TWI224345B - Ion coil and ion metal plasma physical vapor deposition equipment for improving deposition film uniformity of semiconductor chip - Google Patents
Ion coil and ion metal plasma physical vapor deposition equipment for improving deposition film uniformity of semiconductor chip Download PDFInfo
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- TWI224345B TWI224345B TW92115354A TW92115354A TWI224345B TW I224345 B TWI224345 B TW I224345B TW 92115354 A TW92115354 A TW 92115354A TW 92115354 A TW92115354 A TW 92115354A TW I224345 B TWI224345 B TW I224345B
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- 239000002184 metal Substances 0.000 title claims abstract description 30
- 229910052751 metal Inorganic materials 0.000 title claims abstract description 30
- 239000004065 semiconductor Substances 0.000 title claims abstract description 25
- 238000000151 deposition Methods 0.000 title claims abstract description 17
- 230000008021 deposition Effects 0.000 title claims abstract description 17
- 238000005240 physical vapour deposition Methods 0.000 title claims abstract description 17
- 239000000463 material Substances 0.000 claims description 3
- 239000002002 slurry Substances 0.000 claims description 3
- 235000012431 wafers Nutrition 0.000 claims 6
- 239000013078 crystal Substances 0.000 claims 5
- 238000012986 modification Methods 0.000 claims 5
- 230000004048 modification Effects 0.000 claims 5
- 239000012528 membrane Substances 0.000 claims 3
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 claims 2
- 239000010931 gold Substances 0.000 claims 2
- 229910052737 gold Inorganic materials 0.000 claims 2
- 239000004020 conductor Substances 0.000 claims 1
- 230000005611 electricity Effects 0.000 claims 1
- 239000000126 substance Substances 0.000 claims 1
- 150000002500 ions Chemical class 0.000 description 32
- 239000010408 film Substances 0.000 description 17
- 238000000034 method Methods 0.000 description 12
- 238000009826 distribution Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 3
- 239000010409 thin film Substances 0.000 description 3
- 238000000427 thin-film deposition Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 2
- 229910021645 metal ion Inorganic materials 0.000 description 2
- 239000012071 phase Substances 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 239000012808 vapor phase Substances 0.000 description 2
- 230000010485 coping Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000010985 leather Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000008267 milk Substances 0.000 description 1
- 210000004080 milk Anatomy 0.000 description 1
- 235000013336 milk Nutrition 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N rhenium atom Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 238000005728 strengthening Methods 0.000 description 1
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- Physical Vapour Deposition (AREA)
Abstract
Description
1224345 五、發明說明(1) 發明所屬之技術領域 本發明係有關於一種改善半導體晶片沉積薄膜均勻度 之電離子線圈,使用於離子金屬電漿物理氣相沉積設備, 特別係有關一種藉由在該線圈兩端邊緣設置幾何形狀傾 斜,而使該線圈主體投影在該半導體晶片表面上為一封閉 的環形之電離子線圈,該電離子線圈在其間隙亦能有效提 供薄膜沉積所需電磁力,因而可以改善半導體晶片所沉積 薄膜之均勻度。 先前技術 離子金屬電漿物理氣相沉積設備係使用於離子金屬電 漿物理氣相沉積製程,如第1圖所示,為習知之離子金屬 電漿物理氣相沉積設備1,包含有一真空艙11,一電離子 線圈1 2,一高頻交流電壓裝置1 3,一金屬靶1 4,一半導體 晶片承座1 5,此承座上放置半導體晶片;此習知離子金屬 電漿物理氣相沉積設備不同於一般物理氣相沉積設備之處 主要是多了此一電離子線圈12,其設於此一真空艙11内且 位於此一金屬靶1 4與此一半導體晶片承座1 5之間,並使用 與金屬靶1 4相同的材質,在離子金屬電漿物理氣相沉積製 程中,由此一高頻交流電壓裝置1 3施加於電離子線圈1 2之 上,可增加此一真空艙1 1内氣體與此一金屬靶1 4所打下的 金屬原子間有更多碰撞機會,誘導更多金屬離子化帶電, 而使該等帶電之金屬離子在半導體晶片形成之金屬薄膜具 有較佳的填洞能力。1224345 V. Description of the invention (1) Technical field to which the invention belongs The present invention relates to an electric ion coil for improving the uniformity of a semiconductor wafer deposition film, and is used in an ionic metal plasma physical vapor deposition equipment, and particularly relates to an The two ends of the coil are provided with inclined geometric shapes, so that the coil body is projected on the surface of the semiconductor wafer as a closed ring-shaped ion coil, and the ion coil can effectively provide the electromagnetic force required for film deposition in its gap. Therefore, the uniformity of the thin film deposited on the semiconductor wafer can be improved. The prior art ion metal plasma physical vapor deposition equipment is used in the ion metal plasma physical vapor deposition process. As shown in FIG. 1, it is a conventional ion metal plasma physical vapor deposition device 1, which includes a vacuum chamber 11. , An ion coil 12, a high-frequency AC voltage device 13, a metal target 14, a semiconductor wafer holder 15, a semiconductor wafer is placed on this holder; this is known as the physical vapor deposition of ion metal plasma The difference between the equipment and the general physical vapor deposition equipment is that the electric ion coil 12 is mainly provided in the vacuum chamber 11 and located between the metal target 14 and the semiconductor wafer holder 15 And using the same material as the metal target 14 in the ion metal plasma physical vapor deposition process, a high-frequency AC voltage device 13 is applied on the ion coil 12 to increase this vacuum chamber The gas inside 11 has more chances of collision with the metal atoms laid down by this metal target 14 and induces more metal ionization and charging, so that these charged metal ions have better metal film formed on the semiconductor wafer. Ability to fill holes.
0503 -9538twf(nl);tsmc2002-0969;Albert.ptd 第6頁 1224345 五、發明說明(2) 隨著半導體製程演進,元件尺寸愈縮愈小, 沉積均勾的填在整個溝槽壁更為不易,故具=金屬 力的離子金屬電漿物理氣相沉備比一般物^ =洞能 設備更能應付高充填比的需求; 乳相沉積 離子金屬電漿物理氣相沉備因電離 而具有較佳的填洞能力,但也產生另-個問題用 子,圏本身會導致半導體積 ^離 為習知之離子全屬== 爹圖;如圖所示 子線圈12在沉;氣相沉積設備一習知電離 ^ ^ 」輊中由向頻交流電裝置1 3提供交产雷0503 -9538twf (nl); tsmc2002-0969; Albert.ptd Page 6 1224345 V. Description of the invention (2) As the semiconductor process evolves, the component size shrinks and becomes smaller, and the deposition is uniformly filled in the entire trench wall. It is not easy, so the physical vapor deposition of ionic metal plasma with = metal force is more capable of coping with the demand of high filling ratio than the general equipment; the physical vapor deposition of ionized metal plasma with milk phase deposition has the advantages of ionization. Better hole filling ability, but also generates another problem, the rhenium itself will cause the semiconductor ion to be separated from the conventional ions == dad; the sub-coil 12 is sinking as shown in the figure; vapor deposition equipment I ’m familiar with ionization ^ ^ '' 轾 由 由 由 由 by the frequency AC power supply device 1 3
亚弟一^1流電源連結部1 2 1及第二交流電源連^部 122進入此一電離子線圈j 斤運一P 封閉形狀方能構成兩端雷、、A文此電难子、,泉圈1 2必然為非 端之間存在-間^此:回路。非封閉之電料 影在該半導體晶片表面時S隙1 23造成電離子線圈垂直投 體晶片在該環形缺口處附、斤能形成封閉之環形,致使半導 方為薄,而產生晶片沉積;積的薄膜厚度遠較其他地 上述厚度不均勻的情::寻朕厚度不均的問題。 產時良率的主因之—。因;住往超出製程標準,是影響量 隙123所造成薄膜厚度不均何改善此電離子線圈Μ之間 重要課題。 〜9的情形實為生產技術中之一 發明内容 離子金屬電漿物理氣相、_ 、相〉儿積(IMP PVD)設備因電離子Adi 1 ~ 1 current power supply connection part 1 2 1 and second AC power supply connection part 122 enter this electric ion coil j. A P closed shape can form a two-terminal lightning, Spring circle 1 2 must exist between non-ends-this ^ this: loop. When the non-closed electrical material shadow is on the surface of the semiconductor wafer, the S-gap 1 23 causes the ion-ion coil vertical projection wafer to be attached at the annular gap, which can form a closed annular shape, causing the semiconductor to be thin, resulting in wafer deposition; The thickness of the accumulated film is much larger than that of the other thicknesses mentioned above :: Look for the problem of uneven thickness. The main reason for yield during delivery—. The reason is that living beyond the process standard is an important issue between improving the ion coil M and affecting the uneven thickness of the film caused by the gap 123. The case of ~ 9 is really one of the production technologies. SUMMARY OF THE INVENTION The physical vapor phase of ionic metal plasma, _, phase> Ion PVD (IMP PVD) equipment due to electric ions
0503-9538twf(nl);tsmc2002-0969;Albert.ptd0503-9538twf (nl); tsmc2002-0969; Albert.ptd
1224345 五、發明說明(3) 線圈的使用而具有比一般物理氣相設備更好的向下填洞能 力,但因為電離子線圈形狀上有一間隙,造成在間隙處沒 有電離子線圈提供電磁力而導致此處沉積厚度不足,影響 整體薄膜沉積厚度不均勻,往往是影響製程良率的主要原 因之一,有鑑於此,本發明提供一種電離子線圈的設計方 式,此方式是藉由在電離子線圈兩端邊緣設置幾何形狀傾 斜,如此一來該線圈主體投影在該半導體晶片表面為一封 閉之環形,而使線圈在間隙亦能有效提供薄膜沉積所需電 磁力。由此方式所設計之複數種電離子線圈均能有效提高 半導體晶片沉積薄膜的均勻度。 為了讓本發明之上述目的、特徵、和優點能更明顯易 懂,下文特舉數個較佳實施例,並配合所附圖示,作詳細 說明如下: ^ 實施方式 本發明提出一種電離子線圈係藉由在該線圈兩端邊緣 設置幾何形狀傾斜而達成提高薄膜均勻度之目的,以下列 舉本發明幾個較佳之實施例加以說明。 第一實施例: 為明顯區別本發明之第一實施例與傳統技術之差異, 茲分別說明第2a圖及第2 b圖之傳統電離子線圈與第3a圖及 第3 b圖之第一實施例,以進行比較。傳統電離子線圈之上 視圖如第2 a圖所示,側視圖如第2 b圖所示,該線圈包括一 線圈主體2,為一長條形狀而具有一第一端部以及一第二1224345 V. Description of the invention (3) The use of coils has a better ability to fill holes down than ordinary physical vapor phase equipment, but because of the gap in the shape of the ion coil, there is no electromagnetic force provided by the ion coil at the gap. Insufficient deposition thickness here, affecting the uneven thickness of the overall thin film deposition, is often one of the main reasons affecting the yield of the process. In view of this, the present invention provides a design method of an ion coil, which is achieved by The two ends of the coil are provided with inclined geometric shapes, so that the coil body is projected on the surface of the semiconductor wafer into a closed ring shape, so that the coil can effectively provide the electromagnetic force required for film deposition in the gap. The multiple ion coils designed in this way can effectively improve the uniformity of the deposited film on the semiconductor wafer. In order to make the above-mentioned objects, features, and advantages of the present invention more comprehensible, several preferred embodiments are described below, and the accompanying drawings are described in detail as follows: DETAILED DESCRIPTION The present invention provides an electric ion coil. The purpose of improving the uniformity of the film is achieved by setting the geometric shapes of the two ends of the coil to be inclined. The following describes several preferred embodiments of the present invention for illustration. First Embodiment: In order to clearly distinguish the difference between the first embodiment of the present invention and the conventional technology, the conventional implementation of the conventional ion coils of FIGS. 2a and 2b and the first implementation of FIGS. 3a and 3b are described respectively. Example for comparison. The top view of a conventional ion coil is shown in Fig. 2a, and the side view is shown in Fig. 2b. The coil includes a coil body 2, which has a long shape and has a first end and a second
0503-9538twf(nl);tsmc2002-0969;Albert.ptd 第 8 頁 1224345 五、發明說明(4) 端部,該第一端部具有一第一端 第二端面2 5, 23 ,由第2b圖 該第二端面2 5 半導體晶片表 發明之第一實 圖所示,第一 具有一第一端 端面34,該第 該第二端部之 第一實施例之 傾斜面,此傾 面成為如第3 a 的薄膜,其原 以說明。第2 c 隙附近的磁場 間隙處其垂直 現此一區域之 遠比其他有線 例沿第3 b圖之 度分佈,由於 因此第3 c圖的 央部份是慢慢 的垂直劇減, 且於第一端部與該 傳統電離 ,因此該 圖所示並 視圖如第 可發現該 為垂直面 面如第2 a 施例之上 實施例包括一線圈 部以及 面2 4,該第二端部具有一 第二端部之間存在一間隙 子線圈之該第一端面2 4與 傳統電離子線圈投影在該 不能產生封閉之環形。本 3a圖所示,侧視圖如第3b 主體3,為一長條形狀而 端部,該第一端部具有一第 一端部具有一弟 間存在一 該第一端 斜能夠使 圖所示之 理之解釋 圖為傳統 強度與薄 方向上下 磁場強度 圈分佈區 間隙33, 面3 4與該 該線圈主 封閉環形 可由第2c 電離子線 膜沉積厚 均沒有線 極弱,薄 域為薄; 側面在其間隙附近 第一實施例第一端 磁場強度 遞減而非 另外在間 在間隙之 第2 c圖傳 隙中央因 端面3 5,且 由第3b圖可 第二端面3 5 體投影在該 ,因而可以 圖與第3c圖 圈沿第2b圖 度分佈,由 圈分佈,所 膜於此間隙 再比較第3 c 的磁場強度 面34及第二 分佈從兩端 統式電離子 其上下方依 於第一 發現本 為相互 半導體 沉積厚 之圖形 之侧面 第2b圖 以第2c 下方沉 圖為第 與薄膜 端面3 5 面起往 線圈磁 然有來 端部與 發明之 平行之 晶片表 度均勻 比較加 在其間 可知在 圖可發 積厚度 一實施 沉積厚 傾斜, 間隙中 場強度 自線圈0503-9538twf (nl); tsmc2002-0969; Albert.ptd Page 8 1224345 V. Description of the invention (4) The end portion, the first end portion has a first end second end surface 2 5, 23, as shown in Fig. 2b The second end surface 2 5 of the semiconductor wafer is shown in the first actual figure of the invention. The first has a first end surface 34, and the second embodiment has the inclined surface of the first embodiment. The inclined surface becomes as the first The 3 a film was originally described. At the magnetic field gap near the 2c gap, the area perpendicular to this area is far more distributed along the 3b graph than other wired examples. Because of this, the central part of the 3c graph is slowly decreasing vertically, and The first end portion is ionized with the conventional one, so the figure is shown in the figure as shown in the figure. It can be found that the surface is a vertical plane, as in the second embodiment. The embodiment includes a coil portion and a surface 24. The second end portion has A projection of the first end surface 24 of a gap sub-coil between a second end portion and a conventional electric ion coil is formed on the incapable of generating a closed loop. This figure is shown in Figure 3a. The side view is shown in Figure 3b. The main body 3 has a long shape and an end. The first end has a first end. The explanation of the rationale is the gap 33 between the distribution zone of the upper and lower magnetic field strength loops in the traditional direction and the thin direction. The surface 34 and the coil's main closed loop can be deposited by the 2c ion wire film. The side surface is near the gap. In the first embodiment, the magnetic field strength of the first end decreases gradually, but not in the gap 2c. The center of the gap is due to the end face 35, and the second end face 3 5 is projected from the figure 3b. Therefore, the circle of the graph and 3c can be distributed along the 2b scale, and the circle can be used to compare the magnetic field strength surface 34 and the second distribution of 3c in this gap. In the first discovery, the side of the pattern where the semiconductors are deposited thickly is shown in Figure 2b, and the bottom figure of 2c is the first, and the film end surface is on the 5th side. The coil magnetically comes, and the end is parallel to the invention. Add in between FIG embodiment can send a product of the thickness of deposited thick inclined, the gap field strength from the coils
0503-953Stwf(nl);tsmc2002-0969;Albert.ptd 第9頁 1224345 五、發明說明(6) 二端部之間存在一間隙5 3。該第一端面5 4具有中間之垂直 面以及上面與下面相互平行之兩傾斜面,該第二端面5 5形 狀相同於該第一端面5 4,且與該第一端面5 4相互平行。第 三實施例亦能夠使該線圈主體投影在該半導體晶片表面成 為如第5 a圖所示之封閉環形,因而可以沉積厚度均勻的薄 膜。第5 c圖為第二實施例沿第5 b圖之侧面在其間隙附近的 磁場強度與薄膜沉積厚度分佈;由第5 c圖可知第三實施例 的設計方式一樣可使間隙保持磁場強度,其優點是磁場強 度有明顯弱化的區域較窄,缺點是在間隙中央的磁力較 弱。 第四實施例: 第6a圖及第6b圖分別為第四實施例之上視圖及侧視 圖。第四實施例包括一線圈主體6,為一長條形狀而具有 一第一端部以及一第二端部,該第一端部具有一第一端面 6 4,該第二端部具有一第二端面6 5,且於第一端部與該第 二端部之間存在一間隙6 3。該第一端面6 4為一曲面且與該 第二端面6 5相互平行。第四實施例亦能夠使該線圈主體投 影在該半導體晶片表面成為如第6 a圖所示之封閉環形,因 而可以沉積厚度均勻的薄膜。第6c圖為第二實施例沿第6b 圖之侧面在其間隙附近的磁場強度與薄膜沉積厚度分佈; 由第6 c圖可知第四實施例的設計方式一樣可使間隙保持磁 場強度,於間隙中央可由線圈之左右兩端面提供一定強度 的磁場而不致有磁力喪失情形。其優點是間隙中央的磁力 有特別加強效果,而缺點則是該間隙磁場強度明顯弱化之0503-953Stwf (nl); tsmc2002-0969; Albert.ptd Page 9 1224345 V. Description of the invention (6) There is a gap 5 between the two ends. The first end surface 54 has a vertical plane in the middle and two inclined surfaces that are parallel to each other on the upper and lower sides. The second end surface 5 5 has the same shape as the first end surface 5 4 and is parallel to the first end surface 54. In the third embodiment, the coil main body can be projected on the surface of the semiconductor wafer into a closed loop shape as shown in FIG. 5a, so that a thin film having a uniform thickness can be deposited. Fig. 5c shows the magnetic field intensity and film deposition thickness distribution of the second embodiment near the gap along the side of Fig. 5b; from Fig. 5c, it can be seen that the third embodiment is designed in such a way that the gap can maintain the magnetic field strength. The advantage is that the area where the magnetic field strength is significantly weakened is narrower, and the disadvantage is that the magnetic force in the center of the gap is weaker. Fourth embodiment: Figures 6a and 6b are a top view and a side view of the fourth embodiment, respectively. The fourth embodiment includes a coil body 6 having a long shape and having a first end portion and a second end portion. The first end portion has a first end portion 64 and the second end portion has a first end portion. The two end surfaces 65 are provided with a gap 6 3 between the first end portion and the second end portion. The first end surface 64 is a curved surface and is parallel to the second end surface 65. The fourth embodiment can also make the coil body projection on the surface of the semiconductor wafer into a closed loop as shown in Fig. 6a, so that a thin film with a uniform thickness can be deposited. Figure 6c shows the magnetic field strength and film deposition thickness distribution of the second embodiment near the gap along the side of Figure 6b. From Figure 6c, it can be seen that the design method of the fourth embodiment can maintain the magnetic field strength in the gap in the same way as in the fourth embodiment. The center can provide a certain strength magnetic field from the left and right ends of the coil without loss of magnetic force. The advantage is that the magnetic force in the center of the gap has a special strengthening effect, while the disadvantage is that the magnetic field strength of the gap is significantly weakened.
0503-9538twf(nl);tsmc2002-0969;Albert.ptd 第11頁 本發明有以下幾 1224345 五、發明說明(7) 區域較寬。 綜上所述 一、 提供一種簡易且有效的 理氣相沉積製程中由離子金屬電 離子線圈所產生薄膜厚度不均勻 任何其他部份就可以達成上述目 二、 可依不同製程需求選擇 之電離子線圈,例如第三實施例 區域較窄但在間隙中央的磁力則 隙中央的磁力較強,但磁場強度 寬。 雖然本發明已以四個較佳之 非用以限定本發明,任何熟悉本 明之精神和範圍内,當可做更動 護範圍當視後附之申請專利範圍 點優點: 方法可以改善離子金屬物 漿物理氣相沉積設備之電 問題,無需改變該設備中 的。 使用本方法不同概念設計 可使磁場強度有明顯弱化 較弱,第四實施例可使間 有明顯弱化區域就會比較 實施例揭露如上,然其並 項技藝者,在不脫離本發 和潤飾,因此本發明之保 所界定者為準。0503-9538twf (nl); tsmc2002-0969; Albert.ptd Page 11 The present invention has the following 1224345 V. Description of the invention (7) The area is relatively wide. To sum up, one, to provide a simple and effective physical vapor deposition process in which the thickness of the film produced by the ionic metal ion coil is not uniform, and any other part can achieve the above purpose. The ion coil can be selected according to different process requirements. For example, in the third embodiment, the area is narrow but the magnetic force in the center of the gap is stronger, but the magnetic field strength is wider. Although the present invention has been defined by four preferred methods, any person familiar with the spirit and scope of the present invention can change the scope of protection as the scope of the attached patent application. Advantages: The method can improve the physical properties of ionic metal slurry. Electrical problems with vapor deposition equipment do not require changes in the equipment. The use of different conceptual designs of this method can make the magnetic field strength significantly weaker. The fourth embodiment can make the area weaker, and the embodiment will be disclosed as above. However, the skilled artist will not depart from the hair and retouch. Therefore, what is defined in the guarantee of the present invention shall prevail.
0503-9538twf(nl); tsmc,2002-0969;Albert .ptd 第12頁 1224345 圖式簡單說明 第1圖為習知之離子金屬電漿物理氣相沉積設備示意 圖; 第2 a圖為習知之傳統電離子線圈之上視圖; 第2b圖為習知之傳統電離子線圈之侧視圖; 第2 c圖為習知之傳統電離子線圈沿第2 b圖之此線圈側 面在其缺口區域附近的磁場強度與薄膜沉積厚度分佈; 第3 a圖為本發明之第一實施例之上視圖; 第3b圖為本發明之第一實施例之侧視圖; 第3c圖為本發明之第一實施例沿第3b圖之此線圈側面 在其間隙附近的磁場強度與薄膜沉積厚度分佈; 第4a圖為本發明之第二實施例之上視圖; 第4b圖為本發明之第二實施例之側視圖; 第4c圖為本發明之第二實施例沿第4b圖之此線圈侧面 在其間隙附近的磁場強度與薄膜沉積厚度分佈; 第5 a圖為本發明之第三實施例之上視圖; 第5b圖為本發明之第三實施例之侧視圖; 第5c圖為本發明之第三實施例沿第5b圖之此線圈側面 在其間隙附近的磁場強度與薄膜沉積厚度分佈; 第6 a圖為本發明之第四實施例之上視圖; 第6b圖為本發明之第四實施例之側視圖; 第6c圖為本發明之第四實施例沿第6b圖之此線圈侧面 在其間隙附近的磁場強度與薄膜沉積厚度分佈。 符號說明0503-9538twf (nl); tsmc, 2002-0969; Albert .ptd Page 12 1224345 Brief description of the diagram Figure 1 is a schematic diagram of a conventional ion metal plasma physical vapor deposition equipment; Figure 2a is a conventional traditional ionization Top view of the sub-coil; Figure 2b is a side view of the conventional conventional ion coil; Figure 2c is the magnetic field strength and the film of the conventional traditional ion coil along the side of the coil in Figure 2b near the notch area Deposition thickness distribution; Figure 3a is a top view of the first embodiment of the present invention; Figure 3b is a side view of the first embodiment of the present invention; Figure 3c is a first embodiment of the present invention along Figure 3b The magnetic field intensity and film deposition thickness distribution of the side of the coil near its gap; Figure 4a is a top view of the second embodiment of the present invention; Figure 4b is a side view of the second embodiment of the present invention; Figure 4c This is a second embodiment of the present invention along the side of the coil in FIG. 4b, the magnetic field intensity and the thickness of the thin film deposition near the gap; FIG. 5a is a top view of the third embodiment of the present invention; FIG. 5b is this Side view of a third embodiment of the invention Figure 5c is the third embodiment of the present invention along the coil side of the coil side magnetic field strength and film deposition thickness distribution along Figure 5b; Figure 6a is a top view of the fourth embodiment of the present invention; Fig. 6b is a side view of the fourth embodiment of the present invention; Fig. 6c is a distribution of the magnetic field strength and the thickness of the thin film deposition of the fourth embodiment of the present invention along the side of the coil in Fig. 6b near the gap. Symbol Description
0503-9538twf(nl);tsmc2002-0969;Albert.ptd 第13頁 1224345 圖式簡單說明 習知之離子金屬電漿物理氣相沉積設備 11〜真空艙; 1 3〜高頻交流電壓裝置; 15〜半導體晶片承座, 1 2 1〜第一交流電源連結部 1 2 2〜第二交流電源連結部 2〜線圈主體; 2 1〜第一交流電源連結部; 22〜第二交流電源連結部: 2 4〜第一端面; 3〜線圈主體; 3 1〜第一交流電源連結部; 3 2〜第二交流電源連結部; 3 4〜第一端面; 4〜線圈主體; 4 1〜第一交流電源連結部; 4 2〜第二交流電源連結部; 4 4〜第一端面; 5〜線圈主體; 5 1〜第一交流電源連結部; 5 2〜第二交流電源連結部; 5 4〜第一端面; 6〜線圈主體; 6 1〜第一交流電源連結部; 1 2〜電離子線圈 1 4〜金屬革巴; 1 2 3〜間隙 23〜間隙; 2 5〜第二端面 33〜間隙; 3 5〜第二端面 43〜間隙; 4 5〜第二端面 5 3〜間隙, 5 5〜第二端面0503-9538twf (nl); tsmc2002-0969; Albert.ptd Page 13 1224345 The diagram briefly illustrates the conventional ion metal plasma physical vapor deposition equipment 11 ~ vacuum chamber; 1 ~ 3 ~ high frequency AC voltage device; 15 ~ semiconductor Chip holder, 1 2 1 ~ 1st AC power connection part 1 2 2 ~ 2nd AC power connection part 2 ~ coil body; 2 1 ~ 1st AC power connection part; 22 ~ 2nd AC power connection part: 2 4 ~ 1st end face; 3 ~ coil body; 3 1 ~ first AC power supply connection; 3 2 ~ second AC power connection; 3 4 ~ first end face; 4 ~ coil body; 4 1 ~ first AC power connection 4 2 to the second AC power connection portion; 4 4 to the first end surface; 5 to the coil body; 5 1 to the first AC power connection portion; 5 2 to the second AC power connection portion; 5 4 to the first end surface 6 ~ coil body; 6 1 ~ first AC power connection; 1 2 ~ ion coil 1 4 ~ metal leather; 1 2 3 ~ gap 23 ~ gap; 2 5 ~ second end face 33 ~ gap; 3 5 ~ 2nd end face 43 ~ gap; 4 5 ~ second end face 5 3 ~ gap, 5 5 ~ second end face
0503-9538twf(nl); tsmc'2002-0969;Albert.ptd 第14頁 1224345 圖式簡單說明0503-9538twf (nl); tsmc'2002-0969; Albert.ptd Page 14 1224345 Schematic description
0503-9538twf(nl);tsmc2002-0969;Albert.ptd 第15頁0503-9538twf (nl); tsmc2002-0969; Albert.ptd p. 15
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