be quickly dissociated in the electric field, thereby achieving an improved gas dissociation rate. And the purpose of quickly generating the plasma state.

然而,當該上、下電極之操作頻率逐步提升至正常操作頻率13.56 MHz以上,甚至高達VHF(30~100 MHz)時,係因輸出電磁波的波長逐漸變短,而容易於電極表面產生駐波效應(standing wave effect),迫使在該電極上傳遞之電磁波因其相變化,而導致電場產生起伏變動;甚至,係因此造成上、下電極間的電場分佈不均,而導致上、下電極之電壓不穩,相對影響電漿生成的分佈均勻性,使得沉積後之薄膜恐產生厚薄不一之情形,嚴重降低沉積薄膜之品質及效率。However, when the operating frequency of the upper and lower electrodes is gradually increased to a normal operating frequency of 13.56 MHz or higher, even up to VHF (30 to 100 MHz), the wavelength of the output electromagnetic wave is gradually shortened, and a standing wave is easily generated on the surface of the electrode. The standing wave effect forces the electromagnetic wave transmitted on the electrode to change due to its phase, which causes the electric field to fluctuate; even, the electric field distribution between the upper and lower electrodes is uneven, resulting in the upper and lower electrodes. The voltage is unstable, which affects the distribution uniformity of plasma generation, which makes the film after deposition cause different thickness, which seriously reduces the quality and efficiency of the deposited film.

請參照第1圖所示,如中華民國公告第M342906號專利案,其係揭示一種具有均勻電場分佈之電極9,係包含一電極片91,以及對應蝕刻於該電極片91四邊之微擾槽孔92,以由該微擾槽孔92控制該電極片91邊緣上的電場強度分布,藉此提升電漿生成之均勻度。Please refer to FIG. 1 , for example, the Patent No. M342906 of the Republic of China, which discloses an electrode 9 having a uniform electric field distribution, comprising an electrode sheet 91 and correspondingly etched into the four sides of the electrode sheet 91. The hole 92 controls the electric field intensity distribution on the edge of the electrode sheet 91 by the perturbation slot 92, thereby increasing the uniformity of plasma generation.

該習知電極9雖能避免如上述因高頻作用產生駐波效應,而具有穩定電漿生成均勻度之功效。惟,該習知電極9卻始終解決不了電漿中離子因電場直線加速作用,而產生離子過度轟擊成膜基板,導致沉積於基板之薄膜出現折曲度過大之現象,使得沉積後的薄膜品質堪慮。Although the conventional electrode 9 can avoid the standing wave effect due to the high frequency action as described above, it has the effect of stabilizing the plasma generation uniformity. However, the conventional electrode 9 can not solve the problem that the ions in the plasma are linearly accelerated by the electric field, and the ions are excessively bombarded into the film-forming substrate, so that the film deposited on the substrate is excessively bent, so that the quality of the film after deposition is obtained. Worry.

此外,若將該習知電極9應用於上述任一種電漿生成裝置時,係必須同時另搭配一氣體分散板,以於該電極9生成電漿後,自該氣體分散板通入欲沉積薄膜之氣體,方能使氣體均勻分散於該電極9所生成之電場中,完成自由電子撞擊而導致氣體離子化,以沉積薄膜之作業。 In addition, when the conventional electrode 9 is applied to any of the above-mentioned plasma generating devices, it is necessary to simultaneously mix a gas dispersing plate to allow the film to be deposited from the gas dispersing plate after the electrode 9 is plasma-generated. The gas can uniformly disperse the gas in the electric field generated by the electrode 9, and complete the collision of the free electrons to cause ionization of the gas to deposit the film.

如此,不僅需耗費額外成本及時間加裝該氣體分散板,更受限於該氣體分散板設置所需之空間,而導致該習知電極9僅能適用於大型電漿生成裝置,相對降低該習知電極9之應用性。甚至,該習知電極9用於小型電漿生成裝置時,儘管欲沉積薄膜之氣體可以經由數微擾槽孔92通入電極片91之間,卻始終因數微擾槽孔92設置於側邊之特性,而無法徹底達到氣體均勻分散之效果,更可能因此造成氣體離子化不完全,而嚴重影響成膜之品質。 In this way, it is not only necessary to add the cost and time to install the gas dispersion plate, but also more limited to the space required for the gas dispersion plate to be disposed, so that the conventional electrode 9 can only be applied to a large plasma generation device, and the relative reduction is relatively low. The applicability of the electrode 9 is known. Even when the conventional electrode 9 is used in a small plasma generating device, although the gas to be deposited may pass between the electrode sheets 91 via the number of perturbation slots 92, the perturbation slot 92 is always disposed on the side. The characteristics, but can not completely achieve the effect of uniform gas dispersion, it is more likely to cause incomplete gas ionization, and seriously affect the quality of film formation.

有鑑於此,確實有必要發展一種供氣體直接通過而散佈於電場中之導氣電極板,且同時於該導氣電極板具有電位之均勻分佈,以解決如上所述之各種問題。 In view of this, it is indeed necessary to develop a gas guiding electrode plate in which a gas is directly passed through and dispersed in an electric field, and at the same time, the gas guiding electrode plate has a uniform distribution of electric potential to solve various problems as described above.

本發明主要目的乃改善上述目的,以提供一種導氣電極板,其係能夠供氣體均勻散佈於電極間,且同時維持電極上之電位均勻性,以確保電漿生成之均勻度且提升沉積薄膜之良率者。 SUMMARY OF THE INVENTION The main object of the present invention is to improve the above object to provide a gas guiding electrode plate capable of uniformly distributing a gas between electrodes while maintaining potential uniformity on the electrode to ensure plasma uniformity and to enhance deposited film. The rate of success.

本發明次一目的係提供一種導氣電極板,係能夠有效降低電漿中離子過度轟擊之現象,以穩定沉積後的薄膜折曲度,而產出高品質薄膜者。 The second object of the present invention is to provide a gas guiding electrode plate which can effectively reduce the phenomenon of excessive ion bombardment in the plasma to stabilize the film folding degree after deposition, and to produce a high quality film.

為達到前述發明目的,本發明之導氣電極板,係包含:一導通材,係具有一導接部,該導通材係形成一第一表面及一第二表面;及數微孔,係貫穿該導通材,該導通材的長邊中線為一基準線,該數微孔係依據該基準線呈對 稱之分佈型態,且該數微孔於該導通材之分佈係符合下列關係式:0.35≧Ao/A≧0.045,其中,Ao係為該數微孔於該第一表面或該第二表面之透氣面積總和,A係為該導通材之面積。 In order to achieve the above object, the gas guiding electrode plate of the present invention comprises: a conducting material having a guiding portion, the conducting material forming a first surface and a second surface; and a plurality of micropores running through The conductive material, the long-side center line of the conductive material is a reference line, the number of micro-holes is symmetrically distributed according to the reference line, and the distribution of the number of micro-holes in the conductive material conforms to the following relationship: 0.35≧A o /A≧0.045, wherein A o is the sum of the gas permeable areas of the number of micropores on the first surface or the second surface, and A is the area of the conductive material.

其中,該數微孔係皆為圓孔,且具有相同之徑寬,各該微孔之徑寬係為0.5~1毫米,該數微孔之透氣面積總和Ao係為(R×π×ψ2)/4,其中R為該數微孔之數量,ψ為該數微孔之徑寬。 Wherein the number of pores are both circular line, the diameter and having the same width, the line width of each pore diameter of 0.5 to 1 mm, the total number of pores of the gas permeable area of lines A o (R × π × ψ 2 )/4, where R is the number of micropores and ψ is the diameter of the micropores.

本發明之導通材於該第一表面及第二表面還可以另設有一保護層,且該數微孔係貫穿該等保護層,該等保護層係用以抵抗腐蝕性氣體。其中,該等保護層係選自由氧化釔、稀土類元素之氧化物或聚醯亞胺系樹脂之其一所形成之薄膜。 The conductive material of the present invention may further be provided with a protective layer on the first surface and the second surface, and the plurality of micropores penetrate through the protective layers, and the protective layers are used to resist corrosive gases. The protective layer is selected from the group consisting of ruthenium oxide, an oxide of a rare earth element, or a polyimide resin.

其中,該數微孔特別係可以呈輻射狀、同心圓或矩陣式之分佈型態。 The plurality of micropores may be in a radial, concentric or matrix distribution.

其中,該導通材係選自鋁、鋁合金、不鏽鋼、無氧銅、被覆鋁、矽、石英、碳化矽、氮化矽、藍寶石、聚醯亞胺或鐵氟龍之其一。且,該導通材之形狀係為方形、圓形、六角形或多邊形。 Wherein, the conductive material is selected from the group consisting of aluminum, aluminum alloy, stainless steel, oxygen-free copper, coated aluminum, tantalum, quartz, tantalum carbide, tantalum nitride, sapphire, polyimine or Teflon. Moreover, the shape of the conductive material is square, circular, hexagonal or polygonal.

為讓本發明之上述及其他目的、特徵及優點能更明顯易懂,下文特舉本發明之較佳實施例,並配合所附圖式,作詳細說明如下:請參照第2圖所示,其係為本發明一較佳實施例,該 導氣電極板係包含一導通材1及數微孔2,該數微孔2係貫穿該導通材1。藉此,係能由該數微孔2改變該導通材1的內部結構,以避免因高頻輸入而於該導通材1產生駐波效應,配合參照第2~4圖,詳述於下。 The above and other objects, features and advantages of the present invention will become more <RTIgt; It is a preferred embodiment of the present invention, and The gas guiding electrode plate comprises a conductive material 1 and a plurality of micropores 2, and the micropores 2 penetrate the conductive material 1. Thereby, the internal structure of the conductive material 1 can be changed by the number of micropores 2 to avoid the standing wave effect on the conductive material 1 due to the high frequency input, and it will be described in detail below with reference to FIGS. 2 to 4.

該導通材1係可以選擇由鋁、鋁合金、不鏽鋼、無氧銅、被覆鋁、矽、石英、碳化矽、氮化矽、藍寶石、聚醯亞胺或鐵氟龍等其一具導通性質之材料,以構成如方形、圓形、六角形或多邊形之平面板狀物。 The conductive material 1 can be selected from aluminum, aluminum alloy, stainless steel, oxygen-free copper, coated aluminum, tantalum, quartz, tantalum carbide, tantalum nitride, sapphire, polythenimine or Teflon. Material to form a planar plate such as a square, circle, hexagon or polygon.

請再參照第2圖所示,該導通材1係具有一導接部11,該導接部11係設於該導通材1之周壁,用以連接一射頻電流(Radio Frequency,RF),且該導接部11特別係可以選擇採單邊或環繞狀之設置,以穩定提供射頻電流於該導通材1為主要原則,係為熟習該技藝之人士所能輕易理解,於此較佳係以環繞設置於該導通材1周壁之導接部11〔詳如第2圖所示〕為本發明較佳實施例。 Referring to FIG. 2 again, the conductive material 1 has a guiding portion 11 which is disposed on the peripheral wall of the conductive material 1 for connecting a radio frequency (RF), and The guiding portion 11 can be selected from a single side or a surrounding shape to stabilize the supply of radio frequency current to the conductive material 1 as a main principle, which can be easily understood by those skilled in the art. The guiding portion 11 (shown in detail in Fig. 2) disposed around the peripheral wall of the conductive material 1 is a preferred embodiment of the present invention.

特別的是,請續參照第3圖所示,該導通材1係形成一第一表面12〔即如第3圖所示之上表面〕及一第二表面13〔即如第3圖所示之下表面〕,該第一表面12及第二表面13皆設有一保護層14,該保護層14係用以抵抗腐蝕性氣體,以避免氣體長時間接觸電極表面,而因氣體腐蝕降低電極之使用壽命。其中,該保護層14係可以選擇由塗佈等披覆方式成型一薄膜,且較佳係選擇為氧化釔、稀土類元素之氧化物或聚醯亞胺系樹脂等耐蝕性材料。 In particular, referring to FIG. 3, the conductive material 1 forms a first surface 12 (ie, the upper surface as shown in FIG. 3) and a second surface 13 (ie, as shown in FIG. 3). The lower surface of the first surface 12 and the second surface 13 are provided with a protective layer 14 for resisting corrosive gases to prevent gas from contacting the electrode surface for a long time, and reducing the electrode due to gas corrosion. Service life. Here, the protective layer 14 may be selected from a film such as coating or the like, and is preferably selected from a corrosion-resistant material such as cerium oxide, an oxide of a rare earth element, or a polyimide resin.

請配合參照第2及3圖所示,該數微孔2係貫穿該導通材1,特別係由該導通材1的第一表面12成型而貫穿至 該導通材1的第二表面13,尤其當該第一表面12及第二表面13皆設有該保護層14時,係同時貫穿該保護層14,以供氣體能自該數微孔2通過為較佳原則。該數微孔2於該導通材1之設置分佈情形,特別係指該數微孔2於第一表面12或第二表面13所形成之透氣面積〔即該數微孔2於第一表面12所形成之開口的面積總和,與導通材1第一表面12之面積對應關係,或者係該數微孔2於第二表面所形成之開口的面積總和,與導通材1第二表面13之面積對應關係〕,係符合下列關係式:0.35≧Ao/A≧0.045,其中Ao係為該數微孔2之透氣面積之總和,A係為該導通材1之面積,特別係指該導通材1之第一表面12或第二表面13的面積。舉例而言,該數微孔2係皆為圓孔,且具有相同之徑寬ψ,該數微孔2於第一表面12或第二表面13所形成之透氣面積總和Ao即為R×π×ψ2/4,其中R為該數微孔2之數量,藉以因應不同徑寬ψ之微孔2設計,而具有較佳的微孔分佈數量R,用以於該導通材1面積A上呈現較佳的數微孔2分佈態樣。 Referring to the second and third figures, the number of micropores 2 penetrates through the conductive material 1, and is particularly formed by the first surface 12 of the conductive material 1 and penetrates through the second surface 13 of the conductive material 1, in particular When the first surface 12 and the second surface 13 are provided with the protective layer 14, it is a preferred principle to simultaneously penetrate the protective layer 14 for gas to pass through the micropores 2. The distribution of the number of micropores 2 in the conductive material 1 , in particular, the gas permeable area formed by the micropores 2 on the first surface 12 or the second surface 13 (ie, the number of micropores 2 on the first surface 12 ) The sum of the areas of the openings formed corresponds to the area of the first surface 12 of the conductive material 1, or the sum of the areas of the openings formed by the number of micro holes 2 on the second surface, and the area of the second surface 13 of the conductive material 1. Corresponding relationship], the following relationship is satisfied: 0.35≧A o /A≧0.045, where A o is the sum of the gas permeable areas of the number of micropores 2, and A is the area of the conductive material 1 , especially the conduction The area of the first surface 12 or the second surface 13 of the material 1. For example, the number of micropores 2 system are all circular and have the same radial dimension of [Psi], the number of micropores 2 in a first breathable surface area formed by the sum of A 12 or the second surface 13 o is the R × π×ψ 2 /4, where R is the number of the micropores 2, so that the micropore 2 design with different diameters and widths is provided, and the preferred number of micropores R is used for the area A of the conductive material 1 A preferred number of microporous 2 distributions are presented.

值得注意的是,該數微孔2係可以為對稱或非對稱之分佈型態〔即以第4a~4c圖所示之導通材1長邊中線為一基準線L,使得該數微孔2係依據該基準線L呈左、右對稱或非對稱之型態〕,平均散佈於該導通材1之第一表面12及第二表面13,並貫穿該導通材1,特別係可以呈輻射狀、同心圓或矩陣式之分佈〔詳見第4a~4c圖所示〕,且以符合上述0.35≧Ao/A≧0.045之關係式為主要原則,而不僅以型態作為限制。其中,以圓形的微孔2為例,各該微 孔2之徑寬ψ尤其係可以選擇為0.5~1毫米,各該微孔2形成一製程氣體流通之路徑,於製程腔體中可提供一較佳之均勻流場,此外,在該導通材1連接一射頻電流後,可於其上形成一均勻電位場,進而形成一均勻電漿場。 It should be noted that the number of micropores 2 can be a symmetric or asymmetric distribution pattern (ie, the long-side center line of the conductive material 1 shown in FIGS. 4a-4c is a reference line L, so that the number of micro-holes 2 is symmetrical or asymmetrical according to the reference line L, and is evenly distributed on the first surface 12 and the second surface 13 of the conductive material 1, and penetrates through the conductive material 1, in particular, can be irradiated The distribution of the shape, concentric circle or matrix type (see the figures 4a to 4c for details), and the relationship between the above-mentioned 0.35≧A o /A≧0.045 is the main principle, and not only the type is restricted. In the case of the circular micropores 2, the diameter ψ of each of the micropores 2 can be selected to be 0.5 to 1 mm, and each of the micropores 2 forms a path for the circulation of the process gas, which can be in the process chamber. A preferred uniform flow field is provided. Further, after the conductive material 1 is connected to an RF current, a uniform potential field can be formed thereon to form a uniform plasma field.

舉例而言,本實施例係以長425毫米(mm)、寬425毫米之矩型鋁板作為導通材1,並選擇於該導通材1之第一表面12開設徑寬為1毫米的數微孔2,使得該數微孔2之透氣面積總和與導通材1之第一表面12面積的比值為0.12,同時該數微孔2更可以呈矩陣狀之型態平均散佈於該導通材1之第一表面12,且貫穿至該導通材1之第二表面13,以完成本發明導氣電極板之設計。如第6圖所示,其係為該數微孔2於第一表面12開設徑寬為1毫米,而該數微孔2之透氣面積總和與導通材1之第一表面12面積的比值為0.12時,所得之電位場分佈模擬分析結果。 For example, in this embodiment, a rectangular aluminum plate having a length of 425 millimeters (mm) and a width of 425 mm is used as the conductive material 1, and a plurality of micropores having a diameter of 1 mm are selected on the first surface 12 of the conductive material 1. 2, the ratio of the sum of the gas permeable areas of the number of micropores 2 to the area of the first surface 12 of the conductive material 1 is 0.12, and the number of micropores 2 can be evenly distributed in a matrix form on the conductive material 1 A surface 12 extends through the second surface 13 of the conductive material 1 to complete the design of the gas guiding electrode plate of the present invention. As shown in FIG. 6, the micropores 2 have a diameter of 1 mm on the first surface 12, and the ratio of the sum of the gas permeable areas of the micropores 2 to the area of the first surface 12 of the conductive material 1 is At 0.12, the obtained potential field distribution is simulated and analyzed.

本發明導氣電極板較佳係可以應用於常壓化學氣相沉積〔APCVD〕、低壓化學氣相沉積〔LPCVD〕、高密度電漿化學氣相沉積〔HDPCVD〕、電將輔助化學氣相沉積〔PECVD〕、感應耦合電漿離子蝕刻〔ICP〕等系統,藉以控制各種化學氣相沉積系統或電漿蝕刻系統於操作過程的電漿生成密度及均勻性。 The gas guiding electrode plate of the invention can be preferably applied to atmospheric pressure chemical vapor deposition (APCVD), low pressure chemical vapor deposition (LPCVD), high density plasma chemical vapor deposition (HDPCVD), electric auxiliary chemical vapor deposition. [PECVD], inductively coupled plasma ion etching (ICP) and other systems to control the plasma generation density and uniformity of various chemical vapor deposition systems or plasma etching systems during operation.

請參照第5圖所示,其係選擇以電漿輔助化學氣相沉積裝置為例,將本發明導氣電極板裝設於一電漿箱3之腔室31內,以作為該電漿輔助化學氣相沉積裝置之上電極〔即指第5圖圖面上方之電極板P1〕,並相對於該上電極另設有一下電極〔即指第5圖圖面下方之電極板P2〕,該 上、下電極皆分別導接於一射頻電流供應器R,以輸出射頻電流至該上、下電極,且控制該射頻電流之較佳操作頻率為1KHz~100MHz。 Referring to FIG. 5, the plasma-assisted chemical vapor deposition apparatus is selected as an example, and the gas guiding electrode plate of the present invention is installed in a chamber 31 of a plasma box 3 to serve as the plasma auxiliary. The upper electrode of the chemical vapor deposition device (that is, the electrode plate P1 above the surface of FIG. 5), and the lower electrode is further provided with a lower electrode (ie, the electrode plate P2 below the surface of FIG. 5). The upper and lower electrodes are respectively connected to an RF current supply R to output a radio frequency current to the upper and lower electrodes, and a preferred operating frequency for controlling the RF current is 1 kHz to 100 MHz.

如此,射頻電流流通於該上電極時,係因該上電極平均散佈之數微孔2設計,而阻卻電磁波推進發生駐波效應的可能性,故可以於該上、下電極間產生反應所需之均勻電場,而使該上、下電極間具有均勻之電位分佈,當通入一電漿生成氣體〔例如:氬氣、氮氣、氫氣…等〕於該腔室31內,以透過該電場中存在之電子撞擊該電漿生成氣體時,係能全面性地破壞該電漿生成氣體原子或分子間之鍵結而快速產生解離效應,以於該上、下電極間生成具有均勻分佈密度之電漿態氣體。接著,供一成膜氣體〔例如:矽烷、乙矽烷、丙矽烷…等〕自一進氣口32導入該腔室31內時,特別係透過該上電極之數微孔2直接使該成膜氣體通入該腔室31,且能夠均勻散佈於該上、下電極之間,而藉由電漿中均勻散佈之自由電子轟擊該成膜氣體,而逐漸離子化該成膜氣體,以於一成膜基板33表面形成薄膜沉積之作業。 In this way, when the RF current flows through the upper electrode, the number of micropores 2 that are evenly distributed by the upper electrode is designed to block the possibility of the standing wave effect caused by the electromagnetic wave propulsion, so that a reaction chamber can be generated between the upper and lower electrodes. A uniform electric field is required to have a uniform potential distribution between the upper and lower electrodes, and a plasma generating gas (for example, argon, nitrogen, hydrogen, etc.) is introduced into the chamber 31 to transmit the electric field. When the electrons present in the plasma strike the plasma generating gas, the system can completely destroy the bonding between the plasma generating gas atoms or molecules and rapidly generate a dissociation effect to generate a uniform distribution density between the upper and lower electrodes. Plasma gas. Next, when a film forming gas (for example, decane, acetane, propane, etc.) is introduced into the chamber 31 from an air inlet 32, the film is directly formed through the micropores 2 of the upper electrode. The gas is introduced into the chamber 31, and can be evenly dispersed between the upper and lower electrodes, and the film forming gas is bombarded by free electrons uniformly dispersed in the plasma, thereby gradually ionizing the film forming gas. The surface of the film formation substrate 33 forms a film deposition operation.

綜上所述,本發明導氣電極板之主要特徵在於:利用該數微孔2散佈且貫穿該導通材1之設計,係能改變該導通材1的內部結構,而於高頻電流通過該導通材1時,不僅可以降低電漿鞘層〔Plasma sheath〕之電位,避免電漿中離子因電場直線加速作用,而產生離子過度轟擊成膜基板之現象,使得沉積於基板的薄膜折曲度維持於較佳之範圍;甚至,更可以避免因高頻電流輸出的短波電磁波所產 生之駐波效應,而降低電極間可能引起的電場起伏或變動,相對提高電極間的電壓、電位分佈均勻性,以穩定作動過程的電漿生成均勻度,達到維持薄膜厚度均一性且提升成膜品質及效率之功效。 In summary, the main feature of the gas guiding electrode plate of the present invention is that the internal structure of the conductive material 1 can be changed by using the number of micropores 2 dispersed and penetrating through the conductive material 1, and the high frequency current passes through the When the conductive material 1 is used, not only the potential of the plasma sheath can be lowered, but also the phenomenon that the ions in the plasma are linearly accelerated by the electric field, and the ions are excessively bombarded with the film-forming substrate, so that the film is bent on the substrate. Maintained in a better range; even, it can avoid the production of short-wave electromagnetic waves due to high-frequency current output. The standing wave effect of the raw material reduces the fluctuation or variation of the electric field caused by the electrodes, relatively increases the voltage and potential distribution between the electrodes, and uniformizes the plasma generation during the stable operation process, thereby maintaining the uniformity of the film thickness and improving Membrane quality and efficiency.

除此之外,於後續通入成膜氣體時,係可以直接使成膜氣體通過該數微孔2而均勻散佈於電極間,不僅無需耗費額外成本及時間加裝該氣體分散板,更不會受限於該氣體分散板設置所需之空間,而能夠有效提升本發明之應用性;甚至,透過數微孔2之設計徹底達到成膜氣體均勻分散之效果,以於電漿中自由電子的轟擊下,達到全面性離子化成膜氣體之功效,而產出較高品質之薄膜。 In addition, when the film forming gas is subsequently introduced, the film forming gas can be directly dispersed between the electrodes through the micropores 2, and the gas dispersing plate is not required to be added at a cost and time. It is limited by the space required for the gas dispersing plate setting, and can effectively improve the applicability of the present invention; even, the design of the micropores 2 can completely achieve the effect of uniform dispersion of the film forming gas, and free electrons in the plasma. Under the bombardment, the effect of comprehensive ionized film forming gas is achieved, and a higher quality film is produced.

本發明導氣電極板係能夠供氣體均勻散佈於電極間,且同時維持電極上之電位均勻性,以確保電漿生成之均勻度,達到提升沉積薄膜良率之功效。 The gas guiding electrode plate of the invention can uniformly distribute the gas between the electrodes, and at the same time maintain the potential uniformity on the electrode to ensure the uniformity of plasma generation and achieve the effect of improving the yield of the deposited film.

本發明導氣電極板係能夠有效降低電漿中離子過度轟擊之現象,以穩定沉積後的薄膜折曲度,而達到產出高品質薄膜之功效。 The gas guiding electrode plate of the invention can effectively reduce the phenomenon of excessive ion bombardment in the plasma, so as to stabilize the film bending degree after deposition, and achieve the effect of producing a high quality film.

雖然本發明已利用上述較佳實施例揭示,然其並非用以限定本發明,任何熟習此技藝者在不脫離本發明之精神和範圍之內,相對上述實施例進行各種更動與修改仍屬本發明所保護之技術範疇,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。 While the invention has been described in connection with the preferred embodiments described above, it is not intended to limit the scope of the invention. The technical scope of the invention is protected, and therefore the scope of the invention is defined by the scope of the appended claims.

〔本發明〕 〔this invention〕

1‧‧‧導通材 1‧‧‧Connecting materials

11‧‧‧導接部 11‧‧‧Guidance

12‧‧‧第一表面 12‧‧‧ first surface

13‧‧‧第二表面 13‧‧‧ second surface

14‧‧‧保護層 14‧‧‧Protective layer

2‧‧‧微孔 2‧‧‧Micropores

3‧‧‧電漿箱 3‧‧‧The plasma box

31‧‧‧腔室 31‧‧‧ chamber

32‧‧‧進氣口 32‧‧‧air inlet

P1、P2‧‧‧上電極板 P1, P2‧‧‧ upper electrode plate

R‧‧‧射頻電流供應器 R‧‧‧RF current supply

L‧‧‧基準線 L‧‧‧ baseline

〔習知〕 [study]

9‧‧‧電極 9‧‧‧Electrode

91‧‧‧電極片 91‧‧‧electrode

92‧‧‧微擾槽孔 92‧‧‧Missing slot

第1圖:習知電極板之立體示意圖。 Figure 1: A schematic view of a conventional electrode plate.

第2圖:本發明導氣電極板之立體示意圖。 Fig. 2 is a perspective view showing the gas guiding electrode plate of the present invention.

第3圖:本發明導氣電極板之剖面示意圖。 Fig. 3 is a schematic cross-sectional view showing a gas guiding electrode plate of the present invention.

第4a~4c圖:本發明導氣電極板之數微孔不同態樣之分佈圖。 4a-4c: a distribution diagram of different micropores of the gas guiding electrode plate of the present invention.

第5圖:本發明導氣電極板之應用示意圖。 Fig. 5 is a schematic view showing the application of the gas guiding electrode plate of the present invention.

第6圖:本發明導氣電極板之電位場分佈模擬分析圖。 Figure 6: Simulation analysis of the potential field distribution of the gas guiding electrode plate of the present invention.

1...導通材1. . . Conductive material

11...導接部11. . . Guide

12...第一表面12. . . First surface

13...第二表面13. . . Second surface

14...保護層14. . . The protective layer

2...微孔2. . . Microporous

Claims (6)

一種導氣電極板,係包含:一導通材,係具有一導接部,該導通材係形成一第一表面及一第二表面;及數微孔,係貫穿該導通材,該導通材的長邊中線為一基準線,該數微孔係依據該基準線呈對稱之分佈型態,且該數微孔於該導通材之分佈係符合下列關係式:0.35≧Ao/A≧0.045其中,Ao係為該數微孔於該第一表面或該第二表面之透氣面積總和,A係為該導通材之面積;其中,該數微孔係皆為圓孔,且具有相同之徑寬,各該微孔之徑寬係為0.5~1毫米,該數微孔之透氣面積總和Ao係為(R×π×ψ2)/4,其中R為該數微孔之數量,ψ為該數微孔之徑寬。 A conductive gas electrode plate comprising: a conductive material having a guiding portion, the conductive material forming a first surface and a second surface; and a plurality of micropores extending through the conductive material, the conductive material The long-side center line is a reference line, and the number of micro-holes is symmetrically distributed according to the reference line, and the distribution of the number of micro-holes in the conductive material conforms to the following relationship: 0.35≧A o /A≧0.045 Wherein, A o is the sum of the gas permeable areas of the plurality of micropores on the first surface or the second surface, and A is the area of the conductive material; wherein the plurality of micropores are round holes and have the same lane widths, each of the radial dimension of the microporous system is from 0.5 to 1 mm, the number of air-permeable microporous system is sum of the areas A o (R × π × ψ 2) / 4, where R is the number of the number of micropores, ψ is the diameter of the number of micropores. 依申請專利範圍第1項所述之具導氣電極板,其中,該第一表面及第二表面皆設有一保護層,且該數微孔係貫穿該等保護層,該等保護層係用以抵抗腐蝕性氣體。 The gas guide electrode plate according to the first aspect of the invention, wherein the first surface and the second surface are provided with a protective layer, and the plurality of micropores penetrate through the protective layers, and the protective layers are used To resist corrosive gases. 依申請專利範圍第2項所述之導氣電極板,其中,該等保護層係選自由氧化釔、稀土類元素之氧化物或聚醯亞胺系樹脂之其一所形成之薄膜。 The gas-conducting electrode plate according to the second aspect of the invention, wherein the protective layer is selected from the group consisting of a film of cerium oxide, an oxide of a rare earth element or a polyimide resin. 依申請專利範圍第1或2項所述之導氣電極板,其中,該數微孔係呈輻射狀、同心圓或矩陣式之分佈型態。 The gas guiding electrode plate according to claim 1 or 2, wherein the plurality of micropores are in a radial, concentric or matrix distribution. 依申請專利範圍第1項所述之導氣電極板,其中,該導通材係選自鋁、鋁合金、不鏽鋼、無氧銅、被覆鋁、矽、 石英、碳化矽、氮化矽、藍寶石、聚醯亞胺或鐵氟龍之其一。 The gas guiding electrode plate according to claim 1, wherein the conducting material is selected from the group consisting of aluminum, aluminum alloy, stainless steel, oxygen-free copper, coated aluminum, tantalum, One of quartz, tantalum carbide, tantalum nitride, sapphire, polythenimine or Teflon. 依申請專利範圍第1或2項所述之導氣電極板,其中,該導接部係設於該導通材之周壁,用以連接一射頻電流。 The gas guiding electrode plate according to claim 1 or 2, wherein the guiding portion is disposed on a peripheral wall of the conductive material for connecting an RF current.
TW100141473A 2011-11-14 2011-11-14 Air-guiding electrode plate TWI525887B (en)

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TW100141473A TWI525887B (en) 2011-11-14 2011-11-14 Air-guiding electrode plate
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