TWI716725B - Plasma processing device - Google Patents
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本發明有關於一種電漿處理裝置,尤指一種可同時處理多個工件、提昇電漿均勻性及拋光處理程序的材料去除率之高效能大面積平面型大氣電漿處理裝置。 The present invention relates to a plasma processing device, in particular to a high-efficiency large-area planar atmospheric plasma processing device that can process multiple workpieces at the same time, improve plasma uniformity and the material removal rate of the polishing process.
矽基功率元件面臨材料開發的局限性,難以滿足市場對高頻、高溫、高功率、高性能、抗惡劣環境以及便攜性的新需求。碳化矽(SiC)是一種寬帶隙半導體材料,具有高耐壓、高飽和電子漂移速率、高導熱係數等物理特性,適合用作高功率和高溫半導體元件。以SiC為代表的第三代半導體材料將廣泛應用於包括光電子器件和功率電子器件在內的領域;憑藉其出色的半導體性能,將能夠在現代工業領域突出重大的革命性功能,提供巨大的應用前景和市場潛力。 Silicon-based power components face the limitations of material development, and it is difficult to meet the market's new demands for high frequency, high temperature, high power, high performance, resistance to harsh environments, and portability. Silicon carbide (SiC) is a wide band gap semiconductor material with physical properties such as high withstand voltage, high saturated electron drift rate, and high thermal conductivity, and is suitable for high-power and high-temperature semiconductor components. The third-generation semiconductor materials represented by SiC will be widely used in fields including optoelectronic devices and power electronic devices; with its excellent semiconductor performance, it will be able to highlight major revolutionary functions in modern industrial fields and provide huge applications Prospects and market potential.
雖然碳化矽晶片具有優異的材料質量,但由於碳化矽的硬度和脆性(莫氏硬度為9.25~9.5,僅次於鑽石之超硬材料),如在最末段拋光加工製程仍需移除材料1~2微米(μm)之深度,此過程以傳統的化學機械拋光(CMP)製程需要大約需要數小時甚至超過十小時,成為晶圓生產的瓶頸導致處理成本高。因此,晶圓上游製造產業都在尋求提升大尺寸(直徑≧4吋)SiC晶片的拋光加工的材料移除率。 Although silicon carbide wafers have excellent material quality, due to the hardness and brittleness of silicon carbide (the Mohs hardness is 9.25~9.5, second only to diamond's superhard material), the material still needs to be removed in the final polishing process. With a depth of 1 to 2 microns (μm), this process takes about several hours or even more than ten hours with the traditional chemical mechanical polishing (CMP) process, which becomes a bottleneck for wafer production and high processing costs. Therefore, the upstream wafer manufacturing industry is seeking to improve the material removal rate of polishing processing of large-size (diameter ≧ 4 inches) SiC wafers.
平面型的大氣電漿,主要的考量重點在於大氣下電漿產生若以平面電極方式設置,當兩電極間的間隙有傾斜時,在相同參數條件下依據帕邢曲線(Paschen’s curves),電漿會自然集中偏向兩電極間距小的位置產生,且產生後無法重新分佈。故在製作大面積的大氣壓電極,電極間距精確度控制困難。 For planar atmospheric plasma, the main consideration is that if the plasma generation in the atmosphere is set as a planar electrode, when the gap between the two electrodes is inclined, according to the Paschen's curves under the same parameter conditions, the plasma It will be naturally concentrated and generated at a position where the distance between the two electrodes is small, and cannot be redistributed after generation. Therefore, it is difficult to control the accuracy of the electrode spacing when manufacturing large-area atmospheric pressure electrodes.
據此,如何能有一種可同時處理多個工件、提昇電漿均勻性及拋光處理程序的材料去除率之『電漿處理裝置』,是相關技術領域人士亟待解決之課題。 Accordingly, how to have a "plasma processing device" that can process multiple workpieces at the same time, improve the plasma uniformity and the material removal rate of the polishing process, is an urgent issue for those in the relevant technical field.
於一實施例中,本發明提出一種電漿處理裝置,包括:一上電極,其包含凸伸設置於上電極之一面且連接電漿源之複數柱狀電極,於上電極之中心區域具有一個電漿空乏區,於電漿空乏區內無柱狀電極,由電漿空乏區最外圍至上電極周緣之範圍內設有複數柱狀電極,由複數柱狀電極產生一環形電漿分佈區,電漿空乏區最外圍至上電極周緣之範圍內形成一電漿處理區;以及一下電極,具有包覆有介電材質之內藏式電極,下電極接地且被驅動旋轉。 In one embodiment, the present invention provides a plasma processing device, including: an upper electrode, which includes a plurality of columnar electrodes protrudingly disposed on one surface of the upper electrode and connected to a plasma source, and a central area of the upper electrode In the plasma depletion zone, there is no columnar electrode in the plasma depletion zone. A plurality of columnar electrodes are arranged from the outermost periphery of the plasma depletion zone to the periphery of the upper electrode. The plurality of columnar electrodes generate a circular plasma distribution area. A plasma treatment zone is formed from the outermost periphery of the plasma depletion zone to the periphery of the upper electrode; and the lower electrode has a built-in electrode coated with a dielectric material, and the lower electrode is grounded and driven to rotate.
10:上電極 10: Upper electrode
11:座體 11: Seat
111:柱狀電極 111: cylindrical electrode
112:套件 112: Kit
113:隔片 113: spacer
114:第一冷卻流道 114: The first cooling runner
1141:流入端 1141: Inflow
1142:流出端 1142: outflow end
115:第一蓋板 115: first cover
1151:流體入口 1151: fluid inlet
1152:流體出口 1152: fluid outlet
1153:第二氣體入口 1153: second gas inlet
116:第一氣體入口 116: First gas inlet
117:第二冷卻流道 117: Second cooling runner
12:殼體 12: Shell
121:第一孔洞 121: first hole
122:氣孔 122: Stoma
123:第二蓋板 123: second cover
13:電漿空乏區 13: Plasma depleted area
20、20A:下電極 20, 20A: lower electrode
21、21A:承載件 21, 21A: Carrier
23、23A:蓋體 23, 23A: cover
22、22A:內藏式電極 22, 22A: Built-in electrodes
30:工件 30: Workpiece
40:遮罩 40: Mask
41:腔體 41: Cavity
411:出氣孔 411: Vent Hole
412:滾珠 412: ball
42:支撐架 42: support frame
43:連動裝置 43: Linkage device
C1~C9:圈 C1~C9: circle
D1、D2、D3、D4、D5、D6、D7、D8:直徑 D1, D2, D3, D4, D5, D6, D7, D8: diameter
F1:第一方向 F1: First direction
R1:外圍 R1: peripheral
R2:周緣 R2: Perimeter
X1:軸向 X1: axial
圖1為本發明之實施例之分解結構示意圖。 Fig. 1 is a schematic diagram of an exploded structure of an embodiment of the present invention.
圖2為本發明之柱狀電極之分布位置之一實施例之示意圖。 2 is a schematic diagram of an embodiment of the distribution position of the columnar electrodes of the present invention.
圖3為圖1之A-A剖面結構示意圖。 Fig. 3 is a schematic diagram of the A-A cross-sectional structure of Fig. 1.
圖4為本發明之冷卻流道之一實施例之結構示意圖。 Fig. 4 is a schematic structural view of an embodiment of the cooling channel of the present invention.
圖5為本發明將氣孔設置於複數柱狀電極間之實施例之結構示意圖。 FIG. 5 is a schematic structural view of an embodiment of the present invention in which pores are arranged between a plurality of columnar electrodes.
圖6為本發明之遮罩之一實施例與上電極、下電極之俯視組合結構示意圖。 FIG. 6 is a schematic diagram of a top view combined structure of an embodiment of the mask and the upper electrode and the lower electrode of the present invention.
圖7為圖6之B-B剖面結構且遮罩位於製程位置時之示意圖。 FIG. 7 is a schematic diagram of the B-B cross-sectional structure of FIG. 6 and the mask is in the process position.
圖8為圖6之B-B剖面結構且遮罩位於進出料位置時之示意圖。 Fig. 8 is a schematic diagram of the B-B cross-sectional structure of Fig. 6 and the mask is in the feeding and discharging position.
圖9為本發明之下電極之一實施例之立體分解結構示意圖。 FIG. 9 is a three-dimensional exploded structural diagram of an embodiment of the lower electrode of the present invention.
圖10為本發明之下電極另一實施例之立體分解結構示意圖。 FIG. 10 is a three-dimensional exploded structural diagram of another embodiment of the lower electrode of the present invention.
請參閱圖1所示本發明之一種電漿處理裝置之實施例,其包含一上電極10及一接地且被驅動旋轉之下電極20。上電極10可上下移動,亦即相對於下電極20靠近或分離。上電極10用於提供電漿源及製程氣體。下電極20的作用為作為工件30的承載平台以及作為電漿電源的接地電極。上電極10與下電極20之間的區域為電漿產生區。下電極20可單獨做為大面積電漿輔助處理裝置的接地電極,或者與化學機械研磨裝置共用,可同時作為化學機械研磨裝置的拋光盤。
Please refer to FIG. 1 for an embodiment of a plasma processing apparatus of the present invention, which includes an
請參閱圖1及圖2所示,於上電極10之一面(亦即圖示上電極10之底面)設有複數柱狀電極111,於上電極10之中心區域具有一個電漿空乏區13,於電漿空乏區13內無柱狀電極111,由於電漿空乏區13內無柱狀電極分佈,因此電漿空乏區13可為盲板或設置氣體出入孔道。由電漿空乏區13最外圍R1至上電極10周緣R2之範圍內設有複數柱狀電極111,由複數柱
狀電極111產生一環形電漿分佈區,亦即,電漿空乏區13最外圍R1至上電極11周緣R2之範圍內形成一電漿處理區。上述環形電漿分佈區與電漿處理區皆涵蓋工件30放置的範圍,例如圖示工件30呈圓形,上述環形電漿分佈區與電漿處理區的徑向寬度至少等於工件30的直徑。
Please refer to FIG. 1 and FIG. 2, a plurality of
請參閱圖2所示,說明本發明柱狀電極之布置方式,然圖示僅為說明例,並不限於圖示數量、圈數。柱狀電極111為覆蓋有介電材質之導電材質。複數柱狀電極111環繞一圓心形成複數圈C1~C9之同心圓,於每一圈設有至少一柱狀電極111,圖中各柱狀電極111內的數字代表所在的圈,以利於辨識位於各圈C1~C9上的柱狀電極111。相鄰兩圈之同心圓上之柱狀電極111之數目相同,例如,第一圈C1、第二圈C2都設有三個柱狀電極111,第六圈C6、第七圈C7都設有四個柱狀電極111,第八圈C8、第九圈C9都設有五個柱狀電極111;或者,相鄰兩圈之同心圓,位於外圈之柱狀電極111之數目多於位於內圈之柱狀電極111之數目,例如,第五圈C5設有三個柱狀電極111。每一圈上之柱狀電極所形成之圓環形軌跡之外緣與其相鄰之圓環形軌跡之內緣至少相切,例如,第一圈C1、第三圈C3的柱狀電極111的直徑相同,且第一第一圈C1、第三圈C3的徑向距離等於柱狀電極111的直徑,或者,若第一圈C1、第三圈C3的徑向距離小於柱狀電極111的直徑亦可,以此類推。藉由第一圈C1至第九圈C9之柱狀電極111之圓環形軌跡,即可形成一環形電漿分佈區。
Please refer to FIG. 2 to illustrate the arrangement of the columnar electrode of the present invention. However, the illustration is only an illustrative example, and is not limited to the number and number of turns shown. The
關於每一圈的柱狀電極的數量,可依循下列公式:(該圈直徑*圓周率)/基數所得的值四捨五入取整數值。 其中,基數的決定方式依循下列公式:(修正後某圈每個柱狀電極負責的圓周長-基數)/基數*100%而後選取每一圈圓周長差異最小者。例如,當基數設定為80以及100時,最大誤差率~9.2%(柱狀數分別為112、91)。 Regarding the number of columnar electrodes in each circle, the following formula can be followed: (the circle diameter * the ratio of the circumference) / the base number is rounded to an integer value. Among them, the method of determining the base is based on the following formula: (circumference length that each cylindrical electrode is responsible for in a certain circle after correction-base)/base*100%, and then select the smallest difference in the circumference of each circle. For example, when the base number is set to 80 and 100, the maximum error rate is ~9.2% (the bar numbers are 112 and 91 respectively).
若考量擴充處理面積時,外層柱狀電極數目也會隨之提升,最小誤差解的柱狀電極數可能過高,所以可將誤差率加大,例如,圓周長誤差率~10%,但總柱狀電極數較未加大誤差率時低。例如,當基數設定為110時,最大誤差率~10%,總柱狀電極數為82個。 When considering the expansion of the processing area, the number of outer columnar electrodes will also increase. The number of columnar electrodes with the smallest error solution may be too high, so the error rate can be increased. For example, the circumference error rate is ~10%, but the total The number of columnar electrodes is lower than when the error rate is not increased. For example, when the base is set to 110, the maximum error rate is ~10%, and the total number of columnar electrodes is 82.
當基數不同時,對於總柱狀電極數的影響如下:當基數為70時:
當基數為100時:
當基數為130時:
其次,關於柱狀電極的位置設計。依上述得出各圈的柱狀電極數後,運用excel亂數函數rand()*360隨機產生角度變化決定每一圈第一個柱狀電極的分佈角度,該圈第二至第n個柱狀電極,分佈為平均分佈。例如,若第一圈有三個柱狀電極,所以間距為360/3=120;若第三圈有四個柱狀電極,所以間距為360/4=90,以此類推,角度若超過360度則進行修正(減360度);取亂數時,若相鄰兩圈的間距小於柱狀電極的直徑,則重取亂數,而若有重疊部分,則視狀況整圈移動或單點移動。柱狀電極的圖樣排列需整面分佈較均勻,避免造成規則性的圖形,規則性的圖形(例如各圈的柱狀電極排列在同一徑向線上)會使分佈形成處理空乏區,所以柱狀電極須調整以避免該類處理空乏區產生。 Second, the design of the position of the columnar electrode. After obtaining the number of cylindrical electrodes in each circle according to the above, use the excel random number function rand()*360 to randomly generate angle changes to determine the distribution angle of the first cylindrical electrode in each circle, and the second to nth columns of the circle Shape electrodes, the distribution is evenly distributed. For example, if there are three cylindrical electrodes in the first circle, the spacing is 360/3=120; if there are four cylindrical electrodes in the third circle, the spacing is 360/4=90, and so on, if the angle exceeds 360 degrees Correction (minus 360 degrees); when taking random numbers, if the distance between two adjacent circles is less than the diameter of the cylindrical electrode, the random number will be retaken, and if there is an overlap, it will be moved in a full circle or a single point depending on the situation. The pattern arrangement of the columnar electrodes needs to be more evenly distributed across the entire surface to avoid regular patterns. Regular patterns (for example, the columnar electrodes of each circle are arranged on the same radial line) will form a depleted area for processing, so columnar The electrode must be adjusted to avoid this type of processing depletion zone.
關於上述柱狀電極調整的實際驗證數據,可參考下表所示,其係以基數110舉例計算的每圈柱狀電極數以及柱狀電極分佈位置:
其次,可用公式決定柱狀電極的位置設計。當圈數內的柱狀電極相同時,第X圈以及第X+1圈柱狀電極分布夾角間隔計算方式為:360/2n(n為X圈以及X+1圈的柱狀電極個數); 其中,n為奇數時,取負;n為偶數時,取正。以每圈的柱狀數均勻分布在360度的前提下分佈當圈電極。亦即,當柱狀電極數目為3時,分佈的間距為360/3=120度來計算。第一圈以及第二圈的柱狀數均為3個,所以第一圈以及第二圈的柱狀電極排列差異角度為:360/(2*-3)=-60。假設第一圈若柱狀電極設置在0、120、240度的位置,第二圈的柱狀電極則以第一圈第一個柱狀電極0度做為基準,柱狀電極的間隔為360/3=120的前提下,設置在(0(360)-60)300,(300+120)60,(60+120)180(圓角度概念,1圈=360度,320+120=440超過一圈,所以440-360=60)。 Secondly, a formula can be used to determine the position design of the columnar electrode. When the cylindrical electrodes in the number of turns are the same, the calculation method for the angular interval between the X-th circle and the X+1-th circle of the cylindrical electrode distribution is: 360/2n (n is the number of cylindrical electrodes in the X circle and X+1 circle) ; Among them, when n is an odd number, it is negative; when n is an even number, it is positive. Distribute the electrodes in each circle on the premise that the number of columns in each circle is evenly distributed in 360 degrees. That is, when the number of columnar electrodes is 3, the distribution pitch is 360/3=120 degrees to calculate. The number of columns in the first circle and the second circle is 3, so the difference in the arrangement of the column electrodes in the first circle and the second circle is: 360/(2*-3)=-60. Assuming that the columnar electrodes in the first circle are set at 0, 120, and 240 degrees, the column electrodes in the second circle are based on the 0 degrees of the first column electrode in the first circle, and the interval between the column electrodes is 360 Under the premise of /3=120, set at (0(360)-60)300, (300+120)60, (60+120)180 (round angle concept, 1 circle=360 degrees, 320+120=440 over One lap, so 440-360=60).
若x與x+1圈的圈數不同時,所使用的計算公式為:(360/n-360/n+1);其中,n為奇數時,括號前方取負;n為偶數時,括號前方取正。當(360/n-360/n+1)<10時,公式變更為:(360/n-360/n+1)*n/2;其中,n為奇數時,括號前方取負;n為偶數時,括號前方取正。所以第三圈的第一點為60-(360/3-360/4)=30,第三圈分為:30、120、210、300。若第四圈與第三圈凸點數相同,則第一點間距=30+360/(2*4)=75,亦即第四圈分佈為:75、145、235、325 If the number of turns of x and x+1 is different, the calculation formula used is: (360/n-360/n+1); where, when n is an odd number, the front of the bracket is negative; when n is an even number, the bracket Take the front. When (360/n-360/n+1)<10, the formula is changed to: (360/n-360/n+1)*n/2; where n is an odd number, the front of the bracket is negative; n is When the number is even, the front of the parenthesis shall be positive. So the first point of the third circle is 60-(360/3-360/4)=30, and the third circle is divided into: 30, 120, 210, 300. If the number of convex points in the fourth circle is the same as that of the third circle, the distance between the first points=30+360/(2*4)=75, that is, the distribution of the fourth circle is: 75, 145, 235, 325
依上述公式計算,所得柱狀電極各點的分佈為
綜上所述,本發明之柱狀電極的分布原則包括:在柱狀電極分佈的環形區域內,相鄰兩圈的柱狀數目內外圈相同或外圈多於內圈;整體而言,其柱狀的個數由內圈向外圈增加;相鄰兩圈的同心源,外圈與內圈的直徑差異最多不可超過柱狀電極的直徑的兩倍,使內外柱狀電極至少可相切;但較佳的設計為略小於柱狀電極直徑的兩倍,使柱狀內外圈電極處理區域有部分重疊。 In summary, the distribution principle of the columnar electrodes of the present invention includes: in the annular area where the columnar electrodes are distributed, the number of columns in two adjacent circles is the same in the inner and outer rings or the outer ring is more than the inner ring; The number of columns increases from the inner ring to the outer ring; for concentric sources in two adjacent rings, the difference in diameter between the outer ring and the inner ring should not exceed twice the diameter of the cylindrical electrode, so that the inner and outer cylindrical electrodes can at least be tangent ; But the preferred design is slightly less than twice the diameter of the cylindrical electrode, so that the electrode processing area of the cylindrical inner and outer ring partially overlaps.
由內而外每一圈柱狀電極數目規則可包含:最小誤差解:選取「基數」後經計算每一圈圓周長差異最小者;(1)掃略圓周長誤差計算方式:誤差(每一圈柱狀數所負責的圓周長-基數)/基數*100%;(2)考慮柱狀數設置的次佳解:考量柱狀數的總數量越多,若考量擴充處理面積時的外層柱狀數數目也會隨之提升,可選擇次佳解(圓周長誤差率~10%,但總柱狀數低於誤差率最佳解的次佳解)。 The rule for the number of cylindrical electrodes in each circle from the inside to the outside can include: minimum error solution: the smallest difference in the circumference of each circle is calculated after selecting the "base"; (1) the calculation method of sweeping the circumference error: error (each The circumference of the circle column number-cardinality) / cardinality * 100%; (2) Consider the second best solution of the column number setting: consider the total number of column numbers, if you consider the outer column when expanding the processing area The number of bars will also increase, and the next best solution can be selected (circumference error rate ~10%, but the total bar number is lower than the next best solution with the best error rate).
柱狀電極的分佈方法原則為:(1)每一圈柱狀電極分佈為平均分佈;也就是分佈間隔為360度/n,n等於該圈的柱狀電極數目;(2)相鄰兩圈柱狀電極避免於同一個角度的延伸線上,當內外圈間距小於2倍直徑時,會有部分重疊; (3)柱狀電極的分佈可藉由設定某一圈的某一基準點,以加入某一個定值移動角度、以亂數獲取第一點分佈角度的方式、帶入自定公式的方式(公式非唯一)、以及人工分佈的方式進行;(4)若以亂數定第一個點時,若相鄰兩圈的間距小於柱狀電極的直徑,則重取亂數(避免柱狀電極重疊);(5)柱狀電極的分佈需朝向整個盤面分佈均勻,避免造成規則性的圖形形成。 The principle of the distribution method of columnar electrodes is: (1) Each circle of columnar electrodes is evenly distributed; that is, the distribution interval is 360 degrees/n, where n is equal to the number of columnar electrodes in the circle; (2) Two adjacent circles Avoid columnar electrodes on the extension line at the same angle. When the distance between the inner and outer rings is less than 2 times the diameter, there will be partial overlap; (3) The distribution of columnar electrodes can be set by setting a certain reference point of a certain circle, adding a certain fixed value movement angle, obtaining the first point distribution angle with random numbers, and introducing a self-defined formula ( The formula is not unique) and the way of manual distribution; (4) If the first point is determined by random numbers, if the distance between two adjacent circles is less than the diameter of the columnar electrode, then the random number is retaken (to avoid overlapping columnar electrodes ); (5) The distribution of the columnar electrodes must be evenly distributed toward the entire disk surface to avoid the formation of regular patterns.
相鄰圈重疊解決方法:(1)內圈或外圈整體柱狀電極的設定同時移動一個角度;(2)其餘點不動,重疊點移動使該相臨兩點錯開(圓心到圓心的距離至少等於柱狀電極的直徑)。 Solutions for overlapping adjacent circles: (1) The setting of the integral cylindrical electrode of the inner ring or the outer ring moves an angle at the same time; (2) The remaining points do not move, and the overlap point moves so that the two adjacent points are staggered (the distance between the center of the circle and the center of the circle is at least Equal to the diameter of the columnar electrode).
請參閱圖1及圖3所示,上電極10包括一導電材質之座體11及一介電材質之殼體12。於座體11之一面(亦即圖示座體11之底面)設有複數柱狀電極111,柱狀電極111凸伸設置於上電極10之座體11之一面且連接於電漿源,每一柱狀電極111皆為圓柱體,其軸向端部朝向下電極20。如圖3所示,柱狀電極111與該座體11一體成形,除此之外,亦可以連結件固定方式結合柱狀電極111與該座體11,例如,於柱狀電極111之頂部設置一凸柱伸入座體11再以C形環固定。每一柱狀電極111套設有一介電材質之套件112。於殼體12相對應於複數柱狀電極111之位置設有複數第一孔洞121,座體11設置於殼體12內,套設有套件112之複數柱狀電極111由相對應之第一孔洞121凸伸於殼體12外。於上電極10的電漿空乏區13的範圍內分布有複數氣孔122。於座體11設有複數柱狀電極111之面設有一介電材質之隔片
113,例如,陶瓷片、鐵氟龍片。於座體11相對於設有複數柱狀電極111之面(亦即圖示座體11之頂面)設有第一冷卻流道114及一第一氣體入口116。每一柱狀電極111之軸向中心設有一第二冷卻流道117與第一冷卻流道114相通形成一冷卻路徑。
Please refer to FIG. 1 and FIG. 3, the
請參閱圖3及圖4所示,第一冷卻流道114是一連續流道,其具有一流入端1141以及一流出端1142。於座體11相對於設有複數柱狀電極111之面設有一導電材質之第一蓋板115覆蓋於第一冷卻流道114。於第一蓋板115設有一流體入口1151、一流體出口1152及一第二氣體入口1153,第二氣體入口1153透過第一氣體入口116與氣孔122相連通。冷卻流體由流體入口1151進入流入端1141,再由流出端1142經由流體出口1152流出第一冷卻流道114。此外,殼體12具有一介電材質之第二蓋板123,其設置於殼體12相對於設有複數柱狀電極111之面,且覆蓋於第一蓋板115。當第二蓋板123密封後,可使第一冷卻流道114與第二冷卻流道117形成一密閉的循環流道,可導入流體冷卻上電極10,以維持上電極10的溫度。
Please refer to FIG. 3 and FIG. 4, the
請參閱圖5所示,其顯示將氣孔122設置於複數柱狀電極111間之進氣方式之實施例結構,有別於圖3所示將氣孔122設置於電漿空乏區13的範圍內的實施例。
Please refer to FIG. 5, which shows an example structure of an air intake method in which pores 122 are arranged between a plurality of
請參閱圖1及圖5所示,上電極10包括一導電材質之座體11及一介電材質之殼體12。於座體11之一面(亦即圖示座體11之底面)設有複數柱狀電極111,柱狀電極111凸伸設置於上電極10之座體11之一面且連接於電漿源,每一柱狀電極111皆為圓柱體,其軸向端部朝向下電極20。如圖5所示,柱狀電極111與該座體11一體成形,除此之外,亦可以連結件固定方
式結合柱狀電極111與該座體11,例如,於柱狀電極111之頂部設置一凸柱伸入座體11再以C形環固定。每一柱狀電極111套設有一介電材質之套件112。於殼體12相對應於複數柱狀電極111之位置設有複數第一孔洞121,座體11設置於殼體12內,套設有套件112之複數柱狀電極111由相對應之第一孔洞121凸伸於殼體12外。於複數柱狀電極111之間分布有複數氣孔122。於座體11設有複數柱狀電極111之面設有一介電材質之隔片113,例如,陶瓷片、鐵氟龍片。於座體11相對於設有複數柱狀電極111之面(亦即圖示座體11之頂面)設有第一冷卻流道114及一第一氣體入口116。每一柱狀電極111之軸向中心設有一第二冷卻流道117與第一冷卻流道114相通形成一冷卻路徑。
Please refer to FIG. 1 and FIG. 5, the
請參閱圖4及圖5所示,第一冷卻流道114是一連續流道,其具有一流入端1141以及一流出端1142。於座體11相對於設有複數柱狀電極111之面設有一導電材質之第一蓋板115覆蓋於第一冷卻流道114。於第一蓋板115設有一流體入口1151、一流體出口1152及一第二氣體入口1153。冷卻流體由流體入口1151進入流入端1141,再由流出端1142經由流體出口1152流出第一冷卻流道114。製程氣體由外部通過第二氣體入口1153、第一氣體入口116後,再分別經由複數氣孔122流出殼體12,並流至上電極10與下電極20間之電漿產生區。此外,殼體12具有一介電材質之第二蓋板123,其設置於殼體12相對於設有複數柱狀電極111之面,且覆蓋於第一蓋板115。當第二蓋板123密封後,可使第一冷卻流道114與第二冷卻流道117形成一密閉的循環流道,可導入流體冷卻上電極10,以維持上電極10的溫度。
Please refer to FIG. 4 and FIG. 5, the
必須說明的是,上述實施例所採用之介電材質之殼體12、介電材質之套件112、介電材質之隔片113及介電材質之第二蓋板123,其作用在於使每個柱狀電極111均勻激發電漿,並防止電漿產生時,帶電粒子直接轟擊導電電極而形成電弧放電損傷電極。然為達成此目的所能採用的技術手段不限於此,例如,殼體12與套件112可結合為一整體覆蓋於上電極10及柱狀電極111之介電材質。此外,圖1至圖5分別顯示上電極的立體、仰視、剖面結構,僅為示意圖而非等比例繪製。
It must be noted that the
請參閱圖6及圖7所示,上電極10與下電極20之間設有一遮罩40,遮罩40包括一腔體41、一支撐架42及一連動裝置43。腔體41呈環狀,其內徑大於上電極10與下電極20之外徑,腔體41設有至少一氣孔411,腔體41設有閥門(圖中未示出)控制製程氣體進出腔體41之方向。腔體41的材質不限,可為金屬或介電材質。支撐架42設置於腔體41頂部,支撐架42呈中空環形,是作為上檔板用,支撐架42的材質不限,可為金屬或介電材質。連動裝置43連接於腔體41,可驅動腔體41與支撐架42同步移動。
Please refer to FIG. 6 and FIG. 7, a
請參閱圖3及圖7所示,第二氣體入口1153、第一氣體入口116、上電極10的氣孔122、上電極10與下電極20間之電漿產生區、腔體40的氣孔411、腔體41內部形成一相連通的製程氣體通路,據此,若將第二氣體入口1153連接於一製程氣體的氣體混合槽,將腔體41連通一尾氣處理系統時,可將製程氣體導入第二氣體入口1153,流經第一氣體入口116、上電極10的氣孔122、上電極10與下電極20間之電漿產生區、腔體40的氣孔411、腔體41內部後,排放到尾氣處理系統。此時,氣孔122為送氣口,氣孔411為抽氣口。製程氣體的流動方向如圖3及圖7的箭頭方向所示。
Please refer to FIGS. 3 and 7, the
相反地,若將腔體41連通一製程氣體的氣體混合槽,將第二氣體入口1153連接於一尾氣處理系統時,則可將製程氣體導入腔體41內部,流經腔體40的氣孔411、上電極10與下電極20間之電漿產生區、上電極10的氣孔122、第一氣體入口116、第二氣體入口1153後,排放到尾氣處理系統。藉由腔體41的閥門控制製程氣體進出腔體之方向,此時,氣孔411為送氣口,氣孔122為抽氣口。製程氣體的流動方向與圖3及圖7所示箭頭方向相反。
Conversely, if the
請參閱圖7及圖8所示,連動裝置43控制腔體41平行第一方向F1於一製程位置(圖7所示位置)與一進出料位置(圖8所示位置)間往復移動,於腔體41之內側面設有複數滾珠412與上電極10的外側緣接觸,作為導引遮罩40上下移動之用。第一方向F1平行於柱狀電極111之軸向X1且垂直於水平面。如圖7所示,當腔體41位於製程位置時,腔體41的下緣與下電極20之底面切齊或低於下電極20之底面。如圖8所示,當連動裝置43將腔體41上抬,使腔體41位於進出料位置時,腔體41的下緣高於下電極20之頂面,使下電極20可由電漿處理區移出以置換欲進行電漿處理的新工件30,而後再由連動裝置43將腔體41降低至圖9所示製程位置,即可進行工件30的電漿作業。
Please refer to Figures 7 and 8, the
本發明設置遮罩40之作用包括:(1)涵蓋上、下電極間空間,穩定氣體組成成分,避免外界氣體影響;(2)具通、抽氣孔位,製程結束後可快速置換殘留反應氣體;(3)具導引裝置,不干擾上下料;(4)可設置導氣(或抽氣孔)更改製程氣體進氣方式。當使用這種方式時,可
將氣孔122省略。
The functions of the
請參閱圖9所示實施例,下電極20包括一承載件21、一蓋體23及一內藏式電極22,內藏式電極22為一環形件,承載件21與蓋體23為介電材質,將內藏式電極22夾合於其間並包覆於內藏式電極22外。
Please refer to the embodiment shown in FIG. 9, the
請參閱圖2及圖9所示,內藏式電極22所形成之圓環形軌跡之中心圓形區域相對應於電漿空乏區13,內藏式電極22所形成之圓環形軌跡的直徑D1等於或大於位於最外圍之柱狀電極111所形成之圓環形軌跡之外緣直徑D2,內藏式電極22所形成之圓環形軌跡之內緣直徑圓環形軌跡的直徑D3(亦即內藏式電極22之內緣直徑)D3等於或小於位於最內圍之該柱狀電極111所形成之圓環形軌跡之內緣直徑D4。必須說明的是,本實施例將內藏式電極22設計為一環形件之原因在於,由於上電極10的電漿空乏區13不會產生電漿,因此下電極20對應上電極10的電漿空乏區13的位置不需要設置下電極,可節省成本,換言之,於不考量成本的況下,亦可將內藏式電極22設置成一圓形件。
Please refer to Figures 2 and 9, the central circular area of the circular track formed by the built-in
請參閱圖10所示,下電極20A包括一承載件21A、三蓋體23A及三內藏式電極22A,內藏式電極22A為一圓形件,承載件21A與蓋體23A為介電材質,將內藏式電極22A夾合於其間並包覆於內藏式電極22A外。然內藏式電極22A的數量不限於三個。
Please refer to FIG. 10, the
請參閱圖2及圖10所示,內藏式電極22A所形成之圓環形軌跡之中心圓形區域相對應於電漿空乏區13,內藏式電極22A所形成之圓環形軌跡的直徑D5等於或大於位於最外圍之柱狀電極111所形成之圓環形軌跡之外緣直徑D2,內藏式電極22A所形成之圓環形軌跡之內緣直徑圓環形軌跡的
直徑D6等於或小於位於最內圍之該柱狀電極111所形成之圓環形軌跡之內緣直徑D4。內藏式電極22A的直徑D7等於或大於欲處理的工件30的直徑D8。
Please refer to Figures 2 and 10, the central circular area of the circular track formed by the built-in
本實施例將內藏式電極22A設計為圓形件,只要將工件擺放於設有內藏式電極22A的位置即可,如圖1所示態樣。因此相較於圖9所示實施例,本實施例更可降低下電極的製造成本;此外,使用者可決定內藏式電極22A設置的數量,例如,可如圖10所示設置三個內藏式電極22A,亦可僅設置一或二個;當設置三個內藏式電極22A時,可依所需每次處理一個工件、二個工件,最多可處理三個工件;當設置二個內藏式電極22A時,可依所需每次處理一個工件或二個工件。當工件擺放在內藏式電極的相對應位置時才產生電漿,可降低功率耗量。
In this embodiment, the built-in
圖9及圖10顯示本發明之內藏式電極可由單一環形件或多個圓形件組成,使電極凸柱全時或間時產生電漿。 Figures 9 and 10 show that the built-in electrode of the present invention can be composed of a single ring member or a plurality of circular members, so that the electrode protrusions can generate plasma at all times or from time to time.
根據上述設計原則,可歸納出本發明之電漿空乏區13的設置基準包括:(1)確認下電極20的尺寸,例如,直徑為355mm,或其他尺寸;(2)確認欲處理之工件20的尺寸,例如,直徑為4英吋的晶圓,或其他尺寸工件;(3)最外層柱狀電極111分佈:等於或略大於內藏式電極22、22A分佈外圍;(4)最內層柱狀電極111分佈:等於或略小於下電極20。
According to the above design principles, it can be concluded that the setting criteria of the
綜上所述,本發明之電漿處理裝置,係一種可用於硬脆材料(如碳化矽,silicon carbide)提升拋光效率的大面積大氣電漿處理裝置,藉由 電漿解離氣體所產生的反應物種與硬脆材料表面產生物理及化學反應,達到表面改質或形成揮發物種自表面移除的功效,解決機械化學拋光在難加工硬脆材料表面拋光製程移除效率過低導致加工成本居高不下的問題。本發明包括:一具有非對稱柱狀結構分佈的上電極,柱狀電極排列構成一環形電漿處理區域;一具有內藏式電極的下電極,該內藏式電極的設計配合上電極的環形電漿處理區設置。當激發一高頻電漿源(例如RF)於上電極時,電漿在上電極的凸柱結構及下電極對應內藏式電極處產生。下電極與可提供旋轉動能的裝置銜接,可調整旋轉的速率,當下電極旋轉啟動時,上電極的環形區域柱柱狀電極分佈設計,使電漿處理範圍可涵蓋整個處理面而達成多個工件(例如,多片SiC晶圓)同時處理的目標。本發明所使用的電漿系統係於大氣中產生,具大面積、無需真空腔體,但於上下電極間設置可移動式遮罩降低外界環境干擾以及製程完成後快速抽除製程氣體。 In summary, the plasma processing device of the present invention is a large area atmospheric plasma processing device that can be used for hard and brittle materials (such as silicon carbide) to improve polishing efficiency. The reactive species generated by plasma dissociation gas produce physical and chemical reactions with the surface of hard and brittle materials to achieve the effect of surface modification or form volatile species to remove from the surface, and solve the problem of mechanical chemical polishing in the hard and brittle material surface polishing process removal Too low efficiency leads to the problem of high processing costs. The invention includes: an upper electrode with an asymmetrical columnar structure, the columnar electrodes are arranged to form a circular plasma processing area; a lower electrode with a built-in electrode, the design of the built-in electrode matches the ring shape of the upper electrode The plasma processing area is set up. When a high-frequency plasma source (such as RF) is excited on the upper electrode, plasma is generated at the convex pillar structure of the upper electrode and the corresponding built-in electrode of the lower electrode. The bottom electrode is connected with a device that can provide rotational kinetic energy, and the speed of rotation can be adjusted. When the bottom electrode rotates, the cylindrical electrode distribution design in the annular area of the top electrode enables the plasma processing range to cover the entire processing surface to achieve multiple workpieces (For example, multiple SiC wafers) the target of simultaneous processing. The plasma system used in the present invention is generated in the atmosphere, has a large area and does not require a vacuum chamber, but a movable shield is arranged between the upper and lower electrodes to reduce the interference of the external environment and quickly remove the process gas after the process is completed.
此外,本發明為乾式處理且可於大氣環境下進行,易與機械化學拋光設備進行整合。經實驗驗證,市售四吋碳化矽硬脆晶圓材料,拋光移除效率(現階段最佳)由0.23提升至1.51um/hr(提升657%)。 In addition, the present invention is dry processing and can be carried out in an atmospheric environment, and is easy to integrate with mechanical chemical polishing equipment. Experimental verification shows that the polishing removal efficiency (the best at this stage) of commercially available 4-inch silicon carbide hard and brittle wafer materials has been increased from 0.23 to 1.51um/hr (657% increase).
雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。 Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention. Anyone with ordinary knowledge in the technical field can make some changes and modifications without departing from the spirit and scope of the present invention. The scope of protection of the present invention shall be determined by the scope of the attached patent application.
10‧‧‧上電極 10‧‧‧Upper electrode
111‧‧‧柱狀電極 111‧‧‧Cylinder electrode
12‧‧‧殼體 12‧‧‧Shell
122‧‧‧氣孔 122‧‧‧Stomata
123‧‧‧第二蓋板 123‧‧‧Second cover
13‧‧‧電漿空乏區 13‧‧‧Depleted area of plasma
20‧‧‧下電極 20‧‧‧Lower electrode
21‧‧‧承載件 21‧‧‧Carrier
30‧‧‧工件 30‧‧‧Workpiece
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