TW200842213A - Polysilicon dummy wafers and process used therewith - Google Patents
Polysilicon dummy wafers and process used therewith Download PDFInfo
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- TW200842213A TW200842213A TW096149477A TW96149477A TW200842213A TW 200842213 A TW200842213 A TW 200842213A TW 096149477 A TW096149477 A TW 096149477A TW 96149477 A TW96149477 A TW 96149477A TW 200842213 A TW200842213 A TW 200842213A
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- H—ELECTRICITY
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- H01L21/02109—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates
- H01L21/02112—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer
- H01L21/02123—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer the material containing silicon
- H01L21/0217—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer the material containing silicon the material being a silicon nitride not containing oxygen, e.g. SixNy or SixByNz
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- H01L21/02225—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer
- H01L21/0226—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process
- H01L21/02263—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process deposition from the gas or vapour phase
- H01L21/02271—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process deposition from the gas or vapour phase deposition by decomposition or reaction of gaseous or vapour phase compounds, i.e. chemical vapour deposition
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- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/67—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere
- H01L21/673—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere using specially adapted carriers or holders; Fixing the workpieces on such carriers or holders
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Abstract
Description
200842213 九、發明說明: 【發明所屬之技術領域】 本發明大體來說係有關於矽晶圓的熱處理。更明確地 說,係有關於在生產晶圓的批次熱處理中使用之非生產晶 圓。本發明也有關於可用來做為此種非生產晶圓以及做其 他用途的多晶矽類型。 【先前技術】 批次熱處理在矽積體電路製造之數個階段中延續使 用。一低溫熱處理藉由低溫化學氣相沉積(LPCVD)沉積一 層氮化矽,通常在溫度範圍約 7 0 0 °C下使用氣矽曱烷 (chlorosilane)和氨做為前驅物氣體。在一應用中,在每一 個週期中於烘箱内的所有晶圓上沉積約 1 〇 0奈米的氮化 物。使用類似製程來沉積多晶矽和氮氧化矽。另外,高溫 製程包含氧化、退火、矽化、和通常使用較高溫度的其他 製程,例如高於1 000°C或甚至1 3 5 0°C。 就大規模商業生產而言,慣常使用垂直爐管以及在爐 管内支撐大量晶圓的垂直設置的晶圓塔,通常是以第1圖 之簡要剖面圖所示的配置。爐管1 〇包含一絕熱加熱筒1 2, 支撐由未示出的電源供應器供電之電阻加熱線圈14。一鐘 罩1 6,通常由石英組成,包含頂板並裝設在該加熱線圈1 4 内部。一開放式内襯1 8裝設在該鐘罩16内部。一支撐塔 20座落在一台座22上,並且在製程期間,該台座22和支 撐塔20通常是被該内襯18圍繞。其包含垂直設置的狹縫, 5 200842213 以谷納多個欲以批次模式熱處理之水平設置的晶圓。一 體注入器24主要設置在該内襯18之間,擁有一出口在 上端以注入製程氣體至該内襯18内部。一未示出的真空 浦透過該鐘罩16的底部除去製程氣體。該加熱筒ι2、 罩16、和内襯18可被垂直升起,以讓晶圓可傳送進出 塔20,雖然在某些配置中,這些元件在一升降機升起及 下該台座22並载入該塔20進出該爐管10底部的時候保 不動。 該鐘罩16,其上端是封閉的,有助於使該爐管 其中段及上半部分擁有普遍的均熱溫度。這被稱為熱區 其中溫度受到控制以擁有最佳熱製程。但是,鐘罩1 6開 的底部和台座22的機械支撐使該爐管的下半部溫度 低’通常低到使例如化學氣相沉積的熱製程無法有效 行。該熱區可排除該塔2 0的一些較低的狹縫。 習慣上在低溫應用中,該塔、内襯、和注入器係由 英或熔化的矽土組成。但是,石英塔和注入器被矽塔和 入器取代。可從加州 Sunnyvale 的 Integrated Materials 司取得之一種矽塔的配置在第2圖的正交視圖中示出。 包含與三或四個内部形成有狹縫以支撐多個晶圓3 8的 支腳3 4連結的矽基座3 0、3 2。該等狹縫之間的指狀物 形狀和長度隨著應用及製程溫度而改變。此種塔的製造 Boyle等在美國專利第6,455,395號中描述。矽注入器也 從 Integrated Materials 公司取得,如 Zehavi 等在 2005 7月8號提出申請之美國專利申請案第1 1 /1 77,808號, 氣 其 幫 鐘 該 降 持 在 放 較 進 石 注 公 其 矽 之 由 可 年 並 6 200842213 經公開為美國專利申請公開案第1 006/ 1 08 5 5 89號中所揭 示者。矽内襯已由Boyle等在美國專利第7,1 3 7,546號中 提出。 該塔的高度可根據該爐管的高度調整,並且可包含超 過1 00個晶圓用的狹縫。如此大量的晶圓引發熱緩衝晶圓 (thermal buffer wafers)和測試晶圓(dummy wafers)的使 用,以確保生產晶圓在該熱區内遭遇到均勻的熱環境。熱 製程期間該塔内之晶圓堆疊的頂部及底部兩者皆受到熱端 效應。明確地說,底部的晶圓被加熱至顯著較低的溫度, 並且該溫度可能低到使氮化物 CVD製程或其他熱製程失 效。據此,將熱擋晶圓而非實質上單晶的矽生產晶圓置於 最上端和最下端狹缝中,以熱緩衝該堆疊的端點並提供置 於其間的生產晶圓更均勻的溫度分布。通常,台座22係經 配置以容納熱擋晶圓,其被留在烘箱内許多個週期。該等 熱擋晶圓也發揮從該爐管環境中清除不純物的作用,其有 在該爐管頂部和底部較為稠密的傾向。在每一端使用多至 六個或十二個熱擋晶圓並非不尋常。該等熱擋晶圓在多個 週期中重複使用,但目前的熱擋晶圓通常被限制在不多於 四或五次週期。 - 矽生產晶圓通常係以約2 5個晶圓的批次來處理,相當 . 於將其在製造設備之間傳送的承載晶圓匣的容量。大數量 的晶圓狹缝使多個批次可以被同時處理。但是,會有需要 熱處理少於最大數量的批次的情況。這些情況包含實驗室 内的製程研發和生產時偶爾進行之使用測試晶圓的製程校 7 200842213 正。氮化物沉積有對於該烘箱的載荷敏感的趨勢。也就是 說,若沒有填充所有的晶圓狹缝,製程會改變。在這些情 況中,常會藉由在空的狹縫中插入測試晶圓而仍然完全填 滿該塔。多晶矽沉積經受到稍為類似的載荷。另一方面, 氧化則是有對於載荷相對不敏感的傾向。 ' 該烘箱頂部於製程氣流上游側的測試晶圓和熱擋晶圓 需被監控以防過量微粒的產生,因為薄膜的建立。也就是 說,在每一個如此多的週期之後,其需要以新的測試和熱 Ο 擋晶圓或再生的晶圓置換。另一方面,位於該烘箱底部的 熱擋晶圓可能仍然產生微粒,但該等微粒沒有影響上游生 產晶圓的趨勢。 測試和熱擋晶圓會被集體稱為非生產晶圓。 熱缓衝晶圓和測試晶圓會被共同稱為非生產晶圓。 過去,與石英塔搭配,該等非生產晶圓通常是由石英 (熔化的矽土)組成,其不昂貴並擁有對於紅外線輻射不透 明的進一步優點,因此減輕充斥該塔之大於4 · 5微米(石英 I j 的傳輸邊緣)的輻射的端點效應。但是,就像石英塔般,認 知到石英缓衝和測試晶圓會提供微粒的產生至製造先進元 件無法滿意的程度。用生產型單晶矽晶圓來做為非生產晶 圓並沒有完全成功。觀察到其在重覆使用時會很容易斷 裂。進一步在氮化物沉積製程中,在多次使用下氮化矽於 非生產晶圓上沉積至較大厚度並且觀察到剝落,再一次造 成微粒問題。結果是,在先進製造中,單晶矽非生產晶圓 的壽命限制在僅有數個週期,在其被丟棄或再生之前。 8 200842213 目前使用單晶矽晶圓作為測試晶圓。其與生產晶圓非 常相似,除了其可由較低等級的矽製成之外。其並未有十 分令人滿意的表現。在沉積LPCVD氮化矽的應用中,發 現必須在累積約3 3 0奈米的氮化物之後將其置換掉,因為 超過此膜厚就會開始散發微粒。因為某些應用可能在每個 週期沉積1 1 〇奈米的氮化物,該厚度限制表示必須在每三 個週期左右就將該等測試晶圓移除。再清潔該等測試晶圓 然後再使用是很常見的。但是,通常只執行兩次再清潔, 因為單晶晶圓看來會在進一步的再清潔中產生條紋。據 此,在約3 3 0奈米的氮化物或三個週期之後,該等測試晶 圓會被丟棄。 也使用過碳化矽非生產晶圓,特別是在較高溫度下。 但是’碳化砍晶圓’特別是用C V D長成之塊狀碳化碎,是 昂貴的並且也遭遇到碳化矽晶圓和矽塔之間熱膨脹係數的 差異所引起的效應。 據此,希望擁有較不昂貴的非生產晶圓,其仍然提供 優良的效能,包含加固性(ruggedness)和擁有較大的氮化物 和沉積在其上的其他材料之厚度而不會剝落。 【發明内容】 本發明之一態樣包含隨機取向多晶矽(ROP Si),例如, 用柴氏長晶法(C ζ 〇 c h r a 1 s k i,C Z)藉由從石夕炫液拉引晶種長 成。該晶種自身可以是隨機取向多晶矽。其可由原生(virgin) 多晶矽棒切割出,也稱為電子級矽,從矽烷類材料之前驅 9 200842213 物利用化學氣相沉積(CVD)長成。或者,該晶種可從一 CZ 長成的晶棒(i n g 〇 t)切割出,其係運用從起源於C V D的晶種 長成之晶棒切割下的晶種。在後者的情況中’該晶種之至 少一遠端世代係源自原生多晶矽或起源於此種 CVD長成 之晶種的晶種。200842213 IX. Description of the Invention: TECHNICAL FIELD OF THE INVENTION The present invention generally relates to heat treatment of tantalum wafers. More specifically, there are non-productive crystals used in batch heat treatment of wafers. The invention also relates to polysilicon types that can be used as such non-productive wafers and for other applications. [Prior Art] Batch heat treatment is continued for use in several stages of the manufacture of entanglement circuits. A low temperature heat treatment deposits a layer of tantalum nitride by low temperature chemical vapor deposition (LPCVD), typically using chlorosilane and ammonia as precursor gases at a temperature range of about 700 °C. In one application, about 1 〇 0 nm of nitride was deposited on all wafers in the oven in each cycle. A similar process is used to deposit polycrystalline germanium and bismuth oxynitride. In addition, high temperature processes include oxidation, annealing, deuteration, and other processes that typically use higher temperatures, such as above 1 000 ° C or even 1 350 ° C. For large-scale commercial production, a vertically disposed wafer tower that conventionally uses a vertical furnace tube and supports a large number of wafers in the furnace tube is generally configured as shown in the schematic cross-sectional view of Fig. 1. The furnace tube 1 〇 includes a heat insulating heating cylinder 12 that supports a resistance heating coil 14 that is powered by a power supply not shown. A bell cover 1-6, usually composed of quartz, includes a top plate and is mounted inside the heating coil 14. An open inner lining 18 is mounted inside the bell jar 16. A support tower 20 is seated on a pedestal 22, and the pedestal 22 and the support tower 20 are typically surrounded by the lining 18 during the process. It consists of a vertically set slit, 5 200842213 A wafer set at a level that is intended to be heat treated in batch mode. A bulk injector 24 is disposed primarily between the liners 18 and has an outlet at the upper end for injecting process gases into the interior of the liner 18. A vacuum, not shown, removes the process gas through the bottom of the bell jar 16. The heating cartridge ι2, the cover 16, and the liner 18 can be raised vertically to allow the wafer to be transported into and out of the tower 20, although in some configurations these components are raised and lowered on the pedestal 22 and loaded The tower 20 does not move when it enters the bottom of the furnace tube 10. The bell jar 16 has an upper end that is closed to help maintain a common soaking temperature in the middle and upper portions of the bellows. This is called the hot zone where the temperature is controlled to have the best thermal process. However, the bottom of the bell jar 16 and the mechanical support of the pedestal 22 cause the lower half of the furnace tube to be low 'typically low enough that a thermal process such as chemical vapor deposition is not effective. This hot zone can exclude some of the lower slits of the tower 20. Conventionally, in low temperature applications, the tower, lining, and injector are composed of fused or fused alumina. However, the quartz column and injector are replaced by a turret and an inlet. A configuration of a turret that is available from Integrated Materials, Sunnyvale, Calif., is shown in the orthogonal view of FIG. The crucible bases 3 0, 3 2 are joined to three or four legs 3 4 having slits formed therein to support the plurality of wafers 38. The shape and length of the fingers between the slits vary with application and process temperatures. The manufacture of such a tower is described in U.S. Patent No. 6,455,395. The helium injector was also obtained from Integrated Materials, Inc., such as Zehavi et al., filed on July 8, 2005, the US patent application No. 1 1 /1 77,808, which should be lowered to the public. It is disclosed in U.S. Patent Application Publication No. 1 006/1 08 5 5 89. The lining has been proposed by Boyle et al. in U.S. Patent No. 7,133,546. The height of the tower can be adjusted according to the height of the tube and can include slits for more than 100 wafers. Such a large number of wafers initiate the use of thermal buffer wafers and dummy wafers to ensure that the production wafer encounters a uniform thermal environment in the hot zone. Both the top and bottom of the wafer stack within the tower are subjected to a hot end effect during the thermal process. Specifically, the bottom wafer is heated to a significantly lower temperature, and the temperature may be low enough to disable the nitride CVD process or other thermal processes. Accordingly, a hot-wafer wafer, rather than a substantially single-crystalline germanium production wafer, is placed in the uppermost and lowermost slits to thermally buffer the end of the stack and provide a more uniform production wafer therebetween. Temperature Distribution. Typically, the pedestal 22 is configured to accommodate a heat shield wafer that is left in the oven for many cycles. These heat shield wafers also function to remove impurities from the furnace tube environment, which tends to be denser at the top and bottom of the tube. It is not unusual to use up to six or twelve heatsink wafers at each end. These heat shield wafers are reused over multiple cycles, but current heat shield wafers are typically limited to no more than four or five cycles. - 矽 Production wafers are typically processed in batches of approximately 25 wafers, equivalent to the capacity of the carrier wafers that are transferred between manufacturing equipment. A large number of wafer slits allow multiple batches to be processed simultaneously. However, there may be cases where it is necessary to heat treat less than the maximum number of batches. These conditions include process development in the laboratory and occasional use of test wafers during process development. Nitride deposits have a tendency to be sensitive to the load of the oven. That is, if all of the wafer slits are not filled, the process will change. In these cases, the tower is still completely filled by inserting a test wafer into an empty slit. The polycrystalline germanium deposits are subjected to slightly similar loads. On the other hand, oxidation is a tendency to be relatively insensitive to loads. The test wafer and the heat shield wafer on the upstream side of the process gas flow at the top of the oven are monitored to prevent the generation of excess particles due to the build-up of the film. That is, after so many cycles, it needs to be replaced with new test and thermal wafers or regenerated wafers. On the other hand, the heat shield wafer at the bottom of the oven may still produce particles, but the particles do not affect the upstream production of wafers. Test and heat shield wafers are collectively referred to as non-production wafers. Thermal buffer wafers and test wafers are collectively referred to as non-production wafers. In the past, in conjunction with quartz towers, these non-productive wafers were typically composed of quartz (melted alumina), which was inexpensive and had the further advantage of being opaque to infrared radiation, thereby reducing the flooding of the tower by more than 4.5 microns ( The end effect of the radiation of the transmission edge of quartz I j ). However, like quartz towers, it is recognized that quartz buffers and test wafers provide the ability to produce particles that are unsatisfactory to the manufacture of advanced components. The use of production-type single crystal germanium wafers as non-productive crystals has not been entirely successful. It was observed that it would break easily when it was used repeatedly. Further in the nitride deposition process, tantalum nitride is deposited on a non-productive wafer to a large thickness and observed to be peeled off under repeated use, again causing particle problems. As a result, in advanced manufacturing, the lifetime of a single crystal germanium non-production wafer is limited to only a few cycles before it is discarded or regenerated. 8 200842213 Single crystal germanium wafers are currently used as test wafers. It is very similar to a production wafer except that it can be made from a lower grade of tantalum. It did not have a satisfactory performance. In the application of LPCVD tantalum nitride, it has been found that it has to be replaced after accumulating about 3,300 nm of nitride, since particles are emitted beyond this film thickness. Since some applications may deposit 1 1 nanometer of nitride per cycle, this thickness limitation means that the test wafers must be removed every three cycles or so. It is very common to clean these test wafers and then use them. However, re-cleaning is usually performed only twice because the single crystal wafer appears to produce streaks in further re-cleaning. Accordingly, after about 3 300 nm of nitride or three cycles, the test crystals are discarded. Non-carbonized niobium is also used to produce wafers, especially at higher temperatures. However, the "carbonization chopping wafer", especially the bulk carbonization of the C V D, is expensive and also suffers from the effect of the difference in thermal expansion coefficient between the tantalum carbide wafer and the crucible. Accordingly, it is desirable to have less expensive non-productive wafers that still provide superior performance, including ruggedness and the thickness of the larger nitride and other materials deposited thereon without peeling off. SUMMARY OF THE INVENTION One aspect of the present invention includes randomly oriented polycrystalline germanium (ROP Si), for example, by using Chai's long crystal method (C ζ 〇chra 1 ski, CZ) to grow seed crystals from Shi Xi Xuan liquid. . The seed crystal itself may be a randomly oriented polycrystalline germanium. It can be cut from a virgin polycrystalline ruthenium rod, also known as an electronic grade ruthenium, which is grown from decane-based materials by chemical vapor deposition (CVD). Alternatively, the seed crystal may be cut from a CZ grown ingot (i n g 〇 t) using a seed crystal cut from an ingot grown from a seed crystal derived from C V D . In the latter case, at least one of the distal generations of the seed crystal is derived from a primary polycrystalline germanium or a seed crystal derived from such a seed crystal grown into CVD.
本發明之另一觀點包含多晶矽缓衝和測試晶圓,集體 稱為非生產晶圓。更佳地,該等多晶矽晶圓係從一隨機取 向多晶碎晶種長成的晶棒切割下,例如’一起源於C V D的 晶種。 在典型的使用中,本發明之非生產晶圓係與單晶矽生 產晶圓一起置於一塔上,並且在一爐管或其他熱處理設備 内同步處理。 該非生產晶圓可以一多步驟製程製備。在從該晶棒切 割下之後,該晶圓可被蝕刻,例如,在一鹼性溶液中以降 低或消除張力。該晶圓,較佳地在張力蝕刻後,經歷表面 處理而產生次表面傷害在其兩個主要表面上,並且或許在 其周邊上。該次表面傷害可利用喷砂處理(bead blasting) 或利用研磨或加工執行。該表面受損的晶圓然後經歷酸洗 步驟,接著是超音波清潔。 C Z長成或隨機取向多晶矽也可用來形成加工結構,因 為其純度、良好的多晶矽結構、以及加固性。 【實施方式】 我們相信單晶矽晶圓不適合用來做為熱擋及測試晶 10 200842213 圓,集體稱為非生產晶圓。了解到生產晶圓通常並非完美 的單晶,並且可能有一些缺陷,包含錯位(dislocation)和滑 移(slip)。但是,該等缺陷就合理的生產良率而言通常是極 微的,並且典型目標是得到並保持低錯位和無滑移的單晶 生產晶圓。 ΟAnother aspect of the invention includes polysilicon buffer and test wafers, collectively referred to as non-production wafers. More preferably, the polycrystalline silicon wafers are cut from an ingot grown from a randomly oriented polycrystalline seed crystal, such as a seed crystal derived from C V D together. In a typical use, the non-productive wafers of the present invention are placed on a column with a single crystal germanium wafer and processed simultaneously in a furnace tube or other heat treatment apparatus. The non-productive wafer can be prepared in a multi-step process. After being cut from the ingot, the wafer can be etched, for example, in an alkaline solution to reduce or eliminate tension. The wafer, preferably after a etch process, undergoes a surface treatment to cause subsurface damage on its two major surfaces, and perhaps on its periphery. This surface damage can be performed by bead blasting or by grinding or machining. The surface damaged wafer is then subjected to a pickling step followed by ultrasonic cleaning. CZ grown or randomly oriented polycrystalline germanium can also be used to form processed structures due to their purity, good polycrystalline structure, and reinforcement. [Embodiment] We believe that single crystal germanium wafers are not suitable for use as heat shields and test crystals. It is known that production wafers are usually not perfect single crystals and may have some drawbacks, including dislocations and slips. However, such defects are typically minimal in terms of reasonable production yield, and the typical goal is to obtain and maintain low misalignment and no slip single crystal production wafers. Ο
若單晶晶圓的邊緣在重複用做非生產晶圓下碎裂,該 缝隙可能會沿著結晶劈裂面(cleavage planes)在該晶圓上 蔓延並使其斷裂。商業級單晶晶圓更不適合用來做為非生 產晶圓,因為很昂貴。雖然在較舊的晶圓背側做表面處理, 同時在其前表面拋光,但非常先進的製造要求在生產晶圓 的前及後表面兩面皆拋光。單晶晶圓也不利於重複用做緩 衝和熱晶圓,因為其在大量的高溫處理後翹曲成洋芋片形 狀或其他彎曲形狀的傾向。過去曾使用半單晶非生產晶 圓,但其承受許多單晶非生產晶圓的不便,例如,沿著偏 好的結晶面斷裂。 取代單晶生產晶圓,偏好由多晶矽形成該等非生產晶 圓。第3圖之平面圖所示之多晶矽非生產晶圓4 0擁有與單 晶矽生產晶圓非常類似的形狀,但其有可見的隨機晶粒結 構而非單晶晶圓的無特徵表面。非生產晶圓的直徑應落在 生產晶圓適用之工業標準内,也就是,目前晶圓生產最流 通的約2 0 0或3 0 0毫米,但持續使用1 5 0毫米晶圓,並且 預期到4 5 0毫米的晶圓。雖然如此,非生產晶圓會稍微厚 一些,並且不需要有標準晶圓的特徵,例如取向斜角(bevel) 或刻痕(notch)。可見標記42,例如產品編號和序號,可形 11 200842213 成在主表面上。也偏向於表面處理非生產晶圓兩側’以提 供在多個週期中所沉積之較厚層更具附著力的基礎。 原生多晶石夕,也稱為電子級矽(electronic grade silicon, EGS)’是大部分柴氏法(匚乙)長成的用來做為生產晶圓之石夕 的來源材料。近來使用原生多晶石夕來製造晶圓塔和其他結 構’如上面Boyle等之兩個專利文件中所描述者。原生多 曰曰曰石夕係、利用矽烷或鹵矽烷之化學氣相沉積在約6 0 0。(:或更If the edge of a single crystal wafer is broken under repeated use as a non-productive wafer, the gap may spread and break on the wafer along the cleavage planes. Commercial grade single crystal wafers are less suitable for use as non-production wafers because they are expensive. Although surface treatment is performed on the back side of the older wafer while polishing on the front surface, very advanced manufacturing requires polishing both sides of the front and back surfaces of the wafer. Single crystal wafers are also not suitable for repeated use as buffers and hot wafers because of their tendency to warp into a matrix shape or other curved shape after extensive high temperature processing. Semi-monocrystalline non-produced wafers have been used in the past, but they suffer from the inconvenience of many single-crystal non-productive wafers, for example, along a relatively good crystal plane. Instead of producing a single crystal wafer, it is preferred to form the non-productive crystals from polycrystalline germanium. The polycrystalline germanium non-product wafer 40 shown in the plan view of Figure 3 has a very similar shape to a single wafer germanium wafer, but has a visible random grain structure rather than a featureless surface of a single crystal wafer. The diameter of non-production wafers should fall within the industry standard applicable to the production of wafers, that is, the current circulation of wafers is about 200 or 300 mm, but the continuous use of 150 mm wafers is expected. To 450 mm wafers. Nonetheless, non-productive wafers are somewhat thicker and do not require the characteristics of standard wafers, such as orientation bevels or notches. Visible markers 42, such as product numbers and serial numbers, can be formed on the main surface. It is also biased to surface treat both sides of the non-product wafer to provide a more adherent basis for thicker layers deposited over multiple cycles. The original polycrystalline stone, also known as electronic grade silicon (ESS), is the source material used by most of the Chai method (匚乙) to be used as a wafer for the production of wafers. Wafer towers and other structures have recently been fabricated using native polycrystalline slabs as described in the two patent documents of Boyle et al. The primary multi-stone system, chemical vapor deposition using decane or halodecane is about 600. (: or more
南溫中於氫氣存在下在熱的矽晶種棒上長成。例如二矽烷 之’、他石夕燒可以取代。見Wolf等在2000年Lattice Press 之VLSI時代之矽製程:卷1一製程科技,第二版第5-8頁。 來自石夕燒的原生多晶矽成長因為其純度而有潛在優勢,但 從一氯石夕燒或其他鹵矽烷長成的原生多晶矽是更經濟的。 如此長成’一原生多晶矽晶棒5 〇擁有第4圖所示之剖面結 構、纟σ晶樹枝5 2從晶種棒5 4往外延伸。原生多晶矽一般 會長成為帶有高内應力,其通常會防止材料被加工。但是, y e等所解釋者,4退火該原生多晶$,則其可能被 加工’因為退火合消 '、應力。從純矽烷(SiH4)長成的原生 夕晶矽一般擁有比從三氯 私尽说長成者小的微晶。 根據本發明之一態樣,客曰 n 夕日日石夕晶棒也可利用Wolf等在 ibid第8-21頁描述的單 ^ ^ y- ^ η, ^ , 日日棒之柴氏長晶法(CZ)長成(從 矽熔液拉引或推送)。大 … 了的多晶CZ矽可從少許公司取 仟。此種矽含有許多微晶, ^ ^ 一暴路面通常是由表面法線±20 度内的<100>取向微晶組 Χ 雖然可在適當條件下取得例 如<111>或<11〇>的其他偏 野取向。可表面處理此種半單晶 12 200842213 材料。其與單晶矽相比較沒有裂缝蔓延的傾向,但是裂缝 仍可因為較佳取向而蔓延。也可取得在石央每权内每成的 多晶碎,但其純度水準比取自CZ長成的多晶石夕者低。 一般來說,根據本發明之一態樣,多晶cz矽,其傾The south temperature grows on the hot twin seed in the presence of hydrogen. For example, the dioxane's, he can be replaced by Shi Xi. See Wolf et al., Vatti Era, Lattice Press, 2000: Volume 1 Process Technology, Second Edition, pp. 5-8. The growth of native polycrystalline germanium from Shi Xi-sing has potential advantages due to its purity, but native polycrystalline germanium grown from chlorite or other halosilanes is more economical. Such a grown-up polycrystalline twin rod 5 has a cross-sectional structure as shown in Fig. 4, and the 纟σ crystal branch 5 2 extends outward from the seed rod 5 4 . Primary polycrystalline germanium generally grows with high internal stresses, which usually prevent the material from being processed. However, as explained by y e et al., 4 annealing the native polycrystalline $, it may be processed 'because annealing is eliminated', stress. The native cerium grown from pure decane (SiH4) generally has smaller crystallites than those grown from trichlorin. According to one aspect of the present invention, the guest can also use the single ^ ^ y- ^ η, ^ described by Wolf et al. on pages 8-21 of ibid, the Japanese and Japanese Chai's long crystal method. (CZ) grows into (pulsed or pushed from the crucible). The polycrystalline CZ矽 that is large can be taken from a few companies. Such ruthenium contains many crystallites, ^ ^ a turbulent pavement is usually a <100> oriented microcrystal group within ±20 degrees of the surface normal, although it may be obtained under appropriate conditions such as <111> or <11〇 > Other biased orientations. The semi-single crystal 12 200842213 material can be surface treated. It has no tendency to crack propagation compared to single crystal germanium, but cracks can still propagate due to better orientation. It is also possible to obtain polycrystalline shreds per stone in each of the Shiyang, but the purity level is lower than that of the polycrystalline stone grown from CZ. In general, according to one aspect of the invention, polycrystalline cz矽, which is tilted
向於隨機取向,可利用一多晶吵 向多晶石夕(randomly oriented polycrystalline silicon, R0Psi) ’而非典型的單晶晶種或先前偶爾使用的得自半單 晶石夕之多晶晶種。可使用標準柴氏晶體成長爐管,但是應 包含圓錐形熱擋板,其延伸至熔液表面的40亳米内。回填 氯氣的腔室壓力可維持在丨〇至5〇托耳内。在原生多晶矽 或可此*丢棄的柴氏物料(CZ charge)已經熔化並且溫度穩 疋之後’將晶種浸入該熔液表面並保持在其中直到該晶種 炫1液"面形成圓滑的新月型為止。然後以足以讓直徑低 於晶種的頸部不會形成的速率提拉該晶種。一接合該晶種 2〇〇亳米或300毫米晶棒之簡單的圓錐形擴充區域可延 超過1 0至20公分。然後調整提拉速率以維持預期的晶 直k。可以比單晶cz晶棒快的速率提拉多晶矽cZ晶 t在該提拉尾聲只需要最小的尾端結束錐度(end aper)。提拉出的晶棒應在一般環境中慢慢冷卻。 第5圖之剖面圖示出的從利用石夕燒或三氯石夕貌前驅物 鼠體製出之原生多晶的多晶晶種异 勘 夕日日日日種長成之多晶CZ晶棒60被 規察到產生形狀稍微不規則的 ^、 况⑴们傲日日之外側區62以及形狀 ::對稱之尺寸通常…公分的稱為大一些的微晶之内 。。64。該圖式並沒有精準示出微晶的尺寸。在某些實施 13 200842213 中,3至1 0毫米的微晶隨機散佈在晶圓上。一般來說,可 改變成長條件以將該分佈控制在1至1 〇亳米内的預期分 佈。 本發明之CZ多晶成長之一實施例使用退火該晶棒50 以容許其加工之後,沿著該晶棒5 0的軸從該原生多晶晶棒 5 0的外側區切割出的晶種棒6 6,在第4圖中示出。用於 CA成長之原生多晶晶種產生第5圖之剖面圖所示之晶棒 ΓFor random orientation, a polycrystalline silicon (R0Psi) can be used instead of a typical single crystal seed crystal or a polycrystalline seed crystal obtained from a semi-single crystal stone. . A standard C# crystal growth furnace tube can be used, but should include a conical heat shield that extends into the 40 mm surface of the melt surface. The chamber pressure for backfilling chlorine can be maintained in the range of 丨〇 to 5 Torr. After the primary polysilicon or the CZ charge that has been discarded has been melted and the temperature is stable, the seed is immersed in the surface of the melt and held therein until the crystal is smooth and smooth. New moon type. The seed crystal is then pulled at a rate sufficient to prevent the neck of the diameter below the seed crystal from forming. A simple conical expansion region joining the seed 2 m or 300 mm ingot can be extended by more than 10 to 20 cm. The pull rate is then adjusted to maintain the desired crystal k. The polycrystalline crucible cZ crystal can be pulled at a faster rate than the single crystal cz ingot. At this pull tail, only the minimum end end aper is required. The crystal rods that are pulled out should be slowly cooled in the general environment. Fig. 5 is a cross-sectional view showing a polycrystalline CZ crystal rod 60 grown from the day of the day using a polycrystalline seed crystal of the original system of the shovel or the smectite precursor. It is observed that the shape is slightly irregular. (1) The outer side of the outer zone 62 and the shape: the size of the symmetry is usually ... the centimeter is called the larger crystallite. . 64. This figure does not accurately show the size of the crystallites. In some implementations 13 200842213, 3 to 10 mm of crystallites are randomly scattered on the wafer. In general, the growth conditions can be varied to control the distribution to an expected distribution within 1 to 1 mil. One embodiment of the CZ polycrystal growth of the present invention uses a seed rod cut from the outer region of the native polycrystalline ingot 50 along the axis of the ingot 50 after annealing the ingot 50 to allow processing thereof. 6 6, shown in Figure 4. The native polycrystalline seed crystal used for CA growth produces the ingot shown in the cross-sectional view of Figure 5.
6 0。此種C Ζ晶棒6 0的材料可以C V D源矽為特徵,因為 其晶體結構係源自CVD產生之原生多晶。 晶棒60係由紐約之Kayex of Rochester在本發明人之 指示下利用直徑約1公分且長度約2 0公分的矽晶種棒長 成。由矽烷和三氯矽烷做為CVD前驅物氣體所形成的兩種 原生多晶矽材料之晶種產生實質上類似的CZ長晶結果。 利用 Laue X光實驗來建立此種材料的切片或晶圓之 結晶學。判定該多晶矽展現出實質上隨機取向的微晶,且 相對於該晶棒軸或其他軸無較佳的常規取向。 可能使用一種多晶CZ晶棒70,在第6圖的剖面圖中 示出,(其可以是第5圖的晶棒60)做為進一步晶種的來 源,例如藉由從該晶棒7 〇切下一徑向插塞7 8或其厚切片, 並使用該插塞做為多晶CVD來源矽之另一世代的晶種。明 確地說,該插塞7 8末端靠近該晶棒外部邊緣處可能有較小 的微晶尺寸,並且是該晶種接觸該矽熔液的較佳部份。若 需要取得足夠長度的晶種棒,可焊接或以其他方式連結一 較短的ROPSi晶種至一較長的矽晶棒,因為大部分的晶種 14 200842213 棒組件不會浸入該熔液,並且該較長的晶棒可以再 可用從前一個世代發展出的晶種長成下一個世代ά 來源CZ晶棒。CVD來源晶種包含從任何類型的含 驅物材料長成之原生多晶的最初世代,包含但不 烷、一氯矽烷、二氯矽烷、三氯矽烷、和四氯矽烷 他_矽烷和多矽烷,並且從C Ζ多晶矽切下的下世 擁有可追溯至該原生多晶晶種的晶種。 Ρ 其他類型的多晶矽,特別是隨機取向多晶矽, 發明之非生產晶圓並用。該等多晶矽晶圓可由澆鑄 或是以除了原生多晶矽以外的晶種柴氏拉引形成。 始於多晶晶棒之缓衝和測試晶圓的製造在某種 遵循用來從單晶晶棒製造單晶生產晶圓的製程。該 要有比晶圓稍微大一些的直徑。先進商業生產的 2 00毫米逐漸變為300毫米,雖然標準晶圓尺寸仍 亳米、1 0 0毫米、1 2 5毫米、和1 5 0毫米。預期下世 會有4 5 0毫米的直徑。 多晶ROPSi或其他多晶矽晶圓可用第7圖的流 括示出之製程80形成,其合併並改造Wolf等之 22-31頁所描述的標準生產晶圓製程和在Boyle等 - 參考文獻中所述的用來形成原生多晶塔的製程。取 . 能要求和製造結果,某些步驟可以省略。該CZ多 來可輕易加工而不需進一步的退火,可能是因為從 之CZ拉引有效退火該多晶矽。在步驟82,較佳地 石刀刃或鑽石漿以線鋸或是内部或外部圓鋸從該晶 使用。 ή CVD 矽烷前 限於矽 以及其 代晶種 可與本 矽形成 程度上 晶棒需 直徑從 舊是75 代晶圓 程圖概 ibid 第 之兩篇 決於效 晶砍看 該熔液 使用鑽 棒切下 156 0. The material of such a C-crystal rod 60 can be characterized by a C V D source, since its crystal structure is derived from the native polycrystal produced by CVD. The ingot 60 was grown by a Kayex of Rochester, New York, under the direction of the inventors, using a twin seed rod having a diameter of about 1 cm and a length of about 20 cm. Seed crystals of two primary polycrystalline germanium materials formed from decane and trichloromethane as CVD precursor gases produce substantially similar CZ crystal growth results. Laue X-ray experiments were used to create slicing of wafers or wafers of such materials. It is determined that the polycrystalline germanium exhibits crystallites that are substantially randomly oriented and that there is no preferred conventional orientation relative to the ingot axis or other axis. It is possible to use a polycrystalline CZ ingot 70, shown in the cross-sectional view of Fig. 6, which may be the ingot of Fig. 5, as a source of further seeding, for example by crystallization from the ingot 7 The radial plug 7 8 or its thick section is cut and used as a seed for another generation of polycrystalline CVD source. Specifically, the end of the plug 7 8 may have a smaller crystallite size near the outer edge of the ingot and is a preferred portion of the seed that contacts the crucible melt. If it is necessary to obtain a seed rod of sufficient length, a shorter ROPSi seed crystal may be welded or otherwise joined to a longer crystal rod because most of the seed crystal 14 200842213 rod assembly will not be immersed in the melt. And the longer ingot can be grown into the next generation 来源 source CZ ingot from the seed developed from the previous generation. CVD source seed crystals comprise the first generation of native polycrystals grown from any type of flood-containing material, including butane, monochloromethane, dichlorodecane, trichlorodecane, and tetrachlorodecane and decane. And the next generation cut from C Ζ polycrystalline enamel has a seed crystal that can be traced back to the native polycrystalline seed crystal. Ρ Other types of polycrystalline germanium, especially randomly oriented polycrystalline germanium, are used in combination with non-productive wafers of the invention. The polycrystalline silicon wafers may be formed by casting or by seeding of a seed crystal other than the native polycrystalline germanium. The fabrication of buffers and test wafers starting with polycrystalline ingots follows a process that follows the process of fabricating a single crystal from a single crystal ingot. It should have a slightly larger diameter than the wafer. The advanced commercial production of 200 mm gradually changed to 300 mm, although the standard wafer size was still 亳米, 100 mm, 1.25 mm, and 150 mm. It is expected that there will be a diameter of 450 mm in the next life. Polycrystalline ROPSi or other polycrystalline germanium wafers may be formed using the process 80 illustrated in Figure 7, which incorporates and modifies the standard fabrication wafer process described on pages 22-31 of Wolf et al. and in Boyle et al. - references The process described to form a native polycrystalline column. Take. Can require and manufacture results, some steps can be omitted. The CZ can be easily processed without further annealing, possibly because the polysilicon is effectively annealed from the CZ pull. At step 82, preferably the stone blade or diamond slurry is used from the crystal with a wire saw or an internal or external circular saw. CVD CVD 矽 前 前 前 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 矽 CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD CVD Next 15
200842213 多晶晶圓。 在步驟84,研磨該多晶矽晶圓至預期圓形形狀 可以Blanchard研磨機利用鑽石磨粒在與研磨類似 中平磨該多晶矽晶圓兩側。較佳地將其邊緣塑形為 產晶圓。生產晶圓的厚度通常是2〇〇毫米晶圓為〇 米’或3 0 0宅米晶圓的0 · 7 7 5亳米。預期使該緩衝 晶圓盡可能粗糙,所以較厚的非生產晶圓佔有優勢。 初始的非生產晶圓批次係經製備為擁有1〇至15 甚至2毫米的厚度。也就是說,如第8圖的剖面圖 非生產晶圓100較佳地擁有0· 725至15亳米或也許 至2毫米範圍内的厚度t。大部份的生產設備可容 稍微厚一些的晶圓。但預期厚度實質上與生產晶圓 非生產晶圓在商業使用上會有令人滿意的表面,雖 糙度可能比厚的晶圓低。研磨導入次表面加工傷害, 如第8圖所示,裂;廈102和裂、縫1〇4至從厚度t的晶 之兩個主要表面106、1〇8算起25至5〇微米的深200842213 Polycrystalline wafer. At step 84, the polysilicon wafer is ground to the desired circular shape. The Blanchard mill can use diamond abrasive particles to flatten both sides of the wafer in a similar manner to the grinding. The edges are preferably shaped into wafers. The thickness of the production wafer is usually 2 mm. The wafer is 0. 7 7 5 m of the wafer or 300 square meter wafer. It is expected that the buffer wafer will be as rough as possible, so thicker non-production wafers have an advantage. The initial non-production wafer batch is prepared to have a thickness of 1 〇 to 15 or even 2 mm. That is, the cross-sectional view as in Fig. 8 of the non-productive wafer 100 preferably has a thickness t in the range of 0·725 to 15 mm or perhaps to 2 mm. Most of the production equipment can accommodate a slightly thicker wafer. However, it is expected that the thickness will be substantially satisfactory for commercial use of the production wafer, non-productive wafers, although the roughness may be lower than for thick wafers. Grinding introduces subsurface processing damage, as shown in Fig. 8, cracking; Xi 102 and crack, slit 1〇4 to 25 to 5 μm deep from the two main surfaces 106, 1〇8 of the thickness t
ZehaVi等在2006年9月14曰提出申請之美國專利 第11/521,199號,並且公開為美國專利中&丨 2〇〇7/〇006799號中所解釋的,此特徵提供沉積在粗 上之薄膜的穩定依靠。此特徵,當在非生產曰曰曰圓上發 穩定在許多生產週期期間沉積出的厚沉積層之累積 減少剝落和所造成的微粒。晶圓切割可提供所需的 加工傷害。注意到並沒有拋光步驟,如在生產晶圓 者’其會除去該次表面傷害。 ’並且 的製程 類似生 .7 2 5 亳 和測試 據此, 宅米或 所示, 1 0.725 納這些 相當的 然其粗 包含, 圓100 度。如 申請案 開案第 糙的矽 •展時, ,因此 次表面 上執行 16 200842213 執行一選擇性的腐蝕或鹼性降張力蝕刻8 6,藉由將該 多晶晶圓浸泡在稀釋的氫氧化鉀(反〇11)内。該張力蝕刻86 釋放張力並通常清潔晶圓。但是,另一種製程僅在去離子 (DI)水浴中超音波清潔晶圓。在晶圓的兩個主要表面上執 行表面處理步驟88,以除去可見的切割和研磨之表面特 徵’以利進一步發展該次表面加工傷害,並留下均勻的灰 面。該表面處理可包含Blanchard研磨或加工,其產生預 0 期的次表面加工傷害。若不需要利用研磨之此後續表面加 工’可藉由使用碳化矽粉末的喷砂來除去可見的切割和研 磨之表面特徵。 在表面加工後,在步驟8 9 A,超音波清潔該晶圓。在 步驟89B,氧化該晶圓,例如,在空氣環境中於1100DC下 持續1 5小時。一第一酸性清潔步驟9 0係藉由將多晶晶圓 浸泡在稀釋的氫氟酸中執行。該第一酸性清潔步驟9 0在除 去晶圓表面上的任何氧化矽方面是有效的。一第二酸性清 潔步驟92係藉由將晶圓浸泡在水、氫氟酸、和過氧化氫 Ο (H2〇2)的混合液中執行,雖然硝酸(hN03)和氫氯酸(HC1) 可取代氫氟酸。該第二酸性清潔步驟92在從晶圓表面附近 除去重金屬方面是有效的。其它酸性蝕刻劑或其他類型的 ‘ 清潔劑可取代,例如,發展良好的用來清潔商用矽晶圓者 或其他用於晶圓的化學分析和儀器内者。藉由將晶圓浸泡 在去離子(DI)水浴内並超音波刺激DI水以從晶圓表面清 除微粒來執行超音波清潔步驟9 4。注意到所示製程並不包 含至少在生產晶圓的元件側執行的拋光。若希望,可在非 17 200842213 生產晶圓之一主要表面蝕刻上產品編號和序號以及其他識 別標記。此外,取決於晶圓廠實做,可在非生產晶圓的兩 側預先塗上一層 CVD沉積的會與非生產晶圓並用到的材 料,例如,氮化矽,其會穩固依附在裂痕和裂缝内。該多 晶晶圓然後即準備好在晶圓廠生產線上使用。 此種多晶非生產晶圓的壽命比單晶者長很多。其純度 水準比習知石英非生產晶圓高許多,並且其微粒產生低許 ^ 多。若在多晶非生產晶圓上的沉積累積至過量厚度,可再U.S. Patent No. 11/521,199, issued to theU. The stability of the film depends on it. This feature, when grown on a non-production round, stabilizes the accumulation of thick deposits deposited during many production cycles to reduce spalling and resulting particles. Wafer cutting provides the processing damage you need. It is noted that there is no polishing step, such as in the production of wafers, which will remove the surface damage. The process is similar to that of the student. 7 2 5 亳 and the test According to this, the house rice or as shown, 1 0.725 纳 These are quite thick and contain 100 degrees. If the application is opened in the rough 矽 • exhibition time, therefore, the surface is performed on 16 200842213 to perform a selective corrosion or alkaline tension etch 8 6 by immersing the polycrystalline wafer in diluted oxidized hydroxide Potassium (reverse 〇 11). This tension etch 86 releases the tension and typically cleans the wafer. However, another process only ultrasonically cleans the wafer in a deionized (DI) water bath. A surface treatment step 88 is performed on the two major surfaces of the wafer to remove visible surface features of the cut and grind to further develop the surface finish damage and leave a uniform gray surface. The surface treatment can include Blanchard grinding or processing that produces a pre-stage secondary surface processing damage. This subsequent surface finish can be removed by sandblasting using tantalum carbide powder if it is not necessary to utilize the subsequent surface processing of the grinding. After the surface is processed, in step 89 A, the wafer is cleaned by ultrasonic waves. At step 89B, the wafer is oxidized, for example, at 1100 dc for 15 hours in an air environment. A first acid cleaning step 90 is performed by immersing the polycrystalline wafer in dilute hydrofluoric acid. The first acid cleaning step 90 is effective in removing any ruthenium oxide on the surface of the wafer. A second acid cleaning step 92 is performed by immersing the wafer in a mixture of water, hydrofluoric acid, and hydrazine hydride (H2 〇 2), although nitric acid (hN03) and hydrochloric acid (HC1) may Replace hydrofluoric acid. This second acid cleaning step 92 is effective in removing heavy metals from the vicinity of the wafer surface. Other acidic etchants or other types of ‘cleaners can be substituted, for example, for well-developed commercial enamel wafers or other chemical analysis and instrumentation for wafers. The ultrasonic cleaning step 94 is performed by immersing the wafer in a deionized (DI) water bath and ultrasonically stimulating the DI water to remove particles from the wafer surface. It is noted that the illustrated process does not include polishing performed at least on the component side of the production wafer. If desired, the product number and serial number and other identification marks can be etched on one of the major surfaces of the non-2008 200842213 production wafer. In addition, depending on the fab, a layer of CVD-deposited and non-productive wafers, such as tantalum nitride, may be pre-coated on both sides of the non-production wafer, which will be firmly attached to the crack and Inside the crack. The polycrystalline wafer is then ready for use on the fab line. The lifetime of such polycrystalline non-productive wafers is much longer than that of single crystals. Its purity level is much higher than that of conventional quartz non-production wafers, and its particle generation is much lower. If the deposition on the polycrystalline non-production wafer accumulates to an excessive thickness,
P 生晶圓,例如藉由除去一部分的累積厚度,或將其全部除 去並重新進行第7圖的某些晶圓製造步驟。可藉由將多晶 矽晶圓浸泡在氫氟酸内以除去氮化物來將其再生或再清 潔。然後其可回到工作崗位。 初步測試顯示出在一 LPCVD製程中可在如此處理的 多晶矽測試晶圓上沉積2 · 5微米的氮化矽而不會有明顯的 剝落。這遠在過去在丟棄測試晶圓之前所使用的3 3 0奈米 厚度限制之上。晶圓薇生產線施以2微米的厚度限制做為 (J 其使用測試晶圓時進行主要更換的依據。即使是1微米的 厚度限制可代表優於先前技藝的顯著改善。此外,回收的 多晶矽測試晶圓並沒有展現出在回收的單晶矽測試晶圓上 觀察到的斑紋和條紋,因此可能再清潔本發明的測試晶圓 兩次以上。很清楚的,本發明的多晶石夕晶圓可在相同的 LPCVD製程内做為擋板晶圓。 可能希望繼續使用某些石英晶圓做為熱緩衝,特別是 在塔的底部,其係在熱區之外。該等石英緩衝晶圓提供對 18 Γ、 υ 200842213 於紅外線輻射之預期蔽光性。但3 該爐管㈣區内使用多晶晶圓1 ’較佳地在發生沉積之 碎,包含該塔、該内襯、該注入:果是’整個熱區會充滿 等緩衝及測試晶圓。沒有除了 該等生產晶圓、和該 量存在於該熱區内而造成污外的其他材料以重要的 作3叮处7木或煞膨脹的問題。 仁疋,可旎調整多晶晶圓 性’特別是該等緩衝晶圓。可以、供所需的紅外線蔽光 形成測試晶圓的R0PSi材料,以足夠的半導體摻雜來成長 -公分,並且較佳地低於u降低電阻率至低於1歐姆 時矽晶圓實質上對於爐管内的 '公分:或甚至更低’此 見Wo 1 f夕;k · ^! ^日 線熱幅射是不透明的0 兄wolf之lbld關於摻雜的矽之 質,# Η使户# e 成長。硼是較佳的摻 貞並且其在成長擁有此種摻雜 也可鈐箱止—、, 巧CZ石夕方面是習知的。 乜了此預先在測試晶圓上塗覆 JL他姑袓、^ , 句厚的氮化砍(或可能是 八他材枓)’其提供所需的紅外線吸收。 該多晶CZ矽,特別是CVd 非生產曰m ιν & μ β ,原CZ矽,可應用在除了 座日日0以外的其他應用。 工。哕夕β rw u 小的結晶結構促進石夕的加 π夕日日CZ材料有利地擁有 矽之一雁爾θ π々 孕又小的結晶尺寸。多晶cz 應甩疋形成該塔的兩個基座 其他可能用途是做為邊緣支 環1 1 D 地士嘴 牙每’例如第9圖所示的 衣110,擁有薄的往内延伸的 緣,在椒4點制1 狀唇部11 2以支撐晶圓邊 豕在快速熱製程(RTP)中。期 多於20密爾⑺s t 1 降低唇部112的厚度至不 在爾(0·5耄米),這在除7 是很難、去# ΛΑ 、f本發明以外的多晶石夕上 難達成的。兩個_下的擇Μ ^ 朝下的衣狀逢緣11 4、1 1 6攫住在第 圖的正交視圖中所示的旋轉管丨2〇,其支撐並轉動邊緣 19 Ο C^ 200842213 環Π ο以及其上支撐的晶圓。已知有較不複雜的邊緣 構。其他類似的環包含邊緣排除環,其中該唇部或類 突出部份位於晶圓邊緣上方,並且與之隔離以保護其 到沉積,以及夾環,其接觸上晶圓邊緣以在製程期間The P wafer is, for example, removed by removing a portion of the accumulated thickness, or all of it is removed and the wafer fabrication steps of Figure 7 are repeated. The polycrystalline germanium wafer can be regenerated or re-cleaned by immersing it in hydrofluoric acid to remove the nitride. Then it can return to work. Preliminary tests have shown that 2.5 μm of tantalum nitride can be deposited on the polycrystalline germanium test wafer thus treated in an LPCVD process without significant flaking. This is far above the 300 mm thickness limit used in the past before discarding the test wafer. The Wafer production line is subject to a 2 micron thickness limit (J is the basis for major replacements when using test wafers. Even a 1 micron thickness limit can represent a significant improvement over previous techniques. In addition, the recovered polysilicon test The wafer does not exhibit the streaks and streaks observed on the recovered single crystal germanium test wafer, so it is possible to clean the test wafer of the present invention more than twice. It is clear that the polycrystalline silicon wafer of the present invention Can be used as a baffle wafer in the same LPCVD process. It may be desirable to continue to use some quartz wafers as thermal buffers, especially at the bottom of the tower, which is outside the hot zone. The expected opacity of 18 Γ, υ 200842213 in infrared radiation. However, 3 the use of polycrystalline wafer 1 in the tube (4) zone is preferably in the case of deposition, including the tower, the lining, the injection: If it is 'the entire hot zone will be filled with other buffers and test wafers. There is no other material other than the production of the wafer, and the amount of contamination in the hot zone is important. The problem of expansion. Ren Yan, can adjust polycrystalline wafer properties, especially these buffer wafers. It can, for the required infrared shielding, form the R0PSi material of the test wafer, grow with sufficient semiconductor doping - cm, and Good ground below u reduces the resistivity to less than 1 ohm. The wafer is essentially 'cm: or even lower' in the tube. See Wo 1 f; k · ^! ^ Daily heat radiation is opaque 0 brother wolf's lbld about doping 矽 quality, # Η使户# e grow. Boron is the preferred erbium and its growth can have such doping can also be boxed -,, CZ Shi Xifang This is a well-known thing. In this case, JL is applied to the test wafer in advance, and the thickness of the nitride is cut (or possibly the other material). It provides the required infrared absorption. CZ矽, especially CVd non-production 曰m ιν & μ β , original CZ矽, can be applied to other applications except the seat day 0. Work. 哕 β β rw u Small crystal structure promotes Shi Xi's addition π On the eve of the day, the CZ material advantageously possesses a small crystal size of 雁 尔 θ π 々 。 。 。 。 。 。 。 。 。 。 。 。 。 。 The other possible uses of the two bases of the tower are as the edge support ring 1 1 D. The geostatistic mouth of each of the clothes 110 shown in Figure 9 has a thin inwardly extending edge, which is made at 4 o'clock. The lip 11 2 supports the wafer edge in the rapid thermal process (RTP). The period is more than 20 mils (7) s t 1 to reduce the thickness of the lip 112 to not (0.5 mils), which is in addition to 7 It is difficult to go to # ΛΑ, f, the polycrystalline stone other than the invention is difficult to achieve on the eve. Two _ under the choice Μ ^ Down the garment-like edge 11 4, 1 1 6 攫 live in the orthogonal map The rotating tube 丨 2〇 shown in the view supports and rotates the edge 19 Ο C^ 200842213 ring ο and the wafer supported thereon. Less complex edge structures are known. Other similar rings include an edge exclusion ring in which the lip or protrusion is located above and separated from the edge of the wafer to protect it from deposition, and a clamp ring that contacts the upper wafer edge during the process
夾至一台座。該支撐管12〇也可由本發明之多晶CZ 成。由用於RTP矽生產晶圓的矽組成之該等邊緣環和 管不但提供高純度水準,也簡化當這些零組件是由其 料製成時所存在的輻射和熱膨脹問題。 本發明之CZ矽的其他應用包含台座平台,例如 圖所不之平台1 3 0較佳地可由隨機取向c ζ多晶矽形 支撐晶圓進行晶圓製程。通常是碟形的平纟13〇可包 升捎用的軸通孔1 3 2,或樹枝狀結構的淺凹槽工3 4以 傳導氣體之供應孔136。此種微細特徵的加工由於本 ^ H4易。此種塔基座、晶®環、支指 和〇座以及其他腔室構件 微大-些的直徑。但是,直:::比被處理的晶圓直 來形成用於生產晶圓的晶棒二 =多晶cz晶棒可 因為單晶CZ晶棒的直炉實質同的cz拉升器中拉 的直徑,因為加諸於單:晶圓:於從其中拉升起之 求。並不要求結構組件要有此種對於均勾性的嚴 多晶CZ晶棒可利用多晶晶種教::均勻十生’因此較 長條件在相同的設備内長成,例凋整用於較大直徑 -種CZ多晶㈣用途,\’藉由降低拉升速: 源晶種長成的多晶是形成太:從原。生多晶石夕或 罨池140,在第12圖 環結 似的 不受 將其 矽製 支撐 他材 第11 成以 含舉 及熱 發明 t管、 徑稍 在用 升, 坩鍋 袼要 大的 之成 Ψ 〇 CVD 的正 20 200842213 交視圖中示出,其中垂直的p-n接面形成在矽切片内,其 可維持其圓形晶棒的尺寸或切割為矩形。在該太陽能電池 140的前及背側製作電氣接觸142、144。該等隨機取向CZ 微晶產生一較強材料,因此使太陽能電池可由擁有相對小 的微晶尺寸但大表面積的較薄的半導體矽層形成。此外, CZ多晶矽相對於澆鑄矽的高純度提供較佳的半導體性 質,因為咸信多晶矽内的不純物會遷移至晶粒邊界,並造 成沿著該等邊界的漏電。 \ : 雖然本發明之測試晶圓在氮化矽的 LPCVD中發現特 別有益,但用來做為測試和熱擋晶圓的非生產晶圓可與許 多製程並用,包含多晶矽、氮氧化矽、二氧化矽的CVD和 其他沉積製程,並且更廣泛地任何熱製程。 雖然多晶矽非生產晶圓有利地與矽塔合併使用,但其 擁有用於其他材料的塔和晶舟上的優點,包含石英及碳化 石夕。 矽晶舟是有利地用於矽製程内之另一種晶圓支撐設 (j 備。在一晶舟中,晶圓係以水平延伸陣列配置在晶舟内的 狹缝中,並且係以主要表面從垂直方向傾斜幾度的方式定 位。結果是,晶圓邊緣搁置在晶舟底部並且狹縫的齒狀物 接觸並支撐該等晶圓的背側。本發明之非生產晶圓可有利 . 地與晶舟以及塔並用。 本發明之隨機取向多晶矽提供非生產晶圓許多優勢並 適用於其他粗糙構件和結構,並且該材料可用商用單晶晶 圓發展良好的CZ技術長成。 21 200842213 【圖式簡單說明】 第1圖係典型熱處理爐管的簡要剖面圖。 第2圖係有利地與本發明並用之矽塔的正交視圖。 第3圖係本發明之多晶矽非生產晶圓的平面圖。 第4圖係原生多晶矽晶棒的剖面圖。 第5圖係從原生多晶矽晶種長成之柴氏多晶矽晶棒的 剖面圖,以及由其切割出之非生產晶圓的平面圖。 第6圖係CVD源柴氏多晶矽晶棒的剖面圖,以及由其 切割出之非生產晶圓的平面圖。 第7圖係處理多晶矽非生產晶圓之製程程序之一實施 例0 第8圖係兩側皆粗糙化的多晶矽晶圓之剖面圖。 第 9圖係一類型之晶圓環的剖面正交視圖,明確地 說,一 RTP外緣環。 第1 0圖係用來支撐及旋轉第9圖的外緣環之矽管的正 交視圖。 第11圖係一矽台座平台的正交視圖。 第1 2圖係CZ太陽能電池的正交視圖。 【主要元件符號說明】 10 爐管 12 加熱筒 14 電阻加熱線圈 16 鐘罩 18 内襯 20 支撐塔 22 200842213 η 22 台座 24 氣體注入器 30、 32 矽基座 34 矽支腳 38 晶圓 40 多晶矽非生產 42 標記 50 多晶梦晶棒 52 結晶樹枝 54、 66 晶種棒 60 ' 70 柴氏 多 晶 晶棒 62 外側區 64 内側區 78 插塞 80 製程 100 非生產晶圓 102 裂痕 104 裂縫 106 、1 08 主 要 表 面 110 邊緣支撐環 112 唇部 114 > 116 邊緣 120 旋轉管 130 平台 132 軸通孔 134 淺凹槽 136 供應孔 140 太陽能電池 142 、144 電氣接觸Clip to a pedestal. The support tube 12A can also be formed from the polycrystalline CZ of the present invention. These edge rings and tubes, which are composed of crucibles for RTP® production wafers, not only provide high purity levels, but also simplify the radiation and thermal expansion problems that exist when these components are made from their materials. Other applications of the CZ(R) of the present invention include a pedestal platform. For example, the platform 130 can preferably be wafer processed by a randomly oriented c ζ polycrystalline dome. Usually, the dish-shaped flat cymbal 13 can be used for the shaft through hole 133 for lifting, or the shallow groove for the dendritic structure 34 to conduct the gas supply hole 136. The processing of such fine features is easy due to this H4. Such tower bases, crystal® rings, fingers and sley and other chamber components are slightly larger in diameter. However, straight::: directly forms the ingot for the wafer to be processed than the wafer to be processed. The polycrystalline cz ingot can be pulled in the same cz puller as the single crystal CZ ingot. Diameter, because it is added to the single: wafer: from the rise from it. It is not required that the structural components have such a strict polycrystalline CZ ingot for homogenous properties. It can be taught by using polycrystalline crystals:: evenly ten students' so long conditions are grown in the same equipment, and the examples are used for Larger diameter - species CZ polycrystalline (four) use, \' by lowering the pull-up speed: the source crystal grows into a polycrystal that is formed too: from the original. Born in polycrystalline stone or Dianchi 140, in the 12th ring, it is not subject to the support of the eleventh. It is invented with heat and invented the tube, the diameter is slightly used, and the pot is large. The pn 正 正 2008 2008 2008 200842213 cross-sectional view shows that a vertical pn junction is formed in the 矽 slice, which can maintain its circular ingot size or cut into a rectangle. Electrical contacts 142, 144 are made on the front and back sides of the solar cell 140. The randomly oriented CZ crystallites produce a stronger material, thus allowing the solar cell to be formed from a thinner semiconductor germanium layer having a relatively small crystallite size but a large surface area. In addition, the high purity of the CZ polysilicon relative to the cast tantalum provides better semiconducting properties because the impurities in the polycrystalline germanium migrate to the grain boundaries and cause leakage along the boundaries. \ : Although the test wafer of the present invention is particularly advantageous in LPCVD of tantalum nitride, non-product wafers used as test and heat shield wafers can be used in combination with many processes, including polysilicon, bismuth oxynitride, and CVD and other deposition processes for yttrium oxide, and more extensively any thermal process. Although polycrystalline germanium non-produced wafers are advantageously used in conjunction with the crucibles, they have advantages in towers and boats for other materials, including quartz and carbon carbide. The wafer boat is advantageously used in another wafer support in the process. In a wafer boat, the wafer is arranged in a horizontally extending array in a slit in the boat and is mainly surfaced. Positioning from the vertical direction by a few degrees. As a result, the edge of the wafer rests on the bottom of the boat and the teeth of the slit contact and support the back side of the wafer. The non-productive wafer of the present invention can be advantageously used. The wafer and the tower are used in combination. The random orientation polysilicon of the present invention provides many advantages of non-productive wafers and is applicable to other rough components and structures, and the material can be grown by the well-developed CZ technology of commercial single crystal wafers. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic cross-sectional view of a typical heat treatment furnace tube. Fig. 2 is an orthogonal view of a crucible tower advantageously used in conjunction with the present invention. Fig. 3 is a plan view of a polycrystalline silicon non-production wafer of the present invention. Figure 4 is a cross-sectional view of a native polycrystalline twin rod. Figure 5 is a cross-sectional view of a Czd polycrystalline germanium rod grown from a native polycrystalline germanium seed crystal, and a plan view of the non-produced wafer cut therefrom. A cross-sectional view of a VD source Czd polycrystalline germanium rod and a plan view of a non-product wafer cut therefrom. Figure 7 is a process for processing a polycrystalline germanium non-produced wafer. Example 0 Figure 8 is rough on both sides A cross-sectional view of a polycrystalline germanium wafer. Figure 9 is an orthogonal view of a cross section of a type of wafer ring, specifically, an RTP outer edge ring. Figure 10 is used to support and rotate the outer view of Figure 9. Orthogonal view of the rim of the edge ring. Figure 11 is an orthogonal view of a pedestal platform. Figure 12 is an orthogonal view of the CZ solar cell. [Key symbol description] 10 Furnace tube 12 Heater 14 Resistor Heating coil 16 bell jar 18 lining 20 support tower 22 200842213 η 22 pedestal 24 gas injector 30, 32 矽 base 34 矽 foot 38 wafer 40 polycrystalline 矽 non-production 42 mark 50 polycrystalline dream crystal rod 52 crystal branch 54 66 seed rod 60 ' 70 Chua polycrystalline rod 62 outer area 64 inner area 78 plug 80 process 100 non-product wafer 102 crack 104 crack 106, 1 08 main surface 110 edge support ring 112 lip 11 4 > 116 Edge 120 Rotating Tube 130 Platform 132 Shaft Through Hole 134 Shallow Groove 136 Supply Hole 140 Solar Cell 142, 144 Electrical Contact
23twenty three
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