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TW200305932A - Ideal oxygen precipitating silicon wafers with nitrogen/carbon stabilized oxygen precipitate nucleation centers and process for making the same - Google Patents

Ideal oxygen precipitating silicon wafers with nitrogen/carbon stabilized oxygen precipitate nucleation centers and process for making the same Download PDF

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TW200305932A
TW200305932A TW091137013A TW91137013A TW200305932A TW 200305932 A TW200305932 A TW 200305932A TW 091137013 A TW091137013 A TW 091137013A TW 91137013 A TW91137013 A TW 91137013A TW 200305932 A TW200305932 A TW 200305932A
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wafer
oxygen
nitrogen
concentration
scope
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TW091137013A
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Chinese (zh)
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TWI276161B (en
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Mule Stagno Luciano
Jeffrey L Libbert
Richard J Phillips
Milind Kulkarni
Mohsen Banan
J Brunkhorst Stephen
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Memc Electronic Materials
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    • H10P36/07
    • H10P36/00
    • H10P14/20
    • H10P36/20

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Abstract

A silicon wafer having a controlled oxygen precipitation behavior such that a denuded zone extending inward from the front surface and oxygen precipitates in the wafer bulk sufficient for intrinsic gettering purposes are ultimately formed. Specifically, prior to formation of the oxygen precipitates, the wafer bulk comprises dopant stabilized oxygen precipitate nucleation centers. The dopant is selected from a group consisting of nitrogen and carbon and the concentration of the dopant is sufficient to allow the oxygen precipitate nucleation centers to withstand thermal processing such as an epitaxial deposition process while maintaining the ability to dissolve any grown-in nucleation centers.

Description

(1) 200305932 玖、發明說明 (發明說明應敘明:發明所屬 i前技術 領域、先前技術、内容、實施方式及圖式簡單說明) 本發明概括言之俏β 用以製造電子址件導體材料基板之配製,特別是 -種石夕處理過程,為然。質言之’本發明乃關於 /、於只貝上任何電子裝置製程之熱處理 %期期間,使晶圓犯Α、γ , 化成氧沈積物之理想不均勻深度分佈。 4造半導體電子組株 、、平大半過程之起始材料的單晶矽通常 、、奔I刀克普斯基”(Czochralski)法配置,其中將單籽晶 ^ ^ Θ H以緩慢萃取法而生成。在熔石夕盛於掛禍 中日$ ’即與各種雜皙、、3 旧4 雜貝此合,主要與氧混合。氧在熔晶體之 :又上進入晶格,直到達到由晶中熔體溫度上氧之溶度以 曲由口化矽中氧的實際分凝係數所決定之濃度為止。此等 =度^於氧在固㈣中於電子裝置製程之標準溫度上的溶 田曰曰自炝體生成並冷卻時,其中氧的溶解度即迅速降 低制=合成片或晶圓,,氧呈超飽和濃度。 衣化包子裊置通常所採之熱處理週期能導致矽晶圓中氧 ^沈積達到氧超飽和。沈積物的有害或有益端視其在晶圓 壯的位置而定。氧沈積物位於晶圓之有源裝置區中有損於 ,置之刼作。而位於晶圓主體中之氧沈積物卻能捕捉與晶 °、妾觸之無益的金屬雜質。利用晶圓主體中氧沈積物以捕 捉金屬通常稱為内部或内在吸收雜質(IG)。 、4兒子I置製程含有一系列步驟,設計以生產之矽, Q ΓΞΓΪ 、 、L表面之區並無氧沈積物(一般稱為裸露區或無沈 積物區),晶圓其餘主體含充分氧沈積物以供内在吸收雜 (2) 200305932 質之用。裸露區可以高春高熱次序形成,諸如:⑷於高 溫下(攝氏一千一百度以上)惰性環境中氧外擴散熱處理至 少四小時;⑻於,溫下(攝氏六百度至七百五十度)氧沈積 核形成,及(C)在高溫下(攝氏一千度至一千一百五十度)氧 ⑶〇2)沈積物之生A。請參閱1989年加州聖地亞哥Ac—二 Press公司之F. Shimura君所著,,半導體梦晶技術,,第%卜奶頁 以及其中所列之參考資料。 、 不過取近之先進電子裝置如動態隨機存取記憶器之製程 已開始盡量減少採高溫法步驟。雖然若干製程保留足夠的 南溫法步驟以生產裸露區及大批沈積物之充分密度,但材 料的容限過嚴而無法提供商用產品。其它現行高度先進電 子裝置製程皆不含外擴散步驟。由於有源裝置區中氧沈積 物的相關問題’故此等電子裝置製造商必須採用在豆製程 條件下’晶圓中任何處皆無形成氧沈積物之石夕晶圓。結果 一切内在吸收雜質之潛在能力於焉喪失。 " 發明内衮 故在本發明之諸目的中乃提供—種單_晶圓,並於任 電子裝置製程之熱處理週期期間,會形成氧沈積 不均句深度的分佈;提供此種晶圓會優化且可複 衣地形成充分深度之裸露區及晶圓主體内充分密产 提供此種之晶圓,其中裸露區之形成及“心 =之=皆與此晶圓區中氧濃度之差異無關;提供此 I:二 成裸露區之厚度實質上與積體電路製程的 、、’田即無關;提供此種之晶圓,其中晶圓主體中裸露區及氧 (3) (3)200305932 i積物之形成不受切克勞斯基生成單晶錢之熱過程與氧 濃度的影響’晶圓係自該單晶石夕疑切割出者 種 方法,其中裸露區之形成並不依氧之外擴散而定:、= =方法’其切乃以充分濃度之氮及/或碳摻雜,以穩 定氧沈積物成核中心,俏之鲈系為你 " ^ 、 使之此承文後續之快速熱處理而不 έ妨礙裸露區的形成。 簡言之,本發明係針對具有兩主要之大致平行表面之單 晶''圓,其中之一為晶圓之前表面另一為晶圓之後表 面’ δ亥早晶碎晶圓並且右箭你 /、有别後表面間中央平面,接合前後 表面之周'緣’一表面層包括前表面與自前表面至中央平面 所測量之至少約十微米距⑼間之晶圓區,以及_主體戶 包括中央平面與第一區間之晶圓的第二區。此晶圓並具: 沈積物成核中心之不均勺八 妨由 U 不^刀佈’即以主體層中氧沈積物成 ?中心之k度大於表面層中氧沈積物成核中心之濃度,以 ::積物f核中心具有—濃度截面曲線,#中氧沈積物成 二心之奪值密度在中央平面處或其附近,而濃度自峯值 役度位置循晶圓前表面方Λ政Μ ^ ^ 向降低。同日守,晶圓含有選自氮、 反或其混合物組合之松施札 物,採用氮摻雜物時,氮之濃度 約在母立方公分1彳⑴2 $ / — 10至約5χ1〇14原子之間,而碳的濃度約 在母立方公分丨><1〇16至約4χ1〇17原子之間。 本發明並針對一種零g? 1 m ^ i配具控制之氧沈積作用之單晶矽晶 二辦方法此方去包括選定自切克勞斯基法生成之單晶石夕 =切割且含—前表面和後表面及前後表面間—中央平面 曰曰囫’此晶圓並含一前表面層、一主體層及摻雜物;前 (4) 200305932 二面層:盍剛表面與自前表面至中央平面間所測量之距離 :者間的晶圓@;主體層涵蓋中央平面與前表面層間 的t圓區域;而摻雜物選自含氮與碳的組合,當摻雜物為 鼠時,其濃度約為每立方公分lxl〇12至約5χ1〇14原子,2 摻雜物為碳時,其濃度約為每立方公分ΐχΐ〇ΐ6至約4仙7原 I。所選定之晶圓加熱至約攝氏十百五十度,以於前 二及主體層中形成晶格空位。經加熱之晶圓迅速冷 成晶圓中空位5JI 哉%# 中,… 線,其中拳值空位密度在主體層 #而广条值雄度處依晶圓前表面方向大致遞減,且前 沈積物成核中心,氧沈積物形成氧 日认丄 積物成核中心於主體層中形成。而 且’於加熱之晶圓冷卻時, 本騁爲士 %疋之虱沈積物成核中心即於 一曰中形成,主體層中穩定氧 主要依^的濃度㈣。之^積物成核中心的濃度 本發明之其它目的與特徵將明示於下 依據本發明,業已發一 ,, 種里μ的沈積晶圓,其於實際 上任何電子裝置製程期間,會,於只際 有内在吸收雜質用$右八心&成充刀冰度之稞露區及含 理相之y>藉θ π Ή度氧沈積物的aaa圓主體。此- 具在片刻間配製之。此法創通用玉 於電子裝置製程期間氧沈積之方I夕拉板’確定或”印製" 本I明理想沈積晶圓之原始材料 斯其曰興* 屬依R?、傳統性切克勞 曰日體生成法所生成之單晶錠中所切割之單晶梦晶圓。 (5) (5)200305932(1) 200305932 发明, description of the invention (the description of the invention should state: the previous technical field, prior technology, content, embodiment, and drawings of the invention are briefly explained) The summary of the present invention β is used to manufacture electronic address conductor materials The preparation of the substrate, especially the kind of Shixi processing, is true. In summary, the invention relates to the ideal non-uniform depth distribution of wafers A and γ during the heat treatment% period of any electronic device process on the shell. 4Semiconductor electronics, single crystal silicon, which is the starting material for most of the process, is usually configured by the Czochralski method, in which the single seed crystal ^ ^ Θ H is slowly extracted Generated. In the lava stone, it is in the midst of misfortune, that is, it is combined with various miscellaneous, 3, and 4 miscellaneous species, which is mainly mixed with oxygen. Oxygen enters the crystal lattice on the molten crystal: again, until it reaches the crystal The solubility of oxygen at mid-melt temperature is based on the concentration determined by the actual segregation coefficient of oxygen in siliconized silicon. This is equal to the degree of dissolution of oxygen in solids at the standard temperature of the electronic device manufacturing process. When the autogenous body is formed and cooled, the solubility of oxygen in it is rapidly reduced, and the oxygen is in a supersaturated concentration. The heat treatment cycle usually used for the coating of buns can cause oxygen in silicon wafers. ^ Deposition reaches oxygen supersaturation. The harmful or beneficial end of the deposit depends on its position on the wafer. The oxygen deposit is damaged in the active device area of the wafer, and it is operated. It is on the wafer. Oxygen deposits in the main body can trap metal impurities that are not beneficial to the crystal and contact. The use of oxygen deposits in the body of the wafer to capture the metal is commonly referred to as internal or intrinsic absorption impurities (IG). The process of the I-I process involves a series of steps designed to produce silicon. There is no area on the surface of Q ΓΞΓ 无, L Oxygen deposits (commonly referred to as bare or no-deposit areas). The remaining body of the wafer contains sufficient oxygen deposits for internal absorption of impurities (2) 200305932. The exposed areas can be formed in high spring and high heat sequence, such as: ⑷ Oxygen diffusion heat treatment for at least four hours in an inert environment at high temperature (more than 1,100 degrees Celsius); formation of oxygen nucleation at high temperature (from six hundred degrees Celsius to seven hundred and fifty degrees Celsius), and (C) at high temperature (1,000 degrees Celsius to 1,150 degrees Celsius) oxygen ⑶〇2) the birth of the sediment A. Please refer to F. Shimura Jun, Ac-Second Press, San Diego, California, 1989, Semiconductor Dream Crystal Technology, , The milk page and the reference materials listed therein. However, the process of accessing advanced electronic devices such as dynamic random access memory has begun to minimize the use of high temperature methods. Although some processes retain sufficient South temperature methods In order to produce sufficient density in the exposed area and a large number of deposits, the material tolerance is too tight to provide commercial products. Other current highly advanced electronic device processes do not include an external diffusion step. Because of the oxygen deposits in the active device area, Related issues' Thus such electronic device manufacturers must use Shixi wafers where no oxygen deposits are formed anywhere in the wafer under the conditions of the soybean process. As a result, all the inherent ability to absorb impurities is lost. &Quot; Inventiveness 衮Therefore, in the purposes of the present invention, a single wafer is provided, and during the heat treatment cycle of any electronic device process, the distribution of the depth of the uneven deposition of oxygen will be formed; providing such a wafer will be optimized and recoatable The formation of exposed areas with sufficient depth and full dense production in the wafer body provides such wafers, where the formation of the exposed areas and the "heart = of =" are not related to the difference in oxygen concentration in the wafer area; provide this I: The thickness of 20% of the exposed area is essentially independent of the integrated circuit manufacturing process, and the field is not provided; wafers of this type are provided, in which the exposed area of the wafer body and oxygen (3) (3) 200305932 i product The formation of the crystal is not affected by the thermal process and oxygen concentration of Cheklaussky's production of single crystals. 'Wafer system is a method of cutting from the single crystal, in which the formation of the exposed area does not depend on diffusion outside oxygen. Determination :, = = Method 'The cut is doped with sufficient concentration of nitrogen and / or carbon to stabilize the nucleation center of the oxygen deposits, and the perch is for you " ^, to make this Cheng Wen subsequent rapid heat treatment Without hindering the formation of the exposed area. In short, the present invention is directed to a single crystal `` circle '' with two major, substantially parallel surfaces, one of which is the front surface of the wafer and the other is the rear surface of the wafer. The center plane between the rear surfaces is different, and the peripheral edge of the front and back surfaces is joined. The surface layer includes the front surface and the wafer area measured at least about 10 microns from the front surface to the center plane. The second region of the wafer between the plane and the first region. This wafer also has: The unevenness of the nucleation center of the sediment may be formed by the U's knife cloth, that is, the k-degree of the center of the oxygen deposit in the main layer is greater than the concentration of the nucleation center of the oxygen deposit in the surface layer. The core of the ::: f core has a -concentration cross-section curve, and the density of the oxygen deposits in the center of # is at or near the central plane, and the concentration follows the front surface of the wafer from the peak duty position. Μ ^ ^ decreases. On the same date, the wafer contains a pine material selected from the group consisting of nitrogen, trans, or a combination thereof. When a nitrogen dopant is used, the nitrogen concentration is about 1 彳 ⑴2 $ / — 10 to about 5 x 1014 atoms. The concentration of carbon is between the parent cubic centimeters < 1016 and about 4 x 1017 atoms. The present invention is also directed to a second method of single-crystal silicon with zero g? 1 m ^ i equipped with controlled oxygen deposition. This method includes the selection of single crystals produced by the Cheklaussky method = cutting and containing- The front surface and the rear surface and between the front and back surfaces-the central plane says "This wafer does not contain a front surface layer, a main body layer and dopants; front (4) 200305932 second surface layer: the rigid surface and from the front surface to The distance measured between the central planes: the wafers between them; the body layer covers the t-round area between the central plane and the front surface layer; and the dopant is selected from the combination of nitrogen and carbon. When the dopant is a rat, Its concentration is about 1 x 1012 to about 5 x 1014 atoms per cubic centimeter. When the dopant is carbon, its concentration is about ΐxΐ〇6 to about 4 cents per 7 centimeters of original I. The selected wafer is heated to about 150 degrees Celsius to form lattice vacancies in the first two and the main layer. The heated wafer is quickly cooled to 5JI 哉% # in the wafer, where the density of boxing vacancy is at the main layer # and the wideness of the value is roughly decreased according to the direction of the front surface of the wafer, and the front deposits The nucleation center, the oxygen deposit formed the oxygen nucleation accretion nucleation center formed in the main layer. And when the heated wafer cools down, the nucleation center of the lice deposit that is 士% 疋 is formed in the middle of the day, and the stable oxygen in the main layer mainly depends on the concentration ㈣. The concentration of the accumulation nucleation center of the present invention will be further described in accordance with the present invention. According to the present invention, a micro-deposited wafer has been issued during practically any electronic device manufacturing process. There are only intrinsically absorbing impurities with the right eight hearts & the dew area that fills the knife's ice and the aa round body with θ π degree oxygen deposits. This-is formulated in a moment. This method creates a general method for oxygen deposition during the electronic device manufacturing process. "Identify or" print "the original material of the ideal deposited wafer. This is based on R ?, traditional Cek The single crystal dream wafer cut from the single crystal ingot produced by the Rao body generation method. (5) (5) 200305932

此等方法以及標準矽的切片,研磨,蝕刻和拋光等技術載 於1989年Acadeimc Press中F. shimura所著之"半導體矽晶體技 術,,及1982年紐約Springer_Verlag中”石夕化學蝕刻,,(j_ ed.),錄於此以供參考。 切克勞斯基法生成之矽通常所含氧濃度在約每立方公分 5x10"至約9xl〇i7原子的範圍内(ASTM標準F_i2i_83)。由於 氧沈積作用實質上呈現自理想沈積晶圓中氧濃度的退麵 性’故原始晶圓可具有切克勞斯基法所獲範圍以内或以外 之氧濃度。 依據單晶石夕鍵自石夕炼點(約攝氏141〇度)經攝氏約七百五 十度至約三百五十度範圍之冷卻速率,氧沈積物成核中心 可形成於晶圓所切割之單晶矽錠中。原始材料中是否有此 等成核中心存在對本發明無關緊要,但此等中心卻能由在 約攝氏一千三百度以内溫度矽熱處理所分解情形。某些熱 處理’諸如矽於約攝氏八百度退火四小時等,能穩定此等 中心使之不旎在未超過約攝氏一千一百五十度下分解。氧 沈積物的探測極限目前約為每立方公分5χ1〇6沈積物。氧沈 2物成核中心的存在(或密度尚無法利用現有技術直接測 里。但可用各種技術間接探測其存在。如前所述,矽中先 $在之氧沈積物成核中心可由將矽經氧沈積熱處理而獲穩 定,且可在此等位置生成沈積物。故此等成核中心可於氧 沈積熱處理後間接測得,例如將晶圓於攝氏八百度退火四 小時,然後於攝氏一千度退火十六小時之熱處理。 現在請參考圖丨,本發明理想沈積晶圓的原始材料單晶 -10- (6) 200305932 ::::具有一别表面3 ’後表面5及一前與後表面間假想 :中央平面7。本文中"前"與’,後,,詞語乃用以區別晶圓之 '主要大致同平表面’所採用之晶圓前表面一詞並非一定 =而後電子裝置製於其上之表面,而所採晶圓後表面一詞 亦非指晶圓之鱼雷+驻要& + 士 U I /、电子衣置所在表面相對的主要表面。此 外,由於石夕晶圓通常有些總厚度變化如突出彎曲等,故前 表面上的每一點與後表面上的每一點間的中點可能不在同 一準確的平面;不過實際上,f曲之總厚度變化通常極微, 近似而言,諸中點可謂居於假想之中央 為前後表面間相等距離β Χ + 在本發明方法的第-具體實射,晶圓丨於步驟^中在 含乳之環境中做熱處理,以生成包圍晶圓i之外表氧化層 。-般而言’氧化層厚度大於石夕上形成之原生氧化層(約 為15埃),該氧化層至少厚約-+ 杏 夕7子、,々一十埃為宜,而在某些具體 二歹|至少厚約二十五埃或甚至約三十埃。目前所獲之實 :證據提示大於約三十埃之氧化層,雖不干擾所要求效 應’也並不會提供附加益處。 ,在步驟\中’晶圓承受熱處理’其中晶圓加熱至高溫以 形成晶圓1中晶格空位13並增加空位數密度”匕一埶處理 步驟宜於速熱退火器中實施’將晶圓加熱至目標溫度並於 該溫度上做較短時間之退火。-般而言,日日日圓承受之溫度 至少超過攝氏一千一百五十度,較宜至少—千一百七十五 度,更佳至少約一千二百度,及更佳之_千二百度至一千 二百七十五度之間。 -11 - (7) 200305932These methods, as well as standard silicon slicing, grinding, etching and polishing techniques, are described in "Semiconductor Silicon Crystal Technology" by F. shimura, Academicim Press, 1989, and "Shi Xi Chemical Etching in Springer_Verlag, New York, 1982," (J_ ed.), Recorded here for reference. The silicon produced by the Cheklauszki method usually contains an oxygen concentration in the range of about 5x10 " to about 9x10i7 atoms per cubic centimeter (ASTM standard F_i2i_83). Because Oxygen deposition essentially exhibits the degeneration of oxygen concentration from ideally deposited wafers. Therefore, the original wafer may have oxygen concentrations within or outside the range obtained by the Cheklaussky method. The refining point (approximately 1410 degrees Celsius) can be formed in a single crystal silicon ingot cut by a wafer with a cooling rate ranging from approximately 750 degrees to approximately 350 degrees Celsius. Original The existence of such nucleation centers in the material is irrelevant to the present invention, but these centers can be decomposed by heat treatment of silicon at a temperature of about 1,300 degrees Celsius. Some heat treatments such as silicon are at about 80 degrees Celsius. Four hours and so on, these centers can be stabilized so that they do not decompose below about 1,150 degrees Celsius. The detection limit of oxygen deposits is currently about 5 x 106 deposits per cubic centimeter. Oxygen precipitation 2 The existence of a nucleation center (or the density cannot be measured directly using existing technologies. However, various technologies can be used to detect its existence indirectly. As mentioned earlier, the nucleation center of oxygen deposits in silicon can be thermally treated by oxygen deposition of silicon. It is stable and deposits can be formed at these locations. Therefore, these nucleation centers can be measured indirectly after the oxygen deposition heat treatment, such as annealing the wafer at eight degrees Celsius for four hours, and then annealing at sixteen degrees Celsius for sixteen Heat treatment for hours. Now please refer to Figure 丨, the original material of the ideal deposited wafer of the present invention is a single crystal -10- (6) 200305932 :::: having a different surface 3 'rear surface 5 and a front and rear surface hypothesis: Central plane 7. In this article, "front" and "," later, the words are used to distinguish the wafer's "mainly substantially the same as the flat surface". The term used for the front surface of the wafer is not necessarily = then the electronic device is manufactured in it On the surface, and The term "surface after wafer picking" does not refer to the main surface of the wafer torpedo + resident & + UI /, the surface on which the electronic clothing is located. In addition, because Shi Xi wafers usually have some changes in total thickness, such as protruding bending, etc. Therefore, the midpoint between each point on the front surface and each point on the rear surface may not be on the same accurate plane; but in fact, the total thickness of the f-curve usually varies very little. Approximately, the midpoints can be described as imaginary. The center is the equal distance β χ + between the front and rear surfaces. In the first specific shot of the method of the present invention, the wafer is heat-treated in a milk-containing environment in step ^ to generate a surface oxide layer surrounding the wafer i.-General In terms of the thickness of the oxide layer is greater than that of the native oxide layer (about 15 angstroms) formed on the stone, the thickness of the oxide layer is at least about-+ apricot husks, about 10 angstroms, and in some specific | At least about twenty-five Angstroms or even about thirty Angstroms. What has been obtained so far: Evidence suggests that an oxide layer greater than about thirty angstroms, while not interfering with the desired effect, will not provide additional benefits. In step \ 'wafer is subjected to heat treatment', in which the wafer is heated to a high temperature to form lattice vacancies 13 in wafer 1 and increase the vacancy number density. The processing step is suitable to be implemented in a rapid thermal annealing machine. Heating to the target temperature and annealing at that temperature for a short period of time.-In general, the temperature that the Japanese yen will withstand is at least 1,150 degrees Celsius, and preferably at least -175 degrees Celsius, More preferably at least about 12 hundred Baidu, and more preferably _12 Baidu to 1,275 degrees. -11-(7) 200305932

雄、沒)的斷面曲線。 根據目4所獲之實驗證據,速熱退火步驟中之環境最好 少含部分氧,水蒸汽及其它氧化氣體之壓力,亦即,環境 無氧化氣體或此等氣體之壓力,即不足以注入抑制空位濃 度集結之矽自填空位原子。雖然氧化氣體濃度的下限尚未 確切決定,但已顯示(0·01)大氣壓之氧的分壓力或百萬分 之一萬份原子(ppma)並不增加空位濃度且無任何效應。因 此’該環境所含氧或其它氧化氣體之壓力宜小於(〇 〇1)大 氣壓(10,000 ppma),最好不大於約〇 〇〇5大氣壓(5,〇〇〇 ppma), 而在約〇·〇〇2或約〇·〇〇ι大氣壓(2,〇〇〇或i,〇〇〇 ppma)貝彳更佳。 速熱退火步驟除形成晶格空位外,尚導致矽原材中不穩 疋之氣沈積物成核中心分解。此等成核中心會於切割晶圓 之單晶矽錠生成期間形成,或由於晶圓或矽錠以前熱經歷 之其它場合中形成。故衹要此等中心能在速熱退火步驟期 間分解,其是否存在於原始材料中即無關緊要。 速熱退火可於任何商用速熱退火爐中實施,其中諸晶圓 -12- 200305932Male, not) section curve. According to the experimental evidence obtained in item 4, it is best that the environment in the rapid thermal annealing step contains a small amount of pressure of oxygen, water vapor and other oxidizing gases, that is, the environment is free of oxidizing gas or the pressure of these gases, which is not enough to inject Self-filled vacant atoms in silicon that suppress vacancy concentration build-up. Although the lower limit of the oxidizing gas concentration has not yet been determined, it has been shown that the partial pressure of oxygen at atmospheric pressure or parts per million parts per million (ppma) does not increase the vacancy concentration and has no effect. Therefore, the pressure of oxygen or other oxidizing gas contained in the environment should be less than (001) atmospheric pressure (10,000 ppma), preferably not more than about 5,000 atmospheric pressure (5,000 ppma), and about 0 ·· 002 or about 0.0000 atm (2, 000 or 10,000 ppma) is more preferred. In addition to the formation of lattice vacancies in the rapid thermal annealing step, the nucleation centers of unstable radon gas deposits in the silicon raw material also decompose. These nucleation centers may be formed during the generation of single crystal silicon ingots from diced wafers, or other occasions due to previous thermal history of the wafers or silicon ingots. Therefore, as long as these centers can be decomposed during the rapid thermal annealing step, it does not matter whether they exist in the original material. Rapid thermal annealing can be performed in any commercial rapid thermal annealing furnace, including wafers -12- 200305932

(8) 由高功率燈排而個別加熱。速熱退火爐能將石夕晶圓迅速加 熱,例如在數秒鐘内將晶圓自室温加熱至攝氏一千二百 度。此等商用速熱退火爐之一為610型爐,由AG Associate(加 州山景市)產製。(8) Individual heating by high-power lamp bars. The rapid thermal annealing furnace can quickly heat the Shixi wafer, for example, the wafer is heated from room temperature to 1,200 degrees Celsius in a few seconds. One of these commercial rapid thermal annealing furnaces is a Model 610 furnace, manufactured by AG Associate (Mountain View, California).

内在點缺陷(空位及矽自填空位)能經由單晶矽擴散,擴 散速度依溫度而定。故内在點缺陷為内在缺陷擴散率的函 數’且重結合率為溫度的函數。例如,内在點缺陷於晶圓 速熱退火步驟中退火溫度附近移動,而其於攝氏七百度上 在任何商界實用時段大致不移動。目前所獲之實驗證據顯 不在攝氏七百度以下溫度,空位之有效擴散大為減緩,』 即使溫度高至攝氏八百度,九百度或一千度時,亦認為《 位於任何商界實用時段不會移動。 完成步驟S2後,晶圓在步驟\中自晶格空位於單晶矽户 相對T動之溫度範圍迅速冷卻。在晶圓溫度經此溫度範g 下降時,空位擴散至氧化層9而趨於湮滅,從而導致空七 =度斷=中之變化,變化程度依晶圓在範圍内該溫度下a 1長而定。如果晶圓處於此範圍内該溫度下無限長時5 時’晶圓主體11中空位濃度會再度呈大致均句,濃度大! 小於剛完成熱處理步驟時晶格空位濃度之均衡值。不過 位:迅速~卻’可達成晶格空位分佈不均勻。最高3 5方央平面7附近,而空格濃度循前表面3及後表^Intrinsic point defects (vacancies and self-filled vacancies) can diffuse through monocrystalline silicon, and the rate of diffusion depends on the temperature. The intrinsic point defect is therefore a function of the intrinsic defect diffusion rate 'and the recombination rate is a function of temperature. For example, the intrinsic point defect moves near the annealing temperature in the wafer rapid thermal annealing step, and it does not move substantially at any practical time in the business world on Qibaidu. The experimental evidence obtained so far is not at a temperature below seven hundred degrees Celsius, and the effective diffusion of vacancies is greatly slowed down. "Even when the temperature is as high as eight hundred degrees Celsius, nine hundred degrees Celsius or one thousand degrees, it is believed that" it will not move in any practical period of business . After step S2 is completed, the wafer is rapidly cooled from the lattice space in the single crystal silicon relative to the T-movement temperature range in step \. When the temperature of the wafer decreases through this temperature range g, the vacancies diffuse to the oxide layer 9 and tend to annihilate, resulting in a change of vacancy = degree break = medium. The degree of change depends on the length of the wafer a 1 at the temperature within the range. set. If the wafer is in this range, the temperature will be infinitely long at 5 o'clock. The concentration of vacancies in the wafer body 11 will be roughly equal again, and the concentration will be large! It is less than the equilibrium value of the lattice vacancy concentration when the heat treatment step is just completed. But position: quickly ~ but 'can achieve uneven distribution of lattice vacancies. Up to 3 5 near the central plane 7, and the space concentration follows the front surface 3 and the back table ^

3万向遞減。_船而山 L 至少約為每秒攝氏^ 度範圍内之平均冷卻❸ 據裸露區的深度,早广每秒至少約二十度為宜“ X平均冷卻率宜為每秒至少約攝氏五- -13 - (9) 2003059323 million decrease. _Funkershan L is at least about an average cooling in the range of ^ ° C per second. ❸ According to the depth of the exposed area, it is better to have at least about 20 ° C per second. X The average cooling rate should be at least about 5 ° C per second- -13-(9) 200305932

度,最好每秒至少約一百度,就現行若干應用而言,以每 秒約攝氏一百度至二百度為最宜。一旦晶圓冷卻至晶格空 位於單晶矽中相對移動之溫度範圍以外時,則冷卻速度不 太影響晶圓之沈積特性,從而不呈極端重要。就方便古之, 冷部步驟可與加熱步驟在同一環境中實施。 在步驟S4中,晶圓承受氧沈積熱處理。例如,晶圓可在 攝氏八百度下退火四小時,然後在攝氏一千度下退火十六 小時。另外亦宜將晶圓置約攝氏八百度爐内,做為電子裝 置製程的第一步驟。當置入此溫度之爐内日夺,先前速熱退 火之晶圓會有不同氧沈積作用之分隔區。在空位區域(晶 圓主體)中,於晶圓置入爐内後,氧即快速結集。在到達 負載溫度時,結集過程結束且達到結集之分佈,端賴空位 之初始濃度而定。在低空位區域(晶圓表面附近)中,晶圓 用如正#之欠缺先存在之氧沈積成核中心的晶圓;亦 :氧結集並不顯著。當達到攝氏八百度以上時,或若溫度 二持:定,則富於空位區中之結集生成沈積物而耗盡,而 口貧乏中則無任何作用。將晶圓分成各空位濃度區,即 :有效創建-種模板,由之緣出晶圓置人爐内所定之氧圖 如圖1所示,晶圓中氧沈積物之合成深度分佈乃由無氧 二積物材料清除區(裸露區)(15, 15,),自前表面3及後表面 別l伸至冰度(t,t,)予以特化。在無氧沈積物區⑴, )兩者間之區域π含密度大致均勻之氧沈積物。 區域Π中氧沈積物的濃度主要為加熱步驟的函數,次要 -14- 200305932 (ίο) 為冷卻率的函數。總之,氧沈積物濃度隨加熱步驟中温度 上升與退火時間遞增,而以一般所獲每立方公分約至 約5xl〇1Q沈積物範圍之沈積物的密度為準據。 $氧沈積物材料(裸露區)(15,15,)之分別自前與後表面 的冰度(t,主要為晶格空位在矽中相對移動之溫度範圍 ^冷卻率的函t。-般言之,深度(t,t’)隨冷卻率減低而 遞增,而以所獲裸露區深度至少約10,20,30,40,50,70 =一百微米為準。顯然,裸露區的深度大體上與電子裝置 製程無關,且亦與傳統實用之氧的外擴散無關。It is best to use at least about one Baidu per second. For current applications, about one Baidu to two Baidu per second is the most suitable. Once the wafer is cooled to a temperature where the lattice void is outside the relative movement temperature range of the single crystal silicon, the cooling rate does not affect the deposition characteristics of the wafer so much that it is not extremely important. Conveniently, the cold end step can be performed in the same environment as the heating step. In step S4, the wafer is subjected to an oxygen deposition heat treatment. For example, a wafer can be annealed at eight degrees Celsius for four hours, and then annealed at one thousand degrees Celsius for sixteen hours. It is also advisable to place the wafer in a furnace of about 80 degrees Celsius as the first step of the electronic device process. When placed in a furnace at this temperature, the wafers that had previously been rapidly heat-treated will have compartments with different oxygen deposition. In the vacancy area (the body of the wafer), after the wafer is placed in the furnace, the oxygen quickly gathers. When the load temperature is reached, the clustering process ends and the distribution of clusters is reached, depending on the initial concentration of vacancies. In the low vacancy area (near the wafer surface), the wafer is deposited into a nucleation center with oxygen that is absent before the ##; Also: oxygen accumulation is not significant. When it reaches more than eight hundred degrees Celsius, or if the temperature is two: fixed, the accumulation in the vacant area will generate sediment and be depleted, but it will have no effect in poor mouth. Divide the wafer into various vacancy concentration areas, that is, effectively create a kind of template. The oxygen map determined by placing the wafer in the furnace is shown in Figure 1. The synthetic depth distribution of oxygen deposits in the wafer is determined by The area of oxygen dipeptide material removal (exposed areas) (15, 15,) is extended from the front surface 3 and the rear surface to the ice degree (t, t,) for specialization. In the anaerobic sediment zone ⑴, the region π between them contains oxygen deposits having a substantially uniform density. The concentration of oxygen deposits in the region Π is mainly a function of the heating step, and the secondary -14-200305932 (ίο) is a function of the cooling rate. In short, the concentration of oxygen deposits increases with the temperature rise and annealing time during the heating step, and is based on the density of sediments generally obtained in the range of about 5 x 10 1Q per cubic centimeter. $ Oxygen deposit material (exposed area) (15,15,) respectively from the front and back surface ice degrees (t, mainly the temperature range of the relative movement of lattice vacancies in silicon ^ cooling rate function t.-General In other words, the depth (t, t ') increases as the cooling rate decreases, and the depth of the exposed area is at least about 10, 20, 30, 40, 50, 70 = one hundred microns. Obviously, the depth of the exposed area is roughly It has nothing to do with the manufacturing process of the electronic device, and it has nothing to do with the traditional and practical diffusion of oxygen.

It發明方法中所採速熱處理固會導致自晶圓之前後表面 少量氧2外擴散,但外擴散的量遠少於傳統之裸露區形成 法中之量。如此,本發明之理想沈積晶圓具有相當均勻之 真工位氧/辰度,為自矽表面距離之函數。例如,在氧沈積 熱,理之前’日^圓會具有自晶圓中心切表面約十五微米 ::曰圓區域之填空位氧的相當均勻濃度,@以自矽中心至 曰曰圓區域約為矽表面約十微米者較宜,甚且最好自石夕中心 至晶圓諸區域之約石夕表面的約五微米,且以自石夕中心至晶 =域約及三微米者更佳。本文中之相當均句氧濃度係 曰乳’辰度變化不超過約百分之五十,最好不超過百分之二 十,且以不超過百分之十者更宜。 夕=積熱處理通常不會造成大量氧自熱處理之晶圓中向 ^ 口此,裸露區中自晶圓表面數微米距離之填空位 ^ 不έ由於沈積處理而有顯著改變。例如,如果裸 露區包;te Μ 4 又面與自前表面至中央平面所測得之距離 -15- (11) 200305932 二(?少為約十微米)兩者間之晶圓區域時,貝1J自石夕表面等- 於D的一半距離處之裸露區内位置上的氧濃度通常至少- 約為裸露區中任何處填空氧濃度的百分之七十五。就若干 ,沈積熱處理而言’此位置之填空位氧濃度會更高而至裸- 路區任何處最高氧濃度的至少百分之八十五,九十甚至九 十五。 一在本發明之第二具體實例中’採非氮化環境以代替在第 :具體實例之加熱(熱退火)及冷卻步驟中所採用之氮化環籲 境。允宜之非氮化大氣環境包括氬、I、氖,碳化物及其 它此等非氧化非氮化之元素與化合氣體,或此等氣體的混 s物^非氮化環;t兄亦似氮化環境,可含小部分氧壓,亦即 部分壓力小於0·01大氣壓(10,⑻〇 ppma),而以小於0·005大氣 壓(5,000 Ppma)為宜 ’ * 於 〇 〇〇2 或 〇 〇〇1 大氣壓(2 〇〇〇/1,麵 ppma)更佳° 在本發明之第三具體實例巾,省略去步驟(s)(熱氧化步 驟),故起始晶圓僅具固有氧化層。然而當此一晶圓於I 籲 % i兄中退火日守’其效應即異於具有比固有氧化層更厚氧化 層(增大的氧化層)之晶圓於氮中退火時所見者。當含增大 氧化層之晶圓在氮環境中退火時,幾乎在到達退火溫度 时即元成大致均勻之空位農度增加。此外,空位濃度並 不以一定退火溫度上退火時的函數方式而呈現顯著增加。 不過若晶圓缺少大於固有之氧化層,且若晶圓之前後表面 於氮中退火%,則所獲得之晶圓,其空位濃度(數量密度) 曲線會略呈”U”形之橫切面,亦即,最大濃度在前後表面—一 -16- (12) 200305932 :=之内,相當恆定且較小濃度在晶圓全體,最小濃度 产=n #始約等於具增大氧化層晶圓中所獲得之濃 ::匕其缺少大於固有氧化層之晶圓中1火時間 導致空位濃度的增加。 ^驗證據進—步顯示此種不具大於固有氧化層之晶圓及 曰聽層晶圓,兩者作用之差異可由於環境中含分子氧 或另:氧化氣體而得以避免。茲舉另一方於不具大於 固有氧化層之晶圓在含小部分氧壓之氮環境中退火時,晶 圓作用與具增大氧化層晶圓之作用相同。不拘泥於任何原 厚度大於固有氧化層之外表氧化層肖做抑制石夕氮化之 屏蔽。故此一氧化層可能存在於原始晶κ,或於退火步驟 期間產生增大氧化層而形成之。 因此,依據本發明,速熱退火步驟期間,大氣環境宜含 至少約0.0001大氣壓(100 ppma)之分壓力,而以至少約〇⑻⑽ 大氣壓(200 ppma)則更佳。不過,就前述諸原因言之,氧 的分壓力不宜超過0·01大氣壓(10,000 ppma),而以小於〇 〇〇5 大氣壓(5,000 ppma)較好,且0·002或〇 〇〇1大氣壓(2,〇⑼ ppma/l,000 ppma)者更佳。 在本發明之其它具體實例中,晶圓之前與後表面可暴露 於不同之環境中,各含一或多種氮化或非氮化氣體。例如, 晶圓之後表面可暴露於氮化環境而前表面暴露於非氣化環 境中。另外,多個(2,3或更多晶圓)可面對面疊置而同時 退火;以此方式退火時,面對面接觸之諸面於退火期間機 械性地防護環境影響。此外,依據速熱退火期間所採用之 -17- (13) 200305932The rapid heat treatment method used in the It invention method will cause a small amount of oxygen 2 to diffuse from the front and back surfaces of the wafer, but the amount of external diffusion is far less than that in the traditional method of forming exposed regions. As such, the ideal deposited wafer of the present invention has a fairly uniform true station oxygen / degree, as a function of distance from the silicon surface. For example, before the heat of oxygen deposition, the "Japanese yen" would have a fairly uniform concentration of oxygen in the vacancies of the cut-off area of about 15 microns from the center of the wafer: It is more suitable for the silicon surface to be about 10 microns, and it is even better to be about 5 microns from the center of Shixi to the surface of the wafer, and about 5 microns from the center of Shixi to the crystal = domain and about 3 microns. . The equivalent oxygen concentration in this article is that the change in the degree of milk is not more than about 50%, preferably not more than 20%, and more preferably not more than 10%. Evening = accumulated heat treatment usually does not cause a large amount of oxygen self-heating wafers. In the exposed area, the filling space of a few micrometers from the wafer surface ^ does not change significantly due to the deposition process. For example, if the exposed area package; te Μ 4 and the wafer area measured from the front surface to the center plane -15- (11) 200305932 two (? At least about ten microns) wafer area, bei 1J From the surface of Shi Xi, etc.-the oxygen concentration at the location of the exposed area at half the distance of D is usually at least-about 75% of the oxygen concentration of the empty space anywhere in the exposed area. For a number of deposition heat treatments, the oxygen concentration in the vacancies at this location will be higher to at least 85 percent, 90, or even 95 percent of the highest oxygen concentration anywhere in the bare-road area. -In the second embodiment of the present invention, a non-nitriding environment is used instead of the nitriding ring environment used in the heating (thermal annealing) and cooling steps of the first embodiment. Permissible non-nitriding atmospheric environments include argon, I, neon, carbides, and other non-oxidizing non-nitriding elements and compound gases, or mixtures of these gases ^ non-nitriding rings; the same is true for brothers Nitriding environment may contain a small part of the oxygen pressure, that is, part of the pressure is less than 0. 01 atmosphere (10, 00 ppma), and preferably less than 0. 005 atmosphere (5,000 Ppma) '* * 002 or 〇 〇 atmospheric pressure (2000/1, surface ppma) is better ° In the third embodiment of the present invention, step (s) (thermal oxidation step) is omitted, so the starting wafer only has an inherent oxide layer . However, when this wafer is annealed in Japan, the effect is different from that seen when a wafer with a thicker oxide layer (increased oxide layer) than the intrinsic oxide layer is annealed in nitrogen. When wafers with an increased oxide layer are annealed in a nitrogen environment, when the annealing temperature is reached, the element yield becomes substantially uniform. In addition, the vacancy concentration does not increase significantly as a function of annealing at a certain annealing temperature. However, if the wafer lacks an oxide layer larger than that inherent, and if the wafer's front and back surfaces are annealed in nitrogen, the vacancy concentration (quantity density) curve of the obtained wafer will have a slightly “U” -shaped cross section. That is, the maximum concentration is within the front and rear surfaces—a -16- (12) 200305932: =, which is fairly constant and small in the entire wafer. The minimum concentration is equal to n. The obtained concentration :: the lack of a fire time in the wafer with an intrinsic oxide layer leads to an increase in the vacancy concentration. ^ Validation evidence—It is further shown that such wafers that do not have an oxide layer larger than the intrinsic layer and the listening layer wafer, the difference between the two functions can be avoided due to the presence of molecular oxygen or another: oxidizing gas in the environment. Here is another example. When a wafer not having an intrinsic oxide layer is annealed in a nitrogen environment containing a small amount of oxygen pressure, the effect of crystal circle is the same as that of a wafer with an increased oxide layer. It is not restricted to any original oxide layer with a thickness greater than that of the intrinsic oxide layer. Therefore, an oxide layer may exist in the original crystal κ, or may be formed during the annealing step by increasing the oxide layer. Therefore, according to the present invention, during the rapid thermal annealing step, the atmospheric environment preferably contains a partial pressure of at least about 0.0001 atmospheres (100 ppma), and more preferably at least about 0 to atmospheric pressure (200 ppma). However, for the reasons mentioned above, the partial pressure of oxygen should not exceed 0.01 atmospheres (10,000 ppma), but preferably less than 5,000 atmospheres (5,000 ppma), and 002 or 0.001 atmospheres ( 2,000 ppma / 1,000 ppma). In other embodiments of the invention, the front and back surfaces of the wafer may be exposed to different environments, each containing one or more nitrided or non-nitrided gases. For example, the rear surface of the wafer may be exposed to a nitriding environment and the front surface may be exposed to a non-gasifying environment. In addition, multiple (2, 3, or more wafers) can be stacked face-to-face and annealed simultaneously; when annealing in this way, the faces that are in face-to-face contact are mechanically protected from environmental influences during annealing. In addition, according to -17- (13) 200305932 used during rapid thermal annealing

ί:,及所期晶圓的氧濃度斷面,氧化層可僅於晶圓所欲裸 心區的面上形成,例如晶圓的前表面(3)(參見圖1)。 本發明方法所用之原始材料可為一種拋光之矽晶圓,或 屬研磨並㈣之晶圓而未經拋光者。此外,晶圓可具空位 或自/、工位點缺做為主要内在點缺陷。例如,晶圓可自 中心至邊緣屬空位或自填空位佔#,或其含有一空位為主 材料之中央核心圍、繞以自填空位為主之材料的車由向對稱環ί: And the oxygen concentration profile of the desired wafer, the oxide layer can be formed only on the surface of the desired bare core region of the wafer, such as the front surface of the wafer (3) (see Figure 1). The raw material used in the method of the present invention may be a polished silicon wafer, or a polished and polished wafer without polishing. In addition, wafers can have vacancies or lack of work sites as the main intrinsic point defects. For example, the wafer can be empty or self-filled from the center to the edge, or it can contain a central core of a material that is the main material, and a self-centering symmetrical ring around the material that is mainly self-filled.

若要將外延附生層澱積於理想沈積晶圓上,則本發明之 =法可於外延附生澱積之前或其後實施。若在其前實施 蚪,則宜於本發明方法後及外延附生澱積前,以熱退火法 ,疋B曰圓中氧沈積物成核中心。不過,熱退火法歷時頗長 (在約攝氏八百度需約四小時,隨之於約攝氏一千度需約 十小日守)’既降低生產量且令晶圓製造成本大大增高。準 此,本發明之方法可於外延附生澱積後實施,但如此仍需 另增處理步驟,並增高製造成本。 另外,氧沈積物成核中心可用矽晶的氮摻雜加以穩定(參 見F· Shinmra等之應用物理48(3)第224頁(1986)。其中揭示氮 払雜之μ體的氧沈積核高達約攝氏一千二百五十度時仍呈 L疋。依據本發明,矽晶中氮的濃度須嚴加控制以實現穩 疋之利,同時保持形成裸露區的能力。若氮的濃度太低時 (低於母立方公分原子)(約〇⑻⑼2 ppma),即無法實現 知疋效應。另一方面,若氮的濃度太高(高於約每立方公 刀IxlO15原子)(約〇.02 ppma),則晶體生成期間所形成之氧 -18 - 200305932 (14) R咖績貢’ 沈積成核中心於步驟&中不會分解。同時,若矽晶含太多 氮,則在晶圓中會形成氧化引起累積瑕疵(〇ISF),其對外 延附生晶圓的品質有不良影響(參見日本專利局公告第 1999-189493號)。矽晶圓表面上之氧化引起累積瑕疵與其它 空位式缺陷不同,未為外延附生矽層之澱積所掩蓋。〇isf 持續於外延附生層中生成而導致通常稱為外延附生累積瑕 疫之内生成缺陷。外延附生累積瑕疲之最大橫切面寬度, 以現有探測極限之雷射自動觀察裝置測之,其範圍自約〇1 微米至約10微米以上。故依據本發明,石夕晶體宜含之氮推 雜劑原子濃度約為每立方公分1><1()12至5x1q14原子(Μ卯邮) ’而以約每立方公分lx,至1χ1〇13原子(約咖2 ppma)更 、 ^ 7W別胂虱軋介入生成室 及/或將氮添加至聚合石夕炼化物笠 旦山、、;丄> /峪化物寻。加至生成中晶體之氮If an epitaxial epitaxial layer is to be deposited on an ideal deposition wafer, the method of the present invention can be implemented before or after epitaxial epitaxial deposition. If thorium is carried out before it, it is suitable to use a thermal annealing method after the method of the present invention and before epitaxial epideposition, to describe the nucleation center of oxygen deposits in the circle. However, the thermal annealing method takes a long time (it takes about four hours at about eight degrees Celsius, followed by about ten hours at about one thousand degrees Celsius) 'not only reduces the production volume, but also significantly increases the wafer manufacturing cost. In this way, the method of the present invention can be implemented after epitaxial deposition, but this still requires additional processing steps and increases manufacturing costs. In addition, the nucleation center of oxygen deposits can be stabilized by nitrogen doping of silicon crystals (see Applied Physics of F. Shinmra et al. 48 (3), p. 224 (1986). It is revealed that the oxygen-deposited nuclei of nitrogen-doped μ bodies are It is still L 疋 at about 1,250 degrees Celsius. According to the present invention, the concentration of nitrogen in the silicon crystal must be strictly controlled to achieve stable benefits while maintaining the ability to form exposed areas. If the concentration of nitrogen is too low Time (below the parent cubic centimeter atom) (about 0.2 ppma), the cognitive effect cannot be achieved. On the other hand, if the nitrogen concentration is too high (above about IxlO15 atoms per cubic centimeter) (about 0.02 ppma) ), Then the oxygen formed during the crystal formation-18-200305932 (14) R Kaji Gong 'deposition and nucleation center will not decompose in step & At the same time, if the silicon crystal contains too much nitrogen, it will be in the wafer It will form accumulated defects caused by oxidation (〇ISF), which adversely affects the quality of epitaxial epitaxial wafers (see Japanese Patent Office Publication No. 1999-189493). Oxidation on the surface of silicon wafers causes accumulated defects and other vacancies The defects are different and are not covered by the deposition of epitaxial epitaxial silicon layer 〇isf continues to form in epitaxial epigenetic layers, resulting in internally generated defects commonly referred to as epitaxial epiphyseal accumulated defects. The maximum cross-sectional width of epitaxial epiphysial accumulated defects is measured by laser automatic observation devices with existing detection limits. In other words, the range is from about 0.01 micrometers to about 10 micrometers or more. Therefore, according to the present invention, the nitrogen dopant atom concentration suitable for Shi Xi crystals is about 1 > < 1 () 12 to 5x1q14 atoms (M)卯 mail) 'and about 1x per cubic centimeter to 1x1013 atoms (approximately 2 ppma) more, ^ 7W Do not tick the intervening generation room and / or add nitrogen to the polymer stone Xihua refining compound Dandan Mountain, ,; 丄 >

里由、、加鼠至聚合碎溶化物 τήζ JL M /合亿物更精確加以控制,即屬較佳方 法。尤其加至晶體的氮量迅予 里、卞决疋,例如,於既知直徑之 石夕晶圓上澱積既知厚度之 ^ 虱化物(Sl3N4)層,其於形成矽 炼化物之丽納入具聚矽之坩 方公分318克。 _内者⑸3N4)之密度約為每立 依據本發明,氧沈積物 氣共同摻雜以獲稃定。… 用叙以代替虱,或碳 叙中碳的濃度宜在約每立方公分 原子(0.2Ppma)至約4χ1〇17原子(8ppma)之間。 無關特定原理,H命古刃&知 t ^ ^ ^ , W為氮/碳摻雜原子以阻滯矽晶體 中空位的擴散而熱釋定負 /日日體 t疋氣/尤積核心。尤其,已知當生成中 -19- (15) 200305932It is the better method to control the lysate τήζ JL M / heyiwu from the li, zi, and rat to the polymerized lysate. In particular, the amount of nitrogen added to the crystal is rapid, for example, a known thickness ^ lice compound (Sl3N4) layer is deposited on a stone wafer with a known diameter, and it is incorporated into the polysilicon compound. The crucible of silicon is 318 grams. The density of the inner ⑸3N4) is approximately per cubic liter. According to the present invention, the oxygen deposit gas is co-doped to obtain a predetermined value. … Replace lice with carbon, or the concentration of carbon in carbon should be between about 0.2 Ppma to about 4 × 1017 atoms (8 ppma). Irrespective of a specific principle, H is known as t ^ ^ ^, where W is a nitrogen / carbon doped atom to block the diffusion of vacancies in the silicon crystal and pyrolyze the negative / sun-day body t 疋 gas / youji core. In particular, it is known that when generating -19- (15) 200305932

晶體冷卻時,空位濃度達到臨界超飽和位準(即在此點上 產生凝聚)’而導致形成凝聚之空位缺陷或微空白。例如’ 凝聚會在約攝氏115〇_1〇5〇度發纟。晶體冷卻日寺,由於空位 繼續擴散至諸部位,故微空白增大。雖然凝聚作用及持續 生成微空白於繼續冷卻時大大減低晶體中之非凝聚或自由 空位,而在繼續冷卻時,達到臨界超飽和之第二位準,其 中晶體内之自由空位和氧相互作用而形成氧沈積核心。就 非氮與碳所摻雜的晶體而言,臨界超飽和的第二位準乃於 晶體冷卻至約攝氏七百度時發生。在氮/碳摻雜之石夕晶中, 於减承作用期間之空白形成,由於空位擴散率減慢而稍受 抑制。如此即導致在第一凝聚作用後,留存於晶體中之空 位濃度更高。氮/碳摻雜之矽中所增加之自由空位濃度亦 增高了晶體超飽和第二位準發生之溫度,例如於約攝氏八 百度至約-千零五十度。在此增高之溫度上,曰曰 子更活躍,更多氧原子與自由'' T T /、曰田工位作用而使氧之沈積核心 更趨敎。穩定之氧沈積核心,在後續之熱處理諸如生成 外延矽層等期間,更能阻滯分解。 依據本發明以氮/碳摻雜的氧濃度核心之穩定亦可併入 於絕緣體上以離子植人而產切的方法t,離子植入呈有 内在吸收能力而非細年6月22日提出之美國申請案第 6〇/300’2()8號所揭示之熱穩定法’或與之合併行之,兹錄於 此以供參考。 第 依據本發明以氮/碳摻雜的氧濃度核心之穩定亦可併入 6,236,刚號美國專利案所&之於絕緣體上產生石夕的方 -20- (16) (16)200305932When the crystal is cooled, the vacancy concentration reaches the critical supersaturation level (that is, agglomeration occurs at this point) ', which leads to the formation of vacancy defects or micro-blanks in the agglomeration. For example, ’agglomeration will burst at approximately 1150-1050 ° C. As the crystals cooled, the micro-blank increased because the vacancies continued to spread to various parts. Although the coacervation and the continuous generation of micro-blanks greatly reduce the non-cohesion or free vacancies in the crystal when it continues to cool, and when it continues to cool, it reaches the second level of critical supersaturation, in which free vacancies in the crystal interact with oxygen and An oxygen deposition core is formed. For non-nitrogen and carbon doped crystals, the second level of critical supersaturation occurs when the crystals are cooled to about seven hundred degrees Celsius. In the nitrogen / carbon-doped stone evening crystal, the gaps formed during the load-reduction period are slightly suppressed due to the slowing of the vacancy diffusion rate. This results in a higher concentration of vacancies remaining in the crystal after the first agglomeration. The increased free vacancy concentration in the nitrogen / carbon-doped silicon also increases the temperature at which crystal supersaturation occurs at the second level, for example, at about 8 degrees Celsius to about -5050 degrees Celsius. At this increased temperature, the oxygen is more active, and more oxygen atoms and free '' T T /, said the role of the field site to make the oxygen deposition core tends to be more rampant. The stable oxygen deposition core can further retard the decomposition during the subsequent heat treatment, such as the formation of an epitaxial silicon layer. According to the present invention, the stability of the oxygen concentration core doped with nitrogen / carbon can also be incorporated into the insulator to produce a cut by implanting ions into the human body. The ion implantation has an intrinsic absorption capacity instead of being proposed on June 22 The Thermal Stability Act disclosed in US Application No. 60 / 300'2 () 8 'or incorporated with it is hereby incorporated by reference. According to the present invention, the stability of the core of oxygen concentration doped with nitrogen / carbon can also be incorporated into 6,236, U.S. Patent & Law & the method of producing stone eves on insulators -20- (16) (16) 200305932

法中,茲錄於此以供參考。 單晶矽中晶格空位之測量可以鉑擴散分析法實施。一般 言之,於允宜選定之擴散時程與溫度上將鉑澱積於樣品上 並於水平表面擴散,而使Frank-Turnbull機制支配翻之擴散, 但其充分達到鉑擴散所飾空位的穩定狀態。就具有本發明 典型空位濃度之晶圓而言,可採攝氏七百三十度及二十分 鐘之擴散,於較低溫度上,例如約攝氏六百八十度,顯示 可獲更精確執跡。此外,為將矽化過程之可能影響減至最 低,鉑澱積法最好少於一單層之表面濃度。鉑擴散技術在 其它著述中亦有闡釋,例如:Jacob等所著J. Appl· Phvs··第82 卷第 182 頁(1997) ; J. Electrochemical Society 第 139 卷第 256 頁 (1992) ,Zimmermann及Ryssel所著:”於不均衝狀況下石夕中 溶化翻的擴散π ; Journal of Crystal Growth第129卷第582頁 (1993) ,Zimmermann,Goesele,Seilenthal 及 Eichiner 等所著’’ 矽之空位濃度晶圓製圖’’ ;Appl. Phvs. Lett第60卷第3250頁 (1992),Zimmermann及Falster所著π初階段切克勞斯基石夕中 氧沈積物成核的研究π ;以及Appl. Phvs. A.第55卷第121頁 (1992),Zimmermann及 Ryssel 之著作等。 圖式簡單說明 圖1為本發明方法的簡圖。 -21 -It is hereby recorded for reference. The measurement of lattice vacancies in single crystal silicon can be performed by platinum diffusion analysis. Generally speaking, at the diffusion time and temperature selected by Yunyi, platinum was deposited on the sample and diffused on the horizontal surface, so that the Frank-Turnbull mechanism dominated the diffusion, but it fully achieved the stability of the vacancy decorated by platinum diffusion. status. For wafers with the typical vacancy concentration of the present invention, diffusion at 730 degrees Celsius and 20 minutes can be taken. At lower temperatures, such as about 680 degrees Celsius, a more accurate track can be obtained. . In addition, to minimize the possible effects of the silicidation process, the platinum deposition method is preferably less than the surface concentration of a single layer. Platinum diffusion technology has also been explained in other works, for example: Jacob et al., J. Appl. Phvs., Vol. 82, p. 182 (1997); J. Electrochemical Society, Vol. 139, p. 256 (1992), Zimmermann and Ryssel: "Diffusion of Melt Dissolve in Shi Xi under Uneven Distribution; Journal of Crystal Growth, Vol. 129, p. 582 (1993), Zimmermann, Goesele, Seilenthal and Eichiner, etc." Vacancy Concentration of Silicon Wafer Mapping ''; Appl. Phvs. Lett, Vol. 60, p. 3250 (1992), Zimmermann and Falster, π Study on the Nucleation of Oxygen Sediments in the Initial Stages of the Cekrauski Stone; π; and Appl. Phvs. A. Vol. 55, p. 121 (1992), works by Zimmermann and Ryssel, etc. Brief description of the drawings Figure 1 is a simplified diagram of the method of the present invention. -21-

Claims (1)

200305932 拾、申請專利範圍 l二種具有兩主要且大致平行表面之單晶石夕晶圓,其中之 -表面為晶圓之前表面’另—為晶圓之後表面,在前與 後兩表面之間有—中央平面,-周緣結合前後表面,表 面層包括前表面與自前表面至中央平面所測量之至少約 十微米距離(D)間之晶圓區域,以及主體層包括中央平 面^第區域間之晶圓第二區域,該晶圓之特徵在於: 邊晶圓具有氧沈積物成核中心不均勻之分佈,以主體 層中氧沈積物成核中心之濃度大於表面層中氧沈積物成 核中心之濃度,氧沈積物成核中心具濃度曲線,其中氧 沈積物成核中心之峯值密度在中央平面處或其附近,濃 度自峯值密度位置循晶圓前表面方向遞減,以及 晶圓含有選自氮、碳及其混合物之摻雜劑,採用氮推 雜劑時,氮之濃度約在每立方公分1χ1〇12原子與約5χΐ〇ΐ4 原子之間,而碳的濃度約在每立方公外⑻1 2 3 4 5 6 7 8與約4χΐ〇ΐ7 原子之間。 1 _如申請專利範圍第1項之晶圓,其中氮的滚度約為每立 2 方公分lxl〇12原子至約lxl〇u原子。 3 3. 如申請專利範圍第旧之晶圓,其中〇至少為約2〇微米。 4 4. 如申請專利範圍第旧之晶圓,其中〇至少為約%微米。 5 5. 如申„月專利犯圍第】項之晶圓,其中d約在%與約⑽微 6 米之間。 7 6. 如申請專利範圍第旧之晶圓,其中晶圓尚含晶圓表面 8 上之外延附生層。 200305932 [mmmf 7. -種用以製備具控制性氧沈積作用之單晶矽晶圓之方 法,此方法包含·· 乂選定自切克勞斯基法而生成單晶料所切割,且含一 前::和後表面及前後表面間中央平面之晶圓,此晶圓 :二表面層、主體層及摻雜劑,前表面層包括前表面 區别表面至中央平面所測量之距離(D)兩者間的晶圓 而二’主體層包括中央平面與前表面層間的晶圓區域, 而自含氮與碳的組群,當推雜劑為氮時,氮漠 母立方公分lxl〇12原子至約域"原子,而若換雜 :丨“時’碳漠度約為每立方公分1χ1〇16至約—原 將晶圓加熱至少至的摄& , t ϊίϊ: 舻“ 攝氏,Μ度,以於前表面層及主 體層中形成晶格空位; 之r=t晶圓於一速率上冷卻以形成晶圓中空位濃度 :線圖,空位之峯值密度在主體層中,濃度自峯 盾晶圓前表面方向大致遞減,前表面層與主體 2^中空位濃度之差異致使前表面層中並無氧沈積物 二形成,而於主體層中形成氧沈積物成核中心; 中二晶=中,在主體層内形成穩定之氧沈積物成核 *位之=定之氧沈積物成核中心之濃度主要依 二位之濃度而定。 8·"請專利範圍第7項之方法,其 1,Π5度以上。 …、芏、、0攝民 9·如申請專利範圍第7項之方法’其中晶圓加熱至約攝氏 200305932 申#專利輕固續頁 一; 二 1,200度以上。 10·如申請專利範圍第7項之方法,其中晶圓加熱至約攝氏 1,200度與約UK度之間。 11.如申請專利範圍第7項之方法,其中晶圓加熱時暴露於 一種大氣環境,此環境含選自氬、氦、氖、二氧化碳及 氮或含氮氣體等組成之一或多種氣體之組群。 12·如申請專利範圍第11項之方法,其中大氣環境含氬。 13. 如申請專利範圍第丨丨項之方法,其中大氣環境含氮或含 氮之氣體。 14. 如申請專利範圍第丨丨項之方法,其中大氣環境含氬及氮 或含氮的氣體。 15. 如申請專利範圍第丨丨項之方法,其中大氣環境中含有不 大於約0.01大氣壓的氧分壓。 16·如申請專利範圍第丨丨項之方法,其中大氣環境中含有不 大於約0.005大氣壓的氧分壓。 17_如申請專利範圍第丨丨項之方法,其中大氣環境中含有不 大於約0.002大氣壓的氧分壓。 18.如申请專利範圍第11項之方法,其中大氣環境中含有不 大於約0.001大氣壓的氧分壓。 19·如申請專利範圍第11項之方法,其中大氣環境中含有之 氧分壓在約0.0001與約0.01大氣壓之間。 2〇·如申請專利範圍第11項之方法,其中大氣環境中含有之 氧分壓在約0.0002與約0.001大氣壓之間。 21.如申請專利範圍第7項之方法,其中在晶圓加熱至少至 200305932 L------------------- 約攝氏l,l5〇度以於义 、, X M於則表面層及主體層中形成晶袼空位 之前,晶圓加教5小π从 士 …、至^至約攝氏700度以形成一表面之氧 化碎層,可做為曰 為日日格空位的散熱器。 22·如申請專利蔚 , 圍第7項之方法,其中晶圓於晶格空位在 、、移動之度範圍内冷卻的速率至少約為每秒攝 氏5度。 23·如申請專利範 石夕中相對移動 氏20度。 圍第7項之方法,其中晶圓於晶袼空位在 之’里度範圍内冷卻的速率至少約為每秒攝 24·如申請專利範 石夕中相對移動 氏50度。 圍第7項之方法,其中晶圓於晶格空4 之溫度範圍内冷卻的速率至少約為每琴 其中晶圓於晶格空位在 的速率至少約為每秒攝200305932 Patent application scope 1. Two types of single crystal wafers with two main and approximately parallel surfaces, where-the surface is the front surface of the wafer and the other-the rear surface of the wafer, between the front and back surfaces There is-the central plane,-the peripheral edge combines the front and rear surfaces, the surface layer includes a wafer region between the front surface and a distance (D) of at least about ten microns measured from the front surface to the central plane, and the body layer includes the central plane The second region of the wafer, the wafer is characterized in that: the side wafer has an uneven distribution of nucleation centers of oxygen deposits, and the concentration of the nucleation centers of oxygen deposits in the main layer is greater than that of the nucleation centers of oxygen deposits in the surface layer The concentration of the oxygen deposition nucleation center has a concentration curve, in which the peak density of the oxygen deposition nucleation center is at or near the central plane, the concentration decreases from the peak density position along the front surface of the wafer, and the wafer contains a selected Dopants of nitrogen, carbon, and mixtures thereof. When nitrogen dopants are used, the concentration of nitrogen is between about 1 × 1012 atoms and about 5 × ΐ〇ΐ4 atoms per cubic centimeter. Per cubic approximately between an outer well ⑻1 2 3 4 5 6 7 8 and about 4χΐ〇ΐ7 atoms. 1 _ As for the wafer of item 1 of the scope of patent application, the roll of nitrogen is about 1 × 10 12 atoms to about 1 × 10u atoms per cubic centimeter. 3 3. If the oldest wafer in the scope of patent application, 0 is at least about 20 microns. 4 4. If the oldest wafer in the scope of patent application, 0 is at least about% microns. 5 5. If you apply for a wafer of “Monthly Patent Offense”, d is between about% and about 6 meters. 7 6. If you apply for the oldest wafer in the patent scope, the wafer still contains crystals. An epitaxial epitaxial layer on a round surface 8. 200305932 [mmmf 7.-A method for preparing single crystal silicon wafers with controlled oxygen deposition, this method includes ... The wafer cut by the single crystal material and containing a front plane: and a central plane between the rear surface and the front and rear surfaces. This wafer includes two surface layers, a main body layer and a dopant, and the front surface layer includes a front surface distinguishing surface. The distance between the measured plane (D) to the center plane of the wafer and the two 'body layer includes the wafer area between the center plane and the front surface layer, and from the group containing nitrogen and carbon, when the dopant is nitrogen , The nitrogen desert mother cubic cm lxl012 atoms to about the field " atoms, and if you change the impurity: 丨 "carbon desert degree is about 1x1016 to about cubic meters-the original heating of the wafer at least ; t ϊίϊ: 舻 "Celsius, M degrees, to form lattice vacancies in the front surface layer and the main layer; r = t Wafer is cooled at a rate to form the concentration of vacancies in the wafer: line graph, the peak density of vacancies is in the main body layer, and the concentration is roughly decreased from the front surface direction of the peak shield wafer, and the front surface layer and the main body 2 ^ The difference in the vacancy concentration caused no oxygen deposit II to form in the front surface layer, and an oxygen deposit nucleation center was formed in the host layer; Medium two crystals = medium, which forms a stable oxygen deposit nucleation * site in the host layer The concentration of the nucleation center of the fixed oxygen sediment mainly depends on the concentration of the second place. 8 · " The method of the seventh item in the patent scope, which is above 1, Π5 degrees. For example, the method of applying for the scope of the patent No. 7 'in which the wafer is heated to about Celsius 200305932 Application # Patent light solid continuation page 1; 2, 1,200 degrees or more. 10. According to the method of the scope of the patent applying No. 7 in which the wafer is heated To about 1,200 degrees Celsius and about UK degrees. 11. The method according to item 7 of the scope of patent application, wherein the wafer is exposed to an atmospheric environment when heated, and this environment contains a material selected from the group consisting of argon, helium, neon, carbon dioxide and One or more of nitrogen or nitrogen-containing gas Groups of gases. 12. If the method in the scope of patent application No. 11 where the atmospheric environment contains argon. 13. If the method in the scope of patent application No. 丨 丨, where the atmospheric environment contains nitrogen or nitrogen-containing gas. 14. Such as The method according to the scope of the patent application, wherein the atmospheric environment contains argon and nitrogen or a gas containing nitrogen. 15. The method according to the scope of the patent application, wherein the atmospheric environment contains an oxygen partial pressure not greater than about 0.01 atmospheres 16. The method according to item 丨 丨 of the scope of patent application, wherein the atmospheric environment contains an oxygen partial pressure of not more than about 0.005 atm. 17_ The method according to item 丨 丨 of the scope of patent application, wherein the atmospheric environment contains no more than approximately Partial oxygen pressure of 0.002 atm. 18. The method according to claim 11 in which the atmospheric environment contains an oxygen partial pressure of not more than about 0.001 atmospheres. 19. The method according to item 11 of the application, wherein the partial pressure of oxygen contained in the atmospheric environment is between about 0.0001 and about 0.01 atmospheres. 20. The method according to claim 11 in which the partial pressure of oxygen contained in the atmospheric environment is between about 0.0002 and about 0.001 atmospheres. 21. The method according to item 7 of the scope of patent application, wherein the wafer is heated to at least 200305932 L ------------------- about 1,50 degrees Celsius is in the right sense Before XM forms crystal vacancies in the surface layer and the main layer, the wafer is taught to add 5 small π from ± ... to about 700 degrees Celsius to form a surface oxide fragment, which can be referred to as the day Radiator in vacancy. 22. If applying for a patent, the method around item 7, wherein the wafer is cooled at a rate of at least about 5 degrees Celsius per second in the lattice vacancies within a range of degrees of movement. 23. If applying for a patent, Shi Xizhong's relative movement is 20 degrees. The method around item 7, wherein the wafer is cooled at a rate of at least about one second within the vacancy of the crystallite. 24. Such as the patent application Fan Shi Xizhong, the relative movement is 50 degrees. The method around item 7, wherein the cooling rate of the wafer in the temperature range of the lattice space 4 is at least about per second, and the rate of the wafers in the lattice space is at least about 1 second. 25·如申請專利範圍第7項之方法, 石夕中相對移動之溫度範圍内冷部 氏100度。 ’包含主體層中穩定之氧 至二於晶圓的一表面上澱 26·如申請專利範圍第7項之方法 沈積物成核中心已形成之後, 積一外延附生層。25. If the method in the scope of patent application No. 7 is applied, the cold part in the temperature range of Shi Xizhong's relative movement is 100 degrees. ′ Contains stable oxygen in the main layer. It is deposited on one surface of the wafer. 26. The method according to item 7 of the patent application. After the nucleation center of the deposit has been formed, an epitaxial epitaxial layer is deposited.
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