TWI401333B - Sputtering apparatus and sputtering method - Google Patents
Sputtering apparatus and sputtering method Download PDFInfo
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- TWI401333B TWI401333B TW095125494A TW95125494A TWI401333B TW I401333 B TWI401333 B TW I401333B TW 095125494 A TW095125494 A TW 095125494A TW 95125494 A TW95125494 A TW 95125494A TW I401333 B TWI401333 B TW I401333B
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/35—Sputtering by application of a magnetic field, e.g. magnetron sputtering
- C23C14/352—Sputtering by application of a magnetic field, e.g. magnetron sputtering using more than one target
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/0021—Reactive sputtering or evaporation
- C23C14/0036—Reactive sputtering
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Description
本發明,係有關於濺鍍裝置及濺鍍方法。The present invention relates to a sputtering apparatus and a sputtering method.
於膜形成時,從成膜速度快等優點來說,係經常使用磁控管濺鍍方式。磁控管濺鍍方式,係在標靶之後方設置由極性交互變換之複數磁石所構成之磁石組裝體,藉由經此磁石組裝體在標靶前方形成磁束而捕捉電子,提高標靶前方之電子密度,以提高此些電子與被導入至真空處理室內之氣體的衝突機率,提高電漿密度並濺鍍。At the time of film formation, magnetron sputtering is often used in terms of the film forming speed and the like. The magnetron sputtering method is a magnet assembly composed of a plurality of magnetic poles that are alternately transformed by polarity after the target, and the magnet assembly is used to form a magnetic flux in front of the target to capture electrons, thereby improving the front of the target. The electron density increases the probability of collision of such electrons with the gas introduced into the vacuum processing chamber, increasing the plasma density and sputtering.
然而,近年來,隨著基板之大型化,磁控管濺鍍裝置亦成為大型化。作為此種裝置,係熟知有藉由並排設置複數之標靶而能對大面積之基板成膜的濺鍍裝置(例如,專利文獻1)。However, in recent years, as the size of the substrate has increased, the magnetron sputtering apparatus has also become large. As such a device, a sputtering apparatus capable of forming a large-area substrate by arranging a plurality of targets in parallel is known (for example, Patent Document 1).
於此濺鍍裝置,由於在標靶相互之間設置有用以捕捉從標靶所飛出之2次電子等的陽極或是屏蔽等之構成構件,因此無法將各標靶接近設置,而使標靶間之間隔變寬。在此些標靶的相互之間,由於濺鍍粒子不會被放出,故在基板之表面,和標靶間對向之部分之成膜速度變為極緩慢,而使膜厚之面內均勻性變壞。In this sputtering apparatus, since the constituent members for capturing the anode or the shield of the secondary electrons flying from the target are provided between the targets, it is impossible to set the targets close to each other. The interval between the targets is widened. Between these targets, since the sputtered particles are not released, the film forming speed on the surface of the substrate and the opposing portion of the target becomes extremely slow, and the film thickness is uniform in the surface. Sex is bad.
為了解決此種問題點,考慮有如圖1所示之濺鍍裝置。濺鍍裝置1,係具備有:在其真空處理室11內,空下有特定之間隔而並排設置之複數的標靶12a~12d,和連接 相互鄰接之標靶(12a與12b,12c與12d)之2個的交流電源E。此濺鍍裝置1,由於係將與1個的交流電源連接之標靶的其中一方作為陰極,另外一方作為陽極,而交互濺鍍,故不需要在標靶的相互之間設置陽極等之構成構件,而能將標靶接近配置。In order to solve such a problem, a sputtering apparatus as shown in Fig. 1 is considered. The sputtering apparatus 1 is provided with a plurality of targets 12a to 12d which are arranged side by side at a predetermined interval in the vacuum processing chamber 11, and are connected. Two AC power supplies E of the adjacent targets (12a and 12b, 12c and 12d). In the sputtering apparatus 1, since one of the targets connected to one AC power source is used as a cathode and the other is used as an anode and is alternately sputtered, it is not necessary to provide an anode or the like between the targets. Components, and the target can be placed close to the configuration.
〔專利文獻1〕日本國特表2002-508447號公報(例如,申請專利範圍之記載)。[Patent Document 1] Japanese Patent Publication No. 2002-508447 (for example, the description of the patent application).
然而,若將標靶相互接近設置,則由於藉由從鄰接之標靶端部的上部空間212所放出之電子流入陽極,會使電漿P不發生,而使標靶之端部不被濺鍍,作為非侵蝕區域而殘留。此時,就算將磁束平行移動至非侵蝕區域之前方,亦無法將標靶端部侵蝕,而使得無法涵蓋標靶全面而侵蝕,惡化標靶之利用效率。又,由於殘留下非侵蝕區域,而會成為濺鍍中之異常放電或是粒子之原因。However, if the targets are placed close to each other, since the electrons emitted from the upper space 212 of the adjacent target end portion flow into the anode, the plasma P does not occur, and the end portion of the target is not splashed. Plating, remaining as a non-erodible area. At this time, even if the magnetic flux is moved in parallel to the non-eroded area, the target end portion cannot be eroded, so that the target can not be comprehensively eroded, and the utilization efficiency of the target is deteriorated. Further, since the non-erosion area remains, it may cause abnormal discharge or particles in the sputtering.
又,由於在1個的交流電源所連接之相互鄰接的標靶間會產生電漿P,故會產生和其他空間相比電漿密度較低之空間122。此時,若將反應氣體導入濺鍍裝置中並進行反應性濺鍍,則在電漿密度較低之部分會無法促進反應,而使基板S面內之膜質無法成為均勻。Further, since the plasma P is generated between adjacent targets connected to one AC power source, a space 122 having a lower plasma density than other spaces is generated. At this time, when the reaction gas is introduced into the sputtering apparatus and reactive sputtering is performed, the reaction cannot be promoted in the portion where the plasma density is low, and the film quality in the surface of the substrate S cannot be made uniform.
於此,本發明之課題,係為解決上述先前技術之問題點,提供一種在標靶上不會殘留非侵蝕區域,且在進行反 應性濺鍍時,能形成均勻膜質之膜的濺鍍裝置。Accordingly, the problem of the present invention is to solve the above problems of the prior art, and to provide a non-eroded area on the target, and A sputtering device capable of forming a film of uniform film quality during sputtering.
本發明之濺鍍裝置,具備有:於真空處理室內,空出有特定之間隔而並排設置之至少4枚以上的標靶;和對於並排設置之標靶中之2枚標靶交互施加負電位及正電位又或是接地電位的交流電源,其特徵為:各交流電源係與不相互鄰接之2枚的標靶連接。The sputtering apparatus of the present invention includes: at least four or more targets that are arranged side by side at a specific interval in the vacuum processing chamber; and a negative potential is applied to two of the targets arranged side by side. And an alternating current power source having a positive potential or a ground potential, wherein each of the alternating current power sources is connected to two targets that are not adjacent to each other.
藉由將各交流電源與不相互鄰接之2枚的標靶連接,能將陽極與陰極間之距離變廣,而使電子不流入陽極。藉由此,電漿會在標靶之前方產生,並能涵蓋標靶之全面而侵蝕。By connecting each AC power source to two targets that are not adjacent to each other, the distance between the anode and the cathode can be widened, and electrons do not flow into the anode. By this, the plasma will be generated in front of the target and can cover the full erosion of the target.
又,藉由連接隔著1枚以上之標靶之2枚的標靶,由於各電漿會相互重複產生而不會產生電漿密度低的空間,故基板前方之電漿密度成為略為均勻,在進行反應性濺鍍時,能形成膜質均勻之膜。Further, by connecting two targets having one or more targets interposed therebetween, the plasmas are repeatedly generated and a space having a low plasma density is not generated, so that the plasma density in front of the substrate is slightly uniform. When reactive sputtering is performed, a film having a uniform film quality can be formed.
本發明之之濺鍍裝置,以具備有:以在各標靶之前方形成磁束之方式配置在各標靶之後方的由複數磁石所構成之磁石組裝體;和以使磁束相對於標靶作平行移動的方式驅動此些磁石組裝體之驅動手段為理想。藉由將磁石組裝體左右平行移動,能將標靶全面作略為均勻之侵蝕。The sputtering apparatus according to the present invention includes: a magnet assembly including a plurality of magnets disposed behind each target so as to form a magnetic flux in front of each target; and a magnetic flux relative to the target It is desirable to drive the magnet assembly in a parallel manner. By moving the magnet assembly in parallel to the left and right, the target can be completely uniformly eroded.
又,若將此磁石組裝體分別配置於各標靶之後方,則亦可想見到各磁石會相互干涉而造成磁場平衡之崩潰。於此種情況,係以具備有將經由各磁石組裝體所形成之磁束 密度形成為均勻之磁束密度修正手段為理想。Further, if the magnet assembly is placed behind each target, it is also conceivable that the magnets interfere with each other to cause a collapse of the magnetic field balance. In this case, the magnetic flux formed by each magnet assembly is provided. It is desirable that the density is formed into a uniform magnetic flux density correcting means.
又,本發明之濺鍍方法,其特徵係為將基板搬移至與在真空處理室內,空出有特定之間隔而並排設置之至少4枚以上的標靶相對向之位置,對於並排設置之標靶中之不相互鄰接之2枚標靶交互施加負電位及正電位又或是接地電位,在標靶上產生電漿而在基板上形成膜。Further, the sputtering method according to the present invention is characterized in that the substrate is moved to a position facing at least four or more targets which are arranged at a predetermined interval in the vacuum processing chamber, and are arranged side by side. The two targets that are not adjacent to each other in the target alternately apply a negative potential and a positive potential or a ground potential, and plasma is generated on the target to form a film on the substrate.
若藉由本發明之濺鍍裝置,則能得到:在標靶上不會殘留非侵蝕區域,又,在進行反應性濺鍍時,形成之膜的膜質係為均勻之優良效果。。According to the sputtering apparatus of the present invention, it is possible to obtain an excellent effect that the film quality of the formed film is uniform even when the non-erosion region remains on the target. .
若參考圖2,則本發明之濺鍍裝置2,係為葉片式之物,具備有:將基板從大氣環境之晶圓閘(未圖示)搬送,並儲存之裝載鎖定處理室20,和進行濺鍍之真空處理室21,和設置於裝載鎖定處理室20與真空處理室21間之傳送處理室22。裝載鎖定處理室20、傳送處理室22及真空處理室21,係分別經由分隔閥而連接。於裝載鎖定處理室20、真空處理室21及傳送處理室22,雖未圖示,但是在連接有真空幫浦的同時,亦配置有監視其真空度之真空計。Referring to Fig. 2, the sputtering apparatus 2 of the present invention is a blade type, and includes a load lock processing chamber 20 that transports a substrate from a wafer shutter (not shown) in the atmosphere, and stores it. The vacuum processing chamber 21 that performs sputtering and the transfer processing chamber 22 that is disposed between the load lock processing chamber 20 and the vacuum processing chamber 21 are provided. The load lock processing chamber 20, the transfer processing chamber 22, and the vacuum processing chamber 21 are connected via separate valves. Although not shown in the figure, the load lock processing chamber 20, the vacuum processing chamber 21, and the transfer processing chamber 22 are connected to a vacuum pump and a vacuum gauge for monitoring the degree of vacuum.
於裝載鎖定處理室20,設置有搬送裝著有基板S之基板保持具的搬送臂。經由此搬送臂,從外部(晶圓 閘),將裝著於基板保持具之基板S收容於裝載鎖定處理室20。In the load lock processing chamber 20, a transfer arm that transports the substrate holder on which the substrate S is mounted is provided. By this transfer arm, from the outside (wafer In the gate, the substrate S mounted on the substrate holder is housed in the load lock processing chamber 20.
於傳送處理室22,係設置有搬送機器人(未圖示),在將裝載鎖定室20真空排氣至特定之真空度以後,打開分隔閥,將基板S搬送至真空排氣至同樣真空度的傳送處理室22。而後,打開傳送處理室22與真空處理室21之間的分隔閥,藉由搬送機器人來將基板S搬送至真空處理室21內。A transfer robot (not shown) is provided in the transfer processing chamber 22, and after the load lock chamber 20 is evacuated to a specific degree of vacuum, the partition valve is opened, and the substrate S is transferred to the vacuum to the same degree of vacuum. The processing chamber 22 is transferred. Then, the partition valve between the transfer processing chamber 22 and the vacuum processing chamber 21 is opened, and the substrate S is transferred to the vacuum processing chamber 21 by the transfer robot.
於此真空處理室21內,設置有氣體導入手段23(參考圖3)。氣體導入手段23,係經由介於設置在質量流控制器231a、231b之間的氣體導入管232,分別和氣體源233a、233b連接。於氣體源233a、233b,係封入有氬氣等之濺鍍氣體或是H2 O、O2 、N2 等之反應氣體,此些氣體,係經由質量控制器231a、231b而能以一定之流量導入至真空處理室21內。In the vacuum processing chamber 21, a gas introduction means 23 (refer to Fig. 3) is provided. The gas introduction means 23 is connected to the gas sources 233a, 233b via gas introduction pipes 232 provided between the mass flow controllers 231a, 231b, respectively. The gas sources 233a and 233b are sealed with a sputtering gas such as argon gas or a reaction gas such as H 2 O, O 2 or N 2 , and these gases can be fixed by the quality controllers 231a and 231b. The flow rate is introduced into the vacuum processing chamber 21.
在與被搬入真空處理室21內部之基板S相對向之位置,配置有標靶組裝體24。標靶組裝體24,係具有形成為略長方形之6枚的標靶241a~241f。此些之標靶組裝體241a~241f,係為ITO、Al合金、Mo等之因應於成膜在基板上的膜之組成而以周知的方法所製造之物,被接合有冷卻用之背板(未圖示)。The target assembly 24 is disposed at a position facing the substrate S that is carried into the vacuum processing chamber 21 . The target assembly 24 has six targets 241a to 241f formed in a substantially rectangular shape. The target assembly bodies 241a to 241f are ITO, Al alloy, Mo, or the like which are manufactured by a known method in accordance with the composition of the film formed on the substrate, and are bonded to the back sheet for cooling. (not shown).
又,標靶241a~241f,係以位置於和基板S平行之同一平面上的方式,空出間隔D1而並排設置。間隔D1,係被設定為在標靶241a~241f之側面相互之間的空間不會 產生電漿而使標靶241a~241f之側面被濺鍍的距離。此距離,係為1~10mm,理想係為2~3mm。藉由將標靶241a~241f近接配置,濺鍍粒子會到達被配置於和標靶241a~241f對向之位置的基板之全面,而能使膜厚分布均勻化。Further, the targets 241a to 241f are arranged side by side with a space D1 so as to be positioned on the same plane parallel to the substrate S. The interval D1 is set such that the space between the sides of the targets 241a to 241f does not occur. A plasma is generated to cause the sides of the targets 241a to 241f to be sputtered. This distance is 1~10mm, and the ideal system is 2~3mm. By arranging the targets 241a to 241f in close proximity, the sputtered particles reach the entire surface of the substrate disposed at a position opposed to the targets 241a to 241f, and the film thickness distribution can be made uniform.
於標靶241a~241f之背面,係被順序安裝有電極242a~242f和絕緣板243,此些係分別被安裝於標靶組裝體24之特定位置。此電極242a~242f,係分別連接有配置於真空處理室21外部3個的交流電源E1~E3。On the back surfaces of the targets 241a to 241f, electrodes 242a to 242f and an insulating plate 243 are sequentially mounted, and these are attached to specific positions of the target assembly 24, respectively. The electrodes 242a to 242f are respectively connected to three AC power sources E1 to E3 disposed outside the vacuum processing chamber 21.
交流電源E1~E3,係以對不相互鄰接之2枚的標靶交互施加電壓的方式而連接。舉例而言,交流電源E1之其中一方的端子係連接於標靶241a後方之電極242a,另外一方之端子係連接於標靶241d後方的電極242d。另外,交流電源所施加之電壓,係為正弦波或矩形波均可。The AC power supplies E1 to E3 are connected such that voltages are alternately applied to two targets that are not adjacent to each other. For example, one of the terminals of the AC power source E1 is connected to the electrode 242a behind the target 241a, and the other terminal is connected to the electrode 242d behind the target 241d. In addition, the voltage applied by the AC power source may be either a sine wave or a rectangular wave.
藉由如此這般連接交流電源E1~E3,若對其中一方之標靶(241a、241b、241c)從交流電源E1~E3施加負的電壓,則此些之標靶241a、241b、241c係提供作為陰極之功能,而另外一方之標靶241d、241e、241f係提供作為陽極之功能。而後,作為陰極之標靶241a、241b、241c之前方係形成有電漿,而標靶241a,241b、241c係被濺鍍。因應交流電源之頻率,各標靶241a~241f係交互被施加電壓而分別被濺鍍,濺鍍粒子到達基板S之全面,而將膜厚均勻形成。By connecting the AC power sources E1 to E3 in this manner, if one of the targets (241a, 241b, and 241c) applies a negative voltage from the AC power sources E1 to E3, the targets 241a, 241b, and 241c are provided. As the function of the cathode, the other targets 241d, 241e, and 241f provide functions as an anode. Then, plasma is formed in front of the cathode targets 241a, 241b, and 241c, and the targets 241a, 241b, and 241c are sputtered. In response to the frequency of the AC power source, the targets 241a to 241f are alternately applied with a voltage and are respectively sputtered, and the sputtered particles reach the entire surface of the substrate S, and the film thickness is uniformly formed.
於標靶組裝體24,係設置有分別位置於各標靶241a ~241f之後方的6個之磁石組裝體244。各磁石組裝體244係以相同構造而被形成,具有平行設置於標靶241a~241f之支持部245,在支持部245上,以交互改變極性而配置的方式,沿著標靶的長度方向設置有棒狀之中央磁石246。和以包圍中央磁石246之周邊的方式所設置之由複數磁石所構成的周邊磁石247。各磁石,係以使中央磁石換算為同磁化時之體積和將周邊磁石247之換算為同磁化時的體積之和成為相同的方式來設計。藉由此,在標靶241a~241f之前方形成平衡之封閉路徑的隧道狀磁束,捕捉在標靶之前方電離的電子及濺鍍所產生之2次電子,而能提高在作為陰極之標靶的前方所形成之電漿密度。The target assembly 24 is disposed at each target 241a. Six magnet assemblies 244 after ~241f. Each of the magnet assemblies 244 is formed in the same structure, and has a support portion 245 that is disposed in parallel with the targets 241a to 241f, and is disposed along the longitudinal direction of the target so as to be alternately changed in polarity on the support portion 245. There is a rod-shaped central magnet 246. And a peripheral magnet 247 composed of a plurality of magnets disposed to surround the periphery of the central magnet 246. Each of the magnets is designed such that the volume of the central magnet is converted into the same magnetization and the sum of the volume of the peripheral magnet 247 converted to the same magnetization. Thereby, a tunnel-shaped magnetic flux that forms a balanced closed path in front of the targets 241a to 241f captures electrons ionized in front of the target and secondary electrons generated by sputtering, thereby improving the target as a cathode. The density of the plasma formed in front of it.
然而,由於磁石組裝體244亦為相互接近,故磁場互相干涉,會有對應於位置在兩端之標靶241a、241f之後方的磁石組裝體244之磁場,和對應於位置在中央之標靶241c、241d之後方的磁石組裝體244之磁場的平衡崩潰的情況。此時,無法將基板S面內之膜厚分布作為略為均勻。此時,為了修正磁場平衡,在標靶組裝體24設置有輔助磁石248。此輔助磁石248,係和鄰接之磁石組裝體244的周邊磁石247之極性相同。而,此輔助磁石248與周邊磁石247之間隔,係為和各磁石組裝體244之間隔D2相同。藉由如此這般在配置於位置在兩端之標靶241a、241f之外側的防著板249之下方設置輔助磁石248,能改善磁場平衡。However, since the magnet assemblies 244 are also close to each other, the magnetic fields interfere with each other, and there is a magnetic field corresponding to the magnet assembly 244 located behind the targets 241a, 241f at both ends, and a target corresponding to the position at the center. The balance of the magnetic field of the magnet assembly 244 after the 241c and 241d collapses. At this time, the film thickness distribution in the plane of the substrate S cannot be made slightly uniform. At this time, in order to correct the balance of the magnetic field, the auxiliary magnet 248 is provided in the target assembly 24. The auxiliary magnet 248 has the same polarity as the peripheral magnet 247 of the adjacent magnet assembly 244. The spacing between the auxiliary magnet 248 and the peripheral magnet 247 is the same as the interval D2 of each of the magnet assemblies 244. By providing the auxiliary magnet 248 under the prevention plate 249 disposed on the outer side of the targets 241a and 241f at both ends as described above, the magnetic field balance can be improved.
藉由磁石組裝體244,在標靶241a~241f之前方由於 形成有隧道狀磁束,故位置於中央磁石246及周邊磁石247前方之電漿的密度較低。如此則在標靶241a~241f之此電漿密度較低的位於中央磁石246上方之位置,會作為非侵蝕部分而殘留。於此,有必要使隧道狀磁束之位置改變,而將標靶241a~241f均勻侵蝕以提高使用效率。By the magnet assembly 244, in front of the targets 241a to 241f Since the tunnel-shaped magnetic flux is formed, the density of the plasma located in front of the central magnet 246 and the peripheral magnet 247 is low. Thus, the positions of the targets 241a to 241f, which have a lower plasma density, are located above the central magnet 246, and remain as non-erosion portions. Here, it is necessary to change the position of the tunnel-shaped magnetic flux, and uniformly etch the targets 241a to 241f to improve the use efficiency.
為了使隧道狀磁束之位置改變,將磁石組裝體244及輔助磁石248設置在驅動軸250上之特定位置,在此驅動軸250上作為驅動手段,以能使各磁石組裝體244之位置作左右平行移動的方式,設置滾珠螺桿251,作為驅動手段,雖並不限定為如滾珠螺桿251一般的機械式驅動手段,而亦可使用空氣汽缸,但是在使用滾珠螺桿時,更能正確地控制磁石組裝體244的位置。此磁石組裝體244之移動距離,只要能使標靶241a~241f均勻的侵蝕,則並不特別限定。舉例而言,可將磁石組裝體244分別以點A~點B的間隔平行移動。另外,磁石組裝體244係不只是在左右方向,而在長度方向亦可平行移動。藉由此種使磁石組裝體244作2維平行移動,能將標靶241a~241f作更均勻的侵蝕。In order to change the position of the tunnel-shaped magnetic flux, the magnet assembly 244 and the auxiliary magnet 248 are disposed at specific positions on the drive shaft 250, and the drive shaft 250 is used as a driving means to enable the position of each of the magnet assemblies 244 to be left and right. In the parallel movement mode, the ball screw 251 is provided as a driving means, and is not limited to a mechanical driving means such as a ball screw 251, but an air cylinder may be used, but when the ball screw is used, the magnet can be more accurately controlled. The position of the assembly 244. The moving distance of the magnet assembly 244 is not particularly limited as long as the targets 241a to 241f can be uniformly eroded. For example, the magnet assemblies 244 can be moved in parallel at intervals of points A to B, respectively. Further, the magnet assembly 244 is not only moved in the left-right direction but also moved in parallel in the longitudinal direction. By causing the magnet assembly 244 to move in two dimensions in parallel, the targets 241a to 241f can be more uniformly eroded.
磁石組裝體244之移動,雖然係在成膜中或是成膜後均可,但是為了抑制成膜中之磁束移動所伴隨之異常放電的發生,係以成膜後之移動為理想。The movement of the magnet assembly 244 may be either during film formation or after film formation. However, in order to suppress the occurrence of abnormal discharge accompanying the movement of the magnetic flux during film formation, it is preferable to move after film formation.
在成膜中移動的情況,將滾珠螺桿251在濺鍍中驅動,以使標靶241a~241f從點A起至點B為止均勻地被侵蝕的方式,以2.5mm/sec以上,較理想係為4~ 15mm/sec之週期,使磁石組裝體244,亦即是,使磁束平行移動。In the case of moving in the film formation, the ball screw 251 is driven during sputtering so that the targets 241a to 241f are uniformly eroded from the point A to the point B, and are preferably 2.5 mm/sec or more. For 4~ At a cycle of 15 mm/sec, the magnet assembly 244, that is, the magnetic flux is moved in parallel.
在成膜後之移動的情況,係在終止成膜而停止交電源E1~E3,使放電一時停止後,在將作為下一個成膜對象之基板S設置在對向於標靶241a~241f之位置時,驅動滾珠螺桿251,將磁束分別從點A平行移動至點B並保持。此時,只要至少在下一次的成膜開始前將磁石組裝體244平行移動即可。而後,在此被搬送之基板S的成膜結束之後,再度依照同樣之順序,將磁束再度平行移動。經由將此操作依序重複進行,能在於基板上順序成膜的同時,將標靶241a~241f作均勻侵蝕。In the case of the movement after the film formation, the film formation is stopped, the power supply E1 to E3 is stopped, and the discharge is stopped once, and the substrate S as the next film formation target is placed on the target targets 241a to 241f. At the position, the ball screw 251 is driven to move the magnetic flux from point A to point B, respectively, and hold it. In this case, the magnet assembly 244 may be moved in parallel at least until the next film formation starts. Then, after the film formation of the substrate S to be conveyed is completed, the magnetic fluxes are again moved in parallel in the same order. By repeating this operation in this order, the targets 241a to 241f can be uniformly etched while sequentially forming a film on the substrate.
於本實施形態,雖敘述有經由輔助磁石248而能修正磁場之平衡,但只要是能修正磁場平衡之手段,則並不限定於此。舉例而言,亦可經由僅將周邊磁石之寬幅尺寸增大,或是將周邊磁石247變更為使由磁石所產生之磁束密度增大之材料,來修正磁場。In the present embodiment, the balance of the magnetic field can be corrected via the auxiliary magnet 248. However, the present invention is not limited thereto as long as it can correct the balance of the magnetic field. For example, the magnetic field may be corrected by merely increasing the width of the peripheral magnet or changing the peripheral magnet 247 to a material that increases the density of the magnetic flux generated by the magnet.
於本實施形態,雖將濺鍍裝置2作為葉片式之裝置,但亦可為連續式(inline)方式之物。In the present embodiment, the sputtering apparatus 2 is a vane type apparatus, but may be an inline type.
又,於本實施形態,雖係針對並排設置之標靶的枚數為6枚時之情況作說明,但標靶之枚數並不限定於此,可經由基板之大小等來作適當選擇。但是,標靶之枚數係一定要為4枚以上。此乃因為不滿4枚時,係無法作連接相互不鄰接之標靶的動作。又,交流電源E1~E3,由於係為連接2枚之標靶,故標靶之枚數係一定要為偶數。不論 是在任何情況,各交流電源之連接方法,只要是連接相互不鄰接之2枚的標靶,則並不特別限定。In the present embodiment, the case where the number of the targets to be arranged in parallel is six is described. However, the number of the targets is not limited thereto, and may be appropriately selected depending on the size of the substrate or the like. However, the number of targets must be four or more. This is because when there are less than four pieces, it is impossible to connect the targets that are not adjacent to each other. Moreover, since the AC power supplies E1 to E3 are connected to two targets, the number of targets must be an even number. whether In any case, the method of connecting the respective AC power sources is not particularly limited as long as it connects two targets that are not adjacent to each other.
圖4,係展示當標靶之枚數變更時標靶與交流電源之連接例。另外,於圖4中,與圖3相同之構成元件,係附加有相同之符號。Fig. 4 is a view showing an example of connection between a target and an AC power source when the number of targets is changed. In addition, in FIG. 4, the same component as FIG. 3 is attached with the same code|symbol.
當標靶241之數目係為4的倍數,例如標靶數為4時,如圖4(a)所示,若將隔著一枚標靶241而並排設置之2枚的標靶241與各交流電源E連接,則能將所有的標靶241以不相互鄰接的方式連接。於此情況,若如圖3一般將標靶隔著2枚來連接,則一定需要連接相互鄰接之標靶,而無法得到本發明之效果。When the number of the targets 241 is a multiple of 4, for example, when the number of targets is 4, as shown in FIG. 4(a), if two targets 241 are arranged side by side with one target 241 interposed therebetween, When the AC power source E is connected, all the targets 241 can be connected without being adjacent to each other. In this case, if the target is connected by two pieces as shown in FIG. 3, it is necessary to connect the targets adjacent to each other, and the effect of the present invention cannot be obtained.
在並排設置10枚之標靶241的情況,如圖4(b)所示,亦可連接兩端之各標靶,且將剩餘之標靶分別以隔著一枚之標靶而2枚2枚地與電源E連接。In the case where 10 targets 241 are arranged side by side, as shown in FIG. 4(b), each of the targets at both ends may be connected, and the remaining targets are respectively separated by one target and two 2 The ground is connected to the power source E.
另一方面,如圖4(c)所示,亦可將兩端之標靶分別隔著1枚的標靶而連接,將剩餘之標靶分別以隔著2枚之標靶而與電源E連接。就算這樣並排設置10枚之標靶,藉由連接不相互鄰接之標靶,電漿會在標靶之前方產生,並能涵蓋標靶之全面而侵蝕。On the other hand, as shown in FIG. 4(c), the targets at both ends may be connected by one target, and the remaining targets may be separated from the power source E by two targets. connection. Even if 10 targets are placed side by side, by connecting targets that are not adjacent to each other, the plasma will be generated in front of the target and can cover the overall erosion of the target.
以下,針對使用本發明之濺鍍裝置而在基板S之表面成膜之方法作說明。Hereinafter, a method of forming a film on the surface of the substrate S using the sputtering apparatus of the present invention will be described.
首先,經由裝載鎖定處理室20及傳送處理室22,將基板S從晶圓閘搬送至與並排設置之標靶241a~241f對向之位置,並經由真空排氣手段將真空處理室21之內部 真空排氣。接下來,經由氣體導入手段23,將Ar等之濺鍍氣體導入至真空處理室21內,在真空處理室21內形成特定之成膜氣體環境。另外,在進行反應性濺鍍時,在導入濺鍍氣體的同時,作為反應氣體,將選自H2 O氣體、O2 氣體及N2 氣體中之至少一種以上的氣體導入。而後,一面維持成膜環境,一面在標靶241a~241f藉由交流電源E1~E3,以數kHz~數百kHz分別施加正或負的電壓。在作為陰極之標靶上形成電場,在標靶前方產生電漿,則標靶被濺鍍並放出濺鍍粒子。將此動作因應交流電源之頻率而交互進行,則各標靶被均勻濺鍍。而後,停止交流電源,結束成膜。First, the substrate S is transferred from the wafer gate to the position facing the targets 241a to 241f arranged side by side via the load lock processing chamber 20 and the transfer processing chamber 22, and the inside of the vacuum processing chamber 21 is evacuated by means of vacuum evacuation. Vacuum exhaust. Next, a sputtering gas such as Ar is introduced into the vacuum processing chamber 21 via the gas introduction means 23, and a specific film formation gas atmosphere is formed in the vacuum processing chamber 21. In addition, at the time of reactive sputtering, a gas selected from at least one of H 2 O gas, O 2 gas, and N 2 gas is introduced as a reaction gas while introducing a sputtering gas. Then, while maintaining the film formation environment, positive or negative voltages are applied to the targets 241a to 241f by the AC power sources E1 to E3 at several kHz to several hundreds of kHz. When an electric field is formed on the target as a cathode and plasma is generated in front of the target, the target is sputtered and the sputtered particles are released. By performing this action interactively in response to the frequency of the AC power source, each target is uniformly sputtered. Then, the AC power is stopped and the film formation is completed.
另外,亦可在成膜中驅動滾珠螺桿251來驅動磁石組裝體244,又,亦可在終止成膜而停止交流電源E1~E3,使放電一時停止後,在將作為下一個成膜對象之基板S搬送至對向於標靶241a~241f之位置時,驅動滾珠螺桿251,使磁石組裝體244平行移動,亦即是,使磁束平行移動並保持。Further, the ball screw 251 may be driven to drive the magnet assembly 244 during film formation, or the AC power source E1 to E3 may be stopped after the film formation is terminated, and the discharge may be stopped for a while, and then the next film formation target is used. When the substrate S is transported to the position facing the targets 241a to 241f, the ball screw 251 is driven to move the magnet assembly 244 in parallel, that is, the magnetic flux is moved in parallel and held.
於實施例1中,係使用如圖2及圖3所示之濺鍍裝置來成膜,並調查成膜中之弧狀放電之產生次數。In Example 1, a sputtering apparatus as shown in Figs. 2 and 3 was used to form a film, and the number of generations of the arc discharge in the film formation was investigated.
將寬幅200mm,長度1700mm,厚度10mm之由In2 O3 -10Wt%SnO2 (ITO)所成之標靶,以離基板150mm之位置與基板平行之方式來設置。標靶間隔係分別為2mm。 於各標靶之後方,亦以距離各標靶47mm之方式,設置有寬幅170mm,長度1570mm,厚度40mm之磁石組裝體,經由滾珠螺桿251之驅動距離係成為50mm。作為基板S,係準備有寬幅1000mm,長度1200mm厚度0.7mm之玻璃基板。A target made of In 2 O 3 -10 Wt% SnO 2 (ITO) having a width of 200 mm, a length of 1700 mm, and a thickness of 10 mm was provided in parallel with the substrate at a position 150 mm from the substrate. The target interval is 2 mm. After the respective targets, a magnet assembly having a width of 170 mm, a length of 1570 mm, and a thickness of 40 mm was provided at a distance of 47 mm from each target, and the driving distance via the ball screw 251 was 50 mm. As the substrate S, a glass substrate having a width of 1000 mm and a length of 1200 mm and a thickness of 0.7 mm was prepared.
基板搬送後,進行真空排氣,而後經由氣體導入手段將作為濺鍍氣體之氬氣以240sccm來導入並形成0.67Pa之成膜環境。又,作為反應氣體,將H2 O氣體以2.0sccm,O2 氣體1.5sccm來導入。各交流電源E,頻率係為25kHz,電力係從0kw起每次緩慢提高5kW(各投入時間為120秒間),最終係為提升至15kW為止並投入120秒後,暫時停止交流電源,在搬送下一個基板時使磁石組裝體移動。如此這般一面依序成膜,一面監視電壓值及電流值,計數一分鐘內的異常放電(弧狀放電)發生次數。將標靶從濺鍍裝置取出,以目視確認其表面時,各標靶係被全面侵蝕。After the substrate was transferred, vacuum evacuation was performed, and then argon gas as a sputtering gas was introduced through a gas introduction means at 240 sccm to form a film formation environment of 0.67 Pa. Further, as a reaction gas, H 2 O gas was introduced at 2.0 sccm and O 2 gas at 1.5 sccm. Each AC power supply E has a frequency of 25 kHz, and the power is gradually increased by 5 kW from 0 kw each time (each input time is 120 seconds). Finally, after the power is raised to 15 kW and input for 120 seconds, the AC power supply is temporarily stopped. The magnet assembly is moved when one substrate is used. In this way, the film is sequentially formed, and the voltage value and the current value are monitored, and the number of occurrences of abnormal discharge (arc discharge) in one minute is counted. When the target is taken out from the sputtering apparatus to visually confirm the surface thereof, each target system is completely eroded.
於比較例1中,係使用將並排設置之6枚的標靶中相互鄰接之2枚的標靶與交流電源連接之裝置,一面以同樣之條件成膜,一面監視電壓值和電流值並計數異常放電之產生次數。In Comparative Example 1, a device in which two targets adjacent to each other of six targets arranged in parallel are connected to an AC power source, and the voltage and current values are monitored and counted while forming a film under the same conditions. The number of abnormal discharges produced.
結果如圖5所示。圖5,係於橫軸顯示積算電力,(kWh),縱軸係顯示異常放電之次數(次/分)。於比 較例1中,隨著積算電力之增大,異常放電之次數亦增加。相對於此,於實施例1中,隨著積算電力之增大,異常放電之次數亦不會增加。The result is shown in Figure 5. In Fig. 5, the integrated power is displayed on the horizontal axis (kWh), and the vertical axis shows the number of times of abnormal discharge (times/minute). Yubi In the first example, as the integrated power increases, the number of abnormal discharges also increases. On the other hand, in the first embodiment, as the integrated electric power increases, the number of abnormal discharges does not increase.
於實施例2中,係對使用如圖2及圖3所示之濺鍍裝置來進行反應性濺鍍時,膜質之面內均勻性作評價。In Example 2, the in-plane uniformity of the film quality was evaluated when reactive sputtering was performed using the sputtering apparatus shown in FIGS. 2 and 3.
膜質之面內均勻性的評價,係改變成膜時之反應氣體的流量比,調查膜上之各點中阻抗比最為下降之流量比,並以此流量比之差進行。The evaluation of the in-plane uniformity of the film quality was carried out by changing the flow rate ratio of the reaction gas at the time of film formation, and investigating the ratio of the flow rate at which the impedance ratio was the most decreased at each point on the film, and proceeding with the difference in the flow rate ratio.
使用與實施例1中所用之濺鍍裝置相同之物,與實施例1改變反應氣體之流量而形成複數之膜。作為反應氣體,將H2 O氣體以2.0sccm,O2 氣體以0.0~4.0sccm為止以0.5sccm刻度來改變並導入。各交流電源E,頻率係為25kHz,將電力由0kw起緩慢上升,最終係提升至15kw為止來投入,在投入25秒之後停止交流電源,結束成膜。所得之各膜膜厚,係為1000 Å。而後,各基板係被搬送至退火爐並在60分間以200度作大氣退火。針對被形成之膜上的對應於標靶241c之上部的點X,和對應於標靶241b和241c之間的上部之點Y,測定電阻率。Using the same material as the sputtering apparatus used in Example 1, the flow rate of the reaction gas was changed as in Example 1 to form a plurality of films. As a reaction gas, H 2 O gas was changed at 2.0 sccm, O 2 gas was 0.0 to 4.0 sccm, and was introduced at a scale of 0.5 sccm. Each of the AC power supplies E has a frequency of 25 kHz, and the power is gradually increased from 0 kw, and finally increased until 15 kW, and the AC power supply is stopped after 25 seconds of input, and the film formation is completed. The film thickness of each film obtained was 1000 Å. Then, each substrate was transferred to an annealing furnace and atmospherically annealed at 200 degrees for 60 minutes. The resistivity was measured for the point X on the formed film corresponding to the upper portion of the target 241c, and the point Y corresponding to the upper portion between the targets 241b and 241c.
使用將並排設置之6枚的標靶中相互鄰接之2枚的標靶與交流電源連接之裝置,以與實施例2同樣之條件進行 成膜及退火,分別在基板S上形成膜。針對被形成之各膜,亦在點X及點Y之兩點分別測定電阻率。The same conditions as in the second embodiment were carried out using a device in which two targets adjacent to each other among six targets arranged side by side were connected to an AC power source. Film formation and annealing are performed to form a film on the substrate S, respectively. The resistivity was also measured at each of the points X and Y for each of the formed films.
圖6,係於橫軸顯示O2 氣體之流量(sccm),縱軸係顯示各點之電阻率(μ Ω cm)。Fig. 6 shows the flow rate (sccm) of the O 2 gas on the horizontal axis and the resistivity (μ Ω cm) of each point on the vertical axis.
圖6(a),係顯示比較例1之測定結果。以實線所顯示之點X的電阻率值,係在O2 氣體之流量成為0.5sccm時為最低,成為255 μ Ω cm。於以虛線所顯示之點Y,係在O2 氣體之流量成為2.0sccm時電阻率為最低,成為253 μ Ω cm。於點X、點Y之電阻率成為最低的O2 氣體之流量的差係為差異極大之1.5sccm,可以得知於比較例2中,基板面內之膜質係為不均勻。Fig. 6(a) shows the measurement results of Comparative Example 1. The resistivity value of the point X shown by the solid line is the lowest when the flow rate of the O 2 gas is 0.5 sccm, and becomes 255 μ Ω cm. The point Y shown by the broken line is the lowest resistivity when the flow rate of the O 2 gas is 2.0 sccm, and becomes 253 μ Ω cm. The difference in the flow rate of the O 2 gas having the lowest resistivity at the point X and the point Y was 1.5 sccm which was extremely different. It was found that in Comparative Example 2, the film quality in the surface of the substrate was uneven.
相對於此,於圖6(b)所示之實施例2中,以實線所顯示之點X的電阻率值,成為最低之250 μ Ω cm係在O2 氣體之流量成為1.0sccm時,於以虛線所顯示之點Y,電阻率成為最低之248 μ Ω cm係在O2 氣體之流量成為1.5sccm時。於實施例2中,於點X、點Y之電阻率成為最低的O2 氣體之流量的差係為0.5sccm,成為先前裝置之一半以下,可以得知於反應性濺鍍中之膜質的面內均勻性係被改善。On the other hand, in the second embodiment shown in FIG. 6(b), the resistivity value of the point X shown by the solid line is the lowest 250 μ Ω cm when the flow rate of the O 2 gas is 1.0 sccm. At the point Y shown by the broken line, the resistivity becomes the lowest 248 μ Ω cm when the flow rate of the O 2 gas becomes 1.5 sccm. In the second embodiment, the difference in the flow rate of the O 2 gas having the lowest resistivity at the point X and the point Y is 0.5 sccm, which is one-half or less of the previous device, and the film surface in the reactive sputtering can be known. Internal uniformity is improved.
本發明之濺鍍裝置,係藉由改善交流電源之連接方法,而不在標靶上殘留非侵蝕區域,進而能改善被形成之膜的膜質均勻性。故而,本發明係可利用於製造大畫面之 平面面板顯示器的領域。The sputtering apparatus of the present invention improves the film quality uniformity of the formed film by improving the connection method of the alternating current power source without leaving a non-erosion area on the target. Therefore, the present invention can be utilized in the manufacture of large screens. The field of flat panel displays.
241a~241f‧‧‧標靶241a~241f‧‧‧ Target
242a~242f‧‧‧電極242a~242f‧‧‧electrode
244‧‧‧磁石組裝體244‧‧‧Magnetic assembly
250‧‧‧驅動軸250‧‧‧ drive shaft
251‧‧‧滾珠螺桿251‧‧‧Rolling screw
E1~E3‧‧‧交流電源E1~E3‧‧‧AC power supply
S‧‧‧基板S‧‧‧Substrate
〔圖1〕先前裝置之模式圖[Fig. 1] Schematic diagram of the previous device
〔圖2〕本發明之濺鍍裝置的概略構成圖[Fig. 2] A schematic configuration diagram of a sputtering apparatus of the present invention
〔圖3〕本發明之濺鍍裝置中之真空處理室的概略構成圖[Fig. 3] A schematic configuration diagram of a vacuum processing chamber in a sputtering apparatus of the present invention
〔圖4〕展示交流電源之其他連接例的圖[Fig. 4] A diagram showing another connection example of an AC power supply
〔圖5〕展示相對於積算電力之異常放電的發生次數之圖[Fig. 5] A graph showing the number of occurrences of abnormal discharge with respect to integrated power
〔圖6〕(a)展示使用先前裝置來成膜時之O2 氣體流量與電阻率之關係的圖表。(b)展示使用本發明之濺鍍裝置來成膜時之O2 氣體流量與電阻率之關係的圖表。[Fig. 6] (a) is a graph showing the relationship between the flow rate of O 2 gas and the resistivity when a film is formed using a conventional apparatus. (b) A graph showing the relationship between the flow rate of O 2 gas and the resistivity when film formation is performed using the sputtering apparatus of the present invention.
21‧‧‧真空處理室21‧‧‧vacuum processing room
23‧‧‧氣體導入手段23‧‧‧ gas introduction means
24‧‧‧標靶組裝體24‧‧‧Target assembly
231a、231b‧‧‧質量流控制器231a, 231b‧‧‧ mass flow controller
232‧‧‧氣體導入管232‧‧‧ gas introduction tube
233a、233b‧‧‧氣體源233a, 233b‧‧‧ gas source
241a~f‧‧‧標靶241a~f‧‧‧ Target
242a~f‧‧‧電源242a~f‧‧‧Power supply
243‧‧‧絕緣板243‧‧‧Insulation board
244‧‧‧磁石組裝體244‧‧‧Magnetic assembly
245‧‧‧支持部245‧‧‧Support Department
246‧‧‧中央磁石246‧‧‧Central Magnet
247‧‧‧周邊磁石247‧‧‧Surround magnet
248‧‧‧輔助磁石248‧‧‧Auxiliary magnet
249‧‧‧防著板249‧‧‧Anti-board
250‧‧‧驅動軸250‧‧‧ drive shaft
251‧‧‧滾珠螺桿251‧‧‧Rolling screw
E1~3‧‧‧電源E1~3‧‧‧Power supply
S‧‧‧基板S‧‧‧Substrate
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US20150021166A1 (en) * | 2011-08-25 | 2015-01-22 | Applied Materials, Inc. | Sputtering apparatus and method |
CN103014639B (en) * | 2012-12-12 | 2015-02-25 | 京东方科技集团股份有限公司 | Sputtering target material and sputtering device |
CN104878356B (en) * | 2015-06-08 | 2017-11-24 | 光驰科技(上海)有限公司 | A kind of determination method of magnetic control spattering target magnet placed angle |
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Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02258976A (en) * | 1988-09-26 | 1990-10-19 | Tokuda Seisakusho Ltd | Sputtering device |
JPH0364460A (en) * | 1989-07-31 | 1991-03-19 | Hitachi Ltd | Thin film forming device |
TW399245B (en) * | 1997-10-29 | 2000-07-21 | Nec Corp | Sputtering apparatus for sputtering high melting point metal and method for manufacturing semiconductor device having high melting point metal |
TW452601B (en) * | 1997-06-06 | 2001-09-01 | Anelva Corp | Sputtering device and sputtering method |
TW486719B (en) * | 1999-10-13 | 2002-05-11 | Balzers Process Systems Gmbh | Power supply unit and method to reduce the spark formation when sputtering |
TW593714B (en) * | 2000-09-07 | 2004-06-21 | Ulvac Inc | Sputtering apparatus and film manufacturing method |
JP2004346388A (en) * | 2003-05-23 | 2004-12-09 | Ulvac Japan Ltd | Sputtering source, sputtering apparatus and sputtering method |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6093293A (en) | 1997-12-17 | 2000-07-25 | Balzers Hochvakuum Ag | Magnetron sputtering source |
CN1358881A (en) * | 2001-11-20 | 2002-07-17 | 中国科学院长春光学精密机械与物理研究所 | Vacuum multi-unit sputtering plating method |
-
2005
- 2005-07-29 JP JP2005220889A patent/JP4922581B2/en active Active
-
2006
- 2006-07-12 TW TW095125494A patent/TWI401333B/en active
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Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02258976A (en) * | 1988-09-26 | 1990-10-19 | Tokuda Seisakusho Ltd | Sputtering device |
JPH0364460A (en) * | 1989-07-31 | 1991-03-19 | Hitachi Ltd | Thin film forming device |
TW452601B (en) * | 1997-06-06 | 2001-09-01 | Anelva Corp | Sputtering device and sputtering method |
TW399245B (en) * | 1997-10-29 | 2000-07-21 | Nec Corp | Sputtering apparatus for sputtering high melting point metal and method for manufacturing semiconductor device having high melting point metal |
TW486719B (en) * | 1999-10-13 | 2002-05-11 | Balzers Process Systems Gmbh | Power supply unit and method to reduce the spark formation when sputtering |
TW593714B (en) * | 2000-09-07 | 2004-06-21 | Ulvac Inc | Sputtering apparatus and film manufacturing method |
JP2004346388A (en) * | 2003-05-23 | 2004-12-09 | Ulvac Japan Ltd | Sputtering source, sputtering apparatus and sputtering method |
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